Department of Integrative Biology Physiology, 6-125 Jackson Hall, 321 Church Street S.E., University of Minnesota, Minneapolis, MN 55455, USA.
J Neurophysiol. 2010 Mar;103(3):1357-74. doi: 10.1152/jn.00123.2009. Epub 2010 Jan 6.
Trains of action potentials of rat and cat retinal ganglion cells (RGCs) were recorded intracellularly across a temperature range of 7-37 degrees C. Phase plots of the experimental impulse trains were precision fit using multicompartment simulations of anatomically reconstructed rat and cat RGCs. Action potential excitation was simulated with a "Five-channel model" [Na, K(delayed rectifier), Ca, K(A), and K(Ca-activated) channels] and the nonspace-clamped condition of the whole cell recording was exploited to determine the channels' distribution on the dendrites, soma, and proximal axon. At each temperature, optimal phase-plot fits for RGCs occurred with the same unique channel distribution. The "waveform" of the electrotonic current was found to be temperature dependent, which reflected the shape changes in the experimental action potentials and confirmed the channel distributions. The distributions are cell-type specific and adequate for soma and dendritic excitation with a safety margin. The highest Na-channel density was found on an axonal segment some 50-130 microm distal to the soma, as determined from the temperature-dependent "initial segment-somadendritic (IS-SD) break." The voltage dependence of the gating rate constants remains invariant between 7 and 23 degrees C and between 30 and 37 degrees C, but undergoes a transition between 23 and 30 degrees C. Both gating-kinetic and ion-permeability Q10s remain virtually constant between 23 and 37 degrees C (kinetic Q10s = 1.9-1.95; permeability Q10s = 1.49-1.64). The Q10s systematically increase for T <23 degrees C (kinetic Q10 = 8 at T = 8 degrees C). The Na channels were consistently "sleepy" (non-Arrhenius) for T <8 degrees C, with a loss of spiking for T <7 degrees C.
在 7-37°C 的温度范围内,记录了大鼠和猫视网膜神经节细胞 (RGC) 的动作电位序列。通过对解剖重建的大鼠和猫 RGC 的多室模拟,对实验冲动序列的相图进行了精密拟合。动作电位激发采用“五通道模型”[Na、K(延迟整流)、Ca、K(A)和 K(Ca 激活)通道]进行模拟,利用整个细胞记录的非空间钳位条件来确定通道在树突、体和近端轴突上的分布。在每个温度下,RGC 的最佳相图拟合都具有相同的独特通道分布。电紧张电流的“波形”随温度而变化,这反映了实验动作电位的形状变化,并证实了通道分布。这些分布是细胞类型特异性的,足以满足体和树突激发的需要,并有安全裕度。通过温度依赖性的“初始段-体-树突(IS-SD)断裂”,发现最高的 Na 通道密度位于距体约 50-130 µm 的轴突段上。门控速率常数的电压依赖性在 7 和 23°C 以及 30 和 37°C 之间保持不变,但在 23 和 30°C 之间发生转变。在 23 和 37°C 之间,门控动力学和离子通透性 Q10 几乎保持不变(动力学 Q10=1.9-1.95;通透性 Q10=1.49-1.64)。对于 T<23°C,Q10 系统地增加(动力学 Q10=8,T=8°C)。对于 T<8°C,Na 通道一直处于“休眠”状态(非 Arrhenius),T<7°C 时则失去脉冲。