Local Pharmacokinetics and Pharmacodynamics of Angiogenic Growth Factors in Myocardial Tissue by MASSACHUSETTS INSTlJTE Kha N. Le SEP 17 2009 OF TECHNOLOGY B.S., Bioengineering, University of California, San Diego MIT S.M., Electrical Engineering and Computer Science, __. LIBRARIES SUBMITTED TO THE HARVARD-MIT DIVISION OF HEALTH SCIENCES AND TECHNOLOGY IN PARTIAL FULFILLMENT OF THE REQUIREMENTS FOR THE DEGREE OF DOCTOR OF PHILOSOPHY IN ELECTRICAL AND MEDICAL ENGINEERING AT THE MASSACHUSETTS INSTITUTE OF TECHNOLOGY FEBRUARY 2009 © 2009 Kha N. Le. All rights reserved. ARCHIVES The author hereby grants to MIT permission to reproduce and to distribute publicly paper and electronic copies of this thesis document in whole or in part in any medium now known or hereafter created Signature of Author: Division of Health Sciences and Technology February 09, 2009 Certified by: Elazer R. Edelman, M.D., Ph.D. (I Thomas D. and Virginia W. Cabot Professor of Health Sciences and Technology Thesis Supervisor 4ZZZ_7___ Accepted by: Ram Sasisekharan, Ph.D. Director, Harvard-MIT Division of Health Sciences and Technology of Health Sciences & Technology and Biological Engineering Professor Edward Hood Taplin Local Pharmacokinetics and Pharmacodynamics of Angiogenic Growth Factors in Myocardial Tissue By Kha N. Le Submitted to the Harvard-MIT Division of Health Sciences and Technology on February 10, 2009 in Partial Fulfillment of the Requirements for the Degree of Doctor of Philosophy In Electrical and Medical Engineering Abstract Early enthusiasm over angiogenic therapy, a method to induce vascular regeneration to treat ischemic tissue with growth factors, has been tempered by a series of unsuccessful clinical trials with limited late efficacy and a wide range of mixed results. This thesis was designed to examine critically whether the lack of late efficacy of local delivery of angiogenic factors could be explained by a comprehensive understanding of local pharmacokinetics (PK) and pharmacodynamics (PD) in the myocardial tissue. Our central hypothesis is that early success at inducing vessel growth powerfully self-regulates angiogenic therapies by dynamically altering local tissue pharmacokinetic properties and hinders long-term efficacy. We used a multipronged approach to investigate this hypothesis. We characterized the baseline local myocardial PK through a series of ex-vivo isolated heart studies and mathematical analysis, examined the local coupling of PK and PD with an in-vivo ischemic heart model, created a computational model of myocardial PK and PD to predict distribution of growth factors and their biologic effects, discussed implications and future studies. Our findings suggest that microvascular washout impedes myocardial drug transport, early angiogenic response further exacerbates drug washout and is likely responsible for late vessel regression, modulating drug PK properties to mitigate drug clearance through washout can enhance late tissue response. These results imply that local PK-PD interdependence should be carefully examined to improve clinical efficacy of angiogenic therapy with local angiogenic growth factor delivery. Thesis Committee: Prof. Elazer R. Edelman (Thesis Supervisor) Prof. Matthew Nugent Prof. Collin Stultz (Committee Chair) Prof. K. Dane Wittrup Table of Contents A bstract ................................................... ................................................................... 2 T able of C ontents ............................................................................................................................ 3 6 List of Figures ................................................... 8 Acknowledgements.................................. 9 Chapter 1: Background and Significance ............................................................................. Overview of Thesis .............................................................................................................. 9 1.1 Clinical M otivation ................................................ ....................................................... 10 .......... 10 Clinical Problem and Angiogenic Therapy.................................. 1.1.1 1.1.2 Local M yocardial D elivery................................................................................ . 13 1.2 Technical Background ............................................ ...................................................... 14 14 1.2.1 Local Pharmacokinetics and Pharmacodynamics ..................................................... 1.2.2 Pharmacokinetics/Pharmacodynamics Modeling ..................................... ...... 15 1.3 Thesis Theme ................................................. 17 1.4 Thesis Organization ............................................................................................................ 18 1.5 Referen ces ...................................................... ............................................................... 19 Chapter 2: Baseline Local Pharmacokinetics of FGF in Myocardium ......................................... 23 A b stract ...................................................................................................................... ..... . .... 2 3 2.1 Introduction...................................... 24 2.2 M aterials and Methods........................................................................................................ 26 2.2.1 Recombinant FGF2 Production ......................................................................... 26 2.2.2 Fluorescence Labeling of FGF2......................................................................... 27 2.2.3 Size Exclusion Column Chromatography........................................ 28 2.2.4 Measurements of Diffusivity ....................................................... 29 2.2.5 Ex-vivo Myocardial Drug Delivery with and without Perfusion......................... . 30 .............. 33 2.2.6 Fluorescence imaging and processing ......................................... 2.2.7 Measurement of FGF in Outflow................................................. 33 2.2.8 Continuum Pharmacokinetic Model of Myocardial Drug Transport With and Without Perfusion ................................................... 34 2.2.9 Analytical Model Calculation of Cumulative FGF Clearance........................... . 37 2.2.10 Statistical analysis ........................................... ..................................................... 38 2 .3 Results ........................................................................................ ................................... 39 2.3.1 FGF Diffusivity in the Absence of Myocardial Perfusion.......................... .... . 39 2.3.2 FGF Distribution is Limited by Myocardial Perfusion............................. ...... 40 2.3.3 FGF is Washed-out Through Microvascular Clearance Followed Ex-vivo Myocardial D elivery........................................... 41 2.3.4 SOS limits the effects of capillary washout on FGF2.............................................. 42 2.3.5 Effects of Molecular Weight on Myocardial Transport Under Perfusion ................ 44 2.3.6 Drug Diffusivity, Trans-endothelial Permeability and Vessel Density Influence Local Drug Distribution and Deposition......................................................46 2.4 Discussion .................................................................................................................... ...... 50 2.4.1 Capillaries limit drug penetration in a manner dependent on molecular weight ......... 50 2.4.2 Ischemic and non-ischemic tissues present different barriers to transport .............. 51 2.4.3 Angiogenesis limits its own success .................................................... .................. 52 2.5 Summ ary ........................................... ............ ............................................................. 53 2.6 References........................................ 54 Chapter 3: Interdependence of Local Pharmacokinetics and Pharmacodynamics ........... 57 Abstract ................................................................. .......................................... 57 3.1 Introduction...................................... 58 3.2 M aterials and Methods........................................................................................................ 60 3.2.1 Recombinant S35-FGF1 Production.............................................. 60 3.2.2 Fabrication and Kinetics of Controlled Release Device ..................................... . 62 3.2.3 In-vivo Myocardial Drug Delivery .................................................................... 63 3.2.4 Quantification of in-vivo FGF1 and Blood Vessels Distribution ............................. 64 3.2.5 Statistical analysis ............................................ ...................................................... 65 3.3 Results ............................................ 66 3.3.1 Polymeric Devices Sustain Release FGF1 over 30 days in-vivo.............................. 66 3.3.2 In-vivo Angiogenic Response Limits Drug Distribution.......................... ...... 67 3.4 D iscussion ........................................................................................................................... 72 3.5 References ........................................................................................ ......... 75 7............ Chapter 4: Computational Modeling of Local Pharmacokinetics and Pharmacodynamics of FGF in Myocardium......................................... 78 A bstract .................................................................................................................................. 78 4.1 Introduction...................................... 79 4.2 M ethods ............................................. 80 4.2.1 Local Pharmacokinetic Model ...................................... 82 4.2.1.1 Mass Transport Equations....................................... 82 4.2.2 Local Pharmacodynamic Model ............................................................................... 84 4.2.2.1 C apillary sprouting......................................... ................................................. 84 4.2.2.2 Capillary m aturation ............................................................. .......................... 85 4.2.2.3 C apillary regression ............................................................. ........................... 86 4.2.3 M odel Param eters ............................................. ..................................................... 88 4.2.4 N umerical M ethods........................................... ..................................................... 89 4.3 Results ............................................................................................ 90 4.3.1 Local Pharmacokinetic (PK) Model Results: Effects Diffusivity, Trans-endothelial Permeability and Vascularity on Drug Transport. ........................................ ......... 90 4.3.2 Local Pharmacokinetic-Pharmacodynamic (PK-PD) Model Results ....................... 92 4.3.2.1 PK-PD Interdependence: ....................................................... 92 4.3.2.2 Model Sensitivity Analysis: ....................................................... ........... 94 4.3.2.2.1 Timings of Capillary Maturation and Regression Have Little Effect on Steady State C apillary G ain .................................................................. .............................. 94 4.3.2.2.2 Trans-endothelial Permeability, Diffusivity, Biologic Threshold, Initial capillary density and Release Kinetics Have Significant Effect on Steady State Drug Distribution and Capillary gain.................................................................................. 98 4.4 Discussion: ................................................. 103 4.4.1 Traditional Continuum PK vs. Continuum PK-PD Analysis............................. 103 4.4.2 Minimizing Microvascular Clearance as an Approach to Optimize Angiogenic Effect ....................................................................... 10 4 4.4.3 Release Rate and Diffusivity Modification to Optimize Angiogenic Effect.......... 105 4.4.4 Minimizing Late Loss as an Effective Approach to Improve Angiogenic Therapy.. 106 4.5 Summ ary ................................................. 108 4.6 References ........................................ 109 4 Chapter 5: Effects of Tissue Binding on Local Pharmacokinetics of FGF in Myocardium....... A b stract ................................................................................................................................... ....................................... 5.1 Introduction 5.2 Methods............................................. 5.2.1 Effect of Binding on Myocardial Transport ............................ 5.2.2 Long-time point uptake studies................................. 5.3 Results ......................................................................................................................... 5.3.1 Tissue Binding Impedes FGF Transport in Myocardial Tissue .............................. 5.3.2 Modulating tissue binding alters myocardial FGF2 transport ................................ 5.4 D iscu ssion ......................................................................................................................... 5.4.1 Binding reduces effective diffusivity, but can be modulated by protective groups... 5.4.2 Implications for Angiogenic Growth Factor Delivery ..................................... 5.5 Summary ................................................. 5.6 References........................................ Chapter 6: Future Studies and Conclusions ..................................... 6.1 Future Studies ................................................................................................................... 6. 1.1 Characterization of Trans-endothelial Permeability in Myocardium. ..................... 6.1.2 Computational Models of Angiogenesis ...................................... 6.1.3 Characterization of Effect of Binding..................................................................... 6.2 Thesis Sum mary................................................................................................................ 6.3 References ......................................................................... ......................... .................... APPENDIX: ......................................... MATLAB code: PK-PD Model ........................................ 111 111 112 114 114 115 116 116 117 12 1 121 123 125 126 128 128 128 130 130 132 133 134 134 List of Figures Chapter 2: Baseline Pharmacokinetics of FGF in Myocardium Fig. 2-1 Elution profile of FGF2 27 Fig. 2-2 Isolated perfused heart apparatus 30 Table 1-1 Continuum pharmacokinetic model equations 37 Fig. 2-3 FGF2 diffusivity measurements 39 Fig. 2-4 Myocardial capillary perfusion impedes drug penetration 40 Fig. 2-5 FGF is washed-out through microvascular clearance 41 Fig. 2-6 Size exclusion chromatography of FGF2, and its complexes 42 Fig. 2-7 Distribution of TR-(FGF2)2-SOS 43 Fig. 2-8 Deposition with and without flow of EBD, Dextrans, FGF, FGF-SOS, BSA 45 Fig. 2-9 Continuum pharmacokinetic model 46 Fig. 2-10 FGF distribution is sensitive to alteration in drug clearance 47 Chapter 3: Interdependence of Local Pharmacokinetics and Pharmacodynamics 35 Fig. 3-1 Recombinant S-FGF1 production and purification 60 Fig.3-2 In-vivo ischemic heart model of local myocardial delivery of FGF 64 Fig. 3-3 Polymeric devices sustain release FGF1 over 30 days 66 Fig 3-4 Spatial-temporal profiles of 35S-FGF1 in-vivo 69 Fig 3-5 Representative fluorescent images of stained blood vessels 70 Fig 3-6 Vascular to tissue surface fraction at different times 71 Chapter 4: Computational Modeling of Local Pharmacokinetics and Pharmacodynamics Fig. 4-1 Schematics of computational model 83 Table 4-1 Summary of model equations 84 Table 4-2 Summary of angiogenic model algorithm. 87 Table 4-3 Baseline parameter values 88 Fig. 4-2 PK model results 91 Fig. 4-3 PK/PD model results: drug and capillary distributions as a function of time 93 Fig. 4-4 Effects of tfinctional 96 Fig. 4-5 Effects of t regression 97 Fig. 4-6 Effect of initial vascularity 98 Fig. 4-7 Effects of diffusivity, permeability, C,, and release rate 101 Fig. 4-8 Steady state percentage capillary gain as function of model parameters 102 Fig. 4-9 Approaches to improve pro-angiogenic therapy 107 Chapter 5: Effect of Binding on Local PK of FGF in Myocardium Table 5-1 Summary of derivation of effect of tissue binding on effective diffusivity 114 Fig. 5-1 Concentration dependent transport of FGF2 119 Fig. 5-2 Modulation of binding alters myocardial FGF2 transport 120 Acknowledgements I would like to express my gratitude to many people without whom this work would not be possible. First I am especially proud to have worked with my advisor, Prof. Elazer Edelman, a great teacher and scientist. I'm indebted to Prof. Edelman for his mentorship and guidance throughout my academic career, and for allowing me the unique independence and responsibilities. I have learned much from many experiences working with him in the lab and the HST.090 course. Prof. Edelman has been my role model as a critical thinker, problem solver, scientist, and teacher. I would like to thank my Thesis Committee members, Dr. Matthew Nugent, Dr. Collin Stultz, and Dr. K. Dane Wittrup, for agreeing to serve on the committee, asking tough questions to make me think harder about the project, and for their time reading the thesis. I would like to thank all the people in the Edelman lab for their help, encouragement and support. In particular, Rami Tzafriri for many helps in mathematical analysis and publishing process, and for many interesting scientific discussions and friendship, Chao-Wei Hwang for his help in getting my project started and solving many technical problems and friendship, Mark Lovich for advising many experimental aspects of the project and agreeing to be my HST.203 preceptor, Peter Wu for friendship, and help with labeling FGF and many interesting scientific discussions, David Ettenson for answering many questions from biology to job hunting, Abraham Wei, for technical help with FGF, Laurie May for helping with many of the logistics of thesis meetings and defense, and Michele Miele for making sure my radioactive experiments are safe. I would like to also thank Dr. Alison Hayward and Dr. Robert Marini in MIT DCM for their help creating the rabbit ischemic heart model, and helping with the surgeries. I would like to express my gratitude to my family. First and foremost my wife, Thoa, for her love, patience and support throughout my academic years and my sons, Khoi and Ben for making my everyday life meaningful and enjoyable, and my parents without whom none of the work in this thesis would have been possible in the first place. Kha Le 2/2009 Chapter 1: Background and Significance Overview of Thesis The paradox of angiogenesis science is that stable sustained vascular regeneration in humans has not been realized despite promising preclinical findings. The driving hypothesis for this Thesis is that early success at inducing vessel growth powerfully self-regulates angiogenic therapies by dynamically alteringlocal tissuepharmacokineticproperties.This thesis was designed to critically examine this hypothesis and to examine whether it could in part explain the limited late efficacy of local delivery of angiogenic factors. Specifically, this thesis consists of a series of studies designed to examine the interdependence of local pharmacokinetics and pharmacodynamics of local angiogenic growth factor delivery. The aims include: Chapter 2: Defines myocardial PK at a multi-cellular level with ex-vivo experimental studies and quantitative analysis of steady state drug distributions. Chapter 3: Examines the PK-PD interdependence with in-vivo animal model of drug transport and angiogenesis. Chapter 4: Derives a mechanistically based computational model of the local PK-PD of angiogenic growth factors in myocardial tissue to predict distribution of drugs and biologic effects. Chapter 5: Examines the effect of tissue binding on transport and discusses implications and future studies. The quantitative framework presented here may help guide rational selection of specific angiogenic compounds based on a favorable physicochemical profile, and drug delivery strategies that take advantage of the tight regulation between growth factor pharmacokinetics and angiogenic pharmacodynamics. 1.1 Clinical Motivation 1.1.1 Clinical Problem and Angiogenic Therapy Cardiovascular diseases affect more than 70 million Americans and account for 1 out of 2.7 deaths in the United States 1. The most common cause leading to these cardiovascular diseases is coronary artery disease (CAD) causing by blockage of one or more coronary arteries supplying blood to the heart tissue as a result of loss of endothelial integrity, infiltration of monocytes, macrophages and vascular smooth muscle cells, and/or aberrant vasospasm. These partial or complete stenoses of coronary arteries can threaten cardiac tissue integrity. The severity of the consequences of myocardial ischemia as a result of inadequate oxygenation and accumulation of metabolic waste products depends on the magnitude and duration of the reduction in myocardial supply. These range from rapid and full recovery of myocyte function, prolonged contractile dysfunction without myocyte necrosis, to irreversible myocardial necrosis. Rescuing the ischemic myocardium prior to necrosis can restore its function. The few available therapeutic interventions including angioplasty, atherectomy, stenting, and vascular bypass surgery center on mechanical revascularization to increase lumen diameter of the occluded arteries. These interventional procedures are effective for well-defined lesions in large coronary arteries. However, a substantial number of patients with diffuse and small-vessel coronary artery disease whose lesions are not readily accessible by these treatments and those who lack of conduits for bypass surgery cannot be benefited. Almost 1.5 million cardiac catheterization procedures and 0.5 million coronary artery bypass surgeries are performed yearly for attempted relief of the complications of these illnesses '. It has been estimated that up to a third of patients presenting with advanced coronary disease receive incomplete revascularization with conventional percutaneous and surgical techniques due to the presence of diffuse disease and unsuitable coronary anatomy 2 Collateral coronary vessel formation stimulation using angiogenic growth factors has the potential to reduce myocardial infarct size and improve cardiac function 4. Induced angiogenesis may prove to be the optimal therapy for coronary arteries that are not suited for traditional intervention and may also be of benefit when given as an adjunct to mechanical revascularization. While the biological time scale for angiogenesis exceeds the time required for salvaging infracting myocardium for acute myocardial infarction patients, this approach holds promise for those with chronic myocardial ischemia, and may be the only hope for those patients with small-vessel disease and are ill-suited for transplantation. Furthermore, just as coronary artery obstruction induces myocardial ischemia, peripheral artery obstruction can induce skeletal muscle ischemia, causing debilitating symptoms in patients with peripheral artery disease (PAD) intermittent claudication and critical limb ischemia 5. Biological revascularization with angiogenic therapy remains an equally promising therapeutic approach for PAD as well as CAD patients. Fibroblast growth factors 1 and 2 (FGF1 and FGF2) are the most studied growth factors for the induction of myocardial angiogenesis 6. They belong to a large family of polypeptide growth factors that are found in many organisms ranging from worms to humans, and are highly conserved in both gene structure and amino acid sequence 6. In addition to binding to its cognate surface receptors, FGFR, FGFs also exhibit a high affinity for heparan sulfate proteoglycans. These interactions have been shown to stabilize FGFs from thermal denaturation and proteolysis and can result in the formation of dimers or higher order oligomers -10. It has also been suggested that these interactions with heparin/heparan sulfate are required for effective signaling downstream of FGFR activation 11-13. FGFs are known to have diverse roles in regulating cell proliferation, migration and differentiation during embryonic development and in tissue repair in adult life. Upon FGFR activation and FGF endocytosis, FGFs are known to promote angiogenesis not only by stimulating the growth of new blood vessels their apoptotic potential 15. 14, but also by abrogating FGF1 and 2 can promote all of the requisite events for angiogenesis, including endothelial activation, proliferation, increased survival, migration, and differentiation . Yanagisawa-Miwa et. al. 4 was one of the first study to show that intracoronary injection of FGF to ischemic myocardium can stimulate neovascularization, reduce myocardial infarct size studies and improve cardiac function. Despite many subsequent impressive animal 14,16-19 clinical trials of myocardial angiogenesis employing intracoronary infusion have been disappointing 20,21. Local intra-myocardial and pericardial sustained delivery can elevate myocardial drug concentration and lower systemic exposure in animal models 22 but such techniques have not proven uniformly effective in humans. Of the 8 clinical investigations to date 20,' 21, 23-25, Laham et.al. 2 1 is the only one to show any effectiveness of angiogenic therapy using sustained local perivascular delivery of bFGF. The reasons accounting for these mixed results remained unanswered. 1.1.2 Local Myocardial Delivery Angiogenic growth factors are highly potent and short in half-life, but require long retention time to establish chemotactic and survival signals. These properties and requirements pose a challenge to systemic administration and underscore the need for local myocardial delivery 30. Several strategies have been developed to allow local growth factor delivery to the myocardial tissue. Bolus delivery that preferentially deposits drug to myocardium includes intracoronary and intra-myocardial injection 3 1. Controlled-release delivery involves using pumpbased or chemical-based devices, such as polymers, that hold and apply drugs to myocardial tissue through pericardial or intra-myocardial routes release of drugs for months 34-36 17, 32, 33. Polymeric based devices can sustain and can offer better pharmacokinetic advantage than local bolus administration and systemic delivery. Despite advanced local delivery technologies, angiogenic therapy has not endured clinical success. It is unclear whether these mixed successes are related to basic growth factor biology or drug transport issues. With tremendous resources being poured into therapeutic angiogenesis research at both preclinical and clinical stages, a detailed systematic characterization of local myocardial pharmacokinetics therefore is imperative to help answer this question. 1.2 Technical Background 1.2.1 Local Pharmacokinetics and Pharmacodynamics Pharmacokinetics (PK), the science of the kinetics of drug absorption, distribution, and elimination, and pharmacodynamics (PD), the study of relationship between drug concentration and pharmacologic response, are established fields of study in biopharmaceutics 37. These conventional PK and PD analyses although well suited to study drugs targeting the central plasma compartment but in general do not consider spatial aspect of the problem and are not suitable for local drug delivery studies. The large and dynamic concentration gradients imparted by the delivery devices across target tissues have proven difficult to identify, characterize and control. Cells near the source of drug release are likely surrounded by a vastly different concentration than cells far away. Drug levels are not static in time, and indeed can depend on local tissue structures and local transport parameters 36, 38, 39. It is, therefore, anticipated that local tissue response to angiogenic growth factors will track the latter's spatio-temporal distribution 27. Thus, failure to sustain the requisite myocardial growth factor distribution may underlie much of the variability in the results of local approaches in angiogenic therapy. Yet, local pharmacokinetics in the myocardium has not been well characterized. For instance, little is known about the mechanism growth factor transport following local delivery. Studies in arteries suggested that tissue ultrastructure and local physiologic forces influence drug distribution 26-29. The mechanisms of soluble drug transport and elimination are, therefore, most likely responsible for myocardial distribution and deposition of growth factors. For highly vascularized tissues such as the myocardium, in addition to diffusion and tissue binding, these also include the mechanism of drug clearance through microvascular washout. Reversible binding to fixed tissue components that are required for endocytotic internalization and biologic activity is expected to have a significant impact on drug transport. Furthermore, as current drug release technologies allow more growth factors to be released in a controlled manner over a long period of time, the tissue response and remodeling process become increasingly important in altering the local pharmacokinetics by modifying the factors mentioned above, for instance changes in vascular density, trans-endothelial permeability as a result of therapeutic success. A quantitative appreciation and systematic characterization of these local pharmacokinetics and pharmacodynamics factors influencing drug distribution will thus be conducive to a more rational approach to delivery strategy, dosage and drug design. 1.2.2 Pharmacokinetics/Pharmacodynamics Modeling Drugs are in a dynamic state within the body as they move within tissues and between tissues and blood, bind with different cellular and extracellular components, or are cleared and metabolized. The distribution of drugs and their biologic effects is complex since it can be influenced by any of these drug events. Yet detailed understanding of such events is crucial to characterize drug PK and PD. Such complexity requires the use of mathematical models to predict the time course of drug distribution and effects to guide drug and delivery strategy designs. Mathematical modeling of PK is traditionally divided into three categories: empirically, compartmentally, and physiologically or mechanistically based. Empirical models are useful in obtaining specific parameters by curve fitting well controlled experimental data. Compartmental models, lumping various tissues into instantaneously well mixed compartments, are simple and useful for systemic PK studies but not suited for local PK analysis. Mechanistic models based on known physiologic processes are useful for regional analysis, such as local pharmacokinetic models used in arterial drug delivery 26, 28, 29, 40, 41. These mechanistically based models are crucial for predicting drug distribution and optimization studies with local delivery, but require accurate and difficult to obtain model parameters. 1.3 Thesis Theme The paradox of angiogenesis science is that stable sustained vascular regeneration in humans has not been realized despite promising preclinical findings. Our hypothesis is that the limited late efficacy of local delivery of angiogenicfactors stems partlyfrom the very early success at inducing vessel growth because angiogenic therapiespowerfully self-regulate by dynamically alteringlocal tissuepharmacokineticproperties.These local changes can affect global outcome of therapy and require in depth studies of local PK and PD of angiogenic growth factor within myocardial tissues. This interdependence of pharmacokinetics and pharmacodynamics may explain the difficulty of realizing sustained clinical angiogenesis with local release. The quantitative framework presented here may help guide rational selection of specific angiogenic compounds based on a favorable physicochemical profile, and drug delivery strategies that take advantage of the tight regulation between growth factor pharmacokinetics and angiogenic pharmacodynamics. 1.4 Thesis Organization This thesis consists of a series of studies designed to examine the interdependence of local pharmacokinetics and pharmacodynamics of local angiogenic growth factor delivery. The specific aims include: Chapter 2: Defines myocardial PK at a multi-cellular level with ex-vivo experimental studies and quantitative analysis of steady state drug distributions. Chapter 3: Examines the PK-PD interdependence with in-vivo animal model of drug transport and angiogenesis. Chapter 4: Derives a mechanistically based computational model of the local PK-PD of angiogenic growth factors in myocardial tissue to predict distribution of drugs and biologic effects. 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Cardiovasc Res. 2001; 49:532-542. 31. 32. 33. 34. 35. 36. 37. 38. 39. 40. 41. 42. 43. 44. 45. 46. Biswas SS, Hughes GC, Scarborough JE, Domkowski PW, Diodato L, Smith ML, Landolfo C, Lowe JE, Annex BH, Landolfo KP. Intramyocardial and intracoronary basic fibroblast growth factor in porcine hibernating myocardium: a comparative study. J Thorac Cardiovasc Surg. 2004; 127:34-43. Lopez JJ, Edelman ER, Stamler A, Hibberd MG, Prasad P, Caputo RP, Carrozza JP, Douglas PS, Sellke FW, Simons M. Basic fibroblast growth factor in a porcine model of chronic myocardial ischemia: a comparison of angiographic, echocardiographic and coronary flow parameters. J Pharmacol Exp Ther. 1997; 282:385-390. Sakakibara Y, Tambara K, Sakaguchi G, Lu F, Yamamoto M, Nishimura K, Tabata Y, Komeda M. Toward surgical angiogenesis using slow-released basic fibroblast growth factor. Eur J Cardiothorac Surg. 2003; 24:105-111; discussion 112. Edelman ER, Brown L, Langer R. Quantification of insulin release from implantable polymer-based delivery systems and augmentation of therapeutic effect with simultaneous release of somatostatin. J Pharm Sci. 1996; 85:1271-1275. Edelman ER, Mathiowitz E, Langer R, Klagsbrun M. Controlled and modulated release of basic fibroblast growth factor. Biomaterials. 1991; 12:619-626. Raman VK, Edelman ER. Coated stents: local pharmacology. Semin Interv Cardiol. 1998; 3:133-137. Shargel L, Wu-Pong S, Yu ABC. Applied biopharmaceutics& pharmacokinetics.5th ed. New York: Appleton & Lange Reviews/McGraw-Hill, Medical Pub. Division; 2005. Rippley RK, Stokes CL. Effects of cellular pharmacology on drug distribution in tissues. Biophys J. 1995; 69:825-839. Baumbach A, Herdeg C, Kluge M, Oberhoff M, Lerch M, Haase KK, Wolter C, Schroder S, Karsch KR. Local drug delivery: impact of pressure, substance characteristics, and stenting on drug transfer into the arterial wall [see comments]. Catheter Cardiovasc Interv. 1999; 47:102-106. Hwang CW, Wu D, Edelman ER. Impact of transport and drug properties on the local pharmacology of drug-eluting stents. Int J Cardiovasc Intervent. 2003; 5:7-12. Lovich MA, Edelman ER. Mechanisms of transmural heparin transport in the rat abdominal aorta after local vascular delivery. Circ Res. 1995; 77:1143-1150. Mahoney MJ, Saltzman WM. Millimeter-scale positioning of a nerve-growth-factor source and biological activity in the brain. Proc Natl Acad Sci U S A. 1999; 96:45364539. Dowd CJ, Cooney CL, Nugent MA. Heparan sulfate mediates bFGF transport through basement membrane by diffusion with rapid reversible binding. J Biol Chem. 1999; 274:5236-5244. Natke B, Venkataraman G, Nugent MA, Sasisekharan R. Heparinase treatment of bovine smooth muscle cells inhibits fibroblast growth factor-2 binding to fibroblast growth factor receptor but not FGF-2 mediated cellular proliferation. Angiogenesis. 1999; 3:249257. Fannon M, Forsten KE, Nugent MA. Potentiation and inhibition of bFGF binding by heparin: a model for regulation of cellular response. Biochemistry. 2000; 39:1434-1445. Richardson TP, Trinkaus-Randall V, Nugent MA. Regulation of basic fibroblast growth factor binding and activity by cell density and heparan sulfate. J Biol Chem. 1999; 274:13534-13540. 47. Flaumenhaft R, Moscatelli D, Rifkin DB. Heparin and heparan sulfate increase the radius of diffusion and action of basic fibroblast growth factor. J Cell Biol. 1990; 111:1651 1659. Chapter 2: Baseline Local Pharmacokinetics of FGF in Myocardium Abstract While mechanistically attractive, local delivery of angiogenic growth factors has a disappointing record at inducing sustained therapeutic myocardial angiogenesis in human clinical trials. We hypothesized that these results partly stem from the inherent local pharmacokinetics of drugs in myocardium. Transport forces in myocardium include diffusion and microvascular clearance. For some drugs especially growth factors such as FGFs, binding to fixed tissue sites can further complicate drug transport. In non-perfused rat myocardium, drug transport is mainly governed by diffusion and binding processes. Without coronary perfusion, FGF2 distributions followed linear diffusion with low diffusivity (0.024m 2/s) and low tissue penetration (65pm). Restoration of coronary flow enhanced clearance, limiting penetration even further. FGF2 penetration depth contracted by 46% to 35 tm. FGF clearance through washout was confirmed by the presence of FGF in coronary outflow. These findings were well explained by a diffusionclearance analytical model, with a clearance rate constant determined to be K = 1.15x 10-4 se-1 for FGF2 and 4.37x 10- 5 sec l for FGF2 dimer. Penetration of high molecular weight and low capillary permeability (FGF2) 2-sodium octa-sulfate dimer was unaffected by coronary perfusion. Furthermore, studies with additional molecules revealed the relationship between capillary drug washout and drug molecular weight is sigmoidal, with an inflection point at 20 kDa. Our results suggest that capillary networks present physical obstacles to drug uptake following local myocardial delivery, and given the gradations in capillary density and trans-endothelial permeability with angiogenic therapy, uptake and deposition of angiogenic growth factors will vary tremendously across the heart. 2.1 Introduction Different approaches of localizing drugs to myocardial tissue have been studied extensively including Swanz Ganz catheter, left atrial, intracoronary, intramyocardial, and pericardial routes. Intrapericardial delivery have been shown to have a significant pharmacokinetic advantage over the cathether based intravascular local delivery routes 1, 2, and to be a consistent way to deliver drug to the heart tissue 3. As a small fluid filled closed compartment surrounding the heart, pericardial space provides an ideal drug reservoir for local myocardial delivery 4. Intrapericardial application of nitric oxide donors 5,6 and antiarrthymic agents 7have been shown to elicit expected biologic effects on heart functions. Chemotherapeutic drug 8 and glucocorticoids 9 have also been delivered to pericardial space to treat pericardial effusions. These pharmacodynamic studies suggest that pericardial delivery is a promising strategy for local myocardial delivery. Nevertheless, many fundamental pharmacokinetic questions regarding this route of local delivery have not been satisfactorily answered. For instance, it is not clear how the extensive vascular networks within the myocardium affect solute transport within the tissue, and whether this effect can be characterized in a quantitative manner to allow for comparative studies and facilitate predictive computational modeling. Local physiological forces have been shown to significantly influence drug deposition in arterial tissues 1 -' 5 . Unlike arterial wall, cardiac myocytes are perfused by a dense capillary network 16, 17. Theoretically, if downstream convection dominates, capillaries can act as sinks and decrease drug uptake 18. If lumen-tissue interfacial diffusion is rapid, then capillaries act as conduits to other parts of tissue and increase drug penetration. Drug transport within the myocardial tissue therefore is dictated by a balance between downstream convection and lumentissue interfacial diffusion. In this chapter, we sought to understand how physiological factors in myocardium affect delivery of angiogenic growth factors. First, we show that in the absence of coronary perfusion, diffusion and binding are the dominant transport hindrance factors. We attempt to characterize the myocardial effective diffusivity of many drug compounds in this chapter and defer the studies of effects of tissue binding to Chapter 5. Using an ex vivo perfused rat heart model, we also show that myocardial capillaries act primarily as sinks rather than conduits for drugs with physicochemical parameters similar to angiogenic growth factors. Next, we show that the substantial capillary washout of FGF2 can be modulated by physical alteration of the growth factor. This can be accomplished by creating complexes of FGF2 and sugar groups such as sucrose octasulfate (SOS) and inducing FGF2 dimerization. We designed these pharmacokinetic experiments to look at the effect of transport factors in isolation. Our analysis represents a systematic approach to local myocardial pharmacokinetics that may eventually allow the selection of angiogenic compounds based on favorable physicochemical properties, potentially leading to the design of controlled-release strategies that take advantage of local pharmacokinetics to maximize pharmacologic revascularization. 2.2 Materials and Methods 2.2.1 Recombinant FGF2 Production Recombinant FGF2 was expressed in Escherichiacoli strain FICE-127 transformed by plasmid vector pFC80 that confers resistance to ampicillin and encodes FGF2 under the control of the tryptophan promoter (the transformed FICE-127 strain was a gift from John Heath, University of Birmingham, and was originally constructed by Antonella Isacchi, Amersham Pharmacia Biotech and Upjohn). FICE-127 cells containing pFC80 were inoculated into LB Medium (MP Biomedicals) containing 0.29 mmol/L (10 mg/dL) of ampicillin (Invitrogen) and grown overnight at 37C in a shaker at 250 RPM. The inoculums were diluted 1:100 in M9 Minimal Medium (Fisher Scientific) containing 1 g/L amino acids (Becton Dickinson) without tryptophan to induce protein production. Cells were grown for 6 h at 370 C in a shaker at 250 RPM. Cells were collected by centrifugation at 8000 RPM for 10 m and kept frozen at -800 C. Frozen cell pellets were resuspended in 6.94x 10-2 mmol/L (100 mg/dL) lysozyme in GET buffer (100 mmol/L Glucose, 10 mmol/L EDTA, and 50 mmol/L Tris, pH 8.0), vigorously agitated for 5 m and homogenized (Polytron; Kinematica) 5 times for 30 s each with break periods of 60-90 s at 4°C to prevent overheating and denaturation of proteins. Bacterial lysate was collected by centrifugation at 9,000 RPM for 10 m at 40 C. FGF2 was then purified using affinity chromatography with FPLC (Pharmacia Biotech). Lysate was loaded into 5 mL heparin Sepharose column (HiTrap, GE Healthcare) and allowed to bind for 2 h at 4°C. The FPLC system was programmed to wash the column with phosphate buffered saline (PBS) containing incrementally concentrated NaCl with a linear gradient (150 mmol/L to 2000 mmol/L). Elutions were collected in sequential 1 mL fractions, with FGF2 eluting at 1400 mmol/L to 1600 mmol/L NaC1. The FGF2 solution was desalted by centrifugation using centrifugal filters with 10 kDa molecular weight cut-off (Centricon, Millipore). After each purification, the presence of FGF2 was confirmed at a 18kDa band using SDS-PAGE, and protein concentration was quantified with a BCA assay (Pierce). Bioactivity of FGF2 was confirmed by in vitro proliferation assays using bovine aortic endothelial cells. 2.2.2 Fluorescence Labeling of FGF2 A heparin Sepharose -[NaCI] column (HiTrap, GE Healthcare) FGF2 * Fluorescence was loaded with 1 mL of 0.12 mmol/L (200 mg/dL) FGF2 in . PBS and allowed to bind for 1 h 0.5 0 z at room temperature. The FGF2loaded column was washed with 5 mL of 100 mmol/L NaHCO3 to increase the pH to 8.3 and loaded (100 with 1 mL of 1.60 mmol/L 0 5 10 15 Fraction number FIGURE 1: Elution profiles of FGF2 (blue), TR (red), and NaC1 (black). mg/dL) Texas Red succinimidyl ester (Invitrogen). Texas Red succinimidyl ester was allowed to react with FGF2 for 10 m at room temperature. The column was then placed in-line on the FPLC system, and FGF2 was eluted as described above. Elutions of 1 mL were collected and assayed for protein content (absorbance at 280 nm, FPLC System) and Texas Red fluorescence intensity (595 nm/615 nm excitation/emission wavelengths, Fluoroskan II, Lab Systems Oy). Texas Red was appropriately conjugated to FGF2 as indicated by the concurrence of the elution peaks of fluorescence intensity and protein concentration. Both came off the column between 1400 to 1600 mmol/L NaCi (Fig. 1), similar to the elution range of unlabeled FGF2, suggesting that Texas Red conjugation did not change the heparin binding properties of FGF2. Buffer exchange was performed on the Texas Red labeled-FGF2 (TR-FGF2) solution by centrifugation as above. SDS-PAGE indicated that the molecular weight of TR-FGF2 is not significantly different from that of FGF2. Fluorescence intensity was calibrated to protein concentration prior to delivery using microplate fluorometry (Fluoroskan). 2.2.3 Size Exclusion Column Chromatography Size exclusion analysis of FGF2 alone, FGF2 complexed with sucrose octasulfate (FGF2SOS), unfractionated heparin (FGF2-UFH, Sigma-Aldrich) or low molecular weight heparin (FGF2-LMWH, Sigma-Aldrich) was performed by injecting 1 mg of the complexes in PBS into a Superose 12 10/300GL column (GE Healthcare) on a FLPC system (Pharmacia Biotech). The molar ratios of FGF2 to SOS, UFH and LMWH were each 1:100 to ensure all FGF2 molecules are complexed before loading on to the column. Soybean trypsin inhibitor (20.1 kDa), ovalbumin (42.7 kDa), f3-galactosidase (112 kDa) and bovine serum albumin (65 kDa) (SigmaAldrich) were used as gel filtration molecular weight standards. 5 mg of the standards were injected into the column for the chromatographic analysis. 2.2.4 Measurements of Diffusivity In the absence of blood flow, drug transport in the myocardium is dominated by diffusion. The effective diffusivity can be estimated by curve fitting drug spatial concentration profile to the solution of the diffusion equation derived at similar conditions. The most straightforward approach is to employ the solution of the diffusion equation for semi-infinite boundary conditions C(x=O) = Csource and C(x=oo)=0 C/C =erfe [Eq. El] Experimentally, drugs were delivered to myocardium according to the methods described in "Exvivo Myocardial Drug Delivery without Perfusion", imaged and processed according to "Fluorescence imaging and processing" section. Concentration profiles were obtained by averaging multiple drug profiles using an automatic Matlab code (Appendix). Curve fitting was then done on the mean concentration profile with GraphPad Prizm software. 2.2.5 Ex-vivo Myocardial Drug Delivery with and without Perfusion N* Diffusion and permeation -- Convection Perfusate (95%02 / 5%CO 2, T=37 0C) FIGURE 2: Isolated perfused heart apparatus. Rat coronary arteries were perfused antegrade through an aortic canula at constant physiologic mean pressure while a constant, well mixed drug source was applied to the epicardial surface. Spatial drug distribution was quantified in myocardial tissue regions exposed to drug. High magnification schematic illustrates the examined physiologic forces: drug diffusion within tissue and clearance through convection by intravascular flow after permeation across capillary wall. Sprague Dawley rats (0.5-0.6 kg) were anesthetized with 35 mg/kg ketamine and 5 mg/kg xylazine, and anticoagulated with 1000 U subcutaneous heparin prior to CO 2 euthanasia. The aorta was cannulated and heart retrograde perfused with cardioplegia (Osmolality = 289 mOsm/kgH 20 + 5%) composed of Krebs-Henseleit buffer (Sigma-Aldrich) with high potassium (30 mmol/L KC1) and 4 % BSA (Sigma-Aldrich) to establish diastolic arrest. The heart was excised and perfused at 95 mmHg. Coronary flow was monitored periodically and ranged 8-10 ml/minutes throughout experiment. The perfusate was oxygenated by a foam bubble oxygenator with 95 % 02 / 5 % CO 2 at 37oC (Fig. 2). Samples were also examined in the absence of coronary perfusion to eliminate other effects. Here the aorta was cannulated and flushed with perfusate. As blood cleared from the circulation, coronary outflow from coronary sinus was stopped by clamping the right atrium and pulmonary artery ensuring myocardial capillaries patency and that the only difference between the control and perfused cases was coronary perfusion. The entire configuration resided within an enclosed box with 100 % humidity. We ascertained myocardial viability at 6 h by quantitatively documenting no additional tissue edema on H&E stained sections. Experimental protocols were in accordance with NIH guidelines for the humane care and use of laboratory animals and MIT committee on animal care. Texas Red-FGF2 (TR-FGF2, 17 kDa, 5.88x 10-2 mmol/L) and Texas Red labeled FGF2 conjugated to SOS complex (TR-(FGF2) 2-SOS complex, -35 kDa, 2.86x 102 mmol/L) were delivered to the rat myocardium from a drug-releasing chamber affixed to the anterior epicardial surface by a cyanoacrylate based surgical adhesive (Glustitch). The heart was placed on a shaker at 100 RPM to ensure a well mixed epicardial drug source. A core of myocardial tissue in contact with and immediately adjacent to the drug source was harvested 6 h later using an 8 mmdiameter biopsy punch (Miltex). Tissue cores were cryo-sectioned (Leica CM1850) perpendicular to the epicardium for quantitative epifluorescence imaging (Leica DMRA2 microscope, Hamamatsu C4742-95 camera, MetaMorph software, Texas Red filter set). Since the fluorescent intensity of TR-FGF2 is linearly proportional to fluorophore 19, total drug deposition in the absence (Mdg. ) or the presence (Mdfclear) of coronary perfusion were calculated by summing fluorescence intensities in the spatial distributions. Percent clearance of drug from coronary perfusion is %clearance = 100 x (1 - M dff-clear / Mdff). [Eq. E2] 2.2.6 Fluorescence imaging and processing Tissue samples were snap-frozen with liquid nitrogen, mounted onto a cryotome and sectioned into 10 um slides (Leica CM1850). Drug distribution was imaged with a fluorescence microscope (Leica DMRA2, Metamorph software). The images were analyzed with MATLAB (Mathworks) to quantify spatial drug concentration profiles. Tissue autofluorescence at the excitation and emission wavelengths of TR-FGF2 (560nm excitation / 645nm emission) is minimal and readily compensated for by subtracting background fluorescence obtained by imaging myocardium incubated in PBS from the sample fluorescence signal. 2.2.7 Measurement of FGF in Outflow We verified that capillary washout of FGF through microvascular clearance was indeed 35 responsible for the reduction in FGF penetration in the presence of perfusion with S-FGF1. Rat hearts were isolated and perfused using identical procedures and experimental parameters described in the "Ex-vivo Myocardial Drug Delivery" methods section for perfused hearts. 35SFGF1 (4.2 mg/ml) was applied to the epicardial surface (n=3) for 3 hours. The perfusate in these experiments was not re-circulated, hence presence of 35 S-FGF1 in the outflow results from direct washout of exogenous growth fact in tissue. Outflow perfusate was collected in 6-30m fractions. At the end of perfusion experiments, 3ml samples of the outflow fractions were decolorized with 0.5ml hydrogen peroxide at 60 0 C for 1 hour (30%, Sigma-Aldrich), and assayed for 35S radioactivity using liquid scintillation counter (Packard). 2.2.8 Continuum Pharmacokinetic Model of Myocardial Drug Transport With and Without Perfusion Following Tzafriri et. al.20 we model interstitial drug transport in a perfused tissue using the classical diffusion equation with a linear sink term aC D 8 2C = -kC (M1) ax 2 at where the apparent clearance rate constant k is proportional to trans-endothelial permeability as k- MvSmv (1- Omy) (M2) Here Smv is the surface fraction of capillaries and m,,is the capillary volume fraction. Since the surface fraction of a cylinder of radius Rmv is related to the volume fraction as S,, = 2 mv / R., we can rewrite the proportionality between the apparent clearance rate constant and transendothelial permeability as k =R 2 Rmv Pmvm 1- mv (M3) A rich literature exists on the analysis of Eq. Ml. For our purposes, it suffices to note that localization of the experimental growth factor profiles close to the drug source justifies the analysis of distribution profiles in terms of penetration into a semi-infinite domain 21. Namely, we assume that the concentration of growth factor at the far end of the tissue is negligible C=O, x=L. (M4) With this in mind, under the conditions of a constant surface concentration C=CO, x=O (M5) the concentration profile takes the form 21 C/Co=-e-x erfc x - e r-x x/+ . (M6) where £= (M7) k Thus, clearance gives rise to a length scale £ that is independent of the dimensions of the tissue and is inversely related to the clearance rate constant. Correspondingly, using Danckwert's method 21 it is possible to show that net tissue deposition M depends on time as M = C0 erf(i-t) . (M8) Thus, k-' operates as the time scale for the tissue to approach its steady state deposition (M9) M = Cog and distribution C = Coe -x /i. (M10) Hence, increasing the clearance rate constant results in less drug penetration and more significant localization near the drug source. On the contrary, as the clearance rate constant tends to zero, the limitation on drug penetration is lifted (£ >> L ) such that drug penetration and deposition reduce to the classical linear diffusion limits C/Co erfcx 2, D- (Ml1) and M - 2Co -Dt/. (M12) The preceding analysis wherein the surface concentration was held constant provides insights on drug transport during the initial burst release phase. Subsequently drug release from the polymer device occurs at an essentially constant rate. Consider next the extreme limit wherein the flux Fo rather than the concentration is held constant at the surface -D aC= F o ax , x=O (M13) The steady state distribution of drug implied by Eq. Ml is then C = (Fo / D)e - x"~. (M14) Thus , in the face of first order clearance, steady state drug distribution is always exponential with a length scale £; device release kinetics is seen to only impact the steady state concentration of drug at the device:tissue interface (x=0). Integrating the steady state distribution profile Eq. M14 over the entire tissue we find that steady state tissue deposition M scales linearly with flux and inversely with the apparent clearance rate constant M= k (M15) Using the Danckwert's method 21, it is possible to derive the time dependent counterpart of Eq M15, as M = F (1 - e-k'), K (M16) thus confirming that k-1 also operates as the time scale for the attainment of steady state tissue deposition when drug is released at a constant flux from the polymeric device. The main model equations are summarized in Table 1 below. D Eq. 1 k- Eq. 2 2P ". I)1-I . Eq. 3 er C iCo %fc, Eq. 4 C= Eq. 5 = -kC - =. DCe %clearance =100 x 1- (erf(k)] TABLE 1: Continuum Pharmacokinetic Model Equations for Epicardial Drug Delivery. Detailed derivations are included in Supplemental Methods. Eq. 1 describes the transport of drug in the presence of capillary clearance. C represents drug concentration in the tissue as a function of time t, distance from the epicardium x, diffusivity D and apparent clearance constant k. Eq. 2 relates the apparent clearance constant k to capillary permeability Pmv, capillary volume fraction qmy and capillary diameter Rmv. Eq. 3 describes tissue concentration profile normalized to source concentration Co in the absence of capillary perfusion as a function of time and effective diffusivity. Eq. 4 shows the steady state tissue concentration in the presence of capillary perfusion, where -(is drug penetration depth. Eq. 5 shows the percent drug clearance by capillary perfusion as a function of k and D. 2.2.9 Analytical Model Calculation of Cumulative FGF Clearance Cumulative FGF washout through microvascular clearance, between times tl and t2 can be calculated from the experimental value of clearance constant k and the total deposition M (Eqn. M8) by the following relationship: CL = kMdt = JkColerf(k/t tl (M17) tl 2.2.10 Statistical analysis All data were presented as means ± s.e.m., except values for the clearance rate constants k which were reported as means ± propagated standard errors. Propagated errors sk were calculated using the formula( -)2 k = (sD)2 D + 2(sx9 ) 2 , where s D and sx9 are standard errors for X90 effective diffusivity D and penetration depth x 90 , respectively. Statistical analyses were performed with the Student's t test where appropriate. P<0.05 (two-tailed) was considered statistically significant. Non-linear regression was performed using GraphPad software (Prism 5) to fit steady state spatial drug distributions to Eqs. M6 and M11 in obtaining values for clearance rate constant k and effective diffusivity D, respectively. 2.3 Results 2.3.1 FGF Diffusivity in the Absence of Myocardial Perfusion In the absence of coronary perfusion, 2500 SDATA -Cxerfc(x/sqrt(4xDeffxt)) concentration profiles of FGF2 fit well to the2000 - solution of the diffusion equation for semi- Coxerfc(xlsqrt(4x10xDeffxt)) Coxerfc(x/sqrt(4x0.1xDeffxt)) 1500 2 1000 infinite boundary conditions (Fig.3). To U- validate the consistency of our experimental 500 0 method, the experiments were carried out at 50 0 100 150 200 Distance from epicardium two different time points 4hr (Fig.3A) and 96hr (Fig.3B). Effective diffusivity of FGF2 FIGURE 3: FGF2 Diffusivity in excised myocardial tissue performed at 4hr 2 S-1 smfor in myocardium was 0.021 + 0.001 2 TR-FGF2 when measured at 4hr, agrees with the value of 0.018 + 0.001 gm S-' when measured at 96hr, suggesting that the transport of FGF2 in myocardium within these time points is primarily diffusion mediated transport, and that the tissue transport properties were not significantly altered up to 96 hr at 40 C. We further quantified effective diffusivity of similar molecular weight dextrans and dextrans sulfate using the same method. Effective diffusivities of 2 -1 2 10kD, 20kD dextrans and 8kD dextran sulfate were 10.24 + 2.72 pm s', 1.35 ± 0.063 gm S , and 7.88 ± 1.37 [m2s - 1, respectively. Larger molecular weight accounts for slower transport of 20kD dextrans when compared to 10kD dextrans, and negative charge accounts for slower transport of dextran sulfate, consistent with transport studies in arterial tissuelo. The further drop in effective diffusivity of FGF2 is likely due to the effect of tissue binding. Using 10kD dextrans as a reference, the impedance a = Bm Kd + 1 was 512, or B mx Kd = 511. 2.3.2 FGF Distribution is Limited by Myocardial Perfusion Drug transport through and deposition within tissues are governed by molecular weightdependent processes such as diffusion and convection, and physicochemical attributes such as binding, partitioning, and metabolism 2' 22' 23. We 2500 examined the effects of capillary perfusion on myocardial growth factor 2000 a 1500 21000 0 0 500 transport in rat hearts incubated at constant 0 30 90 60 Distance from Epicardium (im) 120 epicardial source concentrations (Fig. 2) with and without controlled coronary flow. When delivered to the ex-vivo FIGURE 4: Myocardial Capillary perfusion Impedes Drug Penetration. Distribution and representative fluorescence microscopy images of TR-FGF2 in rat myocardium with (magenta) and without coronary perfusion (blue). Data represent mean ± s.e.m. (n=3). Penetration depth (x90) is estimated as the location of the 90 % drop-off from the threshold (vertical dashed lines). Error bars were only shown at regular intervals. myocardium in the absence of flow, TR-FGF2 distributed via diffusion to a penetration depth of 66 tm in 6 h (Fig. 4). Restoration of coronary perfusion reduced TR-FGF2 penetration depth more than 2-fold to 28 tm, localizing growth factor closer to the epicardial drug source (Fig. 4). 2.3.3 FGF is Washed-out Through Microvascular Clearance Followed Ex-vivo Myocardial Delivery We further used a highly 10000 sensitive radioactive FGF (35S-FGFl) S 1000 to verify that capillary washout of C 0 FGF through microvascular clearance was indeed responsible for the 100 n 10 reduction in FGF penetration in the 1 0 presence of perfusion. 3 5S-FGF1 was observed in the perfusate at the outflow soon after 35S-FGF1 was delivered at epicardial surface (Fig. 5), suggesting that capillary washout was 0.5 1 1.5 2 2.5 3 3.5 Time (hr) FIGURE 5: FGF is Washed-out Through Microvascular Clearance Followed Ex-vivo Myocardial Delivery. 35 S-FGF1 in the outflow perfusate was measured as a function of time after local epicardial 35 S-FGF1 delivery (n=3). Experimental washout of 35S-FGF-1 (in blue) is well explained by Eq. S 17 (magenta line) using the parameter values of TR-FGF2. indeed responsible for the limited penetration of this growth factor in the presence of perfusion (Fig. 4). These results were further compared to analytical model results of cumulative drug clearance (Eqn M17) calculated using pharmacokinetic parameters of FGF-2 (k = 1.15 + 0.06x 10-4 s-land D=0.02 jm 2/s) derived from experiments. The experimental results fit the model well within one order of magnitude, suggesting that the pharmacokinetics of 35 S-FGF 1 are well explained by our diffusion with clearance model and moreover that the clearance constants and diffusivities of 35S-FGF1 and TR-FGF2 are similar. 2.3.4 SOS limits the effects of capillary washout on FGF2 FGF2 is customarily delivered in association with unfractionated heparin (UFH) to 24 26 protect the growth factor from premature proteolysis - . Given the importance of molecular weight in determining capillary washout and tissue penetration, we characterized the relative effective molecular size of FGF2 when delivered alone and in association with UFH, low molecular weight heparin (LMWH), or SOS. The average molecular size of FGF2 is largest when complexed with UFH and LMWH (Fig. 6). Both FGF2-UFH and FGF2-LMWH span a large range of molecular size, reflecting different degrees of FGF2 multimerization and the intrinsic distribution of 0.04 113kD molecular weights of FGF+UFH 0.03 65kD 42.7kD heparin. Interestingly, > 002 FGF2+SOS FGF2 I FGF2-SOS exhibits an apparent molecular size ooo 7 larger than would be expected from a simple addition of the respective H FGF+L 0.01o 8 9 10 11 12 13 14 15 16 17 Fraction number FIGURE 6: Size exclusion chromatography of FGF2 alone, FGF2 complexed with SOS, FGF2 complexed with low molecular weight heparin (LMWH) and FGF2 complexed with unfractionated heparin (UFH). Molecular weight markers where indicated. molecular weights of the component molecules. This observation is supported by the work of Herr et al. in which they proposed that SOS induced reversible FGF2 dimerization27 We delivered TR-FGF2-SOS via a pericardial reservoir to perfused and non-perfused rat myocardial tissue similarly to the delivery of TR-FGF2 and determined the fluorescence distribution of the drug in tissue. Unlike TR-FGF2, TR-FGF2-SOS appeared to be significantly less sensitive to capillary washout, so that the distributions of TR-FGF2-SOS both with and without coronary flow are nearly Texas red-FGF2-SOS dimer identical (Fig. 7). Therefore, while the 2500 ( 2000 larger size of TR-FGF2-SOS results in lower bulk diffusivity, decreased 8 1500 8 1000 i 500 M sensitivity to capillary washout as a 0 0 30 60 90 120 Distance from epicardium (( m) result of lower trans-endothelial permeability may actually lead to a net tissue drug increased tissue drug uptake uptake and and penetration in a system with capillary perfusion. FIGURE 7: Distribution and representative fluorescence microscopy images of TR-(FGF2) 2 SOS in rat myocardium with coronary perfusion (magenta) and without coronary perfusion (blue). Data represent mean + s.e.m. (n=3). 2.3.5 Effects of Molecular Weight on Myocardial Transport Under Perfusion We further examined the effects of capillary perfusion on myocardial drug transport of model drug compounds of a range of molecular weights (1 kDa Evans Blue Dye, 10 kDa Dextran, 8 kDa 14 14C- C-Dextran sulfate, 17 kDa FGF2, 35 kDa FGF2-SOS, and 65 kDa 125I1 Albumin). For all these drugs, there was less myocardial deposition after 6 hours in the presence of coronary flow compared to no coronary flow (Figs. 8A-F). The reduction in deposited drug with coronary perfusion, computed by normalizing perfused to non-perfused drug deposition, was inversely proportional to molecular weight: 96.3% for Evans Blue Dye (EBD), 91.8% for 14 C-Dextran (14C-Dx), 84.5% for 14 C-Dextran sulfate (14C-DxS) and 53.2% for FGF2. Coronary perfusion did not reduce deposition of FGF2-SOS or 125I-Albumin to a statistically significant degree. The sigmoidal relationship between perfusion-related drug reduction and drug molecular weight appears to have an inflection point at a molecular weight of about 20 kDa (Fig. 8G). 1.5 - A D 1.5 1.0 1.0 0.5 0.5 0.0 0o.o Flow No Flow o 1.5 B 0 1.5 0.5 0.5 a) N 0.0 No FLow Flow No Flow Flow -E 0.0 Flow No Flow 1.5 1.5 0 1.0 1.0 0.5 0.5 0.0 0.0 1000. EBD 8W% - Flow No Flow Flow No Flow 1kD * Dextran 10OkD extran Sulfate 8kD FGF2 7kD FGF2-SOS 35kD 20% G 0 10 20 Albumin 65kD 30 40 50 60 70 Molecular Wght (kD) FIGURE 8: Total drug deposition in rat myocardium following pericardial delivery over 6 hours with and without coronary perfusion, normalized to the no-perfusion case. (A) Evan's Blue Dye in PBS, (B) 8 kDa Dextran sulfate, (C) 10 kDa Dextran, (D) FGF2, (E) FGF2-SOS, and (F) Albumin. (G) Percentage of deposited drug cleared by capillary flow as a function of drug molecular weight displays a sigmoidal pattern. * denotes statistical significance (p < 0.05). 2.3.6 Drug Diffusivity, Trans-endothelial Permeability and Vessel Density Influence Local Drug Distribution and Deposition We examined the impact of coronary 1000 100 flow on drug penetration within the context 0 of a continuum pharmacokinetics model of . 1 10 drug diffusion in the face of microvascular , , , Diffusivity (mlis 2 ) S1000 clearance (Eq. 1, Table 1). In the absence of 100 V perfusion the growth factor distribution 0 curve mimics the analytical solution of the 1.E-05 1.E-04 1.E-03 1.E-02 1.E-01 Permeability (Tlmls) diffusion equation (Eq. 3, Table 1) with an - 1000 0 apparent diffusivity of 0.021 ± 0.001 [im 2s-1 = for TR-FGF2. This value is four orders of 0. 100 10 0.01% magnitude smaller than the reported diffusivity of FGF in free aqueous solution 28, reflecting the impact of steric hindrance and binding within tissues. TR is small (600 Da) and hydrophilic. Its diffusion is significantly higher than FGF in HSPG-rich myocardium and detected fluorescence is likely specific for TR-FGF-2. In the presence of coronary perfusion, the capacity of capillaries to clear drugs is restored and the distribution of TR- 0.10% 1.00% 10.00% volume fraction Capillary FIGURE 9: Continuum Pbarmacokinetic Model. Penetration depth x9o,defined as distance from source to 90 % drop-off threshold,x9o = x ln(O), where f is calculated based on Eq. 4 (Table 1), is expressed as a function of drug diffusivity (A),trans-endothelial permeability (B),and capillary volume fraction (C). Parameter values cover a range of two orders of magnitude below to above those ofFGF2 in the heart. FGF2 diffusivity = 0.02 gm2s1 and clearance constants k were empirically verified, and trans-endothelial permeability derived from Eq. 2 (Table 1). Capillary volume fraction (,,,,) was varied over 3 log orders between the extremes of ischemic and normal tissue vascularity. These relationships are linear in log-log scale axes, demonstrating adherence to power law functions. FGF2 at 6 h approaches an exponential steady state profile 100% .~ 75% consistent with an apparent 50% clearance rate constant k = 1.15 25% * TR-FGF2 " TR-FGF2-SOS - 4 -1 ± 0.06x10 S (Eq. 4, Table 1). Given that normal myocardial capillary density is- 12.9 % 29 and FGF2 aqueous diffusivity (2.2x 102 m2S-1) 28, our estimate of the clearance rate constant of FGF2 implies that trans- 0% 1.E-08 1.E-07 . 1.E-06 1.E-05 1.E-04 1.E-03 1.E-02 1.E-01 1.E+00 k (s "') FIGURE 10: FGF Distribution is Sensitive to Alteration in Drug Clearance. Percent drug cleared by capillaries calculated using the analytical model (Eq. 5, Table 1) as a function of clearance rate constant k (black line). Experimental data points for TR-FGF2 and TR-(FGF2) 2 -SOS analyzed by Eq. Ml (Methods) are superimposed (magenta squares) on model predictions providing perspective on the sensitivity of FGF to manipulation of its clearance constant. endothelial permeability and the 3 permeability-to-diffusivity ratio are approximately 1.9x 10- pms-', and 8.8x 10-6 tm-'. This estimate is in line with the trans-endothelial permeability of a molecule with a molecular size of FGF2 30 Analytic models of drug transport and loss to capillary flow were evaluated across a range of diffusivities, trans-endothelial permeabilities, and microvascular volume fractions. Steady state results (Eq. M7) were used as equilibrium is rapidly achieved. Penetration depth at steady state increases as the square root of the diffusion coefficient (Fig. 9A), and decreases as the square root of the trans-endothelial permeability constant (Fig. 9B). It is worth contrasting our results with those from systemic drug delivery through an intravascular route, where a diametrically opposite relationship exists between tissue penetration and trans-endothelial permeability. Intravascular drugs can only access target tissues by crossing the trans-endothelial barrier. Increasing transvascular penetration in systemic delivery requires drugs that permeate across the endothelium and interventions that increase, rather than decrease, vascular permeability 31 33. Tissues with higher degrees of vascularization, as embodied by the vascular volume fraction, clear drugs faster and have lower steady state drug penetration (Fig. 9C). Thus, steady state drug penetration and distribution are highly dependent on drug diffusivity through tissue and net microvascular clearance, the compounded effect of trans-endothelial permeability and microvascular volume fraction (Eq. 2, Table 1). The theoretical reduction in total deposition due to capillary clearance was calculated (Eq. 5, Table 1) and expressed as a function of the clearance rate constant k (Eqs. M8 and M12). Percent clearance of drug with coronary perfusion is most sensitive for clearance rate constants 1x 10-5 to 1x 10-2 S-1 (Fig. 10). Notably, our measurement of the clearance rate constant of TRFGF2 falls within this range, suggesting that FGF clearance is highly sensitive to transendothelial permeability and microvascular volume fraction. To examine whether the clearance rate constant of FGF might be modulated by altering its physicochemical properties, we used quantitative fluorescence imaging and mathematical modeling to further contrast the distribution of TR-FGF2 alone or in association with sucroseoctasulfate (SOS). SOS induces FGF dimerization and increases the effective molecular weight of TR-FGF2 27. The increase in size was confirmed by size-exclusion chromatography (Fig. 6), and should reduce trans-endothelial permeability, capillary washout, and effective diffusivity. Indeed, in the absence of coronary perfusion, TR-(FGF2) 2 -SOS penetrated 40 % less than TR- FGF2 into the myocardium (40 um,with an effective diffusivity of 0.013 ± 0.001 ~m2S-1) reflecting its increased size (Deff TR-FGF = 0.021 ± 0.001 , Fig. 4 vs. Fig.7). But the larger m2 S-1 compound was also less affected by coronary perfusion, with penetration depth falling only 26 % to 30 um and total deposition falling by only 12 % (Fig. 7). The muted sensitivity of TR(FGF2) 2-SOS to flow (Fig. 10) is consistent with the estimated clearance rate constant (k-4.37 0.33x10-5 s-1), model predictions, and our hypothesis that larger molecules enter capillaries less readily and are less prone to clearance by coronary perfusion. 2.4 Discussion The potential of angiogenic promoters of endothelial cell growth and neocapillary formation is well established in cell and tissue culture models 34 ,35. Unfortunately, when delivered to ischemic myocardium in human clinical trials, angiogenic growth factors have yet to produce stable, sustained angiogenesis36' 37 . While there are undoubtedly biological factors involved38 , our study suggests that fundamental physical barriers can also impair the realization of sustained angiogenesis. Chief among these is capillary washout increasing clearance and restricting penetration of angiogenic growth factors into myocardial tissue. 2.4.1 Capillaries limit drug penetration in a manner dependent on molecular weight For all but the largest molecules, myocardial capillary networks promote drug washout. Having entered the capillary lumen, drugs become subject to downstream convective forces far in excess of trans-endothelial diffusive forces, so that rather than acting as conduits and fostering deposition deeper in the myocardium, capillary flow actually limits drug penetration. Our data show that the degree to which drug penetration is affected depends on the size of the compound. 1 kDa Evans Blue Dye, 8 kDa Dextran Sulfate, 10 kDa Dextran are all essentially entirely washed out in the presence of coronary flow, whereas albumin and FGF2-SOS are relatively unaffected. The relationship between capillary washout and molecular weight is sigmoidal, suggesting an "on-off' mechanism, wherein molecules below a threshold (- 20 kDa) permeate through pores within the endothelium (3.5 to 7 nm diameter 39, 40), and molecules above the threshold do not. The splay in the sigmoidal curve about the inflection point likely reflects the range of sizes of trans-endothelial pores. Vasoactive drugs which affect capillary permeability may affect both the actual threshold and the slope of the splay. 2.4.2 Ischemic and non-ischemic tissues present different barriers to transport In normally vascularized myocardium, cardiac myocytes are arranged in a complicated three-dimensional configuration, with more than 2000 capillaries per square mm between two capillaries is only three times their diameter 17. 41. The distance As myocardium progresses to ischemia and infarction, this density of vascularity declines markedly. Because capillaries act as spatially distributed barriers to the transport of drug molecules, regions with denser functional vascularity will clear drug more efficiently and rapidly create low drug zones. Gradations in vascularity across the myocardium as a result of ischemic events therefore have important consequences for angiogenic drug delivery. Since capillary flows in ischemic and infarcted regions are substantially less than in normal tissue, our data predict that drug penetration would be greater in ischemic and infarcted areas. Therefore, placing delivery devices directly in the ischemic region should confer pharmacokinetic advantages of decreased capillary washout. If placed in well-perfused regions, drug molecules may never reach ischemic areas at sufficient levels. For instance, pericardial delivery of angiogenic growth factors to target endocardial ischemic regions may prove to be futile since drugs will not easily cross the wellperfused epicardial region. Appropriate positioning of the drug source is therefore critical to achieve adequate drug concentrations in target tissues. 2.4.3 Angiogenesis limits its own success An intriguing implication of our data is that drug delivery for therapeutic angiogenesis may ultimately be self-defeating. Since the ultimate purpose of angiogenic therapy is to induce growth of collateral blood vessels, over time capillary density would increase at a rate of growth dependent on the spatial angiogenic factor distribution. As angiogenic treatment proceeds, neocapillaries would begin to increase drug washout, ultimately limiting the very angiogenic process the treatment is trying to promote. This negative feedback could account for why therapeutic angiogenesis has not been sustained in clinical trials. The full implications of a treatment modality can ultimately be limited by its own effect merit detailed investigation, and is the subject of studies in the subsequent chapters. 2.5 Summary Complex pharmacokinetics drives the transport of angiogenic growth factors through myocardium. Capillary networks impede drug uptake and penetration by increasing drug elimination through washout. Trans-endothelial permeability and vessel density increase drug washout in a similar manner. Drug transport in perfused myocardium can be adequately explained by a diffusion-elimination model, and an empirically derived clearance rate constant can be obtained and used to predict the drug's pharmacokinetic advantage. Careful drug selection and device placement are critical to achieve adequate drug concentration in target tissue. Protective groups, if carefully selected, act to curtail the effects of capillary washout. These results further imply that even when angiogenic therapy achieves some degree of neocapillary formation, they may in turn act as sinks for drug washout, ultimately reducing the effectiveness of the growth factors. 2.6 References 1. 2. 3. 4. 5. 6. 7. 8. 9. 10. 11. 12. 13. 14. 15. 16. 17. Lazarous DF, Shou M, Stiber JA, Dadhania DM, Thirumurti V, Hodge E, Unger EF. Pharmacodynamics of basic fibroblast growth factor: route of administration determines myocardial and systemic distribution. Cardiovasc Res. 1997; 36:78-85. 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Persistent primary coronary dilation induced by transatrial delivery of nitroglycerin into the pericardial space: a novel approach for local cardiac drug delivery. J Am Coll Cardiol. 1999; 33:2073-2077. Ayers GM, Rho TH, Ben-David J, Besch HR, Jr., Zipes DP. Amiodarone instilled into the canine pericardial sac migrates transmurally to produce electrophysiologic effects and suppress atrial fibrillation. J Cardiovasc Electrophysiol. 1996; 7:713-721. Kohnoe S, Maehara Y, Takahashi I, Saito A, Okada Y, Sugimachi K. Intrapericardial mitomycin C for the management of malignant pericardial effusion secondary to gastric cancer: case report and review. Chemotherapy. 1994; 40:57-60. Buselmeier TJ, Davin TD, Simmons RL, Najarian JS, Kjellstrand CM. Treatment of intractable uremic pericardial effusion. Avoidance of pericardiectomy with local steroid instillation. Jama. 1978; 240:1358-1359. Elmalak O, Lovich MA, Edelman E. 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Nat Biotechnol. 1998; 16:136-137. Baxter LT, Zhu H, Mackensen DG, Jain RK. Physiologically based pharmacokinetic model for specific and nonspecific monoclonal antibodies and fragments in normal tissues and human tumor xenografts in nude mice. Cancer Res. 1994; 54:1517-1528. Hershey JC, Corcoran HA, Baskin EP, Gilberto DB, Mao X, Thomas KA, Cook JJ. Enhanced hindlimb collateralization induced by acidic fibroblast growth factor is dependent upon femoral artery extraction. Cardiovasc Res. 2003; 59:997-1005. Laham RJ, Rezaee M, Post M, Novicki D, Sellke FW, Pearlman JD, Simons M, Hung D. Intrapericardial delivery of fibroblast growth factor-2 induces neovascularization in a porcine model of chronic myocardial ischemia. J Pharmacol Exp Ther. 2000; 292:795802. von Degenfeld G, Raake P, Kupatt C, Lebherz C, Hinkel R, Gildehaus FJ, Munzing W, Kranz A, Waltenberger J, Simoes M, Schwaiger M, Thein E, Boekstegers P. Selective pressure-regulated retroinfusion of fibroblast growth factor-2 into the coronary vein enhances regional myocardial blood flow and function in pigs with chronic myocardial ischemia. J Am Coll Cardiol. 2003; 42:1120-1128. Herr AB, Omitz DM, Sasisekharan R, Venkataraman G, Waksman G. Heparin-induced self-association of fibroblast growth factor-2. Evidence for two oligomerization processes. J Biol Chem. 1997; 272:16382-16389. Filion RJ, Popel AS. A reaction-diffusion model of basic fibroblast growth factor interactions with cell surface receptors. Ann Biomed Eng. 2004; 32:645-663. Wacker CM, Bauer WR. Myocardial microcirculation in humans--new approaches using MRI. Herz. 2003; 28:74-81. Michel CC, Curry FE. Microvascular permeability. Physiol Rev. 1999; 79:703-761. Dreher MR, Liu W, Michelich CR, Dewhirst MW, Yuan F, Chilkoti A. Tumor vascular permeability, accumulation, and penetration of macromolecular drug carriers. J Natl Cancer Inst. 2006; 98:335-344. Lejeune FJ. Clinical use of TNF revisited: improving penetration of anti-cancer agents by increasing vascular permeability. J Clin Invest. 2002; 110:433-435. Siegal T, Zylber-Katz E. Strategies for increasing drug delivery to the brain: focus on brain lymphoma. Clin Pharmacokinet. 2002; 41:171-186. Dinbergs ID, Brown L, Edelman ER. Cellular response to transforming growth factorbetal and basic fibroblast growth factor depends on release kinetics and extracellular matrix interactions. J Biol Chem. 1996; 271:29822-29829. 35. 36. 37. 38. 39. 40. 41. 42. Nabel EG, Yang ZY, Plautz G, Forough R, Zhan X, Haudenschild CC, Maciag T, Nabel GJ. Recombinant fibroblast growth factor-i promotes intimal hyperplasia and angiogenesis in arteries in vivo. Nature. 1993; 362:844-846. Henry TD, Annex BH, McKendall GR, Azrin MA, Lopez JJ, Giordano FJ, Shah PK, Willerson JT, Benza RL, Berman DS, Gibson CM, Bajamonde A, Rundle AC, Fine J, McCluskey ER. The VIVA trial: Vascular endothelial growth factor in Ischemia for Vascular Angiogenesis. Circulation. 2003; 107:1359-1365. Simons M, Annex BH, Laham RJ, Kleiman N, Henry T, Dauerman H, Udelson JE, Gervino EV, Pike M, Whitehouse MJ, Moon T, Chronos NA. Pharmacological treatment of coronary artery disease with recombinant fibroblast growth factor-2: double-blind, randomized, controlled clinical trial. Circulation. 2002; 105:788-793. Cao R, Brakenhielm E, Pawliuk R, Wariaro D, Post MJ, Wahlberg E, Leboulch P, Cao Y. Angiogenic synergism, vascular stability and improvement of hind-limb ischemia by a combination of PDGF-BB and FGF-2. Nat Med. 2003; 9:604-613. Kellen MR, Bassingthwaighte JB. Transient transcapillary exchange of water driven by osmotic forces in the heart. Am J Physiol Heart Circ Physiol. 2003; 285:H1317-1331. Marcus ML, Chilian WM, Kanatsuka H, Dellsperger KC, Eastham CL, Lamping KG. Understanding the coronary circulation through studies at the microvascular level. Circulation. 1990; 82:1-7. Stoker ME, Gerdes AM, May JF. Regional differences in capillary density and myocyte size in the normal human heart. Anat Rec. 1982; 202:187-191. Finsen AV, Woldbaek PR, Li J, Wu J, Lyberg T, Tonnessen T, Christensen G. Increased syndecan expression following myocardial infarction indicates a role in cardiac remodeling. Physiol Genomics. 2004; 16:301-308. Chapter 3: Interdependence of Local Pharmacokinetics and Pharmacodynamics Abstract The challenge of angiogenesis science is that stable, sustained vascular regeneration in humans has not been realized despite promising preclinical findings. We hypothesized that the challenges faced by angiogenic therapies reflect powerful self-regulation by dynamic alteration of tissue characteristics. In Chapter 2, through ex-vivo and mathematicalmodels we showed that FGF spatial loading was significantly reduced with intact coronary perfusion, and that penetration and loading decreased with trans-endothelial permeability and higher vascularity. Induction of neocapillaries as the goal of angiogenic therapy adds pharmacokinetic complexity because it induces changes in both permeability and vascularity. In this chapter, through an invivo model of local growth factor delivery to ischemic rabbit heart, we showed that sustained local FGF delivery in vivo produced a burst of neovascularization in ischemic myocardium but was followed by drug washout and a five-fold decrease in FGF penetration depth. The very efficacy of pro-angiogenic compounds enhances their clearance and abrogates their pharmacologic benefit. This self-limiting property of angiogenesis may explain the failures of promising pro-angiogenic therapies. 3.1 Introduction Stimulation of neovascularization using angiogenic growth factors might reduce myocardial infarct size and improve cardiac function', and peripheral tissue 2 perfusion. Yet, impressive results in tissue culture and animal studies 3-7 have not been sustained in clinical trials8 11 . Intravascular delivery of angiogenic factors is convenient but challenged by the requirements for high doses and long residence times 8 ' 10. Cell and gene injections might provide a continuous source of growth factor, and intramyocardial or pericardial delivery have elevated local tissue drug concentrations with lower systemic exposure in animal modelsl2. However, the promise of symptomatic improvement and increased capillary density seen in early clinical trials with intramyocardial injections of FGF2 after coronary artery bypass graftingl 3 has not endured in larger clinical trials, and clinical outcomes in general with local growth factor delivery have been mixed9' 14-18 Some have postulated that myocardial growth factor concentrations and/or drug residence time were inadequate for sustained angiogenesis despite controlled release delivery 19 , and yet, the local pharmacokinetic processes governing uptake and distribution of growth factors in highly vascularized tissues such as myocardium remain undefined. It is possible that the reverse is true and concentrations may be more than sufficient. In Chapter 2, we showed that coronary perfusion impedes drug penetration by increasing drug clearance through microvascular washout. In this Chapter, we hypothesized that local delivery can induce neocapillary growth but in doing so changes the balance between drug delivery and microvascular drug clearance favoring the latter, such that the very pharmacologic efficacy of these compounds limits their biological effect. To test this hypothesis, we used sustain growth factor release technology and in vivo ischemic heart model to quantify how drugs move within vascularized tissue, and how neovascularization following delivery of angiogenic growth factors affects their pharmacokinetics and efficacy. These studies are the first to track both drug distribution and angiogenic response simultaneously upon local growth factor delivery, and strongly suggest that angiogenesis is powerfully self-regulating as the capillaries induced by angiogenic drug therapy may increase clearance rates limiting tissue levels of growth factor and subsequent angiogenesis even with sustained delivery. 3.2 Materials and Methods 3.2.1 Recombinant S35-FGF1 Production 35S-FGF1 was chosen as a model SELECTED FRACTIONS S35-FGF1 / for FGF in the in-vivo setting because S- - its high detection sensitivity allows for 0.75 NaCI] Radioactivity S0.75- the possibility of tracking spatial drug distribution in the setting of controlled delivery of therapeutic doses. It also UV Absorbance o.s5 ' , 0.25- 0 . 10 30 . 50 .70 70 Elution Volume (mL) presents a safer alternative to using 25I labeled FGF2 in-vivo. Recombinant human FGF1 was expressed in Escherichiacoli strain BL21-pLysS FIGURE 1: Recombinant S35-FGF1 production and purification. Elution profiles of protein and radioactivity following binding to heparin sepharose column and application of NaCl gradient. Eluted fractions selected for experiments are shown in highlighted area. transformed by plasmid, pET3c that confers resistance to ampicillin and encodes FGF1 (obtained as a gift from the late Dr. Thomas Maciag, Maine Medical Center, Portland, ME). Transfected bacteria stocks were added to LB medium (MP Biomedicals) containing 100 tg/mL Carbenicillin and 35 pg/mL Chloramphenicol (Sigma-Aldrich) and incubated with vigorous shaking at 250 RPM at 370 C overnight. Bacteria culture was then diluted in antibiotics-free LB medium (1:40 v/v of bacteria/medium) and incubated with vigorous shaking at 250 RPM and the optical density of the solution was measured at 600 nm. When cell culture reached an optical density of 0.6-0.8 bacteria were centrifuged and resuspended in DMEM medium deficient in L-cysteine and L-methionine (Invitrogen) supplemented with 1 % L- glutamine and 7.15 mCi of 35S (Promix L- [35S]Methionine and Cysteine, GE Healthcare Life Sciences) and buffered with 25 mM HEPES (Invitrogen) and then induced with 0.4 mM IPTG for 3 h with shaking at 250 RPM at 370 C. Cells were then collected by centrifugation at 8000 RPM for 10 m and kept frozen at -800 C. Frozen cell pellets were resuspended in lmg/ml lysozyme in GET buffer (50 mM Tris, 10 mM EDTA, 100 mM glucose, pH 8.0), mixed well for 5 m and then homogenized (Polytron; Kinematica) 5 times for 30 s each with break periods of 60-90 s at 40 C to prevent overheating and denaturation of proteins. Cell lysate was collected by centrifugation at 9,000 RPM for 10 m at 4°C. 35S-FGF1 was then purified using affinity chromatography with FPLC. Bacterial lysates were loaded into 5 ml heparin sepharose column (HiTrap Heparin HP column, GE Healthcare Life Sciences) and allowed to bind for 1 h at room temperature. The FPLC system was programmed to wash the column with PBS and gradually increase NaCl concentration with a linear gradient (0.15-2 M). Elutions of 1 mL were collected and assayed for protein concentration (absorbance at 280 nm, FPLC System) and radioactivity (2500TR Liquid Scintillation Analyzer, Packard). Elution peaks of protein concentration and radioactivity coincided (Fig. 1). The 35S protein product came out of the heparin sepharose column at 1.4 M to 1.6 M NaC1, similar to FGFI, and indicating 35S was incorporated in FGF 1. These elution fractions were collected and further purified for use in experiments. 35S-FGF1 solution was desalted by centrifugation using centrifugal filter devices with a 10 kDa molecular weight cut-off (Centricon, Millipore). The presence of FGF1 was confirmed at a 18 kDa band using SDS-PAGE and protein quantification was carried out using BCA assay (Pierce). Bioactivity of FGF 1 was confirmed in proliferation assays of bovine aortic endothelial cells. FGF1 was further purified from any endotoxin contamination using endotoxin removing columns (Detoxi-Gel AffinitiPak columns, Pierce), and the FGF1 purity was confirmed with limulus amebocyte lysate assay (Pyrotell-T, Associates of Cape Cod Inc., MA). Purification was continued (typically 2-3 times) until endotoxin concentration is below 0.01 EU/[tg FGF1. 3.2.2 Fabrication and Kinetics of Controlled Release Device A slurry mixture of heparin-Sepharose beads/alginate solution was prepared by mixing sterilized heparin-Sepharose microbeads (GE Healthcare) with filter-sterilized sodium alginate (Sigma-Aldrich, 5 %), placed in a customized 20mm x 20mm x Imm glass mold, and incubated overnight in filter-sterilized 10 % CaCl 2 . The heparin-Sepharose embedded sodium alginate material is exposed to CaCl 2 through two open surfaces of the mold. The gel was further incubated in the 10 % CaCl 2 for 24 h to allow thorough cross-linking of the polymer after being taken out of the mold under UV light for sterilization. The hardened polymeric gel device was then incubated in 35S-FGF solution for 48 h prior to experiment to allow complete and uniform loading of drug. To characterize 35S-FGF 1 release kinetics from the device, 8 mm diameter circular shape devices were made from the 20 x 20 x 1 mm 3 polymeric slab using 8 mm biopsy punch (Miltex). These circular devices were incubated in 1 ml PBS and gently agitated throughout the experiment with a shaker. At various time points the elution mixture was collected and assayed for 35S activity using liquid scintillation counter (Packard). Fresh PBS was used to renew the elution buffer. 3.2.3 In-vivo Myocardial Drug Delivery Rabbits (New Zealand White, 3-3.5 kg) received an intramuscular injection of 35 mg kg' ketamine and 5 mg kg' of xylazine, and inhaled isoflurane anesthesia (1-3%) and positive pressure ventilation via a 3.0 mm endotracheal tube. The chest was shaved and sterilely prepared with Betadine and alcohol. A left thoracotomy was performed after local lidocaine injection. A clamp kept the chest open and a small opening in the pericardium was created with care to minimize pericardial damage. The left anterior descending coronary artery was ligated. Ischemia was confirmed by ST segment elevation on simultaneous continuous electrocardiography (Fig. 2A). Sodium alginate polymeric devices sustain-releasing 35S-FGF1 from encapsulated heparin Sepharose beads (Fig. 2B) were placed in the pericardial space (Fig. 2C) and the pericardiotomy suture-repaired to prevent leakage. The thoracotomy and skin incision were closed. Positive endexpiratory pressure ventilation and a negative pressure chest tube prevented pneumothorax. Analgesia was with 0.03 mg kg'-buprenorphine subcutaneous injections every 8 h for the first 72 h. Control animals received alginate encapsulated heparin Sepharose beads without FGF. Hearts were harvested 2, 8, 16 and 31 days after surgery, the aorta cannulated, flushed retrogradely with PBS, and snap-frozen in liquid nitrogen. Drug release devices were confirmed to be physically intact and adhered to epicardium at up to 1 month (Fig. 2 D&E). B After LAD Coronar Li ation D MYO FIGURE 2: In-vivo ischemic heart model of local myocardial delivery of FGF. Ischemic heart model was induced by ligation of left anterior descending coronary arteries. Evidence of ischemia was checked with EKG (A). Heparin sepharose microbeads 35 embedded in sodium alginate device was used to sustain release S -FGF1 (B). Pericardial cradle was created to allow LAD ligation and placement of controlled release drug devices (C). Devices were physically intact up to 1 month in-vivo (D). Cross section of rabbit heart with zoomed in H&E stained micrograph showing the proximity of drug release device to epicardium. 3.2.4 Quantification of in-vivo FGF1 and Blood Vessels Distribution Two frozen myocardial cores were excised adjacent to the polymeric devices using an 8 mm diameter biopsy punch (Miltex). One core was mounted and cryosectioned (Leica CM1850) into 100 gm sections parallel to the epicardium. Sections were digested in 1 ml of Solvable tissue solubilizer (PerkinElmer) at 60 0 C overnight prior to radioactivity quantification (2500TR Liquid Scintillation Analyzer, Packard). The discrete spatial FGF1 concentration data were fit to the exponential profile implied by Eq. 4 (Table 1) using GraphPad software (Prism 5). The fit was used to estimate the penetration depth x90 , defined as distance from source to 90 % drop-off threshold, as x90 = g x ln(10). The other tissue core was cryo-sectioned into 10 ptm thick sections in transmural direction. Sections were fixed for 5 m with 4 % paraformaldehyde (Electron Microscopy Sciences), washed for 30 s with cold acetone (Sigma-Aldrich), incubated in blocking serum (200ptl of 1 % chicken serum, 1 h, 37°C), then in goat anti-PECAM-1 IgG (Santa Cruz Biotechnology, 200pl of 1:50 dilution, 2 h, 370 C), washed three times in 0.1 % Tween 20 in PBS, incubated further with Alexa Fluor 488 chicken anti-goat IgG (Invitrogen, 200tl 1:200 dilution, 2 h, 370C), washed three times in Tween 20/PBS, cover-slip mounted, and imaged immediately with a fluorescence microscope (Leica DMRA2, FITC filter set). The images were thresholded to maximize the signal to noise ratio with Matlab (Mathworks, MA), yielding binary images of vessel distribution. Neovascular formation of tissue regions within 500 itm from epicardial source was quantified by computing the tissue area fraction stained by PECAM-1 (total number of pixels with PECAM-1 stain / total number of pixels of tissue area). 3.2.5 Statistical analysis All data were presented as means + s.e.m., except values for the clearance rate constants k which were reported as means + propagated standard errors. Statistical analyses were performed with the Student's t test where appropriate. P<0.05 (two-tailed) was considered statistically significant. 3.3 Results 3.3.1 Polymeric Devices Sustain Release FGF1 over 30 days in-vivo S35-FGF1 can be released with heparin sepharose beads / sodium alginate devices over 30 days in-vitro (Fig. 3, dashed line), with the shape consistent with previous study 20. The release kinetics in-vivo was indirectly obtained from the amount of initial drug and drug remained in release devices after each treatment period with the assumption that the burst release phase similar to those in-vitro. This result also suggested that S35 -FGF1 was released at a steady rate 125 o In-vitro - * In-vivo 100 - S....................... 00 * Burst Release 0 0 5 10 15 20 25 30 Time (days) FIGURE 3: Polymeric Devices Sustain Release FGF1 over 30 days. Percentage of cumulative 35S-FGF1 released into PBS buffer in-vitro (white diamonds, data represent mean + s.e.m. (n= 10), 100% corresponds to approximately 90tg 35S-FGF1 per circular disk of 8mm diameter and 1 mm thickness), and throughout in-vivo experiment (black circles, data represent mean ± s.e.m. (n=3), 100% corresponds to approximately 450 gpg 35 S-FGF1 per device (20mm x 20mm x Imm) for in-vivo experiments), calculated by % drug released = (total drug within source - total drug remaining)/ total drug within source x 100 %. in-vivo after the burst phase (Fig. 3, solid line). 3.3.2 In-vivo Angiogenic Response Limits Drug Distribution Conventional pharmacokinetic models for drug distribution do not take into account the potential that drugs can alter capillary density, trans-endothelial permeability or drug clearance. Yet, angiogenic growth factors such as FGF1 and FGF2 are specifically administered to induce capillary growth, and it would be unreasonable to assume that trans-endothelial permeability and drug clearance are not similarly modified. Induced neovascularization implies an increase in the density of blood capillaries that could provide negative feedback limiting growth factor tissue penetration (Fig. 16C, Chapter 2). Our analysis of myocardial drug transport suggested that FGF would be particularly sensitive to induced capillary washout (Figs. 9 and 17, Chapter 2). We tested this hypothesis in vivo using radiolabeled FGF1 (35S-FGF1). TR-FGF2 could not be used in vivo as its labeling intensity is much lower than that of 35S-FGF 1, rendering it virtually transparent at the doses delivered. Following the sustain-release of biologically active 35S-FGF1 fractions with heparin Sepharose-alginate wafers, FGF1 successfully penetrated 442 + 91 pm into the myocardium over the first two days after release initiation. Yet, despite sustained delivery, penetration regressed over time falling 5-fold by day 8 (81 + 30 tm), and remained low through day 31 (Fig. 4B). Enhanced growth factor clearance was associated with the induction of neovasculature (Fig 5A), after controlled for any angiogenesis with devices without FGF1 (Fig. 5B). Two days after device implantation the fraction of PECAM-1 stained tissue was 56 % greater in animals receiving FGF1 (4.4 %) compared to baseline density (2.8 %) in control animals with identical devices devoid of growth factor (P < 0.05, Fig. 6). Neovascularization peaked at day 8 (8.7 %) doubled that from day 2 (P < 0.01, Fig. 6), coinciding with the drop in drug distribution. Similarly, the fraction of PECAM- I1stained tissue decreased significantly from day 8 to day 31 (62 % P < 0.01, Fig. 6), most likely from regression of neocapillaries as the concentration of FGF1 becomes sub-therapeutic. Drug delivery devices were examined for remaining drug content after each treatment period to verify that the decreasing myocardial concentrations arose from increasing capillary clearance rather than decreasing drug delivery. None of the delivery devices were depleted of drug, and all continued to release drug with constant flux (Fig. 3) following the expected burst release of-37.5 % during the first 6 h. 1.5x10 05 B 0o E Day 2 Day8 Penetration depth C 1.0x10 05 S C.. 5.0x10 06 * Day 31 0.0x10 -00 0 200 400 600 Distance from epicardium ( 800 1000 pm) FIGURE 4: FGF1 penetrates myocardium at day 2 but regressedat later time points. Spatial profile of S3 -FGF 1 from epicardium was obtained by serial sectioning of myocardial plug (A). S35 -FGF1 spatial concentration distribution at days 2, 8, and 31 following coronary ligation and implantation of sustained release source was quantified using liquid scintillation counting of sectioned tissues. Data represent mean ± s.e.m. (n=3) HS / Alginate with FGF-1 Day 2 Source B Day 8 Day 31 Pene ration depth Control: HS /Alginate without FGF-1 Day 31 Day 8 Day 2 FIGURE 5: Representative fluorescent images of PECAM-1 labeled blood vessels in tissue regions adjacent to drug source for experimental animals receiving heparin-Sepharose beads / alginate source with S35-FGF1 and control animals receiving devices without FGF1. Dashed red line on the right edge denotes interface between source and epicardium. Magenta, blue and green dashed lines represent the penetration depth at 90 % drop-off threshold from tissue/source interface calculated from spatial S35FGF1 distributions. Scale bars represent 100 pm. 0.10- NS < L 0.08-** 0.06 -*- Control FGF1 . 0.04- 2 0.02- 0 7 14 21 Time (d) 28 35 FIGURE 6: Vascular to tissue surface fraction (calculated by normalizing total number of pixels stained by PECAM-1 to total tissue area within 500 im depth from source) is expressed as a function of time. Data points represent PECAM-1 stained surface fraction of individual hearts (n=3), and connecting lines denote trend of mean value. * denotes P < 0.05. ** denotes P < 0.01 (P = 0.007 between days 2 and 8, and P = 0.003 between days 8 and 31). 3.4 Discussion While biological factors 2 1 might be responsible for unsuccessful realization of angiogenic growth factors potential to induce stable sustained collaterals in clinical trials' 10 , our study suggests a fundamental barrier in local drug delivery, in particular the self-limiting pharmacokinetics of angiogenic therapy to impair the induction and maintenance of sustained neovascularization. The previous chapter revealed that drug trans-endothelial permeability plays a vital role in governing drug distribution. Lower trans-endothelial permeability ensures greater myocardial drug penetration following local application (Fig. 16B). The dependence of drug distribution on trans-endothelial permeability and capillary density takes on further complexity for angiogenic compounds that can remodel the tissue into which they are being delivered. Over the course of treatment, vessel density in ischemic tissues increases in FGF -laden tissue regions (within 500600 p.m depth from epicardium, Fig 5A). Indeed, abundant neovascularization occurs from day 2 to 8, but drug washout rises as well precipitously dropping the local tissue concentration and penetration depth of FGF 1 (Fig 4B), despite no quantifiable change in growth factor delivery. FGF- 's instability in the absence of heparin 22 cannot account for the observed effects, as the factor was released directly from the heparin Sepharose devices to the epicardial tissue (Fig. 2E). Released FGF-1 likely binds reversibly to myocardial HSPGs, prolonging tissue half-life. Indeed, angiogenic activity was observed 8 days after delivery (Fig 5A). Moreover, changes in angiogenic action correlated with regression of FGF distribution, not a decrease in activity or stability. Continuum pharmacokinetic model (Eq. M15, Chapter 2) suggest a 5-fold increase in capillary washout between days 2-8. Such an increase in the FGF1 clearance could arise from an increase in microvascular density and/or trans-endothelial permeability (Eq. 2, Table 1). The observed 65 % rise in capillary density between days 2 and 8 (Fig. 6) indicates that the latter plays a dominant role and suggests that the induced vasculature is immature and highly permeable to FGF1. Our findings in this chapter and in chapter 2, therefore, offer possibilities for engineering drugs to penetrate tissue better by reducing their trans-endothelial permeability. FGF2 lies within the region where drug penetration depth is highly sensitive to the clearance rate constant k (Fig. 17, Chapter 2) which is directly proportional to trans-endothelial permeability (Eq. 2, Table 2, Chapter 2), whereas (FGF2) 2 -SOS with its 2.6 times lower clearance is less affected by flow. More than 50 % of FGF2 is cleared by coronary perfusion, but only 12 % for (FGF2) 2-SOS (Fig. 9 vs. Fig. 14, Chapter 2). Therefore, one way to decrease permeability is to consider drugs of higher molecular weight. While higher molecular weight implies lower myocardial drug diffusivity, the ratio of permeability to diffusivity can drop two orders of magnitude as molecular radius increases from 2.4 to 36 A 23. A different method for modulating trans-endothelial permeability can be modification of drug charge. Indeed, it has been shown that negatively charged dextrans exhibit 10 times lower trans-endothelial permeability than neutral analogs 24. This approach may present a method for lowering trans-endothelial permeability of a drug to increase penetration depth and deposition. These integrated studies (Chapter 2 and 3) suggested that angiogenesis is powerfully selfregulating as the very capillaries induced by angiogenic drug therapy may increase clearance as well. The pharmacodynamic changes during the early angiogenic therapy can tip the pharmacokinetics to conditions that are unfavorable for growth factor penetration, which in turn affects long term therapeutic goals. This mechanism implies a natural upper limit effect for pharmacologic revascularization which restricts angiogenic drug penetration and spatially confines the sprouting of new vessels near the drug source. At day 31, the FGF 1 level in the 100500 jtm tissue region falls to undetectable levels, and significant regression of neovascularization consequently occurs in the absence of local growth factor (Fig. 6, day 31). One might well imagine that such forces are essential to endogenous regulation of tissue morphogenesis and repair, and that loss of such regulation may help explain the growth of vascular tumors, and other arterial-venous malformations and anomalies. The interdependence of the pharmacokinetics and pharmacodynamics elucidated in this study may explain the difficulty of realizing the clinical potential of angiogenic compounds and suggests that efficacy becomes critically dependent on device placement and drug's transendothelial permeability. The quantitative framework presented here and in Chapter 2 may help guide rational selection of angiogenic compounds based on a favorable physicochemical profile, and drug delivery strategies that take advantage of the regulation between growth factor pharmacokinetics and angiogenic pharmacodynamics. In Chapter 4, we will attempt to achieve this goal through computational modeling building on the experimental results presented in Chapter 2 and 3. 3.5 References 1. 2. 3. 4. 5. 6. 7. 8. 9. 10. 11. Yanagisawa-Miwa A, Uchida Y, Nakamura F, Tomaru T, Kido H, Kamijo T, Sugimoto T, Kaji K, Utsuyama M, Kurashima C. Salvage of infarcted myocardium by angiogenic action of basic fibroblast growth factor. Science. 1992; 257:1401-1403. Takeshita S, Pu LQ, Stein LA, Sniderman AD, Bunting S, Ferrara N, Isner JM, Symes JF. Intramuscular administration of vascular endothelial growth factor induces dosedependent collateral artery augmentation in a rabbit model of chronic limb ischemia. Circulation. 1994; 90:11228-234. Harada K, Friedman M, Lopez JJ, Wang SY, Li J, Prasad PV, Pearlman JD, Edelman ER, Sellke FW, Simons M. Vascular endothelial growth factor administration in chronic myocardial ischemia. Am J Physiol. 1996; 270:H1791-1802. Lopez JJ, Edelman ER, Stamler A, Hibberd MG, Prasad P, Thomas KA, DiSalvo J, Caputo RP, Carrozza JP, Douglas PS, Sellke FW, Simons M. Angiogenic potential of perivascularly delivered aFGF in a porcine model of chronic myocardial ischemia. Am J Physiol. 1998; 274:H930-936. Montesano R, Vassalli JD, Baird A, Guillemin R, Orci L. Basic fibroblast growth factor induces angiogenesis in vitro. Proc Natl Acad Sci U S A. 1986; 83:7297-7301. Unger EF, Banai S, Shou M, Lazarous DF, Jaklitsch MT, Scheinowitz M, Correa R, Klingbeil C, Epstein SE. Basic fibroblast growth factor enhances myocardial collateral flow in a canine model. Am J Physiol. 1994; 266:H1588-1595. Watanabe E, Smith DM, Sun J, Smart FW, Delcarpio JB, Roberts TB, Van Meter CH, Jr., Claycomb WC. Effect of basic fibroblast growth factor on angiogenesis in the infarcted porcine heart. Basic Res Cardiol. 1998; 93:30-37. Simons M, Annex BH, Laham RJ, Kleiman N, Henry T, Dauerman H, Udelson JE, Gervino EV, Pike M, Whitehouse MJ, Moon T, Chronos NA. Pharmacological treatment of coronary artery disease with recombinant fibroblast growth factor-2: double-blind, randomized, controlled clinical trial. Circulation. 2002; 105:788-793. Rajagopalan S, Mohler ER, 3rd, Lederman RJ, Mendelsohn FO, Saucedo JF, Goldman CK, Blebea J, Macko J, Kessler PD, Rasmussen HS, Annex BH. Regional angiogenesis with vascular endothelial growth factor in peripheral arterial disease: a phase II randomized, double-blind, controlled study of adenoviral delivery of vascular endothelial growth factor 121 in patients with disabling intermittent claudication. Circulation. 2003; 108:1933-1938. Henry TD, Annex BH, McKendall GR, Azrin MA, Lopez JJ, Giordano FJ, Shah PK, Willerson JT, Benza RL, Berman DS, Gibson CM, Bajamonde A, Rundle AC, Fine J, McCluskey ER. The VIVA trial: Vascular endothelial growth factor in Ischemia for Vascular Angiogenesis. Circulation. 2003; 107:1359-1365. Gyongyosi M, Khorsand A, Zamini S, Sperker W, Strehblow C, Kastrup J, Jorgensen E, Hesse B, Tagil K, Botker HE, Ruzyllo W, Teresinska A, Dudek D, Hubalewska A, Ruck A, Nielsen SS, Graf S, Mundigler G, Novak J, Sochor H, Maurer G, Glogar D, Sylven C. NOGA-guided analysis of regional myocardial perfusion abnormalities treated with intramyocardial injections of plasmid encoding vascular endothelial growth factor A-165 in patients with chronic myocardial ischemia: subanalysis of the EUROINJECT-ONE multicenter double-blind randomized study. Circulation. 2005; 112:I157-165. 12. 13. 14. 15. 16. 17. 18. 19. 20. 21. 22. 23. Lazarous DF, Shou M, Stiber JA, Dadhania DM, Thirumurti V, Hodge E, Unger EF. Pharmacodynamics of basic fibroblast growth factor: route of administration determines myocardial and systemic distribution. Cardiovasc Res. 1997; 36:78-85. Laham RJ, Chronos NA, Pike M, Leimbach ME, Udelson JE, Pearlman JD, Pettigrew RI, Whitehouse MJ, Yoshizawa C, Simons M. Intracoronary basic fibroblast growth factor (FGF-2) in patients with severe ischemic heart disease: results of a phase I open-label dose escalation study. J Am Coll Cardiol. 2000; 36:2132-2139. Hedman M, Hartikainen J, Syvanne M, Stjernvall J, Hedman A, Kivela A, Vanninen E, Mussalo H, Kauppila E, Simula S, Narvanen O, Rantala A, Peuhkurinen K, Nieminen MS, Laakso M, Yla-Herttuala S. Safety and feasibility of catheter-based local intracoronary vascular endothelial growth factor gene transfer in the prevention of postangioplasty and in-stent restenosis and in the treatment of chronic myocardial ischemia: phase II results of the Kuopio Angiogenesis Trial (KAT). Circulation. 2003; 107:2677-2683. Lederman RJ, Mendelsohn FO, Anderson RD, Saucedo JF, Tenaglia AN, Hermiller JB, Hillegass WB, Rocha-Singh K, Moon TE, Whitehouse MJ, Annex BH. Therapeutic angiogenesis with recombinant fibroblast growth factor-2 for intermittent claudication (the TRAFFIC study): a randomised trial. Lancet. 2002; 359:2053-2058. Makinen K, Manninen H, Hedman M, Matsi P, Mussalo H, Alhava E, Yla-Herttuala S. Increased vascularity detected by digital subtraction angiography after VEGF gene transfer to human lower limb artery: a randomized, placebo-controlled, double-blinded phase II study. Mol Ther. 2002; 6:127-133. Stewart DJ, Hilton JD, Arnold JM, Gregoire J, Rivard A, Archer SL, Charbonneau F, Cohen E, Curtis M, Buller CE, Mendelsohn FO, Dib N, Page P, Ducas J, Plante S, Sullivan J, Macko J, Rasmussen C, Kessler PD, Rasmussen HS. Angiogenic gene therapy in patients with nonrevascularizable ischemic heart disease: a phase 2 randomized, controlled trial of AdVEGF(121) (AdVEGF121) versus maximum medical treatment. Gene Ther. 2006; 13:1503-1511. van Royen N, Schirmer SH, Atasever B, Behrens CY, Ubbink D, Buschmann EE, Voskuil M, Bot P, Hoefer I, Schlingemann RO, Biemond BJ, Tijssen JG, Bode C, Schaper W, Oskam J, Legemate DA, Piek JJ, Buschmann I. START Trial: a pilot study on STimulation of ARTeriogenesis using subcutaneous application of granulocytemacrophage colony-stimulating factor as a new treatment for peripheral vascular disease. Circulation. 2005; 112:1040-1046. Gounis MJ, Spiga MG, Graham RM, Wilson A, Haliko S, Lieber BB, Wakhloo AK, Webster KA. Angiogenesis is confined to the transient period of VEGF expression that follows adenoviral gene delivery to ischemic muscle. Gene Ther. 2005; 12:762-771. Edelman ER, Mathiowitz E, Langer R, Klagsbrun M. Controlled and modulated release of basic fibroblast growth factor. Biomaterials. 1991; 12:619-626. Cao R, Brakenhielm E, Pawliuk R, Wariaro D, Post MJ, Wahlberg E, Leboulch P, Cao Y. Angiogenic synergism, vascular stability and improvement of hind-limb ischemia by a combination of PDGF-BB and FGF-2. Nat Med. 2003; 9:604-613. Rosengart TK, Kuperschmid JP, Maciag T, Clark RE. Pharmacokinetics and distribution of heparin-binding growth factor I (endothelial cell growth factor) in the rat. Circ Res. 1989; 64:227-234. Michel CC, Curry FE. Microvascular permeability. Physiol Rev. 1999; 79:703-761. 24. 25. 26. 27. 28. 29. Elmalak O, Lovich MA, Edelman E. Correlation of transarterial transport of various dextrans with their physicochemical properties. Biomaterials. 2000; 21:2263-2272. Martini J, Honig CR. Direct measurement of intercapillary distance in beating rat heart in situ under various conditions of O 2 supply. Microvasc Res. 1969; 1:244-256. Rubio-Gayosso I, Platts SH, Duling BR. Reactive oxygen species mediate modification of glycocalyx during ischemia-reperfusion injury. Am J Physiol Heart Circ Physiol. 2006; 290:H2247-2256. McDonagh PF, Cohen DM, Suaudeau J, Laks H. The effects of myocardial ischemia followed by reperfusion on perfused coronary capillarity. Microcirc Endothelium Lymphatics. 1985; 2:67-84. Van Kerckhoven R, van Veghel R, Saxena PR, Schoemaker RG. Pharmacological therapy can increase capillary density in post-infarction remodeled rat hearts. Cardiovasc Res. 2004; 61:620-629. Xie Z, Gao M, Batra S, Koyama T. The capillarity of left ventricular tissue of rats subjected to coronary artery occlusion. Cardiovasc Res. 1997; 33:671-676. Chapter 4: Computational Modeling of Local Pharmacokinetics and Pharmacodynamics of FGF in Myocardium Abstract Local delivery of angiogenic factors to ischemic tissues for vascular regenerative therapy is a promising treatment for patients with small vessel disease and diffuse atherosclerotic lesions, but this approach has not endured in long term clinical trials. Our experimental studies have shown that capillaries act as sinks to clear drugs and that there is an inherent coupling of local pharmacokinetics and pharmacodynamics in pro-angiogenic therapy. To derive a quantitative framework to examine further the implications of these results, facilitate sensitivity analysis and suggest ways to optimize angiogenic therapy, we have constructed a computational model that couples the continuum pharmacokinetics of angiogenic growth factors with their induced biological effects using experimentally derived parameters. The model accounts for FGF release kinetics from controlled released source, diffusion within myocardial tissue, elimination of FGF through permeation across capillaries, and angiogenic processes: sprouting, maturation and regression. The model predicts that FGF transport in cardiac muscle can be significantly impeded by capillary clearance, despite uniform FGF release. FGF distributions were dependent on FGF diffusivity, trans-endothelial permeability, capillary density, and FGF release rate. FGF-induced capillary sprouting further reduces penetration depth of FGF, increases FGF gradient, and elicits regression of its super-therapeutic threshold wave front through microvascular washout. The trans-endothelial permeability, drug diffusivity, baseline tissue vascularity, drug release rate and biological potency determined the growth factor gradients and steady state distribution of sprouted capillary distribution. Decreasing drug trans-endothelial permeability can potentially result in a significant increase in sustained angiogenic response. This simplified mechanistic model of angiogenic pharmacodynamics combined with local FGF tissue transport support experimental results that angiogenic therapy is self-limited, provides a framework for the study of local growth factor transport in dynamic tissue states, and offers insights into the design and evaluation of therapeutic compounds and delivery approaches. 4.1 Introduction Pharmacokinetic (PK) studies in local drug delivery typically assume that drug transport occurs in a static tissue environment where the tissue is stable and unchanged, and do not account for drug effects in transforming the tissue; in essence the pharmacodynamics (PD). While this conventional approach might be valid for many drugs, it is questionable with regard to angiogenic growth factors that specifically alter tissue ultra-structure drastically and can change the way tissue handles drugs. Such action could have an indirect effect on the drug efficacy that can be difficult to predict, and yet could have tremendous implications for local drug delivery. Indeed, our in-vivo experiments (Chapter 3) showed that FGF1, an angiogenic growth factor, when locally delivered to rabbit epicardial tissue increases the local drug clearance rates significantly above baseline, and as a result limits the drug's spatial penetration and angiogenic effect. Early drug action limits its long term effectiveness. These findings have important implications for optimizing drug delivery not only because they suggested that one should look at both PK and PD in evaluating drug studies but also pointed out limiting factors for drug transport and offered possibility for optimization of system parameters. To effectively carry out optimization studies, it is necessary to have a quantitative understanding of the system. In this chapter, we sought to quantitatively characterize the angiogenic growth factor / myocardial tissue PK-PD system using computational modeling. This approach provides a framework for examining the isolated effects of many tissue and drug parameters that is impossible to study in an in-vivo animal model in this time. Angiogenesis is tremendously complicated process '. It involves interactions between growth factors, inhibitors, and their regulators at molecular, cellular and tissue levels. These interactions are multidimensional, evolving in time and varying throughout the tissue space, and can be highly nonlinear. Previous studies have described and characterized the key angiogenic processes: growth, maturation, and regression. Generation of new blood vessels is initiated with growth factor stimulation and new sprouts can be from preexisting mature or new blood vessels 2. Morbidelli et. al. showed that angiogenesis will not occur if growth factor concentration is below a threshold 3, and others that angiogenesis will reach a plateau if growth factor concentration exceeds a saturation level 4. Stokes and Lauffenburger 5,6 estimated the rate of sprout formation in the rat cornea based on experimental data 7. These newly formed vessels must anastomose or form a closed circuit to preexisting vessels to allow blood flow and become functional. Vessel maturation is an active area of research 8. Maturation requires well orchestrated interactions of many molecular players; disregulation of this cascade of events can lead to leaky vessels with impaired perfusion function 8. Furthermore, regression of blood vessels can take place when immature vessels are not exposed to an adequate dose of survival angiogenic growth factors 7',9 The goal of this Chapter is to create an integrated computational model of angiogenic growth factor effect and transport in myocardial tissue using a continuum approach. The model combines many experimentally derived parameters with known pharmacokinetic and pharmacodynamics processes of FGF in myocardial tissue to provide prediction tool for optimization studies, explain experimental observations and guide future studies. 4.2 Methods To understand the forces that govern the unique interdependence of the pharmacokinetics and pharmacodynamics of angiogenic compounds, we created a computational framework that allows investigation of subtle mechanisms that cannot be elucidated with animal investigations. The pharmacokinetic component of our model accounts for molecular transport through vascularized tissues and allows for an examination of the effects of capillary uptake and clearance on tissue distribution. This allows us to study the impact of capillary density and drug physicochemical properties on myocardial transport. When coupled to the pharmacodynamic model the integrated model describes the response of capillary beds to super-threshold concentrations of angiogenic compounds. The model describes (1) release of growth factor from source (2) diffusion of growth factors within extravascular tissue (3) microvessel uptake and clearance (4) capillary sprouting (5) capillary maturation, and (6) capillary regression. The computational tissue area consists of 200 x 200 nodes with grid size dx = 5 jtm, resulting in a 1000 pm 2 tissue space. The initial capillary distribution is generated randomly and uniformly distributed in both x and y directions. Capillaries are assumed to have an average diameter of 5 pm o 4.2.1 Local Pharmacokinetic Model 4.2.1.1 Mass Transport Equations The myocardium is divided into extravascular and intravascular regions with distinct mass transport properties (Fig. lA). Molecular transport within the extravascular region is governed by: ct = D Ac, (Eq. 1) where ct is the molecular concentration within extravascular space, Deff is effective drug diffusivity in extravascular space, and t is time. Binding of growth factor to tissue components is not explicitly considered, but is included implicitly in the experimentally derived value of the effective diffusion coefficient Deffas measured for FGF-2 in myocardial tissue (Chapter 2). The trans-endothelial flux from tissue to blood is J (Eq. 2) = P(c' (-Ccap) where Pm, is trans-endothelial permeability, and K , the partition coefficient of drug from the intra-vascular space into extra-vascular tissue space. We assumed that convective washout within the intravascular region is significantly faster than the permeation rate into intravascular space, or capillaries act as sinks to molecular transport (Chapter 2), hence set the boundary condition of intravascular concentration ccap= 0 (Fig. 1B). Drug release kinetics is incorporated into the boundary conditions at the tissue-polymer interface, either as constant flux (Fo) or constant concentration (co) boundary conditions, respectively c, or: source = Co (Eq. 3) -D (Eq. 4) c t =FO ax .0 C Permanent Vessel Functional Vessel Nascent Vessel O Nascent Vessel N 0 Regression Maturation Sprouting Functional Vessel Intertitium :% Nascent Vessel 1 a n Permanent Vessel Functional Vessel s c e n t V Regressed Vessel Nascent Vessel 0 FIGURE 1: Schematics of FGF transport and angiogenic response in myocardium A. Cross sectional view of myocardial tissue: background represents a H&E stained image of cardiac tissue cross section with pink regions denoting intracellular space, brown circles denoting permanent vessels including initial vessels prior to therapy, yellow circles denoting nascent vessels, red circles represent functional vessels, black circles with cross represent regressed vessels, dotted green line shows isoconcentration line at biologic effectiveness concentration threshold. B. A two-region continuum pharmacokinetic model for FGF transport includes intravascular and interstitial space. Capillary flow clears drug instantaneously. FGF transport within the interstitium is described by effective diffusivity and passive permeation between capillary and interstitial space. C. Three-step angiogenic model includes sprouting, maturation and regression. 4.2.2 Local Pharmacodynamic Model The angiogenic response to growth factor is modeled by three fundamental events: (1) capillary sprouting, (2) capillary maturation, and (3) capillary regression (Fig. 1C). These events are implemented according the algorithm summarized in Table 2. Source:-D Tissue: aC - =D at + (a2C x = a2 +2 ay2 Trans-endothelial Flux: J = P Capillary Sprouting: Capillary Maturation: 1. Functional: 2. Stabilized: Capillary Regression: C - Ccap ) Psprouting = Pmax f(C)At (tsup-tsprout) > tfunctional t IH(C, - C)dt < H(C, - C)dt > t regression regression TABLE 1: Summary of models: (A) PK model equations, (B) PK-PD model equations. 4.2.2.1 Capillary sprouting We assume that induced capillaries form only from pre-existing capillaries and model this as a stochastic process with a formation probability that is an increasing function of angiogenic growth factor concentration 3. Following Tong et.al.' l , we calculated the probability of vessel formation Pspro,,,,ting for each segment length of capillary dx, and each time interval dt : Pprout,,,g = Pmax f (c)dxdt. Here P,,ax is a rate constant that determines the maximum probability of sprout formation per unit time and vessel length, andf(c) is a threshold function defined as f 0() e-a(c f(c = <c,, 0 -c ) <C where ct is threshold concentration, and a is a constant that controls the rate of transition of the threshold function ". This concentration dependence accounts for the observation that angiogenesis only occurs above some threshold growth factor concentration 3, and that the response is maximal above this threshold 4. A tissue node can become a capillary node only if it is adjacent to any existing capillary node and if its probability of sprouting from Psprouting is greater than a random probability sampled from a uniform distribution using Matlab. 4.2.2.2 Capillary maturation The model draws a distinction between nascent, functional and permanent capillaries (Fig. IC). Nascent capillaries are those of early sprouts, and require anastomosis to support blood flow and become functional capillaries. Maturation progresses from nascent to functional to permanent capillaries, with the exception that initial capillaries have permanent status. We model the maturation process of nascent capillaries to become functional capillaries by tracking the time nascent capillaries are exposed to super-threshold growth factor concentration. This super-threshold duration needs to be above a test condition tfunctional, which is a surrogate for the time taken to make an anastomosis to an existing capillary to establish blood flow. In this context, tfunctional is approximately c where dc is intercapillary distance and vsprouting is Vsprouting sprouting velocity. Stokes et.al. demonstrated that endothelial cells migrate at speed of 20tm/h and can increase to 40[tm/h with FGF stimulation 6. Others have demonstrated that the front edge of vascular networks in cornea pocket assay moves with a speed of 15gtm/h with FGF stimulation 12. We chose the range of tfunctional from 6m to 3h to reflect the heterogeneity of vascular density and to agree with the experimentally determined mean intercapillary distance of 20um/h 13. Functional capillaries further require exposure to growth factors to become permanent. Both functional and permanent capillaries contribute to intra-vascular space and can clear drug, whereas nascent capillaries cannot. 4.2.2.3 Capillary regression Survival of neo-capillaries is dependent on the local presence of angiogenic growth factors 7. In the corneal pocket assay FGF and VEGF induced vessels would regress soon after removal of growth factor sources 9. To account for this property, the model assumed that nascent vessels are regressed when the average growth factor concentration in adjacent tissue is below the sprouting threshold concentration for a period of time tregression. To account for tissue variability we varied tregression over a uniform distribution bounded by tregressionl and tregression2 between 5m and 5d and performed sensitivity analysis on this variation. If satisfying this requirement, functional capillaries will become permanent capillaries and are assumed to be stable and do not regress. Non-vascular Sprouting: and NO --- Non-vascular YES Nascent vessel Maturation: t sup > tfunctional NO -- Nascent vessel NO -- Regression YES Functional vessel Regression: YES Permanent vessel TABLE 2: Summary of angiogenic model. Non-vascular tissue nodes are subjected to several different conditions of sprouting, maturation and avoiding regression to progress to a permanent vessel. 4.2.3 Model Parameters Initial capillary volume fraction is assumed to range from 1%-100% of the normal range of 2000-3000 capillaries per mm 2 14. Baseline trans-endothelial permeability and diffusivity values are assumed to be similar to those observed in arterial tissue for hydrophillic drugs 15. For the constant flux release mode, drug was initiated and maintained with zero-th order kinetics, with a baseline rate of lx10 1 1 ng/s, similar to a published estimate for VEGF release from fibrin glue release device' 6 . The baseline model parameters are summarized in Table 3. Parameter Description Deff PmV Kc Fo Ct a Pmax tfunctional tregression N Effective diffusivity Microvascular permeability Partition coefficient Release rate Biologic threshold Threshold function constant Maximum probabililty of sprout formation Functional delay time Regression half life Initial capillary density Baseline value 1 am 2/s 10 gm/s 1 1x10-T ng/s 0.1 ng/ml 1 5 x 10-4 um'hrVaried Varied Varied TABLE 3: Baseline parameter values 4.2.4 Numerical Methods Numerical simulation of the model was accomplished by dividing the myocardium into computational elements each with a specific drug concentration. A forward difference numerical procedure was applied on the computational grid to solve the transport equations (See Appendix for MATLAB code). 4.3 Results 4.3.1 Local Pharmacokinetic (PK) Model Results: Effects Diffusivity, Trans-endothelial Permeability and Vascularity on Drug Transport. We simulated the PK-only module of the model to examine the isolated effects of diffusivity, and capillary clearance on drug deposition and penetration depth to account for our ex-vivo experimental observations (Chapter 2). This model demonstrated that drug diffusivity, trans-endothelial permeability, and capillary volume fraction have significant impact on drug transport following locally applied drug source of constant concentration. As drug diffusion coefficient increases, it can penetrate tissue easily, however interestingly those with higher diffusion coefficient have lower total deposition at steady state (Fig 2A). Such trend is counterintuitive, and is opposite from those expected in diffusion through solid media where distributed sinks are absent. Drugs with higher diffusivity can transport further into tissue and effectively see more capillaries and are cleared at higher rate hence have lower total deposition. Our analysis also highlights the impact of capillary trans-endothelial permeability and tissue vascularity on drug distribution and elimination (Fig 2B-C). Both drug trans-endothelial permeability and tissue vascularity contribute similarly to drug clearance, and limit tissue penetration and deposition of drug. The sensitivity to permeability and vascularity is highest when permeability and vascularity is lower than 0.5 um/s and 500 capilllaries/mm 2 , respectively. 600 7.50E-07 400 5.OOE-07 . a o 2.50E-07 200 0 0.OOE+00 - 0 100 50 Diffusivity (um2/sec) 250 - - 200 E 4.00E-06 me -3.00E-06 0 150 2.00E-06 .t il 100 - 1.00E-06 50 00 '- a 0.OOE+00 0 0 0 0.5 1 Permeability (um/s) 250 -5.00E-06 ._ 200 4.00E-06 o 150 3.00E-06 a 100 2.00E-06 P 50 1.00E-06 0 0.OOE+O0 a0 0 500 1000 1500 Capillary density (#/mm2) FIGURE 2: Continuum Pharmacokinetics Model: Effects of diffusivity, permeability, and initial vessel volume fraction. Black curves and y-axes represent penetration depth, defined as distance from source to spatial locations with 90% drop-off threshold concentration from source. Blue curves and y-axes represent total drug deposition. 4.3.2 Local Pharmacokinetic-Pharmacodynamic (PK-PD) Model Results 4.3.2.1 PK-PD Interdependence: To provide a conceptual model of how the dynamics of induced angiogenesis affect drug distribution, we coupled an angiogenic pharmacodynamics (PD) model of capillary sprouting and maturation (without regression) to the pharmacokinetic (PK) model. Simulated drug release kinetics recapitulated in vitro release kinetics (Chapter 3). Angiogenesis affects drug distribution significantly (Fig 3A-B). The pure PK model (Fig. 3A) shows drug reaching super-threshold concentration throughout the Imm2 tissue region at up to 48 hours and remaining high over the tissue region at day 10. The PK/PD model predicts that the super-threshold drug concentration front initially penetrates deeper into the tissue with time, similar to the predictions of the PK only model. However, at later times the threshold front slows down and eventually regresses between 72-96 hour as the formation of new capillaries increases drug clearance. Notably, the steady state depth of the threshold front (Fig. 3B) is significantly lower than PK only model (Fig. 3A). Such negative pharmacodynamic feedback on drug transport observed in Fig 3B can have indirect effects on drug action. We studied this possibility by examining the relationship of rate of angiogenesis as a function of tissue angiogenic state measured by vascularity (Fig 3C). The ascending limb of the curve is a manifestation of the fact that new capillaries can only sprout from existing capillaries. The descending limb of the curve represents a negative feedback where the generation of neo-capillaries has an inhibitory effect on drug transport. Capillary growth 1hr 10min 24hr 6hr 2hr 240hr A 400 C " 00 oo S300 o0 OO o0 0 000OM 0140 o0 ooo OO 00 O 0 o OO 0 00 D D o oooo 5 oo a o~o0 0 140 280 0 0 0o00oo O 0 0 00 0 0CD 0 000 0O 00000 0 oo o oo oo 00000 o ooc o a 0 ooo S o(Do o Sooo o oooo 7o o aD oGWoD 420 560 700 Number of Capillaries FIGURE 3: Pharmacokinetic/Pharmacodynamic Model. Drug and capillary distribution as a function of time of (A) PK model, (B) PK/PD model. Orange color regions denote superthreshold drug distribution, and white dots represent functional capillaries. (C) Rate of angiogenesis (#capillary/hr), defined as first time derivative of capillary number, as a function of capillary number. increases drug clearance through washout and impedes drug penetration, reducing the areas of super-threshold concentration and angiogenic response. Thus, there is an interdependence of pharmacokinetics and pharmacodynamics. As the pro-angiogenic therapy starts to become effective, this unique PK-PD coupling inhibits the distribution of the therapeutic drug and limits the intended effect of the therapy. It should be noted that these results also support our experimental observations in-vivo (Fig. 4-5, Chapter 3), and offer a possible explanation for the regression of neo-vascularization observed in early time points: lack of growth factor due to clearance through microvascular washout. 4.3.2.2 Model Sensitivity Analysis: Since capillary washout has significant impact on drug transport and angiogenic response, we performed the sensitivity analysis on model parameters whose baseline values are either not available experimentally or can potentially be altered to optimize the angiogenic effect. 4.3.2.2.1 Timings of CapillaryMaturationand Regression Have Little Effect on Steady State CapillaryGain We modeled the maturation process of new blood vessels by drawing a distinction between nascent, functional and permanent capillaries. Nascent capillaries can become functional capillaries (capable of carrying blood flow and clear drugs) when exposed to growth factor for a period of time above tfunctional. However, our model also allow for regression to occur if vessels are subjected to long period of sub-therapeutic concentration. To implement this requirement, the model imposed a regression condition that if capillaries are exposed to subthreshold growth factor concentration for more than a period of time tregression, which varied over a uniform distribution bounded by tregressionl and tregression2 between 5m and 5d. In principle, because functional capillaries can clear drug, the timings of their occurrence and disappearance are expected to have an impact on the permanent capillary number. However, interestingly although there were differences in transient dynamics, the steady state angiogenesis was not significantly affected by parameters controlling the timings of biologic activities (functional and tregression). Drugs initially distributed within tissue, but as total capillary number increased drug distribution quickly regressed. Greater values of tfunctional correspond to longer delay to gaining of functional vessels (Fig. 4B) and allow for higher drug penetration into tissue (Fig. 4A). The higher drug penetration (higher peak for longer tfunctional in Fig. 4A) in turns leads to higher maximum total capillary number (Fig. 4B). However, greater angiogenic response only occurred transiently. This is because higher functional capillary number attained during the early phase also led to a higher clearance rate of drug washout, resulting in greater regression of penetration depth of super-threshold growth factor concentrations (Fig. 4A). The greater drops in penetration depth, in turns, led to more regression (Fig. 4B), and cancelled out the higher early gains. The sensitivity of late angiogenic gain to regression timings was further examined by changing parameters (tregression and tregression2) controlling the distribution of required maximal duration of sub-threshold exposure before undergoing regression. Peak angiogenic response and drug penetration depth were not sensitive to altering regression conditions as expected since they do not alter the sprouting and maturation properties (Fig 5). These parameters, however, influenced the start time of when functional vessels regress. The regression timings interestingly also did not influence the steady state functional capillary number (in both cases of varying tregressionl (Figs. 5A&C) and tregression2 (Figs.5B&D)), but only the time taken to reach this steady of state (tregression). Therefore, the pharmacodynamic timings only impact the transient response angiogenesis and not steady state angiogenesis (number of permanent capillaries). 180E 0. a I 120- -. t functional = 6min *-t functional = lhr -- tfunctional = 2hr t_functional = 3hr 0 " 60a) 4) 0- .4 Time (hrs) B 500 -L a. 400 0 0 I-- = 1 hr t functional = 2hr E z 300 .7 t functional = 6min -tfunctional t_functional = 3hr 200 100 0 .1 0.1 1 10 Time (hrs) 100 10 00 FIGURE 4: Effects of tfunctional on penetration depth (A) and total capillary number (B) as a function of time. 120 2hr-4hr (3hr +- lhr) 1205m - 48hr (24.5hr +- 23.4hr -- 2hr - 48hr (25hr +- 23hr) E 90 - - -*-2hr-5d (61hr +- 59hr) E 90 12hr - 48hr (30hr +- 18hr) 2hr-48hr (25hr +- 23hr) - aL r 60 0 a, C (U . 30 6 30 0 i i T Timdb rs) 1 aH ,i 0 1000 1 0.1 10 Time (hrs) 10, 100 400 400- 300 300 - 200 o 200 I- 100- 100 5min-48hr (24.5hr +- 23.4hr) 2hr-48hr (25hr +- 23hr) 12hr-48hr (30hr +- 18hr) 0. 1 Time hrs) 1000 i 0.1 m 2hr-4hr (3hr +- 1hr) -- 2hr-48hr (25hr +- 23hr) S2hr-5d (61hr +- 59hr) 10 Time (hrs) FIGURE 5: Effects of tregression range on penetration depth (A&C) and total capillary number (C&D) as a function of time. Legends denote tregressionl-tregression2 (tregression +- 0.5 range of tregression). 1000 4.3.2.2.2 Trans-endothelialPermeability,Diffusivity, Biologic Threshold,Initial capillary density and Release Kinetics Have Significant Effect on Steady State Drug Distributionand Capillarygain. Our results also revealed the factors that have significant impact on steady state angiogenesis. These include ones involved in drug clearance (initial tissue vascularity and transendothelial permeability), bulk transport (diffusivity), drug input (release rate), and biologic threshold. 3000 A 2500 N=2400 Initial tissue vascularity: . 2000 Tissues with higher baseline 1500 vascularity are expected to have 1000 N=8 500 N=400 higher drug clearance to begin with 0.1 and thus would create a local tissue environment with higher impedance 10 Time (hrs) 100 1000 100 1000 600.00% B for drug transport. Indeed, total capillary number sprouted over time 1 t- 400.00% i is inversely proportional to the initial N=10 S200.00% vascularity (Fig 6A), and the trend _ N200 N=400 can be better revealed when looking 0o.oo00% -. 0.1 at the percentage capillary gain over of 50 capillary density of 50 2-0- 1 10 Time (hrs) starting 6: Effect of initial vascularity (N=50, time (Fig 6B). With aFIGURE 100, 200, 400, 800 and 2400 denote the initial number of capillaries per mm 2) on absolute capillary number (A) and percentage capillary gain (B) as a function of time. capillaries/mm 2, the peak percent capillary gain can be as much as 600%. This percent gain decreased with higher baseline vascularities and was as little as 2% for baseline vascularity of 2400 capillaries/mm 2 (Fig 6B). Unlike the effect of tfunctional (Fig. 4), higher peak angiogenic response in this experiment translated to higher steady state percentage capillary gain. Higher initial capillary density led to higher baseline clearance, making it more difficult for drug to penetrate into tissue to achieve super-therapeutic threshold for angiogenesis. Diffusivity: Drugs with higher diffusivity can stimulate higher peak percentage capillary gain (2100%, 570%, and 244% for rD (=D/DFGF) = 10, 1 and 0.1 respectively). Capillary regression reduces the magnitude of the gain, but does not alter the dependence on diffusivity (260%, 71%, and 28% for rD = 10, 1 and 0.1, respectively) (Fig 7A). More readily diffusive drugs can move faster into tissue and effectively increase the penetration depth of supertherapeutic drug front, increasing both peak and steady state angiogenic response. Trans-endothelial permeability: Drugs with lower trans-endothelial permeability can stimulate higher peak percentage capillary gain (2100%, 510%, and 280% for r_P (=P/PFGF) 0.1, 1, 10 respectively), and retain larger gain in permanent capillaries (404%, 71%, and 20% for rP = 0.1, 1, 10 respectively) (Fig 7B). Lower trans-endothelial permeability improved penetration and at the same time also minimized drug loss to microvascular washout, leading to both gain in peak and steady state angiogenesis. Growth factor therapeutic threshold concentration: Potent growth factors elicit effects at lower threshold concentrations, stimulating higher peak percentage capillary gain (1400%, 970%, 570% and 240% for r_Ct (=Ct/Ct FGF) = 0.1, 1, 10, 100 respectively), and higher steady state gain (140%, 108%, 71% and 50% for r_Ct = 0.1, 1, 10, 100 respectively) (Fig 7C). Lowering therapeutic threshold is equivalent to increasing drug penetration depth since it is easier for tissue to achieve therapeutic threshold concentration with the same drug PK properties. Therefore, drugs with higher potency had higher peak and steady state angiogenic gain. Release rate: Releasing drug at a higher rate can stimulate higher peak percentage capillary gain (890%, 570%, and 320% for r RR (=RR/RRbaseline) = 10, 1, 0.1 respectively), and steady state gain (101%, 71%, and 44% for r_RR = 10, 1, 0.1 respectively) (Fig 7D). The response to increasing drug release rate was similar to that of lowering therapeutic threshold in that both act to increase the early capillary gain (elicit higher peak angiogenic response) by increasing the penetration depth of the drug's super-therapeutic wave front, and as a result increased the number of capillaries with permanent status. Comparing the effects of different model parameters on steady state percentage capillary gain (Fig. 8) revealed that capillary permeability is the most sensitive parameter at producing permanent capillaries with local myocardial growth factor delivery. The green line in the curve denotes the sensitivity of the model to changing the drug's biologic threshold but keeping its PK properties unchanged. While modulating release rate (blue line) can achieve a similar response to effect of changing drug potency (green line), altering trans-endothelial permeability of the growth factor (magenta line) can produce a significantly greater return in permanent angiogenesis. 100 2500% L 0 2000% - r D=0.1 - r D=1 - r D=10 a1500% c 2500% 20 ( 2000% . 1500% 01000% C 500%/o S 500% 0% 100 1000 a) Time (hrs) 1000.00% 1500% 1000 100 10 Time (hrs) 1 -rRR= -rRR=1 .a 0 750.00% 0.1 rRR=10 CO c1000% o 500.00% a) (D a C) O C 500% 250.00% a 0.00% 1 1 100 10 1000 100 10 1000 Time (hrs) Time (hrs) FIGURE 7: Effects of diffusivity, trans-endothelial permeability, biologic threshold, and release rate on percent capillary gain over time. r D, rP, and rCt are defined as ratio of diffusivity (A), trans-endothelial permeability (B), and biologic threshold (C), respectively, over the respective baseline values of FGF. rRR is defined as ratio of release rate to baseline release rate (D). 101 500.00% * Release Rate M Permeability 400.00%.831 = 0.8319X yS= " A Bioloqic Threshold 6527 -0.6527 2 R = 0.9921 , 300.00% 2y = -0.1277Ln(x) +y = 0.1249Ln(x) + 0.7225 2 R = 0.9991 R = 0.9925 100.00% 0.00% 0.01 0.1 1 10 100 Folds changed compared to baseline value FIGURE 8: Steady state percentage capillary gain as a function folds change in biologic threshold, drug release rate, and permeability 102 4.4 Discussion: 4.4.1 Traditional Continuum PK vs. Continuum PK-PD Analysis Continuum pharmacokinetic analyses have been successful in providing insights into local drug transport mechanisms 17, 18. This continuum approach adapts traditional compartmental pharmacokinetic analysis to the local environment by supplanting discrete global parameters with continuous local values of concentration, transport and binding. These parameters and local boundary conditions define local drug distribution in space and time. These continuum PK models explain experimental results well and give tremendous insights into optimizing local perivascular 18, and stent based 17 arterial drug delivery for heparin and paclitaxel that have minimal effect on tissue transport properties. Our results suggest that drugs such as angiogenic growth factors significantly modulate the local drug clearance properties of tissue over the course of local sustained delivery, thereby powerfully regulating their biological effects. Therefore, studies of angiogenic growth factor delivery should augment the continuum PK approach with a PD processes in analyzing local drug delivery. As the pro-angiogenic therapy starts to become effective, the balance of transport forces is shifted to clearance dominant regime. In our model, this effect arises primarily as a result of increasing capillary density. We did not specifically examine the changes in trans-endothelial permeability when the tissue is in angiogenic state. It is very likely that trans-endothelial permeability can be significantly higher as angiogenesis occurs 19, 20. Such changes in permeability would further increase drug clearance through washout and tips the balance point even more to the clearance dominant regime, potentially resulting in more powerful negative 103 pharmacodynamics feedback. This further raised the need to consider pharmacodynamic effects of drug on tissue transport properties when studying local drug delivery. 4.4.2 Minimizing Microvascular Clearance as an Approach to Optimize Angiogenic Effect The negative feedback of PD on PK in local growth factor delivery for angiogenic therapy suggests an optimal approach to improve drug penetration and angiogenesis through minimizing microvascular clearance. Indeed, our results revealed that lowering trans-endothelial permeability provide significant improvement in inducing permanent vessel formation by increasing drug retention to prevent vessel regression after they were induced. The effect of lowering trans-endothelial permeability interestingly can be significantly greater than changing the biologic threshold of the growth factor at inducing permanent vessel formation. Since the clinical goal of angiogenic therapy is to maintain permanent collateral vessels, growth factors might be designed through chemical modification or genetic engineering to optimize the balance of opposing forces of drug distribution and drug clearance. For instance, it might be possible to add negative charge chemical groups to drugs to lower trans-endothelial permeability 21 to improve penetration depth and retention to achieve a more uniform and longer lasting angiogenic response. These results suggest that computational modeling of local continuum PK-PD can be used to guide engineering of drug properties to achieve desire biologic response. We used a simple, mechanistic, 2D model in this chapter to focus our studies on the effects drug clearance through microvascular washout in governing drug transport, it can be improved further to consider more realistic three dimensional vascular networks and flow patterns when computational power can be improved. 104 4.4.3 Release Rate and Diffusivity Modification to Optimize Angiogenic Effect Our sensitivity analyses also suggest that the model response is sensitive to changes in diffusivity and drug release rate. The parameter that can perhaps be modulated most easily is the rate of drug release. For example, FGF release rate from heparin alginate device changes as a function of heparin concentration 22 . Increasing the rate of angiogenic drug input achieves a steady angiogenic effect equivalent to lowering the biologic threshold of the drug which might not be so easily to alter. This approach might be advantageous for drugs with large therapeutic window when high tissue concentration does not present toxicity to the myocardial tissue. Different ways of modulating effective diffusivity of growth factor may include altering size, charge, and binding domains. The effect of size and charge on effective diffusivity of macromolecules in tissue has been experimentally determined 21. Our results in Chapter 5 suggest that penetration depth of FGF can be improved by minimizing its interaction with tissue HSPGs through the use of sucrose octasulfate (SOS). This binding interaction may be accountable for an approximately 500 times slower in effective diffusivity and therefore presents a potential optimizing target for enhancing diffusivity. Although, this modification with SOS can be achieved at the expense of increasing steric hindrance, it is perhaps possible some day to engineer binding domains of growth factors to achieve the optimal balance of binding property, molecular size changes, and retention of the drug's biologic effect to improve effective diffusivity. 105 4.4.4 Minimizing Late Loss as an Effective Approach to Improve Angiogenic Therapy One of the most significant implications from our computational model results was that it identified distinct temporal tissue responses following angiogenic therapy (representative response is shown in Fig. 9), and showed the differential response of each phase to changing various drug and tissue properties. "Early gain" phase consists of sprouting of nascent blood vessels and their maturation to functional vessels capable of perfusing ischemic tissue. These new vessels though functional require super-therapeutic growth factor levels to survive, otherwise undergoing regression. The regression process is the main feature of the "late loss" phase. Because functional vessels clear drugs through microvascular washout (Chapter 2), the increase of these vessels in the "early gain" phase act as a powerful negative feedback mechanism to cause vessel regression, accounting for the magnitude of the "late loss" of functional vessels (Fig. 9). Most PK and PD properties of drugs and drug release device, such as effective diffusivity, potency, and release kinetics, can be modulated to directly maximize the response in the "early gain" phase. However, lowering trans-endothelial permeability can both increase "early gain" and minimize "late loss". Therefore, modulation of trans-endothelial permeability contributes most significantly to the permanent angiogenic response (Fig. 8). Furthermore, these results also suggested that minimizing "late loss" phase by any therapeutic means can potentially increase "permanent gain" and unlock the vast angiogenic potential of the "early gain" phase. One way of doing this may be by releasing many drugs with different biologic actions at different times during the therapeutic treatment. An early drug can be FGF or VEGF that act to maximize the "early gain" phase, while a late drug can be 106 angiopoietin-1 23, which act to minimize vessel leakiness to reduce "late loss" and maximizing "permanent gain". With current advances in drug release device technology 24, it may be possible to precisely control the release time of these different drugs to modulate both early and late phases of angiogenesis for optimal effect in long term. D, Pmv, Cth, RR Pmv 600.00% 400.00% 0Early G in Late Loss CU S200.00% Permanent Gain - - 0.00% 0.1 1 100 10 1000 Time (hrs) FIGURE 9: Approaches to improve pro-angiogenic therapy. Typical angiogenic response is represented in brown curve. An early angiogenic gain is followed by a late loss in functional vessels as a result of regression. The difference between the response from these two phases is permanent angiogenic gain. Maximizing this permanent gain is the goal of angiogenic therapy. While many factors can affect the early angiogenic gain, the drug's trans-endothelial permeability is most effective at minimizing late loss, and as a result has a significant effect on permanent gain. 107 4.5 Summary The unique problem faced by angiogenic therapy is that its very success in stimulating blood vessel growth limits further angiogenic activity. Our computational models confirm our experimental results in previous chapters and suggest strategies for drug design and drug delivery systems to enhance drug penetration and subsequent induction of permanent collateral vessels. 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Controlled and modulated release of basic fibroblast growth factor. Biomaterials. 1991; 12:619-626. London NR, Whitehead KJ, Li DY. Endogenous endothelial cell signaling systems maintain vascular stability. Angiogenesis. 2009. Richardson TP, Peters MC, Ennett AB, Mooney DJ. Polymeric system for dual growth factor delivery. Nat Biotechnol. 2001; 19:1029-1034. 110 Chapter 5: Effects of Tissue Binding on Local Pharmacokinetics of FGF in Myocardium Abstract In previous chapters we focused on the effects of microvascular clearance on local myocardial distribution of FGF. In non-perfused rat myocardium, drug transport is mainly governed by diffusion and binding processes. FGF binding to its specific receptor and the more abundant heparan sulfate glycosaminoglycans (HSPGs) binding sites was accounted for in a simplified manner that presumes receptor excess. In this chapter we examined in more detail the effects of myocardial binding on FGF transport. Effective diffusivity of FGF2 in myocardium is -500 times lower than that of similar size Dextrans. Even at 96 hours, myocardial FGF2 accumulated only superficially, and penetration remained below 50 um unless the concentration was increased to 8.82 ptM (150 jtg/ml), presumably due to the saturation of tissue binding sites. Sucrose octasulfate (SOS) partially dampened the effects of binding-related transport hindrance. Conjugation of FGF-2 to SOS decreased general binding, while not significantly affecting superficial drug uptake, thereby increasing the rate of deep tissue drug uptake by 132.8%. As the densities of vascularity and tissue binding sites are both expected to vary with the level of ischemia, our results suggest that uptake and deposition of angiogenic growth factors will vary intricately across the heart. This calls for careful attention in the choice of drug, and formulation and placement of the delivery device. 111 5.1 Introduction The "binding site barrier" hypothesis, the concept that molecular transport is impeded by specific binding to fixed tissue sites has been introduced and experimentally verified in the analysis of antibody distribution in microscopic tumor nodules 1-5. When monoclonal antibodies were administered intravenously, specific binding to tumor tissue antigens retarded their deeper penetration into tumor tissue. Higher binding affinity, antigen density or lower antibody dose can exacerbate the problem. This phenomenon may well be relevant for fibroblast growth factor (FGF) transport since this growth factor binds avidly to its cognate cell receptor (FGFR)6' 7, and less avidly to abundant fixed tissue binding sites including heparin sulfate proteoglycans (HSPGs) 8, 9 . In fact, it has been shown that FGF2 when applied to monolayer of bovine aortic endothelial cells in the presence of heparin stimulate morphological changes at a 10-fold greater radius than bFGF alone as a result of partitioning preferentially in the soluble phase rather than binding to fixed glycosaminoglycans in the extracellular matrix 10. Furthermore, native FGF transport across Descemet's membrane (DM) is 20-fold slower than non-heparin binding form of FGF 9. In this Chapter we examined the degree to which myocardial FGF transport is hindered by binding and whether such hindrance can be controllably modulated. The two classes of receptors for FGF are high affinity, low capacity FGFR, a tyrosine kinase receptor family on cell surfaces, and low affinity, high capacity HSPGs 11, found on cell surfaces as well as in extracellular matrix and basement membrane. FGFR family is composed of four members: FGFR-1, -2, -3 and -4, but only FGFR-1 is found in the heart 12-14. In myocardial tissue, syndecan-3 and glypican are the most abundant types of HSPGs 15. In addition to the abundant presence of HSPG in extracellular matrix and basement membrane, HSPG cell surface 112 density is also approximately 100-fold higher than FGFR density 16. HSPG binding sites are at much higher concentration in basement membranes than extracellular matrix 8,9. Although basement membrane and extracellular matrix concentrations of HSPG in the myocardium have not been reported, Descemet's membrane (DM) has been used as a model basement membrane and the value of HSPG binding site concentration in DM 9 and in extracellular matrix of endothelial cell culture have been quantified 8. As the myocardium is highly vascularized, and that both myocardial capillaries and cardiac myocytes are lined with basement membranes of high HSPG concentration, it is reasonable to expect that the "binding site barrier" limitation to FGF transport in myocardium is significant. In this Chapter, we show that tissue binding is the dominant transport hindrance on FGF transport in a non-perfused myocardium and that while binding enhances local growth factor uptake significantly, it also limits penetration and late uptake. Moreover, we illustrate that this effect that is dampened when general binding is reduced with protective sugar groups. 113 5.2 Methods 5.2.1 Effect of Binding on Myocardial Transport The degree to which reversible FGF binding affects its myocardial transport can be ko B F +R (RI1) quantified following the analysis of effect of koff immobilizing adsorption on gas diffusion in polymers 17. (1) In this analysis, the diffusion equation can be modified to allow for molecules F ax 2 B (2) being trapped in non-diffusing holes according 2 (F + B) t O0 - ct B or B F "ax Kd + F to a simple Langmuir-type isotherm 18. The (3) diffusion in the presence of binding to x ))2 d B.maF/Kd 1+ (1+ = a 22 O 2t immobilizing sites is described by (1) where F D OF B denotes the concentration of FGF, B is the 2 F Kd K+maxOx2 concentration of FGF-receptor bound complex created from the reaction (RI) between FGF and (4) Dqf=D 1+ Bmax /Kd)2 its receptors, assuming to consist of mostly HSPGs. With the quasi-steady state assumption of enzyme kinetics 19, i.e. the change of TABLE 1: Summary of derivation of effect of tissue binding on effective diffusivity. intermediate binding complexes FGF-HSPGs is assumed to be minimal, B can be approximated by (2), where Kd is the dissociation constant defined as the ratio of rate of dissociation to association of FGF-HSPG complex, and Bmax is the maximum tissue binding sites. B can be substituted to equation (1) to arrive at the modified 114 D diffusion equation (3), which defines the ratio S Bmax as effective diffusivity Df. Kd (1+ F/K )2 Therefore, the effect of FGF-HSPG binding on FGF transport can be quantified by the impedance factor a- + 1, which is non-linear and dependent of boundary (1+F/Kd ) 2 concentration F. The larger a is the slower FGF transport would be. We can approximate the value of a by comparing Dff of FGF to comparable molecular weight inert compounds. 5.2.2 Long-time point uptake studies Rat myocardial tissue blocks of 8-10 mm3 in size were obtained from the left ventricular free wall of harvested PBS-flushed hearts following euthanasia. Myocardial tissue sections were incubated in serially diluted concentrations of drug solutions (TR-FGF2 and TR-FGF2-SOS at 0, 19, 38, 75, 150, 300 pg/ml of FGF2 in PBS) for 96 hours at 40 C. Following incubation, tissue sections were processed for quantitative fluorescence imaging. 115 5.3 Results 5.3.1 Tissue Binding Impedes FGF Transport in Myocardial Tissue Our experimental measurement of effective diffusivity of FGF (0.02 Im2/s) is significantly lower than the diffusivity of Dextran 10OkD (10.24 [tm 2/s) in myocardial tissue. With the assumption that steric hindrance of 10OkD Dextran and 17 kD FGF are similar, we can approximate impedance factor a = max +1 to be 512. This number is within 0.25-1- d (1+F/Kd)2 folds values obtained for FGF in Descemet's membrane ( -500-2184 calculated in Tzafriri et.al 20 from data by Dowd. et.al. 9). These results suggested that tissue binding hindrance is significant for FGF transport in myocardium, within one order of magnitude of binding hindrance in DM, which is known to contain high concentrations of heparan sulfate. Because FGF is known to bind to FGFR and HSPG and that HSPG is more abundant than the specific receptor FGFR, this binding hindrance is most likely a result of the reversible HSPG binding. 116 5.3.2 Modulating tissue binding alters myocardial FGF2 transport To further examine the effect of HSPG binding on FGF transport, we incubated explanted plugs of rat myocardium (8-10 mm 3) in varying concentrations of Texas Red FGF2 (TR-FGF2) for 96 hours at 40 C and examined myocardial drug distribution (Fig. 1A). Penetration of TRFGF2 (at 25% source) was extremely limited, with drug mostly residing within the first -50 iim of the surface even at 96 hrs. Increasing the applied concentration raised overall myocardial TRFGF2 uptake in a concentration-dependent manner. The depth of penetration remained unchanged at low concentrations. Only when 8.82 tM (150 pg/mL) or greater of TR-FGF2 was delivered did faster effective diffusion and deeper penetration occur (Fig. 1B). In pure diffusion process, penetration depth at a fraction of source concentration would be independent of source concentration as predicted by solution to diffusion equation c/Csource = erfc(x/2 Dt). A concentration dependent process such as that observed by Fig. IB likely suggests a diffusive transport mechanism that is modulated by saturable binding. Diffusive hindrance by abundant local HSPG binding sites, which only begin to saturate at high drug concentrations, likely accounts for such ineffective tissue penetration. Indeed, tissue equilibration for dextrans, a compound much less encumbered by general binding, is known to occur in similarly sized plugs within 48 hours 21, 22 We further compared the distributions of TR-FGF2 with Texas Red FGF2-SOS (TR-FGF2SOS) to examine the possibility of improving drug penetration depth with altering tissue binding. At a concentration of 4.41 ptM (75 gig/ml), the penetration of TR-FGF2-SOS exceeded that of TR-FGF2 (Fig. 2B). Interestingly, at a concentration of 1.76 ptM (300 gg/mL), the penetration 117 depths were reversed, with TR-FGF2 penetrating deeper than TR-FGF2-SOS (Fig. 2A). Surprisingly, raising the applied drug concentration by over one order of magnitude only increased the penetration depth of TR-FGF2, and not that of TR-FGF2-SOS. A concentrationdependent balance between susceptibility to repeated on/off non-specific binding and sizemediated diffusivity likely accounts for this observation. For TR-FGF2-SOS, the SOS component decreases susceptibility to general binding, accounting for deeper penetration at lower concentration and decreased sensitivity to changes in applied drug concentration. On the other hand, at overwhelmingly high concentrations, TR-FGF2 itself can saturate general binding. As a result, the lower diffusivity of TR-FGF2-SOS conferred by its significantly higher molecular weight likely limits its penetration depth compared to that of TR-FGF2. 118 -19 ug/ml -38 ug/ml 3000 - 75 ug/ml -- 150 ug/ml 2000 -300 1000 ug/ml 0 0 50 200 150 100 Distance from Source (um) -- 300- E CLr G 200- 0C 0 1001 (L Expt Data -4 I 100 200 300 400 Source Concentration (uglml) FIGURE 1: FGF2 concentration profile (A) and penetration depth defined as 25% of source concentration (B) as a function of source concentration. Error bars were only shown at regular intervals. 119 3000 A 3000 -300ug/ml -300 FGF-SOS ug/ml FGF Alone S2000 o0 o I. 10 1000 750 50 0 1000 every 50 u, 500 -75ug/ml FGF-SOS -75ug/ml FGF Alone 150 100 Penetration Distance (urn) 200 (A)Band 75ug/ml (B). Error bars -75ug/m300ug/ml were only shown atOS at FGF2-SOS and -transport. FGF2 ofFGF2 distribution every 50pgm. 120 5.4 Discussion 5.4.1 Binding reduces effective diffusivity, but can be modulated by protective groups Drugs diffusing through myocardium can bind to both their specific receptors and to general fixed tissue binding sites 8. The equilibrium between on-off binding reactions translates into a concentration dependent partition coefficient and a concentration dependent hindrance of myocardial transport. Our data show that the density of binding sites for FGF2 in myocardial tissue is so overwhelming that equilibrium distribution in a 8-10 mm 3 plug of tissue is not reached even after several days. As source concentration was raised, more and more tissue binding sites were saturated and only then was FGF able to penetrate deeper part of tissue (Fig. IB). This implies that binding hindrance accounts for a significantly lower effective diffusivity, several orders of magnitude lower than would be expected for a molecule the size of FGF2 in the myocardium. Our data also suggest that it is possible to circumvent poor FGF penetration by increasing the delivery dose (Fig. 1A), similar to the case of targeting tumor micrometastases with monoclonal antibodies 4 Our studies are the first to report the "binding site barrier" effect of FGF transport in myocardium. This effect is between 1-4 fold lower than that reported for FGF in heparin sulfate rich Descemet's membrane 9 as analyzed by Tzafriri et.al 20. These results are reasonable for extracellular-space-confined FGF as Descemet's membrane is likely to be richer in heparan sulfate content than myocardial extracellular matrix. Nevertheless, the effect of binding on FGF transport in myocardium is highly significant and likely accounts for 500 folds lower in diffusivity of non-binding FGF. FGF binding to the myocardium is then a double edged sword, 121 enhancing uptake in the superficial regions of the tissue, but markedly reducing effective diffusivity and severely limiting tissue penetration. Thus, modulation of FGF binding to the myocardium may improve the efficacy of pro-angiogenic therapy with FGF. It is therefore significant that we have shown that the adverse effects of binding on myocardial transport can be dampened by flooding the tissue with high concentrations of drug or by using protective groups such as SOS or various types of heparins. While delivering high FGF concentrations might give rise to toxicity, the use of protective groups can be promising if done with care. Foremost, protective groups must not adversely affect biological activity. The specific binding activity of the drug to its receptor (e.g., FGF2 to FGFR) should not be perturbed. In general, conjugation of FGF to another molecule can alter its general as well as specific binding. In this case, the reduction in binding is likely limited to general tissue binding (eg., to HSPGs). Since SOS does not reduce FGF2 biological effect in vitro 23,24, our data suggest that SOS primarily blocks general binding only. Indeed, some studies suggest that SOS actually enhances FGF2 activity 23, 24, through imitating heparin role, promoting FGFR dimerization and increasing FGF-FGFR affinity, hence potentiates FGF intracellular signaling. Second, protective groups must not be so large as to increase the steric hindrance experienced by the drug. For example, using unfractionated heparins (UFH) as a protective group for FGF2, while protecting against capillary washout and proteolysis, may actually slow drug penetration due to the large size of the FGF2-UFH complex (well above 100 kDa, Fig. 6, Chapter 2). SOS conjugation presents an attractive approach to improve pro-angiogenic therapy with FGF by enhancing not only cellular PK 23, 24, but also tissue PK by minimizing general tissue binding and maximizing tissue penetration and late uptake. 122 5.4.2 Implications for Angiogenic Growth Factor Delivery We used the non-perfused myocardium model for the studies in this Chapter to highlight the effects of tissue binding. However, in the in-vivo heart, binding and capillary washout act simultaneously on FGF transport. Any gain in penetration depth as a result of binding modulation to increase the free to bound fraction of FGF by increasing source concentration would be dampened by the effect of microvascular flow (previous 3 chapters). Even higher doses of drug must be delivered to overcome both binding and clearance impedance. The myocardial and other vascularized tissue environment, therefore, present a remarkable challenge for growth factor transport, and a possible reason for mixed success in pro-angiogenic therapy. Conjugation of FGF to SOS is an attractive approach for minimizing the effects of binding and of microvascular washout. SOS conjugation reduces general tissue binding by neutralizing HSPG-FGF interactions and also induces dimerization of FGF and effectively minimizes microvascular washout as shown in Chapter 2. This approach, however, can come at a cost of doubling the molecular weight as FGF-SOS complex is twice the size of FGF, but this 2-fold increase in size is still significantly better than the >10-fold increase with the common use of UFH as protective groups for FGFs. The slow transport as a result of increasing in steric hindrance, however, may be overcome with using controlled release sources that can sustain release for longer time. As shown in previous chapters, molecular washout hence transendothelial permeability is more dominant determinant of myocardial transport in-vivo and in the presence of angiogenic response, SOS conjugation provides a possible modulation of transendothelial permeability of FGF while also overcoming transport impedance due to general 123 tissue binding. Furthermore, our results in this Chapter also raise an important implication specific to pro-angiogenic therapy. As capillaries sprout and grow in response to angiogenic therapy, they can retard drug penetration not only by clearing drugs, as highlighted in the previous chapters, but also further by increasing specific and non-specific binding sites to drugs. This is because blood vessels are lined with HSPG rich basement membranes. The increase in vascularity as a result of successful therapy potentially results in a stronger negative feedback response than predicted in Chapter 4, ultimately limiting the very angiogenic process the treatment is trying to promote. This negative feedback could additionally account for the challenge of achieving sustained therapeutic angiogenesis in clinical trials. The increase in binding site density may not be a simple linear function of vascularity and may also drastically over time, which can introduce additional complexity to the system. The full implications of this effect, therefore, merit detailed investigation. 124 5.5 Summary Tissue binding further complicates the complex local myocardial pharmacokinetics of angiogenic growth factors described in previous chapters. Specific and general binding act as double-edged swords, increasing local tissue uptake while drastically restricting tissue penetration. Protective groups, if carefully selected, act to curtail the "binding site barrier" problem. Growth factor formulation and engineering myocardial drug delivery systems based on careful analysis of local myocardial pharmacokinetics and pharmacodynamics can improve drug penetration and potentially angiogenic therapy outcome. 125 5.6 References 1. 2. 3. 4. 5. 6. 7. 8. 9. 10. 11. 12. 13. 14. 15. Baxter LT, Zhu H, Mackensen DG, Jain RK. Physiologically based pharmacokinetic model for specific and nonspecific monoclonal antibodies and fragments in normal tissues and human tumor xenografts in nude mice. Cancer Res. 1994; 54:1517-1528. Juweid M, Neumann R, Paik C, Perez-Bacete MJ, Sato J, van Osdol W, Weinstein JN. Micropharmacology of monoclonal antibodies in solid tumors: direct experimental evidence for a binding site barrier. Cancer Res. 1992; 52:5144-5153. Netti PA, Berk DA, Swartz MA, Grodzinsky AJ, Jain RK. Role of extracellular matrix assembly in interstitial transport in solid tumors. Cancer Res. 2000; 60:2497-2503. Saga T, Neumann RD, Heya T, Sato J, Kinuya S, Le N, Paik CH, Weinstein JN. Targeting cancer micrometastases with monoclonal antibodies: a binding-site barrier. Proc Natl Acad Sci U S A. 1995; 92:8999-9003. van Osdol W, Fujimori K, Weinstein JN. An analysis of monoclonal antibody distribution in microscopic tumor nodules: consequences of a "binding site barrier". Cancer Res. 1991; 51:4776-4784. Rosengart TK, Johnson WV, Friesel R, Clark R, Maciag T. Heparin protects heparinbinding growth factor-I from proteolytic inactivation in vitro. Biochem Biophys Res Commun. 1988; 152:432-440. Filion RJ, Popel AS. Intracoronary administration of FGF-2: a computational model of myocardial deposition and retention. Am J Physiol Heart Circ Physiol. 2005; 288:H263279. Bashkin P, Doctrow S, Klagsbrun M, Svahn CM, Folkman J, Vlodavsky I. Basic fibroblast growth factor binds to subendothelial extracellular matrix and is released by heparitinase and heparin-like molecules. Biochemistry. 1989; 28:1737-1743. Dowd CJ, Cooney CL, Nugent MA. Heparan sulfate mediates bFGF transport through basement membrane by diffusion with rapid reversible binding. J Biol Chem. 1999; 274:5236-5244. Flaumenhaft R, Moscatelli D, Rifkin DB. Heparin and heparan sulfate increase the radius of diffusion and action of basic fibroblast growth factor. J Cell Biol. 1990; 111:1651 1659. Jaye M, Schlessinger J, Dionne CA. Fibroblast growth factor receptor tyrosine kinases: molecular analysis and signal transduction. Biochim Biophys Acta. 1992; 1135:185-199. Kardami E, Liu L, Pasumarthi SK, Doble BW, Cattini PA. Regulation of basic fibroblast growth factor (bFGF) and FGF receptors in the heart. Ann N Y Acad Sci. 1995; 752:353369. Liu L, Pasumarthi KB, Padua RR, Massaeli H, Fandrich RR, Pierce GN, Cattini PA, Kardami E. Adult cardiomyocytes express functional high-affinity receptors for basic fibroblast growth factor. Am J Physiol. 1995; 268:H1927-1938. Sheikh F, Sontag DP, Fandrich RR, Kardami E, Cattini PA. Overexpression of FGF-2 increases cardiac myocyte viability after injury in isolated mouse hearts. Am J Physiol Heart Circ Physiol. 2001; 280:H1039-1050. Asundi VK, Keister BF, Stahl RC, Carey DJ. Developmental and cell-type-specific expression of cell surface heparan sulfate proteoglycans in the rat heart. Exp Cell Res. 1997; 230:145-153. 126 16. 17. 18. 19. 20. 21. 22. 23. 24. Li J, Shworak NW, Simons M. Increased responsiveness of hypoxic endothelial cells to FGF2 is mediated by HIF-1 alpha-dependent regulation of enzymes involved in synthesis of heparan sulfate FGF2-binding sites. J Cell Sci. 2002; 115:1951-1959. Paul D. Effect of immobilizing adsorption on the diffusion time lag. Journal of Polymer Science A-2. 1969; 7:1811-1818. Crank J. The mathematics of diffusion. 2d ed. Oxford, [Eng]: Clarendon Press; 1979. Briggs GE, Haldane JB. A Note on the Kinetics of Enzyme Action. Biochem J. 1925; 19:338-339. Tzafriri A, Levin A, Edelman E. Diffusion-Limited Binding Explains Binary Dose Response for Local Arterial and Tumor Drug Delivery. Cell Proliferation. 2008. Elmalak O, Lovich MA, Edelman E. Correlation of transarterial transport of various dextrans with their physicochemical properties. Biomaterials. 2000; 21:2263-2272. Hwang CW, Edelman ER. Arterial ultrastructure influences transport of locally delivered drugs. Circ Res. 2002; 90:826-832. Yeh BK, Eliseenkova AV, Plotnikov AN, Green D, Pinnell J, Polat T, Gritli-Linde A, Linhardt RJ, Mohammadi M. Structural basis for activation of fibroblast growth factor signaling by sucrose octasulfate. Mol Cell Biol. 2002; 22:7184-7192. Omitz DM, Herr AB, Nilsson M, Westman J, Svahn CM, Waksman G. FGF binding and FGF receptor activation by synthetic heparan-derived di- and trisaccharides. Science. 1995; 268:432-436. 127 Chapter 6: Future Studies and Conclusions 6.1 Future Studies This thesis attempted to identify and characterize the key determinants of local pharmacokinetics and effects of angiogenic growth factors in myocardial tissue. In doing so, we reported an important finding that growth factor deposition and tissue penetration are tightly coupled to the growth factor pharmacodynamics through microvascular clearance. A computational model of myocardial drug delivery and effect incorporating experimental parameters and boundary conditions was constructed to predict tissue distribution of growth factor concentration and biologic effect. This model predicts that steady state angiogenic effect can be significantly affected by altering drug's trans-endothelial permeability and can be for used as a basis for optimization studies. As in any study of complex issues, the work in this thesis also raised several questions that need to be addressed to further our understanding of local myocardial drug transport. 6.1.1 Characterization of Trans-endothelial Permeability in Myocardium. The most important implication from our studies is that microvascular clearance acts as a link between local myocardial pharmacokinetics and angiogenic pharmacodynamics. Microvascular clearance is in turn affected by the vascular density and trans-endothelial permeability. Since the goal of pro-angiogenic therapy is to maximize tissue vascularity, controlling trans-endothelial permeability offers the most effective handle on the negative pharmacodynamic feedback. Many experimental models have offered ways to quantify trans- 128 endothelial permeability. Permeability values of a-lactalbumin, a globular protein of comparable size to FGF, were reported for frog mesenteric capillaries 1, 2 and rat mesenteric capillaries 3 FGF's trans-endothelial permeability, however, has not been reported. Although it remains a technical challenge to experimentally quantify myocardial capillary permeability of molecules, it is important to be able to have an accurate assay for in-vivo permeability. This assay can provide screening tool for evaluating drugs with favorable pharmacokinetic properties prior to pharmacodynamics testing in costly animal experiments. Furthermore, angiogenesis is a highly dynamic process in that vascular properties including trans-endothelial permeability can change drastically. Such dynamic changes have not been explored but its characterization would provide a better understanding of the temporal PKPD changes and suggest ways to design drug delivery strategy. For example, one can design a drug controlled release profile to take advantage of the PK-PD changes and give appropriate maintenance dose of growth factors to sustain long term chemotactic and survival signals for the neo-vascularization. 129 6.1.2 Computational Models of Angiogenesis. The angiogenic model created in this thesis is a simple mechanistic model in twodimensional space to provide both a proof of concept and a first order estimate of the angiogenic response. There exist many models of angiogenesis of varying complexity in the literature 4-9. A unifying model remains to be explored. Since the biology of angiogenesis is an active area of research and many the details of this process have not been fully defined. This is especially true in the context of myocardial tissue. It is envisioned that a more detailed model of angiogenesis in three dimensions can be coupled with local continuum pharmacokinetic model to provide a good tool for predicting biologic response from any drug compound with any delivery modality. 6.1.3 Characterization of Effect of Binding We attempted to characterize the effect of binding on growth factor transport in myocardium using FGF as a model molecule. Although tissue binding was shown to have a significant impact on FGF effective diffusivity, several questions remained unanswered. Since the effect of binding on transport and deposition can be highly non-linear, tissue studies require sensitive and high resolution assay of spatio-temporal distribution of FGF, its intermediate binding complexes, tissue binding sites and biological response. Better knowledge of the effect of binding on growth factor tissue transport can be included in our PK-PD to provide a more comprehensive model to predict tissue response following local drug delivery. 130 Similar to trans-endothelial permeability, tissue binding sites may be altered drastically during the angiogenic process and can further contribute to the negative pharmacodynamic feedback. A high resolution characterization of binding site dynamics as a response to growth factor delivery would be an important contribution in building a better PK-PD model of angiogenic response following therapy. 131 6.2 Thesis Summary Early enthusiasm over angiogenic therapy has been tempered by a series of failed clinical trials with a wide range of mixed results. This thesis was designed to critically examine whether the limited late efficacy of local delivery of angiogenic factors could be explained by a detailed understanding of local pharmacokinetics and pharmacodynamics in the myocardial tissue. Our combination of ex-vivo, in-vivo and computational modeling has provided novel insights into local therapeutic angiogenesis and suggests that early success at inducing vessel growth powerfully self-regulates angiogenic therapies by dynamically altering local tissue pharmacokinetic properties and imply that it may be possible to modulate the local pharmacokinetics by better drug, drug formulation and drug delivery device designs. 132 6.3 References 1. 2. 3. 4. 5. 6. 7. 8. 9. 10. 11. 12. 13. 14. 15. Fu BM, Shen S. Structural mechanisms of acute VEGF effect on microvessel permeability. Am J Physiol Heart Circ Physiol. 2003; 284:H2124-2135. Huxley VH, Curry FE, Adamson RH. Quantitative fluorescence microscopy on single capillaries: alpha-lactalbumin transport. Am J Physiol. 1987; 252:H188-197. Zeng M, Zhang H, Lowell C, He P. Tumor necrosis factor-alpha-induced leukocyte adhesion and microvessel permeability. Am J Physiol Heart Circ Physiol. 2002; 283:H2420-2430. Balding D, McElwain DL. A mathematical model of tumour-induced capillary growth. J Theor Biol. 1985; 114:53-73. Bauer AL, Jackson TL, Jiang Y. A cell-based model exhibiting branching and anastomosis during tumor-induced angiogenesis. Biophys J. 2007; 92:3105-3121. Byrne HM, Chaplain MA. Mathematical models for tumour angiogenesis: numerical simulations and nonlinear wave solutions. Bull Math Biol. 1995; 57:461-486. Levine HA, Sleeman BD, Nilsen-Hamilton M. A mathematical model for the roles of pericytes and macrophages in the initiation of angiogenesis. I. The role of protease inhibitors in preventing angiogenesis. Math Biosci. 2000; 168:77-115. McDougall SR, Anderson AR, Chaplain MA. Mathematical modelling of dynamic adaptive tumour-induced angiogenesis: clinical implications and therapeutic targeting strategies. J Theor Biol. 2006; 241:564-589. Milde F, Bergdorf M, Koumoutsakos P. A hybrid model for three-dimensional simulations of sprouting angiogenesis. Biophys J. 2008; 95:3146-3160. Fannon M, Forsten KE, Nugent MA. Potentiation and inhibition of bFGF binding by heparin: a model for regulation of cellular response. Biochemistry. 2000; 39:1434-1445. Forsten KE, Fannon M, Nugent MA. Potential mechanisms for the regulation of growth factor binding by heparin. J Theor Biol. 2000; 205:215-230. Forsten-Williams K, Chua CC, Nugent MA. The kinetics of FGF-2 binding to heparan sulfate proteoglycans and MAP kinase signaling. J Theor Biol. 2005; 233:483-499. Richardson TP, Trinkaus-Randall V, Nugent MA. Regulation of basic fibroblast growth factor binding and activity by cell density and heparan sulfate. J Biol Chem. 1999; 274:13534-13540. Sperinde GV, Nugent MA. Heparan sulfate proteoglycans control intracellular processing of bFGF in vascular smooth muscle cells. Biochemistry. 1998; 37:13153-13164. Sperinde GV, Nugent MA. Mechanisms of fibroblast growth factor 2 intracellular processing: a kinetic analysis of the role of heparan sulfate proteoglycans. Biochemistry. 2000; 39:3788-3796. 133 APPENDIX: MATLAB code: PK-PD Model %This program calls gencap.m and transport2d.m. %Objective: to analyze sensitivity of Drug Distribution (or Deposition) vs. %number of capillaries started with. %Source location and flux are specified in transport2d.m %Independent variables: D, R, numcap %Variables to try: Flux, maxgrid clear all; warning('off'); rand('state',sum(100*clock)); %maximum computational grid dimension maxgrid=200; %um gridsize=5; %seconds tscale=l; % um^2/sec diffusivity D run um = [0.1 1 10 100]; % sec/um % resistance 1/permeability R run um = [1 10 100]; % initial cap density numcap run = [50 100 200 400 800 2400]; functional delay run = [6/(60*24) 1/24 3/24]; % MEAN functional delay (time to become sink) UNIT:DAYS % threshold of sprouting unit: ng/ml sprouting_threshold_run = [1 .1 .01 .001]; release rate run = [le-5 le-6 le-7 le-8 le-9 le-10 le-ll]; % Release rate unit: ngps MONTECARLONUMBER = 10; endtime = 3600*24*10*tscale; YES = 1; NO = 0; Check for presence of old simulation files % ------- paramfile = 'D_paramfile.mat'; fid = fopen(paramfile); fclose('all'); foundparamfile = 0; if (fid == -1) % NO Paramfiie, start new simulation disp(['--> Starting new simulation.']); disp([' ']); old D loop=l; old R loop=l; old numcap loop=l; oldfunctional delay loop=l; old_sprouting threshold_loop=l; old releaserateloop=l; old N=l; old 1=0; else % Paramfile found, load(paramfile); disp(['--> Continuing simulation.']); disp(['--> Paramfile located, re-starting from last saved file disp([' ']); load(filename); old D loop=Dloop; old R loop=R loop; old numcap_loop=numcap_loop; old_functional delay_loop=functional_delay_loop; old_sprouting_threshold loop=sprouting_thresholdloop; old releaserateloop=release rate loop; old N=N; old l=l+tscale; foundparamfile = 1; 134 ' filename '.']); % ----------------- end; for numcap_loop = old_numcaploop:length(numcap_run) numcap=numcap_run(numcap_loop); for N = old N:MONTECARLONUMBER for D_loop = old D_loop:length(Drun um) % um^2/sec DTissum = Drunum(D loop); %%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%% CHANGE for R loop = old R loop:length(R_run_um) % sec/um R um = Rrunum(R loop); %%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%% %%%%%%%%%%%55555%%%%%%%%%%%%%%%%%%%%% CHANGE for functional delay loop = oldfunctional_delay_loop:length(functional_delayrun) mean fdelay = 3600*24*functional_delay_run(fun seconds stdfdelay = ctional_delay_loop); % MEAN func delay unit: meanfdelay + 6*3600; % STDEV of func delay: seconds for sprouting_threshold_loop = old_sprouting_thresholdloop:length(sprouting thresholdrun) sprouting_threshold = sprouting_threshold_run(sprouting_thresholdloop);% unit: ng/ml for release_rate loop = oldrelease_rate_loop:length(release_rate_run) release rate = release rate run(releaserate loop); % unit: ngps fileroot = ['KL D' num2str(DTissum) ' R' num2str(R_um) 'Cp' num2str(numcap) '_Fd' num2str(meanfdelay) '_Ct' num2str(sprouting_threshold) '_RR' num2str(release_rate) '_N' ]; disp(['D ', num2str(Drun_um(D_loop))]); disp(['R ', num2str(R_run_um(R_loop))]); %disp(['capillary density ', num2str(numcaprun(numcap_loop))]); %disp(['Functional Delay ', num2str(functionaldelay_run(functional_delay_loop))]); %disp(['Sprouting Threshold ', num2str(sprouting_threshold_run(sprouting threshold_loop))]); %disp(['Release Rate ', num2str(release_rate_run(releaserateloop))]); %disp(['Montecarlo number ', num2str(N)]); %disp(['P_age ', num2str(sum(sum(p_age)))]); if (foundparamfile == 1) p=p; foundparamfile == 2; else cummulative dcl = 0; cummulative dcl2 = 0; cummulative dr = 0; cummulative cons =0; 135 cummulativedep =0; cummulative P=0; cummulative dr save =[]; cummulative dcl save =[1; cummulative dcl save2 =[]; cummulative cons save =[]; cummulative dep save =[]; cummulative P save=[]; 1 save =[]; c=zeros(maxgrid+2,maxgrid+2); pl = gencap(maxgrid+2,maxgrid+2,numcap); pl = l.-pl; p = pl; pnonsink = zeros(maxgrid+2); page = (p>O) .* (2); p resorp = zeros(maxgrid+2,maxgrid+2); t sub = zeros(maxgrid+2,maxgrid+2); t sub half = 3600*2 + rand(maxgrid+2)*3600*2*24; fdelay = rand(maxgrid+2)*std_fdelay + mean fdelay; end; RUNTRANSPORT = YES; DIFFERENTCAPILLARIES = YES; for l=old l:endtime, p(1:5,1:5) =0; % TRANSPORT %%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%% if (DIFFERENTCAPILLARIES == YES) RUNTRANSPORT = YES; end; if (RUNTRANSPORT == YES) m , [c,percentchange,DCL_sum,DCL_sum2,DR]=transport2d(c,p,maxgrid,gridsize,tscale,DTissum,R_u se rate); end; if relea (percentchange == 0) RUNTRANSPORT = NO; end; % Tracking drug over time cummulative dr = (cummulative dr + DR) cummulative dcl = (cummulative dcl+ DCL sum) cummulative dcl2 = (cummulative dcl2+ DCL_sum2) cummulative dep = (sum(sum(c(2:maxgrid+1,2:maxgrid+l)*gridsize^3))); cummulative cons = cummulative dr - (cummulative dep + cummulative_dcl2); cummulative-P = sum(sum(p(2:maxgrid+1,2:maxgrid+l))); if mod(1,600)==0 1 save = [1 save 1]; cummulative cummulative cummulative cummulative cummulative cummulative end; dr save = (cummulative dr save cummulative_dr] dcl save = [cummulative dcl save cummulative dcl]; dcl save2 = [cummulative dcl save2 cummulativedcl2]; dep save = [cummulative_dep_save cummulative_dep]; cons save = [cummulativecons save cummulative_cons]; P save = [cummulative P save cummulative P]; if mod(l,3600)==0 % %plot(1_save,cummulative dr save/max(cummulative dr save),'rx',l save,cummulative depsave/max(cu mmulative dr save),'go',1_save,cummulative dcl save2/max(cummulative dr save),'mo',l_save,cummula 136 P save),'k tive cons save/max(cummulative dr save),'ko',l_save,cummulative P save/max(cummulative +');drawnow; end % if mod(1,3600)==0 disp(['Time completed ', num2str(round(1/3600)), end; 'hours']); % ANGIOGENESIS %%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%% DIFFERENTCAPILLARIES = NO; rand mat0 l=get randmat2d(maxgrid); [pr,fc] = pr2d(c,maxgrid,gridsize,tscale,sprouting threshold); %Calculate probability of sprouting p_new = pr>=randmat0 _1; p nonsink = p_nonsink I (p new==l); %pnonsink: new but non-functional capillaries %Calculating local concentration around p_nonsink [avgC] = localconc(c,p_nonsink,maxgrid); % Tracking age of new capillaries p_age = page + ((avgC*lel2>sprouting_threshold).*(p_nonsink*tscale)); p_age = p age .* (1-presorp); p_before = p; % Determine if capillaries are functional p(3:maxgrid,3:maxgrid) = (p(3:maxgrid,3:maxgrid)==l) I ((page(3:maxgrid,3:maxgrid) > fdelay(3:maxgrid,3:maxgrid) (p(1:maxgrid-2,3:maxgrid)~=1) & (p(2:maxgrid-1,3:maxgrid)~=l) & (p(4:maxgrid+1,3:maxgrid)~-=l) & (p(5:maxgrid+2,3:maxgrid)~=1) & (p(3:maxgrid,l:maxgrid-2) =1) & (p(3:maxgrid,2:maxgrid-l)=l) & (p(3:maxgrid,4:maxgrid+l) =l) & (p(3:maxgrid,5:maxgrid+2)~=1) & ... .. .. ... ... ... ... p(1:5,1:5) = 0; p_after = p; p_diff = p_after - pbefore; % Conserve drugs at new nodes where tissue --> capillary if sum(sum(pdiff)) > 0 , 2:maxgrid+l) + = c(l:maxgrid , 2:maxgrid+l) c(l:maxgrid (p_diff(2:maxgrid+1,2:maxgrid+l)==l).*(c(2:maxgrid+1,2:maxgrid+l)/4); = c(3:maxgrid+2 , 2:maxgrid+l) + c(3:maxgrid+2 , 2:maxgrid+l) (pdiff(2:maxgrid+l,2:maxgrid+l)==l).*(c(2:maxgrid+l,2:maxgrid+1)/4); = c(2:maxgrid+l , l:maxgrid) + c(2:maxgrid+l , 1:maxgrid) (p_diff(2:maxgrid+l,2:maxgrid+l)==l).*(c(2:maxgrid+l,2:maxgrid+l)/4); = c(2:maxgrid+l , 3:maxgrid+2) + c(2:maxgrid+1 , 3:maxgrid+2) (p diff(2:maxgrid+1,2:maxgrid+l)==l).*(c(2:maxgrid+l,2:maxgrid+l)/4); c=c.*(l-p); DIFFERENTCAPILLARIES = YES; end; %REGRESSION%%%%%%%%%%%%%%%%%%%%%%%%%%% %%% [avgC] = localconc(c,p,maxgrid); 137 %unit conversion ctngum3 = sprouting_threshold * le-12; t sub = (avgC < ctngum3) .* (t_sub + tscale); p before = p; resorptioncondition = (t sub > t sub half); (p - resorption_condition) p = pl p after = p; p resorp = p before - p_after; clear pt sub p_rand ; %%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%% if (1 <= 3600) & mod(1,600)==0 & (1-~=0) filename = [fileroot wwnum2ipstr(N) '_tmin' num2str(round(1/60)) disp(['Completed ' filename]); save(filename);save(paramfile,'filename'); disp(['Capillaries ', num2str(sum(sum(p)))]); % disp(['P_age ', num2str(sum(sum(p_age)))]); % end if mod(1,7200)==0 & (l~=0) filename = [fileroot wwnum2ipstr(N) ' thr' num2str(round(1/3600)) disp(['Completed ' filename]); % save(filename);save(paramfile,'filename'); disp(['Capillaries ', num2str(sum(sum(p)))]); % disp(['P age ', num2str(sum(sum(p_age)))]); % disp(['RR' num2str(releaserate) ' ' num2str(1/60)]); % '.mat']; '.mat']; end if l==endtime 1 = 1; old 1 = 1; numcap loop=min(numcap_loop+l,length(numcap_run)); N=min(N+1,MONTECARLONUMBER); Dloop=min(D_loop+l,length(D_run_um)); R loop=min(Rloop+l,length(R_run_um)); functional delay loop=min(functional delay_loop+l,length(functional_delay_run)); sproutingthreshold_loop=min(sprouting thresholdloop+l,length(sprouting_threshold_run)); releaserateloop=min(release_rateloop+l,length(release_rate_run)); filename = [fileroot wwnum2ipstr(N) '_thr' num2str(round(1/3600)) disp(['Completed ' filename]); save(filename);save(paramfile,'filename'); disp(['Capillaries ', num2str(sum(sum(p)))]); % disp(['P_age ', num2str(sum(sum(p_age)))]); % disp(['RR' num2str(releaserate) ' ' num2str(1/60)]); % end; end; % 1 loop ie time cummulative cummulative cummulative cummulative cummulative cummulative dcl = 0; dcl2 = 0; dr = 0; cons =0; dep =0; P=0; cummulativedr save =[]; cummulative dcl save =[]; cummulative dcl save2 =[]; cummulative cons save =[]; cummulative dep save =[]; 138 '.mat']; end; cummulative P save=[]; 1 save =[]; c=zeros(maxgrid+2,maxgrid+2); pl = gencap(maxgrid+2,maxgrid+2,numcap); pl = l.-pl; p = pl; p nonsink = zeros(maxgrid+2); page = (p>O) .* (2); p_resorp = zeros(maxgrid+2,maxgrid+2); t sub = zeros(maxgrid+2,maxgrid+2); t sub half = 3600*2 + rand(maxgrid+2)*3600*2*24; fdelay = rand(maxgrid+2)*std_fdelay + mean_fdelay; ') disp(' end; %release rateloop %sprouting thresholdloop end; %functional_delay loop end; end; %R loop end; %D loop end; %MONTECARLONUMBER end; %numcap loop % Function Gencap % capmatrix = gencap (totX,totY,numcap); % totX is dimension in X direction, totY is dimension in Y direction, % numcap is number of capillaries desired % Generates 2D cross section of random capillaries, no two adjacent. % Border of matrix has no capillaries (border is all l's) % 1 = tissue, 0 = capillary % IMPORTANT: BECAUSE OF NO TWO ADJACENT CONDITION, numcap should be % much less than 1/3*(totX-2)*(totY-2), OR ELSE WILL NOT BE ABLE TO % FIT IN ALL THE CAPILLARIES function capmatrix = gencap (totX,totY,numcap); if (numcap > 0.32*(totX-2)*(totY-2)) disp('WARNING: MAY NOT BE ABLE TO FIND SPOTS FOR ALL YOUR CAPILLARIES!'); end; TRUE = 1; FALSE = 0; capmatrix = ones(totX,totY); % Positions of spots that are caps used X = [0]; used Y = [0]; % Resets random seed generator to clock rand('state',sum(100*clock)) for count = l:numcap approvedposition = FALSE; spots tried = 0; while ((approved_position == FALSE) & (spots_tried <= 2*totX*totY)) % Pick numbers between 2 to totX-1 or totY-1 inclusive try X = round(rand*(totX-3))+2; 139 try Y = round(rand*(totY-3))+2; spots_tried = spots_tried + 1; % Find the relative displacement of the trial point from all of % the other "good points" selected thus far displace_X = abs(tryX - used_X); displace_Y = abs(try_Y - used_Y); tot displace = displace_X+displace_Y; % If total displacement is greater than 1, accept if min(tot displace > 1) approved position = TRUE; end; end; if (spots tried > 2*totX*totY) disp(['Placed ' num2str(count) ' points. break; else % Found a spot -> place it in capmatrix capmatrix(try_X,try_Y) = 0; used _X = [used X try X]; usedY = [used Y try Y]; end; Cannot find more spots.']); end; function [C,percentchange,DCLsum,DCL-sum2,DR]=transport2d(C,P,maxgrid,gridsize,tscale,DTiss-um,R-um,relea se rate); YES = 1; NO = 0; CAPILLARY IS SINK = YES; dx = 1; % dx = 1 = gridsize microns dy = 1; % dy = 1 = gridsize microns % Size of simulation space: Each pixel = gridsize microns x = maxgrid+2; y = maxgrid+2; % Scaling of Tissue Diffusion Constants DTiss = DTiss um/(gridsize^2)*tscale; % Convert units into gridsizes and tscales % Scaling of Endothelial Resistances R = R um/tscale*gridsize; % Convert units into gridsizes and tscales if (R um == 0) DEnd = DTiss; else DEnd = dx/R; % Effective Endothelial Diffusion Constant end; % Scaling of Time Constants dt raw = min([l dx^2/(4*max([DEnd DTiss]))]); dt = 1/(ceil(l/dt raw)); % Scaling of Capillary constants K = 0; % Inactivation constant U = 0; % Uptake constant DX = DTiss*ones(x-l,y-2); % Diffusivities in X DY = DTiss*ones(x-2,y-l); % Diffusivities in Y % Change Diffusion Matrices DX(l:x-2,:) = DX(l:x-2,:) DX(2:x-l,:) = DX(2:x-l,:) DY(:,l:y-2) = DY(:,l:y-2) - Based on Capillary Positions P(2:x-1,2:y-1).*DX(l:x-2,:) + P(2:x-1,2:y-l)*DEnd; P(2:x-1,2:y-1).*DX(2:x-l,:) + P(2:x-1,2:y-l)*DEnd; P(2:x-1,2:y-1).*DY(:,l:y-2) + P(2:x-1,2:y-l)*DEnd; 140 DY(:,2:y-1) = DY(:,2:y-1) - P(2:x-1,2:y-1).*DY(:,2:y-1) + P(2:x-1,2:y-l)*DEnd; %DTiss %DEnd %'dt/dx^2*DTiss' %dt/dx^2*DTiss %'dt/dx^2*DEnd' %dt/dx^2*DEnd %'dt*dx*DTiss' %dt*dx*DTiss %'dt*dx*DEnd' %dt*dx*DEnd % Find drug amount olddrug = sum(sum(C(2:x-1,2:y-1))); DCL sum = 0; DCL sum2=0; DR = 0; for fraction of tscale = 1: round(l/dt) %Constant flux BC conditions RR ngps = release_rate; %in ngps %delta V = gridsize^3; C(2,2)= C(2,2) + (RR ngps*tscale*dt)/gridsize^3; %C changes by delta_C due to released substance DR = DR + (RR ngps*tscale*dt); % Impose Symmetry Boundary Conditions C(1,:) = C(2,:); C(x,:) = C(x-l,:); C(:,l) = C(:,2); C(:,y) = C(:,y-l); % Impose Zero Boundary Conditions %C(1,:) %C(x,:) %C(:,l) %C(:,y) = 0; = 0; = 0; = 0; % Calculate Drug Loss through Permeation into Capillary DCL = sum(sum((P(2:x-1,2:y-l)==l).*((dt*dx)*(DX(l:x-2,:).*C(:x-2,2:y -1) + DX(2:x- 1,:).*C(3:x,2:y-1)) + (dt*dy)*(DY(:,l:y-2).*C(2:x-l,l:y-2) + DY(:,2:y-1).*C(2:x-1,3:y))))); DCL sum = DCL sum + DCL; % Diffuse %C(2:x-1,2:y-1) %'sum C*vol BEFORE Diffuse' %sum(sum(C(2:x-1,2:y-l)*gridsize^3)) C(2:x-1,2:y-1) = C(2:x-1,2:y-1) + ... (dt/dx^2)*(DX(1:x-2,:).*C(1:x-2,2:y-)-(DX(1:x-2,:)+DX(2:x-1,:)).*C(2:x-1,2:y-1)+DX(2:x1,:).*C(3:x,2:y-1)) + ... (dt/dy^2)*(DY(:,1:y-2).*C(2:x-1,1:y-2)-(DY(:,l:y-2)+DY(:,2:y-1)).*C(2:x-1,2:y1)+DY(:,2:y-1).*C(2:x-1,3:y)); %C(2:x-1,2:y-1) %'sum C*vol AFTER Diffuse' %sum(sum(C(2:x-1,2:y-l)*gridsize^3)) DCL2 = sum(sum((C(2:x-1,2:y-1).*P(2:x-1,2:y-1))*gridsize^3)); DCL sum2 = DCL sum2 + DCL2; % Impose Capillary Conditions; (CAPILLARY IS SINK == YES) C(2:x-1,2:y-1) = C(2:x-1,2:y-1) .* (1-P(2:x-1,2:y-1)) else C(2:x-1,2:y-1) = C(2:x-1,2:y-1) - (dt*(K+U))*P(2:x-1,2:y-1).*C(2:x-1,2:y-1); if 141 end; %C(2:x-1,2:y-1) %'sum C*vol AFTER Diffuse and SINK' %sum(sum(C(2:x-1,2:y-l)*gridsize^3)) % 'sum C*vol + DCL' %sum(sum(C(2:x-1,2:y-l)*gridsize^3)) + DCL_sum2 %'Permeability Matrix' %P end; newdrug = sum(sum(C(2:x-1,2:y-1))); % Check if steady state has been reached if (olddrug > 0) percentchange = 100*(newdrug-olddrug)/olddrug; else percentchange = 1; end; % in: c (concentration matrix) % out: pr (probability matrix: probability of capillary formation at each position) function [pr,fc] = pr2d(c,maxgrid,gridsize,tscale,sprouting threshold); % Converting ng/um3 to ng/ml: ng/um3*(10^4um/lcm)^3 c-ngml=c*lel2; % [ng/ml] threshold concentration 2 orders of mag below ct=sprouting_threshold; c saturation: 30-3000ng/ml vessel density increases significantly, 3000-30,000 does not produce more vessels: Dellian M et.al.Am.J.Pathol 1996; Yuan & Tong's paper uses 5ng/ml % constant control shape of fc curve alpha=10; fc=(c ngml>=ct).*(l-exp((-alpha)*(c_ngml-ct))); Smax= 5e-4/3600; % (um.sec)^(-l); pr=Smax*fc*tscale*gridsize^3; % function newstr=wwnum2ipstr(num); % Forms a string with leading zeros as in IPLab save format. Output String Input Number % Examples: 0010 10 % % 165 0165 function newstr=wwnum2ipstr(num); if (num==0) newstr='0000'; elseif (num<10) newstr=['000' num2str(num)]; elseif (num<100) newstr=['00' num2str(num)]; elseif (num<1000) newstr=['0' num2str(num)]; else newstr=num2str(num); end 142