Complex Kinetics Systems and Synthetic Biology, 499A Copyright © 2008: Sauro 1 Unit Responses in Biochemical Networks Linear Hyperbolic Sigmoidal Copyright © 2008: Sauro 2 Where does the nonlinearity come from? Conservation Laws Bimolecular Binding Hyperbolic Sigmoidal Copyright © 2008: Sauro 3 Association or Binding Constant Ka the equilibrium constant for the binding of one molecule to another. Copyright © 2008: Sauro 4 Dissociation Constant Kd the equilibrium constant for dissociation. Copyright © 2008: Sauro 5 Enzyme Catalysis The set of reactions shown below is the classic view for enzyme catalysis. Enzyme binds to substrate to form enzyme-substrate complex. Enzyme-substrate complex degrades to free enzyme and product. Copyright © 2008: Sauro 6 Enzyme Catalysis Unfortunately the kinetic constants that describe enzyme catalysis are very difficult to measure and as a result researchers do not tend to use the explicit mechanism, instead they use certain approximations. The two most popular approximations are: 1. Rapid Equilibrium 2. Steady State Copyright © 2008: Sauro 7 Rapid Equilibrium Approximation The rapid equilibrium approximation assumes that the binding and unbinding of substrate to enzyme to much faster than the release of product. As a result, one can assume that the binding of substrate to enzyme is in equilibrium. That is, the following relation is true at all times (Kd = dissociation constant): Copyright © 2008: Sauro 8 Rapid Equilibrium Approximation Let Kd be the dissociation constant: Copyright © 2008: Sauro 9 Rapid Equilibrium Approximation The equilibrium concentration of ES can be found: Copyright © 2008: Sauro 10 Rapid Equilibrium Approximation The rate of reaction is then: Copyright © 2008: Sauro 11 Fractional Saturation Rearrange the equation: Substitute Kd Copyright © 2008: Sauro 12 Fractional Saturation Yields: This shows that the rate is proportional to the fraction of total enzyme that is bound to substrate. This expression gives us the fractional saturation. Copyright © 2008: Sauro 13 Brigg-Haldane Approach Steady State Assumption Simulation Copyright © 2008: Sauro 14 Brigg-Haldane Approach Steady State Assumption Simulation Copyright © 2008: Sauro 15 Steady State Assumption It is possible to relax the constraints that ES should be in equilibrium with E and S by assuming that ES has a relatively steady value over a wide range of substrate concentrations. Copyright © 2008: Sauro 16 Steady State Assumption Vmax Km Copyright © 2008: Sauro 17 Enzyme Catalysis Copyright © 2008: Sauro 18 Reversible Enzyme Catalysis Copyright © 2008: Sauro 19 Haldane Relationships Copyright © 2008: Sauro 20 Haldane Relationships The Haldane relationship puts constraints on the values of the kinetic constants (cf. Principles of Detailed Balance Slide). The relationship can be used to substitute one of the kinetic parameters, eg the reverse Vmax and replace it with the more easily determined equilibrium constant. Thermodynamic Term Saturation Term Copyright © 2008: Sauro 21 Parts of a Rate Law Sometime people will also emphasize the separation of the rate equation in to two parts, a thermodynamic and a saturation part. Thermodynamic Term Saturation Term Copyright © 2008: Sauro 22 Product Inhibition without Reversibility Removes a further parameter from the equation Copyright © 2008: Sauro 23 Multisubstrate Kinetics A B P Q Ordered Reaction A A B P P B Q Q Ping-pong Reaction B A Q P Random Order Reaction Copyright © 2008: Sauro 24 Multisubstrate Kinetics Generalized Rate Laws Irreversible: Reversible: Liebermeister W. and Klipp E. (2006), Bringing metabolic networks to life: convenience rate law and thermodynamic constraints, Theoretical Biology and Medical Modeling 3:41. Copyright © 2008: Sauro 25 Problems with Steady State Derivations Although deriving rate laws using the steady state assumption is more reasonable compared to the rapid equilibrium approach, the algebra involved in deriving the steady state equations can rapidly become wieldy. Graphical methods such as the King and Altman method have been devised to assist is the derivation but the general approach does not scale very well. For many systems, the rapid equilibrium method is the preferred method for deriving kinetic rate laws. Copyright © 2008: Sauro 26 Sigmoidal Responses Copyright © 2008: Sauro 27 Sigmoid responses are generally seen in multimeric systems. Phosphofructokinase Tetramer of identical subunits Copyright © 2008: Sauro 28 Sigmoid responses arise from cooperative interactions Binding at one site results in changes in the binding affinities at the remaining sites. Copyright © 2008: Sauro 29 Many proteins are multimeric The Ecocyc database reports 774 multimeric protein complexes out of 4316 proteins. Copyright © 2008: Sauro 30 Many Proteins are Multimeric The Ecocyc database reports 774 multimeric protein complexes out of 4316 proteins. Phosphoglucose Isomerase Hexokinase Dimer Dimer Fructose 1,6-bisphosphate Aldolase Phosphofructokinase Tetramer Tetramer http://www.rcsb.org/pdb/static.do?p=education_discussion/molecule_of_the_month/pdb50_1.html Copyright © 2008: Sauro 31 Hill Equation – Simplest Model We assume that the ligands bind simultaneously (unrealistic!): Assuming Rapid Equilibrium Copyright © 2008: Sauro 32 Hill Equation Some researchers feel that the underlying model is so unrealistic that the Hill equation should be considered an empirical result. Hill Coefficient Copyright © 2008: Sauro 33 Hill Coefficient The Hill Coefficient, n, describes the degree of cooperativity. If n = 1, the equation reverts to a simple hyperbolic response. n > 1 : Positive Cooperativity n = 1 : No Cooperativity n < 1 : Negative Cooperativity Hill Coefficient Copyright © 2008: Sauro 34 Hill Equation What is wrong with the Hill equation? 1. The underlying model is unrealistic (assuming this is important) 2. It’s a dead-end, no flexibility, one can’t add additional effectors such as inhibitors or activators. Copyright © 2008: Sauro 35 Alternative Models: Sequential Binding S S S S S S S Copyright © 2008: Sauro S S 36 Alternative Models: Sequential Binding S Copyright © 2008: Sauro S S 37 Alternative Models: Sequential Binding S S S Association Constants: Copyright © 2008: Sauro 38 Alternative Models: Sequential Binding S S S Copyright © 2008: Sauro 39 Alternative Models Sequential Binding S S S Copyright © 2008: Sauro 40 Alternative Models Sequential Binding S S S Adair Model Copyright © 2008: Sauro 41 Alternative Models Sequential Binding S S S K1 = 0.2; K2 = 10 f Copyright © 2008: Sauro S 42 Other Models – MWC Model MWC Model or concerted model (Monod, Wyman, Changeux) 1. Subunits exist in two conformations, relaxed (R) and taut (T) S S 2. S S S S Is disallowed One conformation has a higher binding affinity than the other (R) 3. Conformations within a multimer are the same 4. Conformations are shifted by binding of ligand Taut (T) – less active Relaxed (R) – more active Copyright © 2008: Sauro 43 Other Models – MWC Model MWC Model or concerted model (Monod, Wyman, Changeux) S S S Where L = Copyright © 2008: Sauro 44 Other Models – MWC Model MWC Model or concerted model (Monod, Wyman, Changeux) S Copyright © 2008: Sauro S S 45 Modifiers in Sigmoid Kinetics Modifiers can be incorporated into the models by assuming that the modifier molecule can bind either exclusively to the relaxed or taut forms. Thus inhibitors will bind to the taut form while activators can bind to the relaxed form. They effectively change the L constant. A I S S S Copyright © 2008: Sauro 46 Modifiers in Sigmoid Kinetics A I f Activators S Inhibitors S S S Copyright © 2008: Sauro 47 Gene Expression TF = Transcription Factor Copyright © 2008: Sauro 48 Molecular Details - Activation Weak Promoter RNA Poly Gene Binding of a TF can increase the apparent strength of the Promoter TF RNA Poly Gene Copyright © 2008: Sauro 49 Strong Promoter RNA Poly Molecular Details - Inhibition TF TF binding overlaps RNA polymerase binding site. Prevents RNA polymerase from binding. RNA Poly RNA Poly TF TF binding downstream of RNA polymerase binding site. Prevents RNA polymerase from moving down DNA strand. RNA Poly TF TF binding causes looping of the DNA, preventing RNA polymerase from moving down DNA strand. Copyright © 2008: Sauro 50 The Central Equation – Fractional Saturation A state refers to the state of the operator site, eg is it free or bound to a TF. G Gene G G A Gene GA G = Operator Site Copyright © 2008: Sauro 51 Single TF Binds and Activates Expression G A A Equilibrium Condition Copyright © 2008: Sauro 52 Single TF Binds and Activates Expression G A A Fractional Saturation Copyright © 2008: Sauro 53 Single TF Binds and Activates Expression G A A Copyright © 2008: Sauro 54 Single TF Binds and Activates Expression G A A Copyright © 2008: Sauro 55 Probability Interpretation Inside a cell there are of course only a few operator binding sites. Therefore we should strictly interpret the fractional saturation as a probability that a TF will be bound to the operator site. The rate of gene expression is then proportional to the probability of the TF being bound. G A A Copyright © 2008: Sauro 56 Single TF Binds and Inhibits Expression G A A The active state is when the TF is not bound. Copyright © 2008: Sauro 57 Single TF Binds and Inhibits Expression G A A The active state is when the TF is not bound. Copyright © 2008: Sauro 58 Single TF Binds and Inhibits Expression G A A Copyright © 2008: Sauro 59 Summary Activation Repression Copyright © 2008: Sauro 60 Single TF Binds, Activates with Cooperativity 1) G G 2) G TG 3) G TG2 Copyright © 2008: Sauro 61 Single TF Binds, Activates with Cooperativity G TG TG2 Copyright © 2008: Sauro 62 Single TF Binds, Activates with Cooperativity G TG TG2 Copyright © 2008: Sauro 63 Single TF Binds, Inhibits with Cooperativity v/Vmax T Copyright © 2008: Sauro 64 Repression with n binding sites: f n=4 P NOT Gate T Copyright © 2008: Sauro 65 In the literature you’ll often find then following variants: Activation Repression Copyright © 2008: Sauro 66 Two Activating TFs Compete for the Same Site G A A G B B Copyright © 2008: Sauro 67 Two TFs Compete for the Same Site Copyright © 2008: Sauro 68 Two Activating TFs Compete for the Same Site OR Gate Copyright © 2008: Sauro 69 Two Activating TFs Bind to two different sites B B G A A Copyright © 2008: Sauro 70 Two Activating TFs Bind to two different sites ..…but there is a slight complication Two different ways to make GAB GA G GAB GB Copyright © 2008: Sauro 71 Two Activating TFs Bind to two different sites You only need to use one of These relations. But which one? Or does it matter? Copyright © 2008: Sauro 72 Two Activating TFs Bind to two different sites GA G GAB GB The principle of detailed balance means that the energy change along each path must be the same since the end points (G and GAB) are the same. The overall equilibrium constants for the upper and lower routes must therefore be equal. Copyright © 2008: Sauro 73 Two Activating TFs Bind to two different sites GA G GAB GB Using: Using: This is: the equations are identical Copyright © 2008: Sauro 74 Comparing the two: OR Gates Copyright © 2008: Sauro 75 AND Gates: Active only when both are bound Copyright © 2008: Sauro 76 NOR Gates: Active when neither are bound G G A A G B B G B B A A Copyright © 2008: Sauro 77 XOR Gate G G A A Input A Input B Output 1 1 0 1 0 1 0 1 1 0 0 0 G B B G B B A A Copyright © 2008: Sauro 78 Other Configurations When A binds it activates. If B is bound, then A is unable to bind. B therefore acts as an inhibitor of A. G A G B A B Copyright © 2008: Sauro P 79