Computer Mathematical Simulation of the Dynamic
Interactions
Between
Synapsin I, Synaptic Vesicles, and the Cytoskeleton
Robin L. M.
Cheung
Student
#244679
61.498
Honours Thesis
For Dr. J
J. Cheetham
Monday,
April 12, 1999
Carleton University
Abstract
The regulation of neurotransmitter
release has long been an important area in neurochemistry, affecting such
facets of brain and nerve function as cognition, emotion, memory, and
metacognitive processing. To this end,
in vitro studies of indepdendent components of this system have been studied
and characterized. Kinetic constants
obtained through previous studies were used in this work to construct a novel
theoretical model for the pre_synaptic neurotransmitter release.
Synapsins constitute a group of three
types of phosphoproteins that interact with synaptic vesicles and are a vital
component in the regulation of neurotransmitter release. By acting as a cytoskeletal "tether,"
they are able to mediate the translocation of synaptic vesicles containing
neurotransmitter within a cell. Their
affinity for actin filaments and synaptic vesicles is modulated by their
phosphorylation thereby allowing the dynamic modelling of the interaction of
these components.
A computer mathematical model was
proposed to illustrate the interactions between Synapsin (phosphorylated and
dephosphorylated forms), actin filaments of the cytoskeleton, and synaptic
vesicles. Literature constants were
used to approximate the in vivo interactions between the four components. Attempts were made to formulate a related
system to integrate calcium/calmodulin_dependent Kinase (CaM Kinase II) and its
interactions with Synapsin Ia.
Introduction
Synapsins represent a family of abundant
synaptic vesicle-associated phosphoproteins which are involved in synaptic
vesicle dynamics in nerve terminals (Hosaka and Sudhof, 1998; Geppert et al.,
1994; Sudhof, 1995). They account for
approximately 9% of the membrane proteins associated with synaptic vesicles
(Esser et al., 1998). Synapsin
were originally discovered in 1977 by Ueda and Greengard and were originally
called “Protein 1.” Until recently, two
synapsin genes were known: Synapsin I and Synapsin II (Sudhof, 1995). The products of these two genes are
alternatively spliced to produce the four synapsin proteins: synapsins Ia, Ib,
IIa, and IIb (Sudhof, 1995). Hosaka and
Sudhof (1998) recently, however, proposed the existence of a novel
Synapsin–Synapsin III.
Thus far, synapsin interactions with
brain spectrin, actin filaments, neurofilaments, and microtubules have been
reported (Bennett et al., 1991).
Virtually all neurons, regardless of the neurotransmitter released,
contain synapsins (Greengard et al., 1994). In nerve terminals, Synapsin I is specifically located on the
cytoplasmic surface of small synaptic vesicles (Benfenati et al.,
1989). There is strong evidence that
synapsin I is a regulator of neurotransmitter release through the
immobilization of these small synaptic vesicles to the cyotoskeleton, thereby
allowing the accumulation of a releasable pool of neurotransmitter (Bahler et
al., 1989). The maintenance of this releasable pool of neurotransmitter
allows the rapid recovery and firing of neurons. Further, Bahler et al. (1989) proposed that this
regulation is strongly dependent upon the phosphorylation of the synapsin I
molecule itself.
In the rat, Synapsins Ia and Ib are 704-
and 668-amino acid proteins and Synapsins IIa and IIb are 586- and 479-amino
acid proteins, respectively (Greengard et al., 1994). Between rat, bovine, and human forms,
Synapsin maintains a high degree of identity (Esser et al., 1998). In each case, it comprises five domains: A,
B, C, D, and E/F. Each domain is
distinguished by its composition and conservation. Of these, Esser et al. (1998) point out that the C-domain
is the most highly conserved. It is 39%
hydrophobic and 27% charged, and is located in the amino terminal, globular
region of the protein.
Synapsin I has a collagenase-insensitive
head domain and a collagenase-sensitive tail region (Benfenati et alI.,
1989). It has three recognized
sites at which it may be phosphorylated by cAMP-dependent protein kinase or Ca2+/calmodulin-dependent
protein kinase (CaMKII). Benfenati et
al. (1989) discovered one serine
residue in the head domain (“Site 1"), which is phosphorylated by
cAMP-dependent protein kinase, and two serine residues in the tail domain,
phosphorylated by CaMKII. It has been shown that phosphorylation at these
residues influences the affinity of synapsin for synaptic vesicles (Benfenati et
al., 1989; Esser et al., 1998; Benfenati et al., 1989).
Neurotransmitters are stored in synaptic
vesicles and released by exocytosis.
The only known function of these small synaptic vesicles is the storage
and release of neurotransmitters. This
relative simplicity has led to the synaptic vesicle being one of the
best-studied organelles in biology. Although
synapsin I is a very well-characterized protein, and many equilibrium interactions
have been demonstrated, as yet there have been no attempts at simulating the
real-time interactions between synapsin I, synaptic vesicles, and the
cytoskeleton. The purpose of this
project is therefore to construct a real-time mathematical computer simulation
that reflects possible interactions between phosphorylated and dephosphorylated
synapsin I with synaptic vesicles and actin filaments using estimated kinetic
constants and computer simulation software.
There is a general consensus that
synapsins are necessary for regulation of synaptic vesicle exocytosis and
therefore neurotransmitter release. In
spite of this vital regulatory function, several experimenters have proven that
the lack of synapsins is not lethal.
Experiments on mice have led to more debate regarding the necessity of
synapsins to normal neurological function.
Certain experiments have revealed that mice lacking synapsins expressed
no gross anatomical abnormalities, yet experienced grand mal seizures
proportional to the number of mutant synapsin alleles (Rosahl et al.,
1995) and others revealed that mice lacking synapsin I exhibited no apparent
changes in well-being or gross nervous system function. This evidence suggests that synapsin I
normally functions to inhibit neurotransmitter release on a millisecond
timescale immediately following a calcium signal, generally thought to occur
through C-terminal phosphorylation of synapsin by CaM Kinase II (Sudhof, 1995).
Benfenati et al. (1989) used
hydrophobic photolabelling to study the interactions between synaptic vesicles
and synapsin I. The synapsin-synaptic
vesicle complexes were preserved by solubilizing and reconstituting in
phosphatidyl choline.
There is evidence that the head of the
protein is involved in the binding of the phospholipid bilayer while the tail
binds a separate vesicle protein, which is strongly modulated by
phosphorylation events and ionic strength (Benfenati et al., 1989;
HUttner et al., 1993). This
implies two types of interactions between synapsin and synaptic vesicles. One interaction, purely hydrophobic in
nature, does not seem to be influenced by phosphorylation state or ionic
strength. Another interaction, due to
protein-protein interactions in the tail region, allows regulation of interactions
by changes in phosphorylation state or ionic strength of the environment. The proposed computer simulation would
incorporate the phosphorylation state of the medium, but not ionic strength or
hydrophobic factors into the simulation.
The main focus of the synaptic vesicle
cycle is exocytosis by membrane fusion.
The study of the synaptic vesicle cycle is vitally important to the
study of neurotransmitter release and design of neural networks.
Although the synaptic environment imposes
special requirements on signalling, such as localized and rapid signals which
can be repeated at high frequencies, both up- and down-regulated, the process
of exocytosis employed by synaptic vesicles in man is identical to the process
used by yeasts. Sudhof (1995) described
four main methods to study the synaptic vesicle cycle:
|
Botulinum and Tetanus
toxin inhibition of neurotransmitter release |
Dreyer et al. (1983)
recorded presynaptic membrane currents at mouse motor endplates. Using potassium blockers, they observed
blockage of neuromuscular transmissions using botulinum and tetanus
toxins. The general theory behind
this practice is that botulinum and tetanus toxins enter nerve terminals and
irreversibly inhibit synaptic vesicle exocytosis by proteolytic cleavage of a
single target site, thereby preventing priming of synaptic vesicles for
exocytosis. This results in the
victim becoming incapacitated.
Facchiano et al. (1993) proposed that synapsin is a target of tetanus
toxin through experiments with transglutaminase and tetanus toxin. |
|
Invertebrate preparations with
disrupted synaptic vesicle traffic |
Llinas et al. (1985)
studied the effects of intraterminal injection of synapsin on
neurotransmitter release of squid giant synapses. This and other similar experiments have provided valuable
evidence that synapsin I is responsible for regulating the availability of
synaptic vesicles for release. |
|
Gene knock-outs in mice |
This method, employed by Rosahl
et ai. (1993 and 1995), was used to study the functions of synapsins in
morphology and neurology |
The
synaptic vesicle cycle takes approximately one minute to complete. Of this, the actual exocytosis event takes
approximately one third of a second. The
endocytotic event requires approximately 5 seconds. Sudhof (1995) describes nine distinct steps which comprise the
synaptic vesicle cycle:
Docking |
Docking occurs at the active
zone, opposite to the synaptic cleft.
This implies specific targetting of synaptic vesicles. |
|
Priming |
Most of the docked synaptic
vesicles cannot be triggered by calcium for fusion and exocytosis. This implicates an additional intervening
step where synaptic vesicles mature. The
existence of the priming step is further supported by evidence that after
extended periods of repetitive stimulation, vesicle exocytosis wanes before
the number of docked synaptic vesicles. |
|
Fusion and Exocytosis |
Primed synaptic vesicles are
stimulated for rapid fusion and exocytosis by a calcium spike during the
action potential of a neuron. This
step is one of the shortest parts of the synaptic vesicle cycle. It lasts approximately 0.3 ms. Only approximately one in three action
potentials leads to an actual exocytosis event. Calcium triggering is therefore quite inefficient. |
|
Receptor-Mediated Endocytosis |
The now-empty storage vesicles
are rapidly internalized via receptor-mediated endocytosis and subsequently
become clathrin-coated vesicles. |
|
Translocation |
The coated vesicles shed their
coats, acidify, and translocate to the interior |
|
Endosome Fusion |
The recycling synaptic vesicles
fuse with early endosomes. This is
evident by the presence of ran5, an endosomal marking protein |
|
Budding |
Synaptic vesicles are primarily
generated by budding from endosomes |
|
Neurotransmitter Uptake |
Neurotransmitter accumulates in
synaptic vesicles by active neurotransmitter uptake |
|
Translocation |
Synaptic vesicles filled with
neurotrasmitter translocate back to the active zone by diffusion or by active
cytoskeletal transport |
Proposed
Kinetic Simulation of Synapsin I Interactions
Synapsin I interactions with actin, ATP, and
synaptic vesicles are well documented (Sudhof, 1995; Hosaka and Sudhof, 1998;
Bennet et al., 1991; and Esser et al., 1998). To date, however, a mathematical simulation
of the kinetic interactions of all four players concurrently has not been
published. Using literature kinetic and
affinity constants for both phosphorylated and dephosphorylated Synapsin I
interactions with actin and synaptic vesicles, a pre-equilibrium computer-based
mathematical simulation of these interactions can be constructed. In order to do this, the kinetics between
each of the players is characterized independently, and integrated as the sum
of parallel processes using a computer-based solving engine.
Synapsin I
Interactions with Small Synaptic Vesicles
There are two main aspects to
interactions between Synapsin I and small synaptic vesicles (SV): hydrophobic
binding of the head region to the phospholipid membrane and binding of the tail
region to a non-lipid component of the membrane (Schiebler et al., 1986;
Benfenati et al., 1989). Studies
by Benfenati et al. (1989) and Schiebler et al. (1986) showed
that binding of the hydrophobic head group to the membrane is largely the same
whether interacting with native synaptic vesicles or mixed liposomes mimicking
synaptic vesicles.
As previously noted, tail binding to
synaptic vesicles is strongly affected both by phosphorylation of sites 2 and
3, and by ionic environment, implying a protein-protein interaction more
comlpex than the simple hydrophobic interaction of the head group. Benfenati et al. (1989) reported a
differential binding affinity for synaptic vesicles according to
phosphorylation of sites 1, 2, and 3 and ionic environment. Dephosphorylated synapsin-bound synaptic
vesicles with high affinity and saturability, exhibiting KD=10 mM at
40 mM NaCl and Bmax=800 fmol/:g of synaptic vesicles. This
affinity could be decreased substantially by phosphorylation of the tail domain
serine residues or by increasing the ionic strength of the mixture beyond 40
mM. Synapsin I phosphorylated at site I
did not show a high degree of difference to dephosphorylated synapsin in
experiments with both native synaptic vesicles and artificial phospholipid
bilayers. This is consistent with the theory
that hydrophobic interactions are largely responsible for the hydrophobic head
domain of Synapsin I. A single
phosphate group is not likely to supply either enough charge differential or
steric hindrance to disrupt the strong hydrophobic interactions between the
rest of the head domain and the phospholipid membranes. There is a difference, however, in the
results when considering phosphorylation at sites 2 and 3 in the tail domain,
which is not known to interaction significant through hydrophobic interactions
with membranes. The tail domain is also
known to be involved in interactions with non-lipid components in native
synaptic vesicles. These components may
not be present in artificial phospholipid bilayers which may explain why there
is little difference in binding affinity for synapsin I phosphorylated at sites
2 and/or 3 compared to dephosphorylated synapsin or site 1-phosphorylated
synapsin. In experiments with native
synaptic vesicles, however, there is a six-fold increase in dissociation constants
when the tail region is phosphorylated.
In non-hydrophobic interactions with non-lipid components, the steric
hindrance or charge differential caused by the addition of the phosphate groups
may explain the six-fold increase in dissociation constants relative to the
non-phosphorylated synapsin-vesicle complex.
In considering other factors affecting
non-hydrophobic binding, pH and ionic strength support the theory that
protein-protein interactions are responsible for the tail binding. According to Schiebler et al. (1986),
Synapsin I-vesicle binding was weakened by pH # 5 and binding was not observed at pH less than 3. This indicates either a partial denaturation
of the protein, steric profile differences in protonated versus deprotonated
amino acids, or interference with charge interactions between the tail region
and vesicle. Additionally, when bovine
Synapsin I was extracted at pH less than 3, affinities two- to three-fold lower
than detergent-salt-extracted synapsin I were observed (Schiebler et al.,
1986).
Actin
Nucleation and Elongation
There is evidence that the regulatory
function synapsins play in the release of neurotransmitters through exocytosis
is accomplished through the tethering of synaptic vesicles to cytoskeletal
elements (Bahler et al., 1989).
The study and analysis of interactions between actin microfilaments and
Synapsin I provides valuable insight into the synaptic vesicle cycle and
neurotransmitter regulation. Normally,
actin monomers will spontaneously polymerize when it has fulfilled three
requirements: 1. the preparation has reached a certain critical concentration
of G-actin, 2. there is a nucleation “seed” oligomer of F-actin, and 3.
elevated concentrations of potassium and magnesium are present (Fesce et al,
1992). In 1992, Fesce et al.
demonstrated that Synapsin I was able to form Synapsin-G actin complexes which
caused actin to polymerize where spontaneous polymerization is neglibile;
furthermore, this interaction is strongly affected by phosphorylation and
dephosphorylation of synapsin.
|
Synapsin
I-Actin |
KD
(nM) |
|
|
|
Dephosphorylated |
Phosphorylated |
|
29 kDa
Head Fragment |
2 |
1.8 |
|
40 kDa
Head/Middle |
168 |
|
|
51/41 kDa
Middle/Tail |
0.6 |
1.7 |
|
Tail
Fragment |
No
binding observed |
|
Actin polymerization rate is
dependent upon a number of factors.
These include number of pre-existing filaments, the concentration of
monomeric actin, and the rates at which monomers are added to the barbed end of
the filament and removed from the pointed end (Fesce et al., 1992).
The relationship between Synapsin I and G-actin, however, proves much
more complex. According to Fesce et
al. (1992), the interactions do not follow simple stoichiometric
ligand-receptor kinetics; in fact, the concentration of monoeric G-actin itself
influences the interactions. When
Synapsin I is added to actin preparations not in conditions normally amenable
to spontaneous polymerization, is is able to trigger the formation of actin
filaments, likely due to the formation of synapsin I- G-actin pseudonuclei
(Fesce et al., 1992).
Interactions between filamentous actin, however, and Synapsin I have not
yet been investigated and so the precise rate constants are unknown between
filamentous actin and Synapsin I. For
the purposes of this computer model, they have been estimated. Additional complications may be introduced
with modulation of Synapsin I-actin polymerization by ionic strength and
Synapsin phosphorylation. Synapsin I
affects the microfilament polymerization rate.
For the purposes of this computer model, it was determined that as a
simplifying assumption, the interactions of Synapsin I with actin are with
filamentous actin; monomeric actin is not considered.
By virtue of its interactions with microtubules, Synapsin I is
a member of the membrane-bound microtubule-associated proteins (Bennett et
al., 1991). Baines and Bennett
(1986) found that it co-isolates with microtubules from both whole-brain
extracts put through polymerization and depolymerization cycles, as well as
purified tubulin preparations. To
demonstrate this, they pelletted taxol-stabilized microtubules prepared from
phosphocellulose-purified bull brain.
The pellets were then analyzed by SDS-PAGE. The Synapsin I head and tail fragments consistently co-sedimented
with microtubules, the tail being more common than the head. The experimenters, however, were not able to
extrapolate specific association constant values from this experiment. These results seem surprising considering
that sequence comparisons between Synapsin I and the microtubule-binding bovine
tau protein revealed no significant sequence identities or resemblance to MAP
1b microtubule binding domain motif “Lys-Lys-Glu-Glu.” Studies of the tubulin-binding portions of
Synapsin may yield valuable information about its actin-binding activity;
Correas et al. (1990) found that the microtubule-associated protein 2
(MAP 2) tubulin binding sites also had significant actin-binding activity. Immunoelectron microscopy also indicated a
relationship between the tubulin-binding sites of tau protein and actin-binding
activity. The microtubule- and
microfilament-binding sites of Synapsin I may be one and the same (or at least
shared). This, however, could imply a
competitive relationship between actin and tubulin binding. For purposes of this simulation, it is
assumed that interactions at potential microfilament/microtubule binding sites
are with actin filaments only.
The simulation of real-time interactions between
phosphorylated and dephosphorylated Synapsin I, synaptic vesicles, and actin
microfilaments will be simplified to consider the affinities for these four
components only. Because a change in
concentration of any one of the components implies a change in all of the
others, the changes in concentration for each of the four molecules must be
simultaneously solved. Facilitating
this feat, the SCoP software program will allow the tedious and insurmountable
task of manual calculations to be completed by computer. As per the kinetic reaction web illustrated
below, each potential reaction will be represented by an equation for which a
forward and backward reaction are characterized by a discrete constant. For
example, the reaction of dephosporylated synapsin binding to synaptic vesicles
is represented by:
S + V W SV
The forward
reaction is characterized by a kon constant, and the reverse by a koff. The software program is able to calculate
the concentration of bound synaptic vesicles as by the following relationship:
![]()

Similarly, kcat1 and kcat2
are used to calculate the population of phosphorylated versus
non-phosphorylated synapsin.
Materials
and Methods
Real-time computermathematical modeling
was accomplished using Simulation Control Program (Simulation Resources, Inc.;
Redland CA). The programming involved writing
a MOD file using a text editor and compiling this MOD script using
MAKESCOP. The end result is an
executable DOS file, which can be used to run the simulation. Output was taken in the form of a tabulated
DOS text file, which was imported into Microsoft Excel97 and plotted as a
graph.
Kinetic constants used for simulation
were estimated from literature constants.
In order to vary the constants used in each run of the program, separate
“VAR” files were created according to each condition. The “VAR” file contents were constructed for each condition as
follows:
|
K1on
(/M/sec) |
1.2 x 107 |
K1off
(/sec) |
1.0 x 10-1 |
K2on
|
2.0 x 104 |
K2off |
1.0 x 10-1 |
|
K3on |
1.0 x 105 |
K3off |
1.0 x 10-1 |
|
K4on |
1.0 x 105 |
K4off |
1.0 x 10-1 |
|
Kcat1 |
1.0 x 10 |
Kcat2 |
1.0 x 103 |
|
S0
(mol/L) |
1.0 x 10-6 |
V0
(mol/L) |
1.0 x 10-5 |
|
A0
(mol/L) |
1.0 x 10-5 |
Time |
0 to 20s
(100 parts) |
In order to
simulate a higher population of phosphorylated versus non-phosphorylated
Synapsin, the kcat values were modified to favour the phosphorylated
forms.
Results
Output from the SCoP software consisted
of a graphical representation of the amount of synaptic vesicles bound to the
cytoskeleton versus time.
Figure 1 illustrates the proportion of
synaptic vesicles bound to actin filaments by synapsin. It is expressed as a proportion of the
starting concentration of synapsin in the mixture, 1 x 10-6.
Figure 2 illustrates the proportion of
synaptic vesicles bound to actin filaments by synapsin when a large population
is phosphorylated. In vivo, this
would be effected by phosphorylation at sites 2, 3 by
calcium/calmodulin-dependent protein kinase.
In the simulation, it was simulated by changing the two constants
representing the phosphorylation of synapsin to favour the phosphorylated
form.
Discussion
Synapsin Ia represents one member of a
family of five types of neuron-specific phosphoproteins. It is believed that its role in regulation
of neurotransmitter release by synaptic vesicle fusion and exocytosis in the
presynaptic nerve terminal involves the differential association and
dissociation with neurotransmitter-carrying synaptic vesicles and elements of
the cytoskeleton (Bahler and Greengard, 1987; Stefani G et al., 1997).
Because of the high frequencies with which action potentials may occur, it is
necessary that a releasable pool of neurotransmitter be maintained and cycled
quickly. The elucidation of the
mechanisms responsible for these interactions is therefore critical in the
understanding of the processes governing complex psychological processes, such
as memory, cognition, emotion, and psychological disorders.
Many studies to date have involved
equilibrium analysis of individual interactions between Synapsin proteins and
either synaptic vesicles or cytoskeletal elements, but not as a whole. The value of a computer-based real-time
simulation lies in the flexibility and ease of changing controlled variables,
and especially in the reductionist approach to simplifying a problem to its
most critical components. The use of
Pareto analysis is therefore a valuable tool in the selection of the most
critical factors in a relationship the modulation of which factors yields the
greatest variability. The direct
observation of the pre-equilibrium kinetics of the interactions between
Synapsin and both actin filaments and synaptic vesicles has proven to be
difficult, and although pre-equilibrium rate constants have been obtained for
various aspects of this relationship through such techniques as flourescence
resonance energy transfer (Stefani G, et al., 1997), some critical
aspects remain to be characterized. For
example, Stefani et al. (1997) found that it was not possible to obtain
the specific kinetic kon and koff rates for synapsins and synaptic
vesicles using traditional methods involving exogenously-added activated
phosphorylating calcium/calmodulin kinase; fluorescence transfer in the case of
phosphorylation at the C-terminal sites by CaMKII greatly reduced binding of
synapsin to synaptic vesicles, and the increase in ionic strength meant to
cause dissociation did not cause appreciable change to the already-low levels
of bound synaptic vesicles.
Although Synapsins have been shown to
have significant binding relationships with actin filaments, neurofilaments,
and microtubules, the major component believed to be involved in the storage of
synaptic vesicles are actin filaments (Bahler and Greengard, 1987) because
previous studies had shown that neither neurofilaments nor microtubules are
present in appreciable amounts in the region of the presynaptic nerve terminal
where synaptic vesicles are generally located (Roots, 1983).
Synaptic vesicles have been shown to have
two types of interactions with synapsin proteins. The hydrophobic interaction between the head portion of the
synapsin molecule and the synaptic vesicles was demonstrated to be strictly
hydrophobic in nature, and affected by neither ionic strength nor
phosphorylation state. A second
interaction, more relevant to regulatory function, is the protein-protein
interaction between the tail portion of synapsin and a protein component of
synaptic vesicles. Stefani et al.
(1997) reported that the dissociation constants for mixed phospholipid vesicles
versus actual synaptic vesicles was higher, implying that there is a specific
component in synaptic vesicles which allows for greater binding potential. The effects of phosphorylation of synapsin
in the simulation was therefore designed with site 2/3 phosphorylation as a
target, implying further work to incorporate CaM Kinase II regulation into the
model.
Figure 1 illustrates the simulation using
the default parameters derived both from literature values and estimated
values. The rapid binding and high
saturability exhibited by the fluorescence resonance energy transfer
experiments (Stefani et al., 1997) are also exhibited by the computer
simulation.
Literature values for the rate constants
governing the association of both the phosphorylated and dephosphorylated forms
of synapsin for synaptic vesicles were obtained from Stefani et al.
(1997). Literature had previously
existed which described the equilibrium relations between synapsin and actin
filaments, but as yet, no pre-equilibrium binding kinetics data are
available. It is possible that using
the same FRET technology used to determine the rate constants for the
synapsin-vesicle binding this constant could be determined in future
studies.
It has been demonstrated that the
affinity of synapsin for synaptic vesicles can be based on the state of
phosphorylation of sites 2 and 3 in the tail region and is irrespective of the
phpshorylation state of site 1 in the head region (Stefani et al.,
1997). For this reason, the modelling
of the phosphorylation state assumes phosphorylation of sites 2 and 3 by
calcium/calmodulin-dependent protein kinase II (CaM KII) and not site 1 by
protein kinase A (PKA). This is
represented in the model by a pair of static constant, kcat1 and kcat2. In an in vivo system, these two
constants would be supplanted by the specific activity of the CaMKII present in
the system. Future direction would
include the incorporation of a CaMKII model which would, in turn, replace the
static constants used in this model.
In order to take into account the
phosphorylation of the tail sites by CaMKII, the factors affecting the activity
of CaMKII must be analyzed. Studies
have shown that CaMKII is a multisubstrate kinase which is able to
phosphorylate any of a given set of substrates in the presence of
calcium/calmodulin and given a phosphate source, ATP (Stefani et al.,
1997; Hanson et al., 1994). The
actual implementation of such a model, however, is much more complex than the
simple unimolecular case of synapsin.
CaMKII often polymerizes into multimers of up to ten subunits, the
activity of which is further affected by their respective phosphorylation
states and presence or absence of calcium/calmodulin. It is through this mechanism by which action potentials are
thought to be decoded and possibly amplified.
Matters of CaMKII modelling are further
complicated because of the ability of CaMKII to trap calmodulin for a brief
period even at sub-threshold calcium concentrations (Hanson et al.,
1994). This causes a
frequency-dependent accumulation of holoenzyme activity dependent upon number
of subunits and frequency of calcium spikes.
The activity profile of CaMKII is therefore quite complex and unless a
complete analysis of the priorities of the factors affecting CaMKII and its in
vivo substrates is completed, the integration of such a model would prove
useless as a model of an in vivo system. For the purposes of this project, therefore, the activity of
CaMKII was reprented by the pair of static kinetic constants. In the case of low CaMKII activity, and
therefore low levels of phosphorylated synapsin, a low kcat1 was
selected relative to kcat2, resulting in a lower population of
phosphorylated synapsin versus non-phosphorylated synapsin. The result of this is evident in a visual
comparison between figures 1 and 2.
Note that in figure 2, the simulation of an increased population of
phosphorylated synapsin yielded a significantly reduced population of cytoskeleton-bound
synaptic vesicles. This supports the
theory that a releasable pool of neurotransmitter may be maintained close to
the presynaptic nerve terminal for regulated release by modulation of the
phosphorylation state of synapsin present.
In fact, previous studies involving gene knockouts in mice exhibited
synaptic depression as a result of the lack of synapsin protein. This lack of synapsin protein precluded the
maintenance of a releasable pool of neurotransmitter, and disallowed sustained
exocytosis of neurotransmitter.
There are two possibilities speculated
for the mechanism of neurotransmitter release involving the tethering of
synaptic vesicles to the cytoskeleton by synapsin I. Actin filaments are often associated with mobility functions. This is evident from the polarity and nature
of actin filaments and subunits. In
fact, Bahler and Greengard (1987) described the ability of synapsin I to
nucleate actin subunits and affect polymerization. It is therefore conceivable that synaptic vesicles are
translocated within the cell via a “treadmill”-like mechanism involving
polymerization and disintegration of filamentous actin within the cell. How the synaptic vesicles are able to
translocate to the boundary of the nerve terminal when an action potential is
to be decoded could result either by active transport of the synaptic vesicles
tethered to the cytoskeleton, or by diffusion. Although diffusion is often a
slow process over large distances, it is quite effective at microscopic scales and
could be efficient enough for the translocation of synaptic vesicles. It is unlikely, however, that evolutionary
pressure would allow to allow neurotransmitter to diffuse without strict
directional control. Sudhof (1995)
proposed, however, that translocation of synaptic vesicles was due to diffusion
rather than active cytoskeletal transport due to the apparent dearth of
cytoskeletal elements close to the active zones.
Conclusion
It is possible to construct a
computer-based mathematical model of the dynamic interactions between synapsin
phosphoproteins, synaptic vesicles, and the cytoskeleton. The model provides a simplified view of the
binding kinetics involved. In order to
determine whether or not the model accurately reflects a real-world system, it
is possible to conduct further experimentation involving each of these
components in vitro.
Experimentation has been done using fluorescence resonance energy
transfer to characterize the kinetics of synapsin-synaptic vesicle
interactions, and it is possible to do the same with actin filaments. The computer model, however, provides a
convenient method of projecting the effects of changes in phosphorylation state
of synapsin based on changes in phosphorylation state. To further increase the relevance of this
model, it is conceivable that a CaMKII model be integrated into the system,
replacing the static kcat variables with a dynamic subroutine, which has
its own activators and inhibitors.
Appendix 1
Parameterization of the Interactions to be Modelled

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