Glavinovíc M I
Department of Anaesthesia Research, McGill University, 3655 Drummond Street, Montreal, PQ H3G 1Y6, Canada.
Pflugers Arch. 1999 Feb;437(3):462-70. doi: 10.1007/s004240050802.
The release of vesicular glutamate, spatiotemporal changes in glutamate concentration in the synaptic cleft and the subsequent generation of fast excitatory postsynaptic currents at a hippocampal synapse were modeled using the Monte Carlo method. It is assumed that glutamate is released from a spherical vesicle through a cylindrical fusion pore into the synaptic cleft and that S-alpha-amino-3-hydroxy -5-methyl-4-isoxazolepropionic acid (AMPA) receptors are uniformly distributed postsynaptically. The time course of change in vesicular concentration can be described by a single exponential, but a slow tail is also observed though only following the release of most of the glutamate. The time constant of decay increases with vesicular size and a lower diffusion constant, and is independent of the initial concentration, becoming markedly shorter for wider fusion pores. The cleft concentration at the fusion pore mouth is not negligible compared to vesicular concentration, especially for wider fusion pores. Lateral equilibration of glutamate is rapid, and within approximately 50 micros all AMPA receptors on average see the same concentration of glutamate. Nevertheless the single-channel current and the number of channels estimated from mean-variance plots are unreliable and different when estimated from rise- and decay-current segments. Greater saturation of AMPA receptor channels provides higher but not more accurate estimates. Two factors contribute to the variability of postsynaptic currents and render the mean-variance nonstationary analysis unreliable, even when all receptors see on average the same glutamate concentration. Firstly, the variability of the instantaneous cleft concentration of glutamate, unlike the mean concentration, first rapidly decreases before slowly increasing; the variability is greater for fewer molecules in the cleft and is spatially nonuniform. Secondly, the efficacy with which glutamate produces a response changes with time. Understanding the factors that determine the time course of vesicular content release as well as the spatiotemporal changes of glutamate concentration in the cleft is crucial for understanding the mechanism that generates postsynaptic currents.
利用蒙特卡罗方法对海马突触中囊泡型谷氨酸的释放、突触间隙中谷氨酸浓度的时空变化以及随后快速兴奋性突触后电流的产生进行了建模。假设谷氨酸从球形囊泡通过圆柱形融合孔释放到突触间隙,且S-α-氨基-3-羟基-5-甲基-4-异恶唑丙酸(AMPA)受体在突触后均匀分布。囊泡浓度的变化时间进程可用单指数描述,但也观察到一个缓慢的尾部,不过这仅在大部分谷氨酸释放之后出现。衰减时间常数随囊泡大小和较低的扩散常数增加,且与初始浓度无关,对于更宽的融合孔明显更短。与囊泡浓度相比,融合孔口处的间隙浓度不可忽略,尤其是对于更宽的融合孔。谷氨酸的横向平衡很快,平均在约50微秒内所有AMPA受体都能看到相同浓度的谷氨酸。然而,从平均-方差图估计的单通道电流和通道数量在根据上升电流段和衰减电流段估计时是不可靠且不同的。AMPA受体通道更高的饱和度提供了更高但并非更准确的估计。有两个因素导致突触后电流的变异性,使平均-方差非平稳分析不可靠,即使所有受体平均看到相同浓度的谷氨酸。首先,谷氨酸瞬时间隙浓度的变异性与平均浓度不同,首先迅速下降,然后缓慢增加;间隙中分子越少变异性越大,且在空间上不均匀。其次,谷氨酸产生反应的效能随时间变化。了解决定囊泡内容物释放时间进程以及间隙中谷氨酸浓度时空变化的因素对于理解产生突触后电流的机制至关重要。