A two-dimensional compartment model for the reaction-diffusion system of acetylcholine in the synaptic cleft at the neuromuscular junction
Introduction
In processing of the neuronal signals, the synaptic chemical transmission is an important process, and investigation of the molecular events in the process has led to the neurotransmitter theory (Mathews, 1986). The dynamic behavior of the neurotransmitter in diffusion through the synaptic cleft and action at the synaptic membranes is engaged in a fundamental function for the transmission process. Analysis of such behavior can be performed most appropriately with representation of the transmission process as a reaction-diffusion system (RD system) for the neurotransmitter because the experimental analysis still is practically difficult for the molecular processes in the cleft. Some mathematical models for the dynamic behavior of acetylcholine (ACh), a typical neurotransmitter, in spontaneous generation of the miniature endplate current (MEPC) at the neuromuscular junction have been proposed to analyze the transient process of the synaptic chemical transmission. In the model of Rosenberry (Rosenberry, 1979), the radial diffusion of ACh is treated in the two axis-symmetrical compartments with homogeneity in the transverse direction, while in the model of Thomas (Friboulet and Thomas, 1993) the transverse coordinate is discretized and the radial diffusion undergoes simple efflux of ACh due to the concentration gradient.
In this study, the one-dimensional compartment models of Rosenberry and Thomas are extended to a two-dimensional compartment model for examination of the effects of transverse and radial diffusion of ACh on the transient behavior of the chemical transmission process. The process is hence represented as an RD system, in which the ACh concentration varies with time and position in a two-dimensional space of axis-symmetrical disc of the synaptic cleft, due to transverse and radial diffusion of ACh and its interaction with the ACh receptor (AChR) and acetylcholinesterase (AChE). The variation in concentration of the open channel form of AChR in response to the interaction of AChR with incoming ACh corresponds to transient evolution of the MEPC. The behavior of this RD system of ACh is mathematically expressed by a two-dimensional diffusion equation with nonlinear reaction terms for ACh and a set of nonlinear ordinary differential equations governing the rate processes for AChR and AChE, which are distributed at the spatial points in the disc.
The analysis of temporal behavior of the RD system employs computer simulation, that is, discretization of both the transverse and radial coordinates in the space for the partial differential equation and numerical integration of the governing ordinary differential equations under various conditions (Hayashi and Sakamoto, 1986). Simulation of the response of the RD system to release of a single quantal packet of ACh into the cleft leads to characterization of the transverse and radial diffusion processes of ACh in the chemical transmission with reference to their effect on spontaneous generation of the MEPC. Based on an optimal selection of the subdivision numbers and critical radius for the simulation, a minimal compartment model is proposed which comprises three and ten compartments in the transverse and radial directions, respectively, in a disc with 500 nm of radius and 50 nm of height. Evaluation of the diffusion coefficients in the transverse and radial directions suggests anisotropic diffusion for this two-dimensional compartment model to represent the characteristic behavior of the chemical transmission process.
Section snippets
Formulation of the reaction-diffusion system
The following phenomena are essential in the chemical transmission with ACh as described in the construction of Thomas' model (Friboulet and Thomas, 1993), and taken into consideration for mathematical modeling of the RD system in this study. The RD system occupies a space of axis-symmetrical disc with a radius responsible for spontaneous generation of the MEPC and 50 nm height for transverse distance in the synaptic cleft. In the disc, the radial distribution of ACh concentration is assumed to
Simulation method
The partial differential equation governing the RD system of ACh in Eq. 3 is numerically solved under the specified boundary and initial conditions to reveal the behavior of the system after the release of ACh into the synaptic cleft. The boundary conditions for ACh are expressed byandso that ACh cannot leak out at either end of the disc, but its removal by radial diffusion takes place at the side surface of the disc. The initial
Effects of diffusion rates on the response characteristics
The behavior of the RD system of ACh is naturally dependent on the value of diffusion coefficient of ACh. Its accurate value in the milieu of the synaptic cleft is unknown, but certainly is smaller than the value in water (7.6×10−6 cm2 sec−1). A rational evaluation is possible by simulation of the minimal compartment model with various values of Dt and Dr. In optimal selection of the critical radius and compartment numbers for the model, it is noted that the radial diffusion process, in
Discussion
In this study, a compartment model is constructed to represent the chemical transmission process of ACh at the neuromuscular junction as an RD system in a two-dimensional space of axis-symmetrical disc of the synaptic cleft for spontaneous generation of the MEPC. The model is comprised of three compartments in the transverse direction and ten compartments in the radial direction in the disc so that the compartment numbers in the respective directions are minimal and yet suited for
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