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Biophys J, February 2002, p. 591-604, Vol. 82, No. 2

A Unified Model for Signal Transduction Reactions in Cellular Membranes

Jason M. Haugh

Department of Chemical Engineering, North Carolina State University, Raleigh, North Carolina 27695-7905 USA


    ABSTRACT
TOP
ABSTRACT
INTRODUCTION
MATHEMATICAL MODEL FORMULATION
RESULTS AND DISCUSSION
APPENDIX
REFERENCES

An analytical solution is obtained for the steady-state reaction rate of an intracellular enzyme, recruited to the plasma membrane by active receptors, acting upon a membrane-associated substrate. Influenced by physical and chemical effects, such interactions are encountered in numerous signal-transduction pathways. The generalized modeling framework is the first to combine reaction and diffusion limitations in enzyme action, the finite mean lifetime of receptor-enzyme complexes, reactions in the bulk membrane, and constitutive and receptor-mediated substrate insertion. The theory is compared with other analytical and numerical approaches, and it is used to model two different signaling pathway types. For two-state mechanisms, such as activation of the Ras GTPase, the diffusion-limited activation rate constant increases with enhanced substrate inactivation, dissociation of receptor-enzyme complexes, or crowding of neighboring complexes. The latter effect is only significant when nearly all of the substrate is in the activated state. For regulated supply and turnover pathways, such as phospholipase C-mediated lipid hydrolysis, an additional influence is receptor-mediated substrate delivery. When substrate consumption is rapid, this process significantly enhances the effective enzymatic rate constant, regardless of whether enzyme action is diffusion limited. Under these conditions, however, enhanced substrate delivery can result in a decrease in the average substrate concentration.


    INTRODUCTION
TOP
ABSTRACT
INTRODUCTION
MATHEMATICAL MODEL FORMULATION
RESULTS AND DISCUSSION
APPENDIX
REFERENCES

The behavior of a living cell is dictated by its ability to integrate information about its changing environment, a complex biochemical process known as signal transduction. In animal cells, the plasma membrane plays a central role in organizing early signaling events, because it is accessible to intracellular and extracellular molecules. Indeed, signaling pathways are most often initiated by transmembrane receptors, which typically possess separate domains for engaging extracellular ligands and intracellular proteins. A well-characterized example is the class of receptor tyrosine kinases, which includes all growth factor receptors. Upon ligand binding and activation of their intrinsic tyrosine kinase domains, these receptors are autophosphorylated on multiple residues, which then participate in specific binding interactions with cytosolic enzymes (van der Geer et al., 1994; Pawson, 1995). The formation of such receptor-enzyme complexes is the first step in the activation of specific signaling pathways by receptor tyrosine kinases and many other signaling receptors.

When recruited by an activated receptor, a cytosolic protein is transiently confined within a thin layer adjacent to the plasma membrane. This leads to an interesting physical situation, because receptor-bound signaling enzymes often act upon specific lipid or lipid-anchored protein substrates that diffuse laterally in the membrane. For example, this is true of the three signaling cascades that have received the most attention over the past decade, the Ras, phospholipase C (PLC), and phosphoinositide (PI) 3-kinase pathways. Ras is a small GTPase most noted for its role in cell proliferation, which is inactive for signaling when bound to GDP and active when bound to GTP. It is anchored in the membrane by lipid modifications, and its nucleotide-binding state is regulated by cytosolic enzymes (Wittinghofer, 1998). PLC isoforms and type I PI 3-kinases are enzymes that modify a common lipid substrate, PI(4,5)P2. PLC-mediated hydrolysis of PI(4,5)P2 has varying functions in different cell types, including cell migration and gene expression, whereas phosphorylation of the lipid by PI 3-kinases has been implicated in chemotaxis and cell survival (Rhee and Bae, 1997; Rameh and Cantley, 1999). In each of these three major signaling pathways, recruitment of the relevant enzyme to the membrane is expected to have a significant impact on its observed activity. Indeed, enzymes isolated from lysates of stimulated cells often show little or no change in activity, whereas modifying these enzymes for stable membrane insertion is generally sufficient for activating downstream signaling in cells (Buday and Downward, 1993; Aronheim et al., 1994; Quilliam et al., 1994; Klippel et al., 1996).

The importance of enzyme localization in intracellular signaling suggests that significant insights could be gained through a combined biochemical and biophysical approach, whereby concentrations of membrane components, reaction-rate constants, and diffusion coefficients are quantitatively determined. The ability to accurately predict measured signaling pathway fluxes in cells would validate such an approach, but this would require an appropriate theoretical framework. In this paper, a generalized continuum model is formulated to describe various signaling pathways in which receptor-enzyme complexes modify laterally diffusing membrane substrates, with the primary goal of relating steady-state reaction rates to physical and kinetic constants.

The influence of translational diffusion on molecular interactions in two-dimensional (2D) domains has been the subject of numerous theoretical studies. With the mean capture time (MCT) approach, individual absorbers are placed at the centers of independent, circular domains, and molecules are reflected at the boundary to balance diffusion into and out of the domain (Adam and Delbrück, 1968; Berg and Purcell, 1977). Thus, the MCT approach introduces an ad hoc boundary condition and imposes that absorbers are evenly spaced, a nonrandom distribution. In contrast, the mean field (or effective medium) approximation smears absorbers throughout the domain, accounting for the depletion of molecules available to one absorber by each of the others (Wiegel and DeLisi, 1982; Goldstein et al., 1988; Khakhar and Agarwal, 1993). The problem of 2D diffusion in a random array of absorbers is mathematically analogous to the Brinkman equation describing fluid flow past an array of disks; for this system, it was found that the effective medium approximation is accurate for disk area fractions less than 0.3 (Howells, 1974; Dodd et al., 1995). Finally, an analysis of linearized statistical fluctuations about the average concentration has also been used to calculate diffusion-limited reaction rates (Keizer et al., 1985). Like the mean field approach, this theory allows the average concentration to be reached at infinite separation from an absorber.

Considering intracellular signaling interactions in particular, the effect of membrane localization on enzyme action has been estimated previously. Diffusion and reaction rate limitations have been considered simultaneously for both cytosolic and receptor-bound enzyme pools, using the MCT equation for the diffusion-limited contribution in the membrane (Haugh and Lauffenburger, 1997). A similar analysis considered that both pools experience either diffusion- or reaction-limited behavior, and the time-dependent diffusive flux to a single absorber in a semi-infinite membrane was used (Kholodenko et al., 2000). A different signaling mechanism, activation of heterotrimeric G proteins by direct interaction with ligated receptors, has been analyzed using Monte Carlo simulations on a 2D lattice (Mahama and Linderman, 1994). These simulations described, for the first time, how the average lifetime of receptor-ligand complexes can significantly affect steady-state G-protein activation rates in the diffusion limit. Indeed, Shea et al. (1997) used similar simulations to show that major discrepancies exist between effective rate constants obtained using Monte Carlo techniques and the various analytical approaches described above. However, the extent to which fundamental differences between lattice and continuum models affect the values of computed rate constants is unclear.

The results of the simulations performed by Linderman and colleagues reinforce the fact that the effective rate constant for a membrane reaction depends on all parameters that influence the substrate concentration profile in the membrane. The model presented here is therefore designed to be sufficiently general, including reactions that compete with, reverse the action of, or supply substrate to a receptor-recruited enzyme. Limitations imposed by diffusion and reaction on the action of this enzyme are considered simultaneously. Perhaps most importantly, it is demonstrated for the first time that a continuum approach can be used to describe receptor-enzyme complexes of finite average lifetime. Following the formulation of the general model, the implications of these various effects on the substrate concentration profile will be examined, with an emphasis on the Ras and PLC signaling pathways.


    MATHEMATICAL MODEL FORMULATION
TOP
ABSTRACT
INTRODUCTION
MATHEMATICAL MODEL FORMULATION
RESULTS AND DISCUSSION
APPENDIX
REFERENCES

Model considerations

To construct a realistic model with as few adjustable parameters as possible, three major assumptions are invoked:
1.   There is a random distribution of cell surface receptors active for signaling within the membrane domain of interest. Although certainly reasonable as a default assumption, the theory may not be accurate in certain regions of the membrane, such as near clathrin-coated pits when internalization of receptors is diffusion-limited (Goldstein et al., 1988).
2.   The enzymatic reaction in the membrane follows a second-order rate law, with a rate proportional to the concentrations of substrate and receptor-enzyme complexes in the membrane. Thus, in terms of Michaelis-Menten kinetics, the Michaelis constant KM is significantly greater than the membrane concentrations of either species. The resulting second-order rate constant is given by the kcat/KM ratio of the enzyme at the membrane, where kcat is the first-order catalytic rate constant.
3.   The mobility of substrate molecules relative to receptor-enzyme complexes is described by 2D Fickian diffusion in a semi-infinite domain, with a constant diffusion coefficient. In making this assumption, nonidealities associated with diffusion in cellular membranes, and complex media in general, must be acknowledged (Sheetz, 1993; Feder et al., 1996; Pralle et al., 2000). However, the motion of the lipid or lipid-anchored substrate is expected to dominate the diffusion coefficient in this case. Unlike many transmembrane receptors, such molecules exhibit diffusion coefficients close to theoretical values and essentially complete fluorescence recovery after photobleaching (Schlessinger et al., 1977; Niv et al., 1999).

In the sections that follow, models describing two distinct signaling-pathway types will be presented (Fig. 1). Major signaling pathways adequately simulated by each model are discussed, and the appropriate equations are formulated. It is then shown that a generalized model encompasses both pathway types, and analytical solutions are derived for the effective enzymatic rate constant at steady state. Finally, the theory is extended to account for the finite mean lifetime of receptor-enzyme complexes.



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FIGURE 1   Pathway types described by the general model. (a) Two-state mechanism. A membrane-anchored substrate is converted back and forth between inactive and activated states. Activation and inactivation occur in the bulk membrane with observed first-order rate constants ka and ki, respectively. Substrate activation is enhanced by receptor-enzyme complexes, which act upon inactive substrate with second-order rate constant kRE. (b) Regulated supply and turnover. The concentration of a membrane-anchored substrate is determined by the relative rates of consumption and transfer to the membrane. The first-order rate constant describing basal consumption is kc, and RT,0 is the basal rate of substrate transfer. Both the turnover and supply of the substrate are modulated by activated receptors. Receptor-enzyme complexes consume substrate with second-order rate constant kRE, whereas receptor-transfer protein complexes deliver substrate with first-order rate constant kRT.

Pathway type 1: reversible, two-state mechanism

In signaling pathways of this type (Fig. 1 a), a membrane-associated substrate is converted to an activated state by a receptor-recruited enzyme. The inactive substrate is later recovered by a first-order reaction, such that the total number of molecules in the active and inactive states is conserved on the time scale of interest. Regulation of the membrane-anchored GTPase Ras, which is inactive in the GDP-bound state and active in the GTP-bound state, is well described by this two-state model. In numerous cell types, an increase in Ras-GTP is mediated by the recruitment of guanine nucleotide exchange factors (GEFs) from the cytosol to the plasma membrane, in complex with adaptor proteins that link them to signaling receptors (Medema et al., 1993; Buday and Downward, 1993). GEFs catalyze the dissociation of bound nucleotides from Ras in cells; the subsequent rebinding of nucleotides is extremely rapid, favoring uptake of the more abundant GTP (Lenzen et al., 1998). To recover Ras-GDP, the GTPase activity of Ras hydrolyzes bound GTP, a reaction that is significantly accelerated by GTPase-activating proteins (GAPs). These GAP activities help maintain the majority of Ras in the GDP-bound state prior to cell stimulation (Wittinghofer et al., 1997). The two-state mechanism also serves as an idealized model of G-protein activation. Ligand-bound G protein-coupled receptors interact directly with heterotrimeric G proteins, which are composed of alpha , beta , and gamma  subunits (Hamm and Gilchrist, 1996). The GDP-bound alpha  subunit is thereby converted to the active GTP-bound state and liberated from the beta gamma subunits; following the GTPase reaction and recovery of the GDP-bound state, the alpha  and beta gamma subunits rapidly reassociate.

In this model pathway, substrate in the inactive state is conserved by
<FR><NU>∂n<SUB><UP>S</UP></SUB></NU><DE>∂t</DE></FR>=<UP>D</UP>∇<SUP><UP>2</UP></SUP><SUB><UP>r</UP></SUB>n<SUB><UP>S</UP></SUB>−(k<SUB><UP>a</UP></SUB>+k<SUP><UP>eff</UP></SUP><SUB><UP>RE</UP></SUB>n<SUB><UP>RE</UP></SUB>)n<SUB><UP>S</UP></SUB>+k<SUB><UP>i</UP></SUB>n<SUB><UP>S*</UP></SUB>, (1)
where nS is the 2D concentration of the inactive substrate as a function of radial distance r from a receptor-enzyme complex and time t. The lateral diffusion coefficient of the substrate relative to receptor-enzyme complexes, D, is assumed to have the same value for the inactive and active states. The first-order rate constants ka and ki characterize constitutive activation and inactivation steps, respectively; the latter acts upon the active form of the substrate, which has a 2D concentration nS*. The mean field approximation is introduced through the inclusion of a rate term that accounts for consumption of substrate by each of the neighboring receptor-enzyme complexes (2D concentration nRE), with effective second-order rate constant k<UP><SUB>RE</SUB><SUP>eff</SUP></UP>. Substituting the relation nS + nS* = nS,tot = constant, one finds that
<FR><NU>∂n<SUB><UP>S</UP></SUB></NU><DE>∂t</DE></FR>=<UP>D</UP>∇<SUP><UP>2</UP></SUP><SUB><UP>r</UP></SUB>n<SUB><UP>S</UP></SUB>−(k<SUB><UP>a</UP></SUB>+k<SUB><UP>i</UP></SUB>+k<SUP><UP>eff</UP></SUP><SUB><UP>RE</UP></SUB>n<SUB><UP>RE</UP></SUB>)n<SUB><UP>S</UP></SUB>+k<SUB><UP>i</UP></SUB>n<SUB><UP>S,tot</UP></SUB>. (2)
Eq. 2 is subject to two boundary conditions. At the enzyme-substrate encounter distance (r = s, interpreted as the sum of the associating molecules' radii), the flux of inactive substrate to each receptor-enzyme complex is balanced by the rate of the enzymatic reaction. The true second-order rate constant of the reaction is kRE. The second boundary condition maintains a finite value of nS at infinite separation from the receptor-enzyme complex; this value of nS is equivalent to its average in the membrane, defined as nS,
2&pgr;s<UP>D </UP><FENCE><FR><NU>∂n<SUB><UP>S</UP></SUB></NU><DE>∂r</DE></FR> </FENCE><SUB><UP>r=s</UP></SUB>=k<SUB><UP>RE</UP></SUB>n<SUB><UP>S</UP></SUB><UP>‖<SUB>r=s</SUB></UP>;  n<SUB><UP>S</UP></SUB><UP>‖<SUB>r=∞</SUB></UP>≡<A><AC>n</AC><AC>&cjs1171;</AC></A><SUB><UP>S</UP></SUB>. (3)
Finally, the enzymatic reaction rate, k<UP><SUB>RE</SUB><SUP>eff</SUP></UP>, and kRE are related by
<UP>rate</UP>=k<SUP><UP>eff</UP></SUP><SUB><UP>RE</UP></SUB>n<SUB><UP>RE</UP></SUB><A><AC>n</AC><AC>&cjs1171;</AC></A><SUB><UP>S</UP></SUB>=k<SUB><UP>RE</UP></SUB>n<SUB><UP>RE</UP></SUB>n<SUB><UP>S</UP></SUB>‖<SUB><UP>r=s</UP></SUB>. (4)
It follows that the effective rate constant k<UP><SUB>RE</SUB><SUP>eff</SUP></UP> deviates from kRE when the substrate is not homogeneously distributed, and so the magnitude of k<UP><SUB>RE</SUB><SUP>eff</SUP></UP> can be used to assess the influence of spatial effects on the reaction rate.

Pathway type 2: regulated substrate supply and turnover

In signaling pathways of this type (Fig. 1 b), a membrane-associated substrate is consumed by receptor-enzyme complexes, but here the action of the enzyme cannot be reversed by another reaction in the membrane. Rather, the substrate is delivered to the membrane continuously by a cytosolic transfer protein. Like the enzyme, a fraction of the transfer protein is engaged by activated receptors, and it is assumed that the enzyme and transfer protein bind to independent receptor sites. The formation of receptor-transfer protein complexes enhances substrate delivery, allowing higher reaction rates through the receptor-enzyme complexes, and the availability of substrate is determined by the relative extents to which its supply and consumption are modulated.

The action of receptor-recruited PLC, which hydrolyzes the membrane lipid PI(4,5)P2, is well described by this model. The products of PI(4,5)P2 hydrolysis are inositol (1,4,5)-trisphosphate, released into the cytosol, and (1,2)-diacylglycerol, which remains in the membrane. These products are metabolized and then recombined to form phosphatidylinositol in the endoplasmic reticulum, and this lipid precursor must be transferred to the plasma membrane for reconstitution of the substrate PI(4,5)P2 (Hsuan and Tan, 1997; Toker, 1998). To prevent depletion of PI(4,5)P2, its supply to the plasma membrane is also positively modulated by receptor stimulation (Batty et al., 1998; Willars et al., 1998). The PI(4,5)P2 delivery rate is probably influenced by direct interactions between receptors and proteins involved in phosphatidylinositol transfer and phosphorylation (Kauffmann-Zeh et al., 1994, 1995). The regulated supply and turnover model is also suitable for the PI 3-kinase pathway, in which PI(4,5)P2 is phosphorylated to form the lipid second messenger PI(3,4,5)P3 (Vanhaesebroeck and Waterfield, 1999). Though this reaction can be reversed in the membrane by different routes, the action of PI 3-kinase is expected to be influenced by the aforementioned regulation of the PI(4,5)P2 concentration.

The substrate conservation equation for the regulated supply and turnover model is
<FR><NU>∂n<SUB><UP>S</UP></SUB></NU><DE>∂t</DE></FR>=<UP>D</UP>∇<SUP><UP>2</UP></SUP><SUB><UP>r</UP></SUB>n<SUB><UP>S</UP></SUB>−(k<SUB><UP>c</UP></SUB>+k<SUP><UP>eff</UP></SUP><SUB><UP>RE</UP></SUB>n<SUB><UP>RE</UP></SUB>)n<SUB><UP>S</UP></SUB>+R<SUB><UP>T,0</UP></SUB>+k<SUB><UP>RT</UP></SUB>n<SUB><UP>RT</UP></SUB>. (5)
Again, nS(r, t) and D are the concentration and relative diffusion coefficient of the substrate, nRE is the concentration of receptor-enzyme complexes, and k<UP><SUB>RE</SUB><SUP>eff</SUP></UP> is the effective second-order rate constant for enzyme action at the membrane. The first-order rate constant kc describes basal substrate consumption, and RT,0 is the basal rate of substrate delivery to the membrane. Substrate delivery is accelerated by receptor-transfer protein complexes (2D concentration nRT), which insert substrate with first-order rate constant kRT. The boundary condition at the enzyme-substrate encounter distance (r = s) is given by
2&pgr;s<UP>D</UP> <FENCE><FR><NU>∂n<SUB><UP>S</UP></SUB></NU><DE>∂r</DE></FR></FENCE><SUB><UP>r=s</UP></SUB>=k<SUB><UP>RE</UP></SUB>n<SUB><UP>S</UP></SUB>‖<SUB><UP>r=s</UP></SUB>−<FENCE><FR><NU>n<SUB><UP>RT</UP></SUB></NU><DE>n<SUB><UP>R</UP></SUB></DE></FR></FENCE>k<SUB><UP>RT</UP></SUB>, (6)
where kRE is the second-order rate constant of the enzymatic reaction. The second term on the right-hand side of Eq. 6 accounts for the possibility that the receptor engaging the enzyme may be bound to a transfer protein as well, in which case substrate will be delivered at this location. This probability is given by nRT/nR, where nR is the total concentration of activated receptors in the membrane. The boundary condition at r = infinity and the relationship between k<UP><SUB>RE</SUB><SUP>eff</SUP></UP> and kRE are the same as in the two-state model.

General model and solution for stable receptor-enzyme complexes

A conservation equation and encounter-distance boundary condition that encompass both of the pathway models illustrated in Fig. 1 can be posed,
<FR><NU>∂n<SUB><UP>S</UP></SUB></NU><DE>∂t</DE></FR>=<UP>D</UP>∇<SUP><UP>2</UP></SUP><SUB><UP>r</UP></SUB>n<SUB><UP>S</UP></SUB>−(k<SUB>0</SUB>+k<SUP><UP>eff</UP></SUP><SUB><UP>RE</UP></SUB>n<SUB><UP>RE</UP></SUB>)n<SUB><UP>S</UP></SUB>+V<SUB>0</SUB>+k<SUB><UP>v</UP></SUB>n<SUB><UP>R</UP></SUB>,

2&pgr;s<UP>D</UP><FENCE><FR><NU>∂n<SUB><UP>S</UP></SUB></NU><DE>∂r</DE></FR></FENCE><SUB><UP>r=s</UP></SUB>=k<SUB><UP>RE</UP></SUB>n<SUB><UP>S</UP></SUB>‖<SUB><UP>r=s</UP></SUB>−k<SUB><UP>v</UP></SUB>. (7)
Here, the identities of the rate constants k0 and kv and the source term V0 will depend on the pathway type. In the two-state model, k0 triple-bond  ka + ki, V0 triple-bond  kinS,tot, and kv = 0; in the regulated supply and turnover model, k0 triple-bond  kc, V0 triple-bond  RT,0, and kv triple-bond  (nRT/nR)kRT. To reduce the number of constant parameters, Eq. 7 is nondimensionalized,
<FR><NU>∂&PSgr;</NU><DE>∂&tgr;</DE></FR>=∇<SUP>2</SUP><SUB>&rgr;</SUB>&PSgr;−(<UP>Da</UP>+&agr;&eegr;<SUB><UP>RE</UP></SUB>)&PSgr;+1+&bgr;&eegr;<SUB><UP>R</UP></SUB>;

2&pgr; <FENCE><FR><NU>∂&PSgr;</NU><DE>∂&rgr;</DE></FR></FENCE><SUB>&rgr;=1</SUB>=&kgr;&PSgr;‖<SUB>&rgr;=1</SUB>−&bgr;;

&PSgr;≡<FR><NU><UP>D</UP>n<SUB><UP>S</UP></SUB></NU><DE>s<SUP>2</SUP>V<SUB>0</SUB></DE></FR>; &tgr;≡<FR><NU><UP>D</UP>t</NU><DE>s<SUP>2</SUP></DE></FR>; &rgr;≡<FR><NU>r</NU><DE>s</DE></FR>;&eegr;<SUB><UP>R</UP></SUB>≡s<SUP>2</SUP>n<SUB><UP>R</UP></SUB>; &eegr;<SUB><UP>RE</UP></SUB>≡s<SUP>2</SUP>n<SUB><UP>RE</UP></SUB>;

<UP>Da</UP>≡<FR><NU>s<SUP>2</SUP>k<SUB>0</SUB></NU><DE><UP>D</UP></DE></FR>; &agr;≡<FR><NU>k<SUP><UP>eff</UP></SUP><SUB><UP>RE</UP></SUB></NU><DE><UP>D</UP></DE></FR>; &bgr;≡<FR><NU>k<SUB><UP>v</UP></SUB></NU><DE>s<SUP>2</SUP>V<SUB>0</SUB></DE></FR>; &kgr;≡<FR><NU>k<SUB><UP>RE</UP></SUB></NU><DE><UP>D</UP></DE></FR>. (8)
The dimensionless parameter Da is a Damköhler number comparing the rates of basal consumption and diffusion of the substrate. The effective and actual second-order enzymatic rate constants are scaled to the diffusion coefficient D to yield alpha  and kappa , respectively. The dimensionless density of activated receptors is given by eta R, and eta RE is the corresponding density of activated receptors bound to enzyme. The enhancement of the substrate delivery rate by activated receptors is characterized by beta . The identities of these dimensionless parameters and their estimated value ranges are summarized in Table 1.


                              
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TABLE 1   Dimensionless model parameters

When the lifetime of a receptor-enzyme complex is much longer than the time required for the substrate profile to evolve around it, the following steady state solution is obtained:
&PSgr;<SUB><UP>ss</UP></SUB>(&rgr;)=<A><AC>&PSgr;</AC><AC>&cjs1171;</AC></A><SUB><UP>ss</UP></SUB>−<FR><NU>(&kgr;<A><AC>&PSgr;</AC><AC>&cjs1171;</AC></A><SUB><UP>ss</UP></SUB>−&bgr;)<UP>K</UP><SUB>0</SUB>(<UP>Da</UP>*<SUP>1/2</SUP>&rgr;)</NU><DE>2&pgr;<UP>Da</UP>*<SUP>1/2</SUP><UP>K</UP><SUB>1</SUB>(<UP>Da</UP>*<SUP>1/2</SUP>)+&kgr;<UP>K</UP><SUB>0</SUB>(<UP>Da</UP>*<SUP>1/2</SUP>)</DE></FR>;

<A><AC>&PSgr;</AC><AC>&cjs1171;</AC></A><SUB><UP>ss</UP></SUB>=<FR><NU>1+&bgr;&eegr;<SUB><UP>R</UP></SUB></NU><DE><UP>Da*</UP></DE></FR>; <UP>Da*</UP>≡<UP>Da</UP>+&agr;&eegr;<SUB><UP>RE</UP></SUB>, (9)
where Ki are modified Bessel functions of order i, and Psi ss is the dimensionless analog of nS at steady state. Finally, an implicit solution relating the steady-state effective rate constant alpha  to the other parameters is found,
&agr;=&kgr; <FR><NU>&PSgr;<SUB><UP>ss</UP></SUB>(1)</NU><DE><A><AC>&PSgr;</AC><AC>&cjs1171;</AC></A><SUB><UP>ss</UP></SUB></DE></FR>=<FR><NU>&kgr;[2&pgr;f(<UP>Da</UP>*<SUP>1/2</SUP>)+&bgr;<UP>Da*</UP>/(1+&bgr;&eegr;<SUB><UP>R</UP></SUB>)]</NU><DE>&kgr;+2&pgr;f(<UP>Da</UP>*<SUP>1/2</SUP>)</DE></FR>;

f(x)≡x <FR><NU><UP>K<SUB>1</SUB></UP>(x)</NU><DE><UP>K<SUB>0</SUB></UP>(x)</DE></FR>. (10)
A possible modification of Eq. 8 is to distinguish receptor-enzyme complexes that are contributing to substrate delivery from those that are not with separate boundary conditions. It was confirmed that such an approach, with an overall alpha  computed as a weighted sum of the alpha  values for the two receptor pools, yields the same result as in Eq. 10 (not shown).

At this stage, it is instructive to review limiting cases of Eq. 10 and compare these with previous analytical theories. In the limit of low receptor-enzyme density, the term in Eq. 8 invoking the mean field approximation vanishes, and Eq. 10 becomes an explicit function of constant parameters (Da* = Da). For the case of beta  = 0, this low-density limit was derived previously to describe the Langmuir-Hinshelwood surface reaction mechanism with reactant absorption/desorption (Freeman and Doll, 1983). In the limit of very high receptor-enzyme density (Da* Da) and beta  = 0, the result of Wiegel and DeLisi (1982) describing binding of ligands to cell receptors through nonspecific membrane adsorption and diffusion is obtained. The effective rate constant at any receptor-enzyme density, again with beta  = 0, also agrees with results derived for other systems. Goldstein et al. (1988) described diffusion-limited capture of cell surface receptors by internalizing traps, and Khakhar and Agarwal (1993) extended the work of Freeman and Doll to describe the Langmuir-Hinshelwood mechanism for higher reactant densities.

General model solution for receptor-enzyme complexes with finite mean lifetime

In general, an individual enzyme-receptor complex may dissociate before the substrate concentration can achieve the profile predicted from Eq. 9, though a constant concentration of such complexes will be maintained, on average, at steady state. Hence, the mean field approach was used to calculate the impact of receptor-enzyme complex stability on the effective enzymatic rate constant. It should be noted that the receptor-dependent source term, characterized by beta , might involve a receptor-transfer protein complex; this interaction is assumed to be stable, because its lifetime is not considered here.

Eq. 8 is used to derive the evolution of the substrate concentration profile surrounding an individual enzyme-receptor complex during its lifetime (the "enzyme-on" phase), with the average density of receptor-enzyme complexes at steady state reflected in the effective rate term. The transient solution is given by
&PSgr;(&rgr;, &tgr;)=&PSgr;<SUB><UP>ss</UP></SUB>(&rgr;)+<LIM><OP>∫</OP><LL>0</LL><UL>∞</UL></LIM><FENCE>&THgr;(0)+<FR><NU>(&kgr;<A><AC>&PSgr;</AC><AC>&cjs1171;</AC></A><SUB><UP>ss</UP></SUB>−&bgr;)&PHgr;(1)</NU><DE>2&pgr;(&lgr;<SUP>2</SUP>+<UP>Da*</UP>)</DE></FR></FENCE>

×<FENCE><FR><NU>&PHgr;(&rgr;)<IT>e</IT><SUP><UP>−</UP>(<UP>&lgr;<SUP>2</SUP>+Da*</UP>)<UP>&tgr;</UP></SUP></NU><DE>1+g<SUP>2</SUP>(&lgr;)</DE></FR></FENCE>&lgr;<UP> d</UP>&lgr;;

&PHgr;(&rgr;)≡<UP>J<SUB>0</SUB></UP>(&lgr;&rgr;)−g(&lgr;)<UP>Y<SUB>0</SUB></UP>(&lgr;&rgr;);

g(&lgr;)≡<FR><NU>&kgr;<UP>J<SUB>0</SUB></UP>(&lgr;)+2&pgr;&lgr;<UP>J<SUB>1</SUB></UP>(&lgr;)</NU><DE>&kgr;<UP>Y<SUB>0</SUB></UP>(&lgr;)+2&pgr;&lgr;<UP>Y<SUB>1</SUB></UP>(&lgr;)</DE></FR>;

&THgr;(0)≡<LIM><OP>∫</OP><LL>1</LL><UL>∞</UL></LIM>[&PSgr;(&rgr;, 0)−<A><AC>&PSgr;</AC><AC>&cjs1171;</AC></A><SUB><UP>ss</UP></SUB>]&PHgr;(&rgr;)&rgr;<UP> d</UP>&rgr;, (11)
where Psi ss(rho ) is the steady-state substrate profile in the infinite lifetime limit (Eq. 9), Psi (rho , 0) is the initial substrate profile, and Ji and Yi are Bessel functions of order i. Eq. 11 is obtained using either Fourier-like integral transform or Laplace transform (Carslaw and Jaeger, 1940) solution methods. The dimensionless mean lifetime of the complex, inversely proportional to the dissociation rate constant of the receptor-enzyme interaction, is defined as tau RE. The effective enzymatic rate constant is then found using the implicit relation,
&agr;=&kgr;<FR><NU>∫<SUP>&tgr;<SUB><UP>RE</UP></SUB></SUP><SUB>0</SUB>&PSgr;(1, &tgr;)<UP>d</UP>&tgr;</NU><DE><A><AC>&PSgr;</AC><AC>&cjs1171;</AC></A><SUB><UP>ss</UP></SUB>&tgr;<SUB><UP>RE</UP></SUB></DE></FR>. (12)
After the complex dissociates, the substrate profile around the free activated receptor homogenizes. The transient for this "enzyme-off" phase is found by analogy to Eq. 11, with kappa  = 0. The initial condition is given by the substrate profile at the end of the enzyme-on phase, calculated from Eq. 11. The dimensionless average duration of the enzyme-off state is defined as tau R, and
&tgr;<SUB><UP>R</UP></SUB>=<FENCE><FR><NU>&eegr;<SUB><UP>R</UP></SUB></NU><DE>&eegr;<SUB><UP>RE</UP></SUB></DE></FR>−1</FENCE>&tgr;<SUB><UP>RE</UP></SUB>. (13)
This process is important because the substrate profile at the end of the enzyme-off phase is the initial condition for the next enzyme-on phase, and so on. This implicit condition is required to completely specify the problem, but the solution simplifies greatly for the interesting limiting cases. As tau R vanishes (eta RE/eta R approx  1), it is readily shown that Psi  = Psi ss; the finite complex lifetime does not matter, because the cytosolic concentration of the enzyme is high enough to saturate all activated receptors. As tau R becomes large (eta RE/eta R 1), it is apparent that Psi (rho , 0) = Psi ss at the beginning of each enzyme-on phase, and the implicit relation for the effective enzymatic rate constant becomes
&agr;=&kgr; <FR><NU>&PSgr;<SUB><UP>ss</UP></SUB>(1)</NU><DE><A><AC>&PSgr;</AC><AC>&cjs1171;</AC></A><SUB><UP>ss</UP></SUB></DE></FR>+<FR><NU>8</NU><DE>&pgr;&tgr;<SUB><UP>RE</UP></SUB></DE></FR> <FENCE>1−<FR><NU>&bgr;<UP>Da*</UP></NU><DE>&kgr;(1+&bgr;&eegr;<SUB><UP>R</UP></SUB>)</DE></FR></FENCE>

×<LIM><OP>∫</OP><LL>0</LL><UL>∞</UL></LIM><FR><NU>[1−e<SUP><UP>−</UP>(<UP>&lgr;<SUP>2</SUP>+Da*</UP>)<UP>&tgr;<SUB>RE</SUB></UP></SUP>](&lgr;<SUP>2</SUP>+<UP>Da*</UP>)<SUP>−2</SUP>&lgr;<UP> d</UP>&lgr;</NU><DE><FENCE><FR><NU><UP>J<SUB>0</SUB></UP>(&lgr;)+2&pgr;&lgr;<UP>J<SUB>1</SUB></UP>(&lgr;)</NU><DE>&kgr;</DE></FR></FENCE><SUP>2</SUP>+<FENCE><FR><NU><UP>Y<SUB>0</SUB></UP>(&lgr;)+2&pgr;&lgr;<UP>Y<SUB>1</SUB></UP>(&lgr;)</NU><DE>&kgr;</DE></FR></FENCE><SUP>2</SUP></DE></FR>. (14)
Eq. 14 was obtained from Eq. 12 by specifying the initial condition as the homogeneous Psi ss and evaluating Psi (1, tau ) from Eq. 11. The integral is evaluated numerically. In the purely diffusion-limited regime (kappa  right-arrow infinity ), Eq. 14 further simplifies to
&agr;=2&pgr;<UP>Da</UP>*<SUP>1/2</SUP><FR><NU><UP>K<SUB>1</SUB></UP>(<UP>Da</UP>*<SUP>1/2</SUP>)</NU><DE><UP>K<SUB>0</SUB></UP>(<UP>Da</UP>*<SUP>1/2</SUP>)</DE></FR>+<FR><NU>&bgr;<UP>Da*</UP></NU><DE>1+&bgr;&eegr;<SUB><UP>R</UP></SUB></DE></FR>+<FR><NU>8</NU><DE>&pgr;&tgr;<SUB><UP>RE</UP></SUB></DE></FR><LIM><OP>∫</OP><LL>0</LL><UL>∞</UL></LIM><FR><NU>[1−e<SUP><UP>−</UP>(<UP>&lgr;<SUP>2</SUP>+Da*</UP>)<UP>&tgr;<SUB>RE</SUB></UP></SUP>]&lgr;<UP> d</UP>&lgr;</NU><DE>(&lgr;<SUP>2</SUP>+<UP>Da*</UP>)<SUP>2</SUP>[<UP>J</UP><SUP><UP>2</UP></SUP><SUB><UP>0</UP></SUB>(&lgr;)+<UP>Y</UP><SUP><UP>2</UP></SUP><SUB><UP>0</UP></SUB>(&lgr;)]</DE></FR>. (15)
A satisfying result is the presence of three clearly separated contributions to the effective rate constant in this regime. The first term describes a receptor-enzyme complex of infinite lifetime, the second describes the contribution of receptor-mediated substrate delivery (nonzero beta ), and the third contains the influence of a finite lifetime tau RE.


    RESULTS AND DISCUSSION
TOP
ABSTRACT
INTRODUCTION
MATHEMATICAL MODEL FORMULATION
RESULTS AND DISCUSSION
APPENDIX
REFERENCES

Two-state mechanism

Influences of substrate inactivation and neighboring receptor-enzyme complexes on the effective enzymatic rate constant

The major difference between the two pathway types illustrated in Fig. 1 is the nature of the receptor-mediated substrate delivery term, characterized by the dimensionless parameter beta . In pathway type 1 (Fig. 1 a), a two-state mechanism appropriate for modeling activation of small GTPases such as Ras, beta  = 0. Another difference is the definition of the Damköhler number Da. In the two-state mechanism, Da reflects the sum of the basal activation and inactivation rate constants (ka and ki, respectively). Pathways of this type typically exhibit low levels of activation in the absence of receptor stimulation, and ki ka when this is the case. Indeed, with ka = 0 and diffusion-controlled enzyme action (kappa  right-arrow infinity ), pathway type 1 is indistinguishable from the collision coupling mechanism (Tolkovsky and Levitski, 1978). Thus, the value of Da generally describes how rapidly the activated substrate molecules are inactivated as they diffuse away from receptor-enzyme complexes.

The model formulation allows reaction and diffusion limitations in the action of receptor-enzyme complexes to be considered simultaneously. In Fig. 2 a, the effective enzymatic rate constant, alpha , is plotted versus the true reaction rate constant, kappa , for various values of Da; here, receptor-enzyme complexes are sparse but highly stable (eta RE right-arrow 0, tau RE right-arrow infinity ). With kappa   1, the action of the enzyme is expected to be reaction-limited, with minimal depletion of inactive substrate at the encounter distance r = s. As expected, alpha  approx  kappa  in this limit. With kappa   1, the action of the enzyme is limited by the translational diffusion of the substrate, at the same time that the enzyme depletes the majority of the inactivated substrate molecules in its vicinity. The value of alpha  is insensitive to kappa  and positively dependent on Da in this limit (Fig. 2 a). The gradient of inactivated substrate at the encounter distance gets larger as Da increases, because the inactivation process replenishes the substrate of the enzyme. The influence of the inactivation process on the diffusion-limited value of alpha  in the low-density, stable-complex limit has also been derived using a different approach (Molski, 2000). The diffusion-limited value of alpha  becomes sensitive to Da when the time scale of substrate inactivation is comparable to s2/D (Da ~ 1). For typical membrane substrates, s2/D < 1 ms, faster than most unsaturated enzymes can process substrate. Therefore, the diffusion-limited value of the effective activation-rate constant alpha  is expected to fall within a relatively narrow range of 0.7-2.5 for stable receptor-enzyme complexes at low density.



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FIGURE 2   Effective enzymatic rate constant, two-state mechanism: stable receptor-enzyme complexes. (a) The effective rate constant alpha  is computed as a function of the dimensionless rate constant kappa  = kRE/D, for the indicated values of Da = (ka + ki)s2/D and stable receptor-enzyme complexes at low density (eta RE right-arrow 0, tau RE right-arrow infinity ). (b) The effective rate constant alpha  is computed as a function of the dimensionless receptor-enzyme density eta RE = s2nRE for the indicated values of Da, diffusion-limited enzyme action, and stable receptor-enzyme complexes (kappa  right-arrow infinity , tau RE right-arrow infinity ). The dashed line is the prediction of the MCT approach (Eq. 16).

The theory can also predict the diffusion-limited enzymatic rate constant at relatively high densities of receptor-enzyme complexes, an effect incorporated using the mean field approach. This is illustrated in Fig. 2 b, in which the effective enzymatic rate constant alpha  is plotted versus the receptor-enzyme density eta RE for various Da in the diffusion-limited, stable-complex limit (kappa  right-arrow infinity , tau RE right-arrow infinity ). As values at the high end of the estimated eta RE range are approached, alpha  increases above the low density limit and becomes insensitive to the value of Da. In the high-density regime, neighboring receptor-enzyme complexes interfere with the substrate concentration profile surrounding each complex; substrate activation dominates over the inactivation process (alpha eta RE > Da), and the inactive substrate profile becomes more homogeneous. Hence, the diffusion-limited value of the effective rate constant alpha  increases. Also plotted in Fig. 2 b is the prediction of the MCT approach (Berg and Purcell, 1977),
&agr;<SUB><UP>MCT</UP></SUB>=2&pgr;<FENCE><UP>ln</UP><FENCE><FR><NU>1</NU><DE>(&pgr;&eegr;<SUB><UP>RE</UP></SUB>)<SUP>1/2</SUP></DE></FR></FENCE>−<FR><NU>(3−&pgr;&eegr;<SUB><UP>RE</UP></SUB>)(1−&pgr;&eegr;<SUB><UP>RE</UP></SUB>)</NU><DE>4</DE></FR></FENCE><SUP>−1</SUP>. (16)
In this form, the MCT equation accounts for diffusion between evenly spaced activating enzymes but does not include the inactivation process. However, even when Da = 0, Fig. 2 b shows that the organization of receptor-enzyme complexes in regularly spaced domains yields noticeable deviations from the mean field approach, which considers a random distribution of complexes.

Influence of receptor-enzyme complex lifetime on the enzymatic rate constant and comparison with Monte Carlo simulations

By solving for the transient substrate profile surrounding an average receptor-enzyme complex, the theory was extended to incorporate the kinetics of complex association and dissociation. Based on the results of Monte Carlo simulations, a short-lived receptor-enzyme pair is not expected to disturb the initially homogeneous substrate distribution as drastically as a stable complex would (Shea et al., 1997). This yields a sharper substrate gradient, averaged over the lifetime of the complex. Analytical theories, which heretofore have not accounted for these effects, therefore tend to underestimate the activation rate constant when the lifetime of the enzyme at the membrane is relatively short.

The influence of the dimensionless receptor-enzyme complex lifetime, tau RE, on the effective rate constant alpha  for the two-state mechanism is shown in Fig. 3. In Fig. 3 a, alpha  is plotted versus tau RE for various values of Da and a vanishing density of receptor-enzyme complexes in the diffusion limit (kappa  right-arrow infinity , eta RE right-arrow 0). In accord with the Monte Carlo study cited above, alpha  is a decreasing function of the receptor-enzyme-complex lifetime for very low values of tau RE, and this trend is independent of Da. However, as tau RE is increased above Da-1, alpha  approaches the stable-complex limit, which is solely dependent on the value of Da (Fig. 3 a). The latter effect was not described in the Monte Carlo simulation study, because the Da values used were less than 10-3 and never exceeded tau <UP><SUB>RE</SUB><SUP>−1</SUP></UP>. Hence, the conclusion that the effective rate constant scales with 4DtRE, the mean-squared displacement of substrate during the lifetime of the active complex (Shea et al., 1997), needs to be qualified. At low receptor-enzyme densities, the value of alpha  is determined by the fastest process that limits the spread of active substrate molecules in the membrane, either receptor-enzyme dissociation or substrate inactivation. A quantitative comparison of effective rate constant values obtained using the general model and Monte Carlo simulations is explored in the Appendix.



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FIGURE 3   Effective enzymatic rate constant, two-state mechanism: receptor-enzyme complexes with finite mean lifetime. (a) The effective rate constant alpha  is computed as a function of the dimensionless receptor-enzyme lifetime tau RE = DtRE/s2 for the indicated values of Da, diffusion-limited enzyme action, and receptor-enzyme complexes at low density (kappa  right-arrow infinity , eta RE right-arrow 0). (b) The effective rate constant alpha  is computed as a function of the dimensionless receptor-enzyme density eta RE for the indicated values of tau RE, Da = 10-3, eta RE/eta R 1, and diffusion-limited enzyme action (kappa  right-arrow infinity ).

Figure 3 b shows the effect of increasing the density of receptor-enzyme complexes, eta RE, on the diffusion-limited effective rate constant when the mean lifetime of these complexes is finite. For all values of eta RE, it is assumed that few activated receptors are in complex with enzyme molecules (eta RE eta R; Eq. 13), such that Eq. 15 can be used to compute alpha . The effective rate constant alpha  is shown to be a positive function of the receptor-enzyme density, and this trend becomes independent of the receptor-enzyme lifetime as eta RE increases (Fig. 3 b). Indeed, it is apparent that the effects of a finite lifetime, when tau <UP><SUB>RE</SUB><SUP>−1</SUP></UP> Da (Fig. 3 b), and the inactivation process, when Da tau <UP><SUB>RE</SUB><SUP>−1</SUP></UP> (Fig. 2 b), show similar behavior across the spectrum of receptor-enzyme density values. Taken together, the results shown in Figs. 2 and 3 demonstrate that any one of three processes can limit the spread of the inactivated substrate gradient surrounding each receptor-enzyme complex and set the value of the effective enzymatic rate constant. These include substrate inactivation, characterized by Da, receptor-enzyme complex dissociation, characterized by tau <UP><SUB>RE</SUB><SUP>−1</SUP></UP>, and the action of neighboring receptor-enzyme complexes, characterized by eta RE.

Predicting the fraction of substrate in the activated state

With steady or pseudo-steady state signaling through the two-state mechanism, the fraction of substrate in the activated state is given by
<FR><NU><A><AC>n</AC><AC>&cjs1171;</AC></A><SUB><UP>S*</UP></SUB></NU><DE>n<SUB><UP>S,tot</UP></SUB></DE></FR>=<FR><NU>k<SUB><UP>a</UP></SUB>+k<SUP><UP>eff</UP></SUP><SUB><UP>RE</UP></SUB>n<SUB><UP>RE</UP></SUB></NU><DE>k<SUB><UP>a</UP></SUB>+k<SUB><UP>i</UP></SUB>+k<SUP><UP>eff</UP></SUP><SUB><UP>RE</UP></SUB>n<SUB><UP>RE</UP></SUB></DE></FR> (17)

=<FR><NU><FR><NU>K<SUB>a</SUB>S<SUP>2</SUP></NU><DE>D</DE></FR>+&agr;&eegr;<SUB><UP>RE</UP></SUB></NU><DE><UP>Da</UP>+&agr;&eegr;<SUB><UP>RE</UP></SUB></DE></FR>.
One of the interesting features of the mean field model, as well as the MCT equation (Eq. 16), is that the effective rate constant alpha  is a function of the receptor-enzyme density eta RE in the diffusion limit (Figs. 2 b and 3 b). This offers the possibility that the activated substrate fraction, given by Eq. 17, is a complex function of eta RE. This possibility is explored in Fig. 4, in which the activated substrate fraction is plotted versus the receptor-enzyme density eta RE with ka = 0 and diffusion-limited enzyme action (equivalent to the collision coupling mechanism).



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FIGURE 4   Fraction of substrate in the activated state, two-state mechanism. The activated substrate fraction is computed as a function of the receptor-enzyme density eta RE and constant rate parameters from Eq. 17, with ka = 0 and diffusion-limited enzyme action (kappa  right-arrow infinity ). (a) Stable receptor-enzyme complexes (tau RE right-arrow infinity ). The value of alpha  in Eq. 17 was calculated using: solid lines, the full mean field theory; dotted lines, the low eta RE limit (alpha  constant); dashed lines, the MCT approach (Eq. 16). (b) Receptor-enzyme complexes with finite mean lifetimes. Plots are for eta RE eta R, Da = 10-3, and various tau RE values (infinity , 100, 10, and 1), with curves for lower tau RE shifted to the left.

In Fig. 4 a, complexes are long-lived (tau RE right-arrow infinity ), and substrate activation curves are plotted for various values of Da. Also shown in Fig. 4 a are the corresponding activation curves computed using the constant, low-density limit of alpha . For the values of Da shown, the constant alpha  curves underestimate the exact values when activated substrate fractions exceed 0.2, with a maximum deviation of 5-10% seen at activated substrate fractions of 0.8-0.9. Neglecting the action of neighboring receptor-enzyme complexes therefore introduces a minor but noticeable error. The error is mitigated by the fact that the strong dependence of alpha  on eta RE occurs in a regime of nearly complete substrate activation (alpha eta RE Da; see Eq. 17). Finally, activation curves using the MCT equation for alpha  (Eq. 16) are also plotted for comparison in Fig. 4 a. In this case, the deviations are significant, particularly at high Da values. Substrate activation is underpredicted at low eta RE and overpredicted at high eta RE.

The impact of decreasing the mean receptor-enzyme complex lifetime, tau RE, is shown in Fig. 4 b. Based on the analysis of Fig. 3, it was concluded that a reduction in tau RE has a similar effect on alpha  as an increase in Da, for the same value of eta RE. With respect to the level of activated substrate, however, a decrease in tau RE shifts the activation curve to the left (Fig. 4 b), in qualitative contrast with the effect of a Da increase. The value of eta RE that elicits half-maximal substrate activation is given by Da/alpha , and, unlike an increase in Da, a reduction in tau RE increases only the denominator in this ratio. In agreement with Monte Carlo results (Mahama and Linderman, 1994), neglecting receptor-enzyme dissociation can lead to a significant overestimate of the receptor-enzyme density required for half-maximal signaling.

Regulated supply and turnover

Receptor-mediated substrate delivery affects the enzymatic rate constant, even when enzyme action is reaction limited

The regulated supply and turnover mechanism (Fig. 1 b), like the two-state mechanism, involves a receptor-recruited enzyme that acts upon a membrane-associated substrate. However, the enzymatic reaction cannot be reversed in the membrane, and so the substrate must be supplied to the membrane if steady-state signaling is to be maintained. The dynamics of the membrane lipid PI(4,5)P2, involving the well-characterized PLC and PI 3-kinase pathways, are well described by this pathway type. In the unstimulated cell, the constitutive rate of delivery balances basal substrate consumption; in terms of the general model, the Damköhler number, Da, is the dimensionless rate constant characterizing basal substrate turnover. Upon stimulation, activated receptors have two roles: enzyme recruitment, which increases substrate turnover, and enhanced substrate delivery. The dimensionless parameter beta , absent from the two-state model, characterizes the enhancement of substrate delivery by activated receptors. To the extent that this activity affects the distribution of substrate in the membrane, it can impact the effective enzymatic rate constant.

Figure 5 shows the impact of a nonzero beta  value on the effective rate constant alpha . As in Fig. 2 a, alpha  is plotted as a function of the dimensionless reaction rate constant kappa  in Fig. 5 a, in the limit of stable receptor-enzyme complexes at low density (eta R, eta RE right-arrow 0, tau RE right-arrow infinity ). Curves are plotted for various basal turnover rates (Da = 10-4 - 0.1), with beta  = 0 or beta  = 500. Not surprisingly, supplying substrate in proximity to a receptor-recruited enzyme increases the effective enzymatic rate constant, an observation referred to hereafter as the beta  effect. At a low density of receptor-enzyme complexes, a requirement for a significant beta  effect is found to be beta Da 1 (Fig. 5 a). When Da = 10-4 and beta  = 500, alpha  is not significantly enhanced above values for beta  = 0, whereas for Da = 0.1 and beta  = 500, alpha  is enhanced by an order of magnitude. Thus, receptor-mediated substrate delivery spatially biases reactant consumption toward the action of receptor-enzyme complexes when the basal turnover rate is rapid. Further, Fig. 5 a demonstrates that this is true even in the reaction-limited regime (kappa  < 1), because the supply mechanism increases the substrate level near activated receptors (relative to the average concentration) under these conditions.



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FIGURE 5   Effective enzymatic rate constant, regulated supply and turnover. In this pathway type, the dimensionless rate constant Da = kcs2/D, and the parameter beta , describing receptor-mediated receptor transfer, comes into play. (a) The effective rate constant alpha  is computed as a function of kappa  for the indicated values of Da and stable receptor-enzyme complexes at low density (eta RE right-arrow 0, tau RE right-arrow infinity ). Solid lines and closed symbols, beta  = 0; dot-dashed lines and open symbols, beta  = 500. (b) The effective rate constant alpha  is computed as a function of the dimensionless receptor-enzyme density eta RE for the indicated values of Da and beta , diffusion-limited enzyme action, and stable receptor-enzyme complexes (kappa  right-arrow infinity , tau RE right-arrow infinity ). Closed symbols, beta  = 0; open symbols, beta  = 500. Solid lines, eta RE = eta R; dotted lines, eta RE = 0.1eta R.

The influence of the activated receptor density, eta R, on the diffusion-limited effective rate constant with nonzero beta  is shown in Fig. 5 b. Curves of alpha  versus eta R are plotted for Da values at the extremes of the range presented in Fig. 5 a (10-4 and 0.1), again with beta  = 0 or beta  = 500. Two values of eta RE/eta R are explored (1 and 0.1). An increase in eta R has two effects: enhancing recruitment of the enzyme, which tends to increase alpha  in the diffusion limit, and enhancing the average substrate concentration through receptor-mediated supply, which tends to decrease alpha  (Eq. 15). Comparing the beta  = 0 and beta  = 500 curves for Da = 10-4 and eta RE = eta R in Fig. 5 b, a strong beta  effect appears at high activated receptor densities. As eta R and eta RE vanish, the low Da value yields a negligible beta  effect, whereas, at high receptor densities, alpha  increases and tends to be independent of Da (Fig. 2 b), increasing the magnitude of the beta  effect. This synergy is strongly dependent on the value of eta RE/eta R; with Da = 10-4 and eta RE = 0.1eta R, the beta  effect is significantly reduced. When Da = 0.1, beta  = 500, and eta RE = eta R, the beta  effect is large at all densities, and so the increase in alpha  with increasing eta R is less dramatic. When eta RE = 0.1eta R, however, a different effect is observed: the effective rate constant decreases at high eta R. Under these conditions, the major effect of an increase in eta R is an enhancement of the average substrate concentration through receptor-mediated supply. This opposes the beta  effect seen at low receptor activation, resulting in a merging of the beta  = 500 and beta  = 0 curves.

Prediction of enzymatic reaction rates and comparison with PI(4,5)P2 hydrolysis data

To the extent that the regulated supply and turnover mechanism accurately depicts the action of PLC, the theory can be used to estimate the rate of PI(4,5)P2 hydrolysis. In terms of the general model, the enzymatic reaction rate at steady state is given by