Lux H D, Schubert P
Adv Neurol. 1975;12:29-44.
An understanding of the neuronal function requires the knowledge of the electroanatomy of dendrites, which comprise the major area and receive the main input in most neurons. Some simplifying assumptions are necessary to describe the electrical characteristics of the dendritic tree. The applicability of the simplified model of a combined equivalent dendritic cylinder proposed by Rall, was tested and verified by a combined analysis of anatomic and electrical data from the same spinal motoneurons. Assuming a uniform somadendritic membrane, estimates of the specific membrane resistance (RM: 2,700 +/- 920 omegacm2) were made by relating the neuronal input resistance with the combined dendritic trunk parameter (sigmaD3/2: 320 +/- 150-10(-6) CM3/2). From these combined anatomic and electrical data the dendritic electrotonic lengths (Lgeom: 1.5 +/- 0.3 times the length constant) were derived. Comparable L values (Ltrans: 1.5 +/- 0.3) resulted independently from analysis of membrane voltage transients during current steps. The linear dendritic cable model has proved its applicability for the analysis of small voltage deflections during current step applications at the soma as well as for the analysis of the majority of minimal postsynaptic potentials (PSP's). During the transmission along the dendritic cable the PSP undergoes changes in shape. These changes often permit a determination of the distance of the dendritic input from the soma. Unfortunately, the attenuation of the dendritic signal cannot be directly assessed. Dendritic synaptic transmission can be observed in isolation in chromatolytic motoneurons because the somal synapses are peeled off from the soma by proliferating glial cells in the course of retrograde reaction. These observations support the prediction that the PSP's with relatively short rise-times and duration originate from synapses near the soma. It may be questioned as to whether the linear dendritic cable approximation also applies to the larger voltage displacements during excitatory synaptic action. Particularly interesting is an increase of the apparent membrane resistance during depolarization known as anomalous rectification. The anomalous rectification could be reversibly eliminated and turned into a normal rectification by the application of cobalt ions or other calcium antagonists. Therefore, it appears likely that this phenomenon is caused by a voltage-(and time-) dependent reaction of the membrane, consisting of a smoothly increased calcium conductance during depolarizations that are even subthreshold for eliciting action potentials. Such a process would result in a shortening of the dendritic electrotonic length and in facilitating the postsynaptic excitatory transmission.
要理解神经元功能,需要了解树突的电解剖结构,树突构成了大多数神经元的主要区域并接收主要输入。为了描述树突树的电学特性,需要一些简化假设。通过对来自同一脊髓运动神经元的解剖学和电学数据进行综合分析,对拉尔提出的组合等效树突圆柱体简化模型的适用性进行了测试和验证。假设体细胞 - 树突膜均匀,通过将神经元输入电阻与组合树突干参数(σD3/2:320±150 - 10(-6) CM3/2)相关联,对特定膜电阻(RM:2,700±920欧姆·厘米2)进行了估计。从这些综合的解剖学和电学数据中得出了树突电紧张长度(Lgeom:1.5±0.3倍长度常数)。通过对电流阶跃期间膜电压瞬变的分析独立得出了可比的L值(Ltrans:1.5±0.3)。线性树突电缆模型已证明其适用于分析体细胞电流阶跃应用期间的小电压偏转以及大多数最小突触后电位(PSP)。在沿树突电缆传输过程中,PSP的形状会发生变化。这些变化通常允许确定树突输入距体细胞的距离。不幸的是,树突信号的衰减无法直接评估。在染色质溶解的运动神经元中可以单独观察到树突突触传递,因为在逆行反应过程中,体细胞突触被增殖的神经胶质细胞从体细胞上剥离。这些观察结果支持了以下预测:上升时间和持续时间相对较短的PSP起源于体细胞附近的突触。对于线性树突电缆近似是否也适用于兴奋性突触作用期间的较大电压位移可能存在疑问。特别有趣的是去极化期间表观膜电阻的增加,称为反常整流。通过施加钴离子或其他钙拮抗剂,反常整流可以被可逆地消除并转变为正常整流。因此,这种现象似乎很可能是由膜的电压(和时间)依赖性反应引起的,该反应包括在甚至低于引发动作电位阈值的去极化期间钙电导的平滑增加。这样的过程将导致树突电紧张长度缩短并促进突触后兴奋性传递。