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通过计算机模拟重建海马体CA1锥体细胞电生理学。

Reconstruction of hippocampal CA1 pyramidal cell electrophysiology by computer simulation.

作者信息

Warman E N, Durand D M, Yuen G L

机构信息

Department of Biomedical Engineering, Case Western Reserve University, Cleveland, Ohio 44106.

出版信息

J Neurophysiol. 1994 Jun;71(6):2033-45. doi: 10.1152/jn.1994.71.6.2033.

Abstract
  1. We have developed a 16-compartment model that reproduces most of the features of the CA1 pyramidal cell electrophysiology observed experimentally. The model was constructed using seven active ionic conductances: gNa, gCa, gDR, gCT, gA, gM, and gAHP whose kinetics have been, inferred, in most cases, from the available voltage-clamp data obtained from these cells. We focussed the simulation on the initial and late accommodation, the slow depolarization potential and the spike broadening during repetitive firing, because their mechanisms are not well understood. 2. Current-clamp records were reproduced by iterative adjustments to the ionic maximum conductances, scaling and/or "reshaping" of the gates' time constant within the experimental voltage-clamp data, and shifting the position of the steady-state gate opening. The final properties of the ionic channels were not significantly different from the voltage-clamp experiments. 3. The resulting model reproduces all four after-potentials that have been recorded to follow activation of the cell. The fast, medium, and slow after-hyperpolarization potentials (AHPs) were, respectively, generated by ICT, IM, and IAHP. Furthermore, the model suggests that the mechanisms underlying the depolarization after potential (DAP) is mostly due to passive recharging of the soma by the dendrites. 4. The model also reproduces most of the firing features experimentally observed during injection of long current pulses. Model responses showed a small initial decrease in the firing frequency during a slow underlying depolarization potential, followed by a more significant frequency decrease. Moreover, a gradual broadening of the action potential and loss of the fast AHP were also observed during the initial high-frequency firing, followed, as the firing frequency decreased, by a gradual recovery of the spikes' original width and fast AHP amplitude increase. 5. A large reduction of the K repolarizing current was required to reproduce the spike broadening and reduction of the fast AHP experimentally observed in CA1 cells during repetitive firing responses. The incorporation of a transient Ca- and voltage-dependent K current (ICT) into the model successfully reproduced these experimental observations. In contrast, we were unable to reproduce this phenomenon when a large persistent Ca- and voltage-dependent K current (generally named IC) was included in the model. These results suggest that there is a strong contribution to action-potential repolarization and fast AHP by a transient Ca- and voltage-dependent K current (ICT). 6. The two accommodation steps were induced by a progressively enlargement of two K currents IM (initial) and IAHP (late).(ABSTRACT TRUNCATED AT 400 WORDS)
摘要
  1. 我们开发了一个16室模型,该模型再现了实验观察到的CA1锥体细胞电生理的大部分特征。该模型是使用七种主动离子电导构建的:gNa、gCa、gDR、gCT、gA、gM和gAHP,在大多数情况下,其动力学是根据从这些细胞获得的可用电压钳数据推断出来的。我们将模拟重点放在初始和晚期适应性、缓慢去极化电位以及重复放电期间的动作电位展宽上,因为它们的机制尚未完全理解。2. 通过对离子最大电导进行迭代调整、在实验电压钳数据内对门控时间常数进行缩放和/或“重塑”以及移动稳态门控开放位置,来重现电流钳记录。离子通道的最终特性与电压钳实验没有显著差异。3. 所得模型再现了记录到的跟随细胞激活的所有四种后电位。快速、中等和缓慢的超极化后电位(AHPs)分别由ICT、IM和IAHP产生。此外,该模型表明去极化后电位(DAP)的潜在机制主要是由于树突对胞体的被动再充电。4. 该模型还再现了在注入长电流脉冲期间实验观察到的大多数放电特征。模型响应显示,在缓慢的基础去极化电位期间,放电频率最初有小幅下降,随后下降更为显著。此外,在初始高频放电期间还观察到动作电位逐渐展宽以及快速AHP消失,随着放电频率降低,动作电位逐渐恢复到原来的宽度,快速AHP幅度增加。5. 需要大幅降低K复极化电流,以再现实验中在CAI细胞重复放电反应期间观察到的动作电位展宽和快速AHP降低。将瞬态钙和电压依赖性K电流(ICT)纳入模型成功再现了这些实验观察结果。相比之下,当模型中包含大量持续的钙和电压依赖性K电流(通常称为IC)时,我们无法再现这一现象。这些结果表明,瞬态钙和电压依赖性K电流(ICT)对动作电位复极化和快速AHP有很大贡献。6. 两个适应性步骤是由两种K电流IM(初始)和IAHP(晚期)逐渐增大引起的。(摘要截断于400字)

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