Thurbon D, Lüscher H R, Hofstetter T, Redman S J
John Curtin School of Medical Research, Australian National University, Canberra, Australia.
J Neurophysiol. 1998 May;79(5):2485-502. doi: 10.1152/jn.1998.79.5.2485.
Recordings were made from large neurons located in the ventral horn of transverse spinal cord slices from young rats (7-15 days). Whole cell recordings were made simultaneously with two electrodes from the soma of these neurons, visualized using infra-red differential interference contrast optics. Positive identification of motoneurons could not always be achieved. The response of a neuron to a brief pulse of current delivered by one electrode, and recorded by the other electrode, were matched optimally to responses of a compartmental model of the same neuron with an identical current pulse as input. The compartmental model was based on a reconstruction of the neuron, using Biocytin staining. The compartmental model had three free parameters: specific membrane capacitance (Cm), membrane resistivity (Rm), and cytoplasmatic resistivity (Ri), all assumed to be uniform throughout the neuron. The experimental and model responses could be matched unequivocally for four neurons, giving Cm = 2.4 +/- 0.5 microF/cm2, Rm = 5.3 +/- 0. 9 kOmega/cm2, and Ri = 87 +/- 22 Omega/cm. No somatic shunt was required. For the remaining six neurons, a less perfect fit (but still within 95% confidence limits) was indicative of nonhomogeneous membrane properties. The electrotonic length of uncut dendrites was 0.85 +/- 0.14 lambda. The results resolve the issue of a somatic shunt conductance for motoneurons, relegating it to a microelectrode impalement artifact. They are consistent with previous reports on the electrical compactness of motoneurons to steady state currents and voltages. However, the much higher value of Cm (than the previously assumed 1 microF/cm2) implies much greater dendritic attenuation of fast synaptic potentials, and a much enhanced integrative response of motoneurons to synaptic potentials.
记录取自幼鼠(7 - 15日龄)横断脊髓切片腹角中的大神经元。使用两个电极从这些神经元的胞体同时进行全细胞记录,通过红外微分干涉对比光学显微镜进行观察。并非总能明确识别出运动神经元。一个电极施加短暂电流脉冲,另一个电极记录神经元的反应,并将其与以相同电流脉冲作为输入的同一神经元的房室模型的反应进行最佳匹配。房室模型基于使用生物胞素染色对神经元的重建。房室模型有三个自由参数:比膜电容(Cm)、膜电阻(Rm)和细胞质电阻(Ri),所有这些参数在整个神经元中都假定是均匀的。对于四个神经元,实验反应和模型反应能够明确匹配,得出Cm = 2.4 ± 0.5微法/平方厘米,Rm = 5.3 ± 0.9千欧/平方厘米,Ri = 87 ± 22欧/厘米。无需体细胞分流。对于其余六个神经元,拟合效果不太理想(但仍在95%置信区间内),这表明膜特性不均匀。未切断树突的电紧张长度为0.85 ± 0.14λ。这些结果解决了运动神经元体细胞分流电导的问题,将其归结为微电极刺入伪迹。它们与先前关于运动神经元对稳态电流和电压的电致密性的报道一致。然而,Cm的值(比先前假定的1微法/平方厘米)高得多,这意味着快速突触电位的树突衰减要大得多,并且运动神经元对突触电位的整合反应大大增强。