The AAPS Journal, Vol. 16, No. 3, May 2014 ( # 2014) DOI: 10.1208/s12248-014-9585-8 Research Article A Network Modeling Approach for the Spatial Distribution and Structure of Bone Mineral Content Hui Li,1 Aidong Zhang,1 Lawrence Bone,2 Cathy Buyea,2 and Murali Ramanathan3,4,5 Received 22 November 2013; accepted 28 February 2014; published online 27 March 2014 ABSTRACT. This study aims to develop a spatial model of bone for quantitative assessments of bone mineral density and microarchitecture. A spatially structured network model for bone microarchitecture was systematically investigated. Bone mineral-forming foci were distributed radially according to the cumulative normal distribution, and Voronoi tessellation was used to obtain edges representing bone mineral lattice. Methods to simulate X-ray images were developed. The network model recapitulated key features of real bone and contained spongy interior regions resembling trabecular bone that transitioned seamlessly to densely mineralized, compact cortical bone-like microarchitecture. Model-simulated imaging profiles were similar to patients’ X-ray images. The morphometric metrics were concordant with microcomputed tomography results for real bone. Simulations comparing normal and diseased bone of 20–30 to 70–80 year-olds demonstrated the method’s effectiveness for modeling osteoporosis. The novel spatial model may be useful for pharmacodynamic simulations of bone drugs and for modeling imaging data in clinical trials. KEY WORDS: bone; imaging; modeling; osteoporosis. INTRODUCTION According to the International Osteoporosis Foundation, osteoporosis is estimated to affect 200 million women and cause approximately 9 million fractures worldwide (1,2). About one in three women and one in five men, 50 years or older, are at risk of having an osteoporotic fracture in their lifetime (1,3,4). The prevalence and costs of osteoporotic fractures will increase in many parts of the developed world because of demographic shifts that have resulted in an increasing proportion of older adults in the population (5). Bone fractures and diseases of the musculoskeletal system, which includes the bones and joints, frequently cause death, permanent disability, and loss of quality of life and independence in the geriatric population. Repairing damaged bone and restoring bone homeostasis is a therapeutic goal in diseases ranging from osteoporosis, many cancers including multiple myeloma, and in autoimmune diseases such as multiple sclerosis and rheumatoid arthritis (6,7). 1 Department of Computer Science and Engineering, State University of New York, Buffalo, New York, USA. 2 Department of Orthopedics, State University of New York, Buffalo, New York, USA. 3 Department of Pharmaceutical Sciences, State University of New York, Buffalo, New York, USA. 4 Department of Neurology, State University of New York, Buffalo, New York, USA. 5 To whom correspondence should be addressed. (e-mail: murali@buffalo.edu) 1550-7416/14/0300-0478/0 # 2014 American Association of Pharmaceutical Scientists Furthermore, many commonly prescribed drugs including the corticosteroids, anticancer agents, and certain antiepileptics increase bone loss. The molecular pathways regulating bone remodeling are thus major targets in drug discovery and development. A spatiotemporal model of bone could be very useful in many drug development settings because clinical trials for evaluating bone-modulating drugs require very large sample sizes and long study durations to enable meaningful assessment of fracture risk as a clinical endpoint. Pharmacologically, bone mineral density can be increased by either promoting osteoblast-mediated bone mineral deposition or by inhibiting bone resorption by osteoclasts. However, the increases in bone mineral density that result from administration of some bone drugs does not always correspond to decreased fracture risk. Although the antiresorptive bisphosphonates are potent and effective at increasing bone density and decreasing fracture risk in the first 5 years of use, their long-term effects on bone are not known (8). The orthopedics community is now increasingly limiting the duration use of bisphosphonate drugs because of reports of unexpected drug-related side effects including temporomandibular (jaw) joint osteonecrolysis (9–11) and increased risk of sudden femur fractures with unusual morphology (12,13) that are drawing increased regulatory scrutiny to this important class of drug. There are several pharmacokinetic-pharmacodynamic models for drugs that target bone homeostasis, e.g., antiresorptive agents and parathyroid hormone (14,15). These models are capable of describing drug kinetics and 478 Spatial Modeling of Bone 479 the time course of biomarkers of bone turnover (e.g., bone resorption biomarkers such as telopeptides of collagen and bone formation biomarkers such as bone alkaline phosphatase). However, it is currently very challenging to assess temporally distal clinical outcomes such as bone mineral density, bone microarchitecture changes, and fracture risk from the kinetics of drugs and the dynamics of biomarkers from these models, which change over shorter time scales. Consequently, regression techniques and Hill-type transduction functions are often used to empirically relate pharmacodynamic outputs to these important clinical outcomes. Our goal is to develop a novel spatiotemporal model and an effective mechanism-based in silico platform for evaluating the efficacy and pharmacodynamics of drugs and drug dosing regimens in diseases that affect bone health. A good spatiotemporal model can be useful in clinical and drug development settings because: (1) model-derived measures of drug effects on bone mineral density, bone mineral distribution, and microarchitecture can be investigated in silico; (ii) bone imaging results from dual-energy X-ray absorptiometry (DEXA) can be visualized; (3) the differential impact of drugs on different body sites that have different proportions of trabecular and cortical bone can be evaluated; and (4) a mechanistic understanding of the relationship of bone mineral distribution and microarchitecture to fracture risk can be obtained. In this research, we focus on developing the spatial characteristics of such a modeling strategy. We demonstrate how bone mineral distribution and microarchitecture can be incorporated to obtain spatially informative models that can be individualized from imaging data obtained in clinical settings. MODELING AND METHODS Spatial Model Geometry We modeled a cylindrical region of bone with outside radius R O and length L because we had dual X-ray absorptiometry data for the femur available. For ease of understanding, a schematic of spatial approach in its simplest two-dimensional form is shown in Fig. 1. The three-dimensional extension of the schematic approach represented in Fig. 1 was used for modeling. The steps in the spatial model are as follows: Step 1. Distribution of Bone-Forming Foci for Voronoi Tessellation The radial distribution of the mean number of bone-forming foci c(r) followed a cumulative normal distribution: c0 cðrÞ ¼ pffiffiffiffiffi σ 2π Zr −ðu−uÞ2 =2σ2 e du −∞ r is the radial coordinate, the mean and standard deviation of the normal distribution are denoted by μ and σ, respectively, c0 is a constant of proportionality, and u is a dummy integration variable for the radial coordinate. Within a differential region dA=2πr dr, the actual number of bone mineral-forming foci was obtained as Poisson variate, Poisson(λ(r)), whose rate parameter λ(r) was set to c(r). The axial and angular distribution of the foci was assumed to follow a uniform distribution. These foci were used as the centers or sites for the Voronoi tessellation in step 2. Step 2. Voronoi Tessellation Voronoi tessellation is an algorithmic procedure that takes as input a set of points called Voronoi centers or sites and generates a closed lattice called Voronoi regions or cells that are bounded by straight lines or edges. In the two-dimensional case, the boundaries of Voronoi regions contain polygons and in the threedimensional case, the regions are closed polyhedra with polygonal faces. Every point on the polygonal face of a polyhedral Voronoi region is equidistant from the two nearest Voronoi sites. Thus, every point inside of a given Voronoi region is closer to its own site than to adjoining sites. The field of bone mineral-forming foci created in step 1 provided the set of Voronoi centers or sites that were subject to Voronoi tessellation. The edges of Voronoi cells were interpreted as the structural matrix upon which bone mineral was laid down. Step 3. Distribution of Bone Mineral Weights were assigned to the edges of the Voronoi lattice. Operationally, the weights were interpreted as the cross-sectional area of the bone mineral in the edge, which was interpreted to be cylindrical. The distribution of the circular cross-sectional area of bone mineral w(r) was also varied in the radial direction r according to a cumulative normal distribution: w0 wðrÞ ¼ pffiffiffiffiffi σ 2π Zr e−ðu−μÞ 2 =2σ2 du −∞ For calculations, the radial distance of the center of the edge was used to determine the weights, which were obtained by sampling random variates from the cumulative normal distribution. The mean, μ, and standard deviation, σ, of this cumulative normal distribution were fixed at the values used for the distribution of bone forming foci; w0 is a constant of proportionality and u is a dummy integration variable for the radial coordinate. Step 4. Stochastic Edge Pruning To generate a lattice with spatial characteristics that more closely resembled the real bone mineral lattices, the edges in the closed Voronoi lattice were randomly deleted with a low probability p. Random variates from the Bernoulli distribution, Bernoulli(p), were used to identify edges that were deleted or pruned. This created a lattice with containing both open and closed Voronoi regions. We refer to the lattice remaining after this Li et al. 480 a b the edges in the PVL: m¼ρ X wi l i edges The wi denotes the cross-sectional area of the edge, and li is the length of the edge. The true density of the bone mineral is denoted by ρ. Domain of Interest c Distribution of Centers Expression for Bone Mineral Density The bone mineral density (BMD) is the mass of bone mineral per unit of projected area. The BMD was calculated from the bone mineral mass, m, and the projected area, Ap, using: d BMD ¼ m m ρ X ¼ ¼ wi l i Ap 2R0 L 2R0 L edges Relationship to Imaging Data Voronoi Tessellation e Bounded Vornoi Tessellation We used Beer’s law to quantitatively relate the model to imaging findings from DEXA and X-ray imaging methods. According to Beer’s law, the logarithm of the fraction of electromagnetic energy absorbed is a linear function of the concentration of the absorbing species and the path length. Because the concentration of bone mineral varies along the direction y of the imaging beam, integration (summation) of Beer’s law over every differential element δy is needed for calculating the image intensity at position x from the center: X ln AðxÞ ¼ − αδyi f Weighted Graph Edge Pruning Fig. 1. A simple two-dimensional schematic of the Voronoi tessellation modeling procedure used to creating a spatial model for bone. a An annular region representing bone. b The random distribution of Voronoi centers from a cumulative normal distribution function with μ=0.3, σ=0.02, and c0 =1,500. c The result from Voronoi tessellation. d The Voronoi tessellation bounded by its outer boundary. e The result after the weights were assigned to the edges. f The weighted Voronoi tessellation after stochastic pruning stochastic edge-pruning step as the pruned Voronoi lattice (PVL). The probability of deletion was an exponential function of the edge weight wi, which represents the level of bone mineral. −βwi =wmax p¼e The wmax is the maximum value of wi and β is a nondimensional parameter akin to a rate constant that determines the extent of edge pruning. Expression for Bone Mineral Mass The mean mass of bone mineral m for a given realization of the network model was obtained as the summation over all j where A(x) is the fraction of the input intensity that is absorbed by bone mineral at position x from the center, α is the extinction coefficient, and δy is the differential path length of bone mineral along the path of the imaging beam. The summation is taken over every element of bone j traversed by the imaging beam. The procedure is equivalent to a Radon transform, which was computed using a MATLAB routine (MathWorks, Natick, MA, USA). The transmitted energy T(x) reaching the imaging device produces the intensity variations responsible for image formation: T ðxÞ ¼ 1−AðxÞ This equation can be extended to complex tissue containing for example, soft tissue, fat, and blood by incorporating different extinction coefficients for each material type in the tissue. Image Analysis We conducted image analysis of DEXA scans of the femur from patients to identify macroscopic radial and axial variations in BMD. The imaging data were analyzed using ImageJ (16,17) and BoneJ software tools (18). The values of μ and σ were estimated iteratively from imaging data. Spatial Modeling of Bone 481 computed using CTAn (v.1.13) software (SkyScan Software, http:// www.skyscan.be/products/downloads.htm). (R2, ) (R1, ) Image Processing (r2 = r1 R2/R1 , ) (r1, ) C1 C2 The MATLAB Image Processing Toolbox (MathWorks) was used. The bwboundaries routine was used to trace exterior boundaries in images from published papers. The boundary points were connected with a closed cubic B-spline using the bspline_deboor subroutine. Simulations of Diseased Bone Circle Arbitrary Shape Fig. 2. A schematic of the procedures used to model arbitrary shapes. Each vertex of the Voronoi polyhedral on the circle (left) is mapped to the corresponding position on the arbitrary shape (right). The centroids of the circle and the arbitrary shape are denoted by C1 and C2, respectively. The points (R1, θ) and (R2, θ) are the radial coordinates on the boundary. The radial coordinates of the Voronoi vertex at (r1, θ) in the circle are mapped to the corresponding point (r2, θ) on the arbitrary shape using the constant of proportionality R2/R1 Extension to Irregular Geometries We extended our approach to irregular geometries by mapping the vertices of the Voronoi polyhedra from a cylindrical geometry to the irregular three-dimensional geometry of interest. Consider the irregular geometry of interest summarized in Fig. 2. The coordinates of centroid of the shape at each value of distance z along the axis were computed. The outer perimeter of the irregular geometry was obtained using an alpha shape edge detection algorithm (alphavol, written for MATLAB by Jonas Lundgren) and fitted to a cubic spline to obtain a continuous function. The radial coordinates of the Voronoi polyhedra vertices from the center of the circle were mapped proportionately from the circle to the corresponding radial distances from centroid of the irregular geometry for each z. The proportionality factor was based on the ratio of the radius of the circle to the radial distance of the perimeter of the irregular shape from the centroid. The angular and axial coordinates and edges of the Voronoi polyhedra were identity mapped. For simulating examples of interindividual variability in BMD, we obtained the transverse dimensions and shape of the midline of right femur (23 cm from the proximal end) of a 52-year-old woman from Fig. 3d of the report by Locke (20). The bone mineral density and projected bone areas were obtained from statistical analyses of the National Health and Nutrition Examination Survey (NHANES) (21). The simulations were conducted with 1,000 centers and the modeling procedure for irregular bone shape. To allow direct comparisons of the microarchitecture of normal and diseased bone, we conducted analysis from the same Voronoi tessellation. RESULTS Schematic Representation of Bone Microarchitecture by Spatial Model Figure 1a schematically shows the procedure in a twodimensional form for obtaining the spatial model of bone architecture. The procedure involves (1) distributing points corresponding to the Voronoi centers in a circular regency. The density of the Voronoi centers was varied in the radial direction according to the cumulative normal distribution, (2) identification of the external boundary, (3) Voronoi tessellation, (4) the edges of the Voronoi polyhedra were randomly pruned, and (5) the edges remaining were assigned weights. Figure 2 shows how the approach of Fig. 1 can be extended to irregular geometry, and Fig. 3 is a schematic of the threedimensional version of the approach. The details of the simulations are provided in the “MODELING AND METHODS” sections. Concordance of Model with X-ray Images of Bone Quantitative Bone Morphometry Computed tomography (CT) enables the three-dimensional characteristics of bone to be obtained from imaging. We compared the results from our modeling to CT findings from using multiple bone morphometric metrics that have been established to assess structural properties of cortical and trabecular bone from CT data (19): (1) bone surface density, BS/TV, where BS is the bone surface area and TV is the total volume of the sample; (2) bone volume density, BV/TV, where BV is the bone mineral volume; (3) trabecular thickness, Tb.Th, is computed by filling maximal spheres into the bone mineral structure; (4) trabecular separation, Tb.Sp, is calculated by filling maximal spheres into the nonbone voxels; (5) trabecular number, Tb.N, is the inverse of the mean distance between the mid-axes of the structure. These parameters were Figure 4 shows the results from a three-dimensional model simulation that includes both top and side views. Figure 4e shows that the resulting representation visually resembles real bone in several key characteristics. For example, the regions closer to the outer circumference of the region are densely connected and compact like cortical bone, and the interior regions are more loosely connected and less dense like trabecular bone. The results suggest that our model provides an intuitive and parameterefficient approach for simulating the geometric appearance of bone tissue. Figure 4 shows the extensive concordance between the imaging results from spatial model and X-ray imaging of patient bone. Figure 4a is a representative region of interest in the femur on an X-ray image obtained from a Li et al. 482 a b c d e f g h i Fig. 3. The results from a three-dimensional implementation of the Voronoi tessellation modeling procedure. The six figures in the top two rows are the top-down views of the three-dimensional spatial structures obtained from steps shown in Fig. 1a–g. The lowest row shows the front views of the three-dimensional structures corresponding to Fig. 1b, e, and f. The outer surface was removed so that the interior can be seen h and i. The simulation parameters μ=0.25, σ=0.05, β=0.5, and c0 =3,000 were used postmenopausal patient with hip replacement. The red line in Fig. 4b represents the cross-section along the femur at which the observed variation of X-ray absorption plotted is shown in Fig. 4a. The corresponding results from the spatial model along a typical line, overlaid in Fig. 4b, demonstrate that the spatial model provides simulated X-ray profiles that are concordant with observed data. We computed the model Xray absorption profile across 20 transverse lines at equally spaced axial positions. The profiles were scaled to obtain the grayscale images in Fig. 4e. Figure 4e is granular because the grayscale images were obtained from a low-resolution axial scan with only 20 sections. Figure 4f was computed from Fig. 4e with an elliptical Gaussian filter and provides a two- dimensional grayscale image that is visually concordant with t he original bone image. Modeling Irregular Bone Shape To assess the usefulness of our method to irregular bone, we used the images and imaging results of the mandible from Moon et al. who provided imaging data and detailed information on multiple bone morphometric metrics (22). Notably, the morphometric metrics included multiple regions of interest and both regional measures as well as metrics that were representative of the microarchitecture. Figure 5a shows Spatial Modeling of Bone 483 a b 1 Image Intensity 0.8 0.6 0.4 0.2 0 0 0.25 0.5 0.75 1 Dimensionless Radial Distance Original X-ray Image Radial Profiles: Image vs. Model c d Front View from Model e z-Stack from Model f Top View from Model g Gaussian Filterd z-Stack from Model Tilted and Scaled Fig. 4. Modeling bone images. a A section of the X-ray image of femur from a postmenopausal hip transplantation patient with BMD of 0.90 g/cm2. b The distribution of image intensity across the radial section of bone shown as red line in a; also shows the normalized imaging intensity and the corresponding fit using the image modeling procedure. c, d The front and top view from a simulation with parameters μ=0.25, σ= 0.05, β=0.5, and c0 =6000 containing 20 z slices, respectively. e A z stack obtained by simulating an X-ray image in transmission mode using the Radon transform on the model. f Obtained with a Gaussian filter to “smooth” the boundary of the z stack image of Fig. 4e. g Simply rotates Fig. 4e by a 3° angle so that it can be compared more effectively with the original X-ray image of Fig. 4a, which is tilted relative to the vertical Li et al. 484 a b Model BV/TV (%) 40 30 20 10 0 0 10 20 30 40 50 Reported BV/TV (%) Model BS/BV (1/pixel) 16 c 14 12 10 8 8 10 12 14 16 Reported BS/BV (1/pixel) d 1.5 Model Tb.Sp (pixel) Model Tb.Th (pixel) 0.35 0.3 0.25 e 1 0.5 0.2 0.2 0.25 0.3 0.35 Reported Tb.Th (pixel) 0.5 1 1.5 Reported Tb.Sp (pixel) Fig. 5. Modeling results for an irregular geometry. a An image of the mandible that was analyzed in detail by Moon et al (22). These authors derived quantitative morphometric measures in the alveolar region (marked with Ts and Ti), the basal bone superior to the mandibular canal (marked M) and the basal bone inferior to the mandibular canal (B). b–e Comparison of the results for bone volume fraction (BV/TV), bone surface density (BS/BV), trabecular thickness (Tb.Th), and trabecular separation (Tb.Sp), respectively, from the modeling to the measurements obtained by Moon et al (22). The simulation parameters were μ=0.25, σ=0.05, β=1 and c0 =4,000. The slopes for the best-fit lines in b–e were 0.924, 0.84, 1.02, and 1.21, respectively. The Pearson correlation coefficients were greater than 0.99 in each case the irregular-shaped bone analyzed by Moon et al. and the three bone regions of interest for which they reported morphometric data. Figure 5b–d demonstrate the concordance between the morphometric metrics obtained from our modeling approach to those reported by Moon et al. These results indicate that our modeling approach can be generalized to bones with more complex geometries. Simulations of Diseased Bone Figure 6 summarizes our simulations of healthy and diseased femurs from 20- to 30- and 70- to 80-year-old women that were based on BMD statistics from the National Health and Nutrition Survey. The simulations were done for women because osteoporosis is more common in women after the onset of menopause. Spatial Modeling of Bone 485 20 to 30-year old 70 to 80-year old b 95th Percentile a d 50th Percentile c f 5th Percentile e Fig. 6. Top views of simulations of normal and diseased bone. a, c, and e The bone mineral density values at the 95th percentile, 50th percentile (median), and 5th percentile for 20- to 30-year-old women, respectively. b, d, f Bone mineral density values at the 95th percentile, 50th percentile (median), and 5th percentile for 70- to 80-year-old women, respectively. The shape and dimensions were obtained from the report by Locke, and the mean bone mineral density values for these age groups were obtained from Looker et al (21). The 5th, 50th (median), and 95th percentiles for BMD of the 20- to 30-year-old groups were 0.870, 1.078, and 1.292 g/cm2, respectively. The corresponding values for the 70- to 80-year-old groups were 0.731, 0.960, and 1.210 g/cm2. The values of μ were 0.5 for a and b, and 0.25 for c–f. The values of σ were 0.05 for a–d and 0.025 for the e–f. The β values for a–f were 1,000, 1, 10, 1, 5, and 1, respectively. The value of c0 =3,000 for a–f Figure 6a, c, e shows that at all of the three percentiles, the bone network lattice of the younger group was visually denser and more extensively connected than those of the older 70- to 80-year-old group. The 5th, 50th (median), 95th percentiles for BMD of the 20- to 30-year-old group were 0.870, 1.078, and 1.292 g/cm2, respectively. The corresponding values for the 70- to 80-year-old group were 0.731, 0.960, and 1.210 g/cm2. The loss of bone mineral is most apparent in Fig. 6f, which represents the 5th percentile of BMD values for the 70- to 80-year-old group. These findings suggest that the model may be sensitive to and capable of identifying changes in bone structure associated with age-related bone loss and osteoporosis. DISCUSSION We have systematically investigated a novel approach for modeling bone structure, the distribution of bone mineral content, and microarchitecture. The network-based threedimensional spatial model utilizes Voronoi tessellation and it yields structures that contain cortical and trabecular bone-like regions. We demonstrated that the modeling approach can be used to compute simulated X-ray images and that the resulting imaging profiles are concordant with the profiles obtained from patient bone. Li et al. 486 One of the unique aspects of our model is that structures similar to loosely organized, spongy trabecular bone and densely mineralized, compact cortical bone emerge spontaneously and transition seamlessly as a result of the modeling strategy. There is therefore no necessity for an artificially enforced boundary between cortical and trabecular bone in our model. The density distribution of the Voronoi centers and the pruning steps are the primary determinants of the trabecular-cortical structural variation that emerges. The radial location over which the transition between cortical and bone occurs is determined by the standard deviation term of the density distribution function. Another feature of our model is that interindividual variability in bone mineral lattice structure also emerges naturally in the modeling process. This is because of the stochastic nature of the initial distribution of Voronoi centers and the pruning steps. Delaunay triangulation, a mathematical method closely related to the Voronoi tessellation, is widely used in finite element modeling and has been used in biomechanical analyses of bone (23,24). However, our use of Voronoi tessellation in bone modeling differs substantially from the use of Delaunay triangulation in finite element modeling. In our model, Voronoi tessellation is used to create the microarchitecture of bone mineral. In finite element modeling, Delaunay triangulation is used to create a grid of points across which partial differential equations can be solved numerically. A limitation of our current approach is that it focuses principally on the spatial aspects of the bone mineral distribution. In the next step of our approach, the spatial pruned Voronoi lattice-based model will be elaborated to obtain a structural model through segmentation into a threecomponent composite material consisting of bone mineral, extracellular matrix, and blood. Recently, “universal” composition, hydration, and mineralization rules for bone tissues have been proposed that describe bone tissues of different ages, anatomical locations, and species (25–27). There is a linear relationship between mineral and organic content of bone. These rules can be leveraged as constraints that will provide a powerful strategy for parsimoniously elaborating our model from a spatial description of bone mineral to a richer model of bone tissue. The composition, microarchitecture, and dimensions of the bone would be needed as inputs for modeling. Such a structural model could be used to compute the mechanical properties of bone and simulate the risks of different types of fracture. However, the development of structural models to satisfactorily describe the loading patterns, complex biomechanics, and the fracture risk present many challenges that will require further research. It may be possible to apply approaches similar to those proposed by Fritsch et al. for this purpose (28). Additionally, further improvements to the method have to be made so that nonlinear regression techniques can be used more efficiently for parameter estimation. Many morphometric metrics have been developed to analyze bone images, particularly those from microcomputed tomography. A 2D box-counting algorithm has been used to obtain the fractal index, which is a geometric measure of bone (29) that takes on a value of 1 for hollow and a value of 2 for solid structures. Measurements of normal, osteopetrotic, and osteoporotic bone in clinical settings have fractal indices that are intermediate in magnitude. The fractal index is strongly correlated with trabecular spacing and number of trabeculae (30). However, our approach is not focused on the development and validation of individual morphometric measures for image analysis but instead on the development of comprehensive modeling framework. In Fig. 5, we demonstrated how the morphometric methods from images of real bone were concordant with those obtained from simulations of bone from our model. Compartmental, noncompartmental, and physiologically based compartmental models have been widely used in pharmacokinetic and pharmacodynamics modeling with great success. Some of these approaches have also been used to describe bone-modulating drugs (14,31). However, spatial information is lost within compartmental models because each compartment is treated as a well-mixed homogeneous region. Separate compartments are needed to describe interacting organs and spatial distributions. Furthermore, although plasma bisphosphonate concentrations decrease rapidly (within days) after dosing, bisphosphonate disposition is complex because of their avid binding to bone tissue. Bisphosphonate binding to bone is heterogeneous and exhibits preference for regions that have a high remodeling rate. The half-life of tissue-bound bisphosphonates has been reported to be as long as 1–10 years (32,33). Numerous modeling challenges are still unresolved in bisphosphonate pharmacokinetics and pharmacodynamics. Imaging has been an integral part of orthopedics diagnosis and treatment since the discovery of X-rays. With the advent of advanced imaging techniques, there is an even greater need of more effective and innovative modeling techniques that can better describe spatiotemporal processes parsimoniously. There is, however, a dearth of an effective repertoire of spatial models for pharmaceutical and clinical applications. Therefore, the development of conceptually novel spatial modeling techniques that have imaging capabilities may prove useful. ACKNOWLEDGMENTS AND DISCLOSURES Support from the National Multiple Sclerosis Society (RG4836-A-5) to the Ramanathan laboratory is gratefully acknowledged. CONFLICT OF INTEREST There are no conflicts of interest related to the work in the manuscript. 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