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猫脊髓中已鉴定类型的α运动神经元的电紧张结构

Electrotonic architecture of type-identified alpha-motoneurons in the cat spinal cord.

作者信息

Fleshman J W, Segev I, Burke R B

机构信息

Laboratory of Neural Control, National Institute of Neurological and Communicative Disorders and Stroke, Bethesda, Maryland 20892.

出版信息

J Neurophysiol. 1988 Jul;60(1):60-85. doi: 10.1152/jn.1988.60.1.60.

Abstract
  1. Measurements of input resistance (RN), time constant (tau 0), and electrotonic length (Lpeel) were derived from intracellular voltage changes produced by injection of current pulses in six type-identified triceps surae alpha-motoneurons. The motoneurons were labeled with horseradish peroxidase and subsequently reconstructed and measured from serial sections. These quantitative morphological and physiological data were incorporated into detailed computer models of the motoneurons. 2. Steady-state and dynamic models were used to determine values for specific membrane resistivity (Rm) that matched the experimental estimates of RN, tau 0, and Lpeel for each motoneurons. The models were based on the following assumptions 1) the membrane was electrically passive, 2) cytoplasmic resistivity (Ri) was 70 omega-cm, and 3) "sealed-end" boundary conditions were present at dendritic terminations. We also considered the nature and magnitude of possible errors introduced by using linear (passive) computer models to match responses from motoneurons with nonlinear (i.e., voltage-dependent) conductances. 3. If we assume that the experimental measurements of RN and tau 0 were correct, uniform Rm values that reproduced the experimentally measured RN required widely varying values of Cm (1.4-8.6 microF/cm2) to match the experimental tau 0. Furthermore, the electrotonic distance to dendritic terminals was generally much greater than expected from physiological estimates of Lpeel. However, if we assumed that the RN measurements could have been underestimated by as much as 30% and that Cm = 1.0 microF/cm2, it was possible to choose spatially uniform Rm that matched the observed tau 0 in three of six cases. 4. Relaxing the assumption of spatially uniform membrane resistivity permitted us to reconcile the anatomical and physiological characteristics of all six motoneurons. Two qualitatively different models of Rm nonuniformity gave equally good fits to the experimental results 1) a step-wise increase in Rm from a low value at the soma to a much higher but uniform value over the entire dendritic tree, and 2) a monotonic increase in Rm from soma to distal dendrites as a sigmoidal function of path distance along the dendrites. The step and sigmoidal models of the spatial distribution of Rm generated different electrotonic architectures in motoneuron dendritic trees, but both gave essentially identical electrical responses at the soma.(ABSTRACT TRUNCATED AT 400 WORDS)
摘要
  1. 通过向6个已鉴定类型的腓肠肌α运动神经元注入电流脉冲所产生的细胞内电压变化,得出输入电阻(RN)、时间常数(tau 0)和电紧张长度(Lpeel)的测量值。这些运动神经元用辣根过氧化物酶标记,随后从连续切片中进行重建和测量。这些定量的形态学和生理学数据被纳入运动神经元的详细计算机模型中。2. 使用稳态和动态模型来确定特定膜电阻率(Rm)的值,使其与每个运动神经元的RN、tau 0和Lpeel的实验估计值相匹配。这些模型基于以下假设:1)膜是电被动的;2)细胞质电阻率(Ri)为70Ω·cm;3)在树突末梢存在“密封端”边界条件。我们还考虑了使用线性(被动)计算机模型来匹配具有非线性(即电压依赖性)电导的运动神经元的反应所引入的可能误差的性质和大小。3. 如果我们假设RN和tau 0的实验测量是正确的,那么再现实验测量的RN所需的均匀Rm值需要广泛变化的Cm值(1.4 - 8.6微法/平方厘米)来匹配实验tau 0。此外,到树突末梢的电紧张距离通常比根据Lpeel的生理学估计所预期的要大得多。然而,如果我们假设RN测量可能被低估了多达30%,并且Cm = 1.0微法/平方厘米,那么在6个案例中的3个案例中,可以选择与观察到的tau 0相匹配的空间均匀的Rm。4. 放宽膜电阻率在空间上均匀的假设使我们能够协调所有6个运动神经元的解剖学和生理学特征。两种性质不同的Rm不均匀性模型对实验结果的拟合效果同样好:1)Rm从胞体处的低值逐步增加到整个树突树上更高但均匀的值;2)Rm从胞体到远端树突呈单调增加,是沿树突路径距离的S形函数。Rm空间分布的阶跃模型和S形模型在运动神经元树突树中产生了不同的电紧张结构,但在胞体处给出的电反应基本相同。(摘要截断于400字)

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