Department of Chemical Engineering, North Carolina State
University, Raleigh, North Carolina 27695-7905 USA
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 |
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 |
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
,
, and
subunits (Hamm and Gilchrist, 1996
). The GDP-bound
subunit is
thereby converted to the active GTP-bound state and liberated from the

subunits; following the GTPase reaction and recovery of the
GDP-bound state, the
and 
subunits rapidly reassociate.
In this model pathway, substrate in the inactive state is conserved by
|
(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
. Substituting the
relation nS + nS* = nS,tot = constant, one finds that
|
(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
S,
|
(3)
|
Finally, the enzymatic reaction rate,
k
, and kRE are
related by
|
(4)
|
It follows that the effective rate constant
k
deviates from
kRE when the substrate is not homogeneously distributed, and so the magnitude of k
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
|
(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
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
|
(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 =
and the relationship between k
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,
|
(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
ka + ki,
V0
kinS,tot, and
kv = 0; in the regulated supply and
turnover model, k0
kc, V0
RT,0, and kv
(nRT/nR)kRT. To reduce the number of constant parameters, Eq. 7 is
nondimensionalized,
|
(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
and
, respectively. The dimensionless density of activated receptors is
given by
R, and
RE is the corresponding
density of activated receptors bound to enzyme. The enhancement of the
substrate delivery rate by activated receptors is characterized by
.
The identities of these dimensionless parameters and their estimated
value ranges are summarized in Table 1.
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:
|
(9)
|
where Ki are modified Bessel functions of order i,
and
ss is the dimensionless analog of
S at steady state. Finally, an implicit
solution relating the steady-state effective rate constant
to the
other parameters is found,
|
(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
computed as a
weighted sum of the
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
= 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
= 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
= 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
, 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
|
(11)
|
where
ss(
) is the steady-state substrate
profile in the infinite lifetime limit (Eq. 9),
(
, 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
RE. The
effective enzymatic rate constant is then found using the implicit
relation,
|
(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
= 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
R, and
|
(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
R vanishes
(
RE/
R
1), it is readily shown
that
=
ss; the finite complex lifetime does not
matter, because the cytosolic concentration of the enzyme is high
enough to saturate all activated receptors. As
R becomes large (
RE/
R
1), it is apparent that
(
, 0) =
ss at the beginning of each
enzyme-on phase, and the implicit relation for the effective enzymatic
rate constant becomes
|
(14)
|
Eq. 14 was obtained from Eq. 12 by specifying the initial
condition as the homogeneous
ss and evaluating
(1,
) from Eq. 11. The integral is evaluated numerically. In the
purely diffusion-limited regime (
), Eq. 14 further
simplifies to
|
(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
), and the third contains the influence of a
finite lifetime
RE.
 |
RESULTS AND DISCUSSION |
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
. In pathway type 1 (Fig. 1 a), a two-state mechanism appropriate for modeling
activation of small GTPases such as Ras,
= 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 (
), 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,
, is plotted versus the true reaction rate
constant,
, for various values of Da; here, receptor-enzyme
complexes are sparse but highly stable (
RE
0,
RE
). With
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,
in this limit. With
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
is insensitive to
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
in the low-density, stable-complex limit has also been derived
using a different approach (Molski, 2000
). The diffusion-limited value
of
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
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 is computed as a function of the dimensionless rate
constant = kRE/D, for the indicated
values of Da = (ka + ki)s2/D and stable
receptor-enzyme complexes at low density ( RE 0, RE ). (b) The effective rate constant
is computed as a function of the dimensionless receptor-enzyme
density RE = s2nRE
for the indicated values of Da, diffusion-limited enzyme action, and
stable receptor-enzyme complexes ( , RE ). 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
is plotted versus the receptor-enzyme density
RE
for various Da in the diffusion-limited, stable-complex limit (
,
RE
). As values at the high end of the
estimated
RE range are approached,
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
(
RE > Da), and the inactive substrate profile
becomes more homogeneous. Hence, the diffusion-limited value of the
effective rate constant
increases. Also plotted in Fig.
2 b is the prediction of the MCT approach (Berg and
Purcell, 1977
),
|
(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,
RE, on the effective rate constant
for the two-state mechanism is shown in Fig. 3. In Fig.
3 a,
is plotted versus
RE for various
values of Da and a vanishing density of receptor-enzyme complexes in
the diffusion limit (
,
RE
0). In accord
with the Monte Carlo study cited above,
is a decreasing function of
the receptor-enzyme-complex lifetime for very low values of
RE, and this trend is independent of Da. However, as
RE is increased above Da
1,
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 
. 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
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 is computed as a function of the
dimensionless receptor-enzyme lifetime RE = DtRE/s2 for the indicated
values of Da, diffusion-limited enzyme action, and receptor-enzyme
complexes at low density ( , RE 0).
(b) The effective rate constant is computed as a
function of the dimensionless receptor-enzyme density RE
for the indicated values of RE, Da = 10 3, RE/ R 1, and
diffusion-limited enzyme action ( ).
|
|
Figure 3 b shows the effect of increasing the density of
receptor-enzyme complexes,
RE, on the diffusion-limited
effective rate constant when the mean lifetime of these complexes is
finite. For all values of
RE, it is assumed that few
activated receptors are in complex with enzyme molecules
(
RE
R; Eq. 13), such that Eq. 15 can
be used to compute
. The effective rate constant
is shown to be
a positive function of the receptor-enzyme density, and this trend
becomes independent of the receptor-enzyme lifetime as
RE increases (Fig. 3 b). Indeed, it is
apparent that the effects of a finite lifetime, when

Da (Fig. 3 b), and the
inactivation process, when Da

(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

, and the action of neighboring
receptor-enzyme complexes, characterized by
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
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(17)
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One of the interesting features of the mean field model, as well
as the MCT equation (Eq. 16), is that the effective rate constant
is a function of the receptor-enzyme density
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
RE. This possibility is
explored in Fig. 4, in which the
activated substrate fraction is plotted versus the receptor-enzyme density
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 RE and constant rate
parameters from Eq. 17, with ka = 0 and
diffusion-limited enzyme action ( ). (a) Stable
receptor-enzyme complexes ( RE ). The value of
in Eq. 17 was calculated using: solid lines, the full
mean field theory; dotted lines, the low RE
limit ( constant); dashed lines, the MCT approach (Eq. 16). (b) Receptor-enzyme complexes with finite mean
lifetimes. Plots are for RE R,
Da = 10 3, and various RE values ( ,
100, 10, and 1), with curves for lower RE shifted to the
left.
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|
In Fig. 4 a, complexes are long-lived (
RE
), 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
. For the values of Da shown, the constant
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
on
RE occurs in a regime of nearly complete substrate
activation (
RE
Da; see Eq. 17). Finally,
activation curves using the MCT equation for
(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
RE and overpredicted
at high
RE.
The impact of decreasing the mean receptor-enzyme complex lifetime,
RE, is shown in Fig. 4 b. Based on the
analysis of Fig. 3, it was concluded that a reduction in
RE has a similar effect on
as an increase in Da, for
the same value of
RE. With respect to the level of
activated substrate, however, a decrease in
RE shifts
the activation curve to the left (Fig. 4 b), in qualitative contrast with the effect of a Da increase. The value of
RE that elicits half-maximal substrate activation is
given by Da/
, and, unlike an increase in Da, a reduction in
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
, 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
value on the effective rate constant
. As in Fig.
2 a,
is plotted as a function of the dimensionless
reaction rate constant
in Fig. 5 a, in the limit of
stable receptor-enzyme complexes at low density (
R,
RE
0,
RE
). Curves are plotted
for various basal turnover rates (Da = 10
4
0.1), with
= 0 or
= 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
effect. At a low density of receptor-enzyme complexes, a
requirement for a significant
effect is found to be
Da
1 (Fig. 5 a). When Da = 10
4 and
= 500,
is not significantly enhanced above values for
= 0, whereas for Da = 0.1 and
= 500,
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 (
< 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 , describing receptor-mediated receptor transfer, comes
into play. (a) The effective rate constant is computed
as a function of for the indicated values of Da and stable
receptor-enzyme complexes at low density ( RE 0, RE ). Solid lines and closed
symbols, = 0; dot-dashed lines and open
symbols, = 500. (b) The effective rate
constant is computed as a function of the dimensionless
receptor-enzyme density RE for the indicated values of
Da and , diffusion-limited enzyme action, and stable receptor-enzyme
complexes ( , RE ). Closed
symbols, = 0; open symbols, = 500. Solid lines, RE = R;
dotted lines, RE = 0.1 R.
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The influence of the activated receptor density,
R, on the diffusion-limited effective rate constant with
nonzero
is shown in Fig. 5 b. Curves of
versus
R are plotted for Da values at the extremes of the range
presented in Fig. 5 a (10
4 and 0.1), again
with
= 0 or
= 500. Two values of
RE/
R are explored (1 and 0.1). An
increase in
R has two effects: enhancing recruitment of
the enzyme, which tends to increase
in the diffusion limit, and
enhancing the average substrate concentration through receptor-mediated
supply, which tends to decrease
(Eq. 15). Comparing the
= 0 and
= 500 curves for Da = 10
4 and
RE =
R in Fig. 5 b, a
strong
effect appears at high activated receptor densities. As
R and
RE vanish, the low Da value yields a negligible
effect, whereas, at high receptor densities,
increases and tends to be independent of Da (Fig. 2 b),
increasing the magnitude of the
effect. This synergy is strongly
dependent on the value of
RE/
R; with
Da = 10
4 and
RE = 0.1
R, the
effect is significantly reduced. When Da = 0.1,
= 500, and
RE =
R, the
effect is large at all densities, and so the
increase in
with increasing
R is less dramatic. When
RE = 0.1
R, however, a different
effect is observed: the effective rate constant decreases at high
R. Under these conditions, the major effect of an
increase in
R is an enhancement of the average substrate
concentration through receptor-mediated supply. This opposes the
effect seen at low receptor activation, resulting in a merging of the
= 500 and
= 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