University of Calgary, AB, Canada.
Channels (Austin). 2011 Nov-Dec;5(6):530-7. doi: 10.4161/chan.5.6.17484. Epub 2011 Nov 1.
The resting membrane potential, E(m), of mammalian cells is a fundamental physiological parameter. Even small changes in E(m) can modulate excitability, contractility and rates of cell migration. At present accurate, reproducible measurements of E(m) and determination of its ionic basis remain significant challenges when patch clamp methods are applied to small cells. In this study, a mathematical model has been developed which incorporates many of the main biophysical principles which govern recordings of the resting potential of 'small cells'. Such a prototypical cell (approx. capacitance, 6 pF; input resistance 5 GΩ) is representative of neonatal cardiac myocytes, and other cells in the cardiovascular system (endothelium, fibroblasts) and small cells in other tissues, e.g. bone (osteoclasts) articular joints (chondrocytes) and the pancreas (β cells). Two common experimental conditions have been examined: (1) when the background K(+) conductance is linear; and (2) when this K(+) conductance is highly nonlinear and shows pronounced inward rectification. In the case of a linear K(+) conductance, the presence of a "leakage" current through the seal resistance between the cell membrane and the patch pipette always depolarizes E(m). Our calculations confirm that accurate characterization of E(m) is possible when the seal resistance is at least 5 times larger than the input resistance of the targeted cell. Measurement of E(m) under conditions in which the main background current includes a markedly nonlinear K(+) conductance (due to inward rectification) yields complex and somewhat counter-intuitive findings. In fact, there are at least two possible stable values of resting membrane potential for a cell when the nonlinear, inwardly rectifying K(+) conductance interacts with the seal current. This type of bistable behavior has been reported in a variety of small mammalian cells, including those from the heart, endothelium, smooth muscle and bone. Our theoretical treatment of these two common experimental situations provides useful mechanistic insights, and suggests practical methods by which these significant limitations, and their impact, can be minimized.
哺乳动物细胞的静息膜电位(E(m))是一个基本的生理参数。即使 E(m) 发生微小变化,也可以调节兴奋性、收缩性和细胞迁移率。目前,当应用膜片钳方法测量小细胞时,精确、可重复地测量 E(m) 并确定其离子基础仍然是一个重大挑战。在这项研究中,已经开发了一种数学模型,该模型结合了许多控制“小细胞”静息电位记录的主要生物物理原理。这种典型细胞(约 6 pF 的电容,5 GΩ 的输入电阻)代表了新生心肌细胞以及心血管系统中的其他细胞(内皮细胞、成纤维细胞)和其他组织中的小细胞,例如骨骼(破骨细胞)关节(软骨细胞)和胰腺(β 细胞)。已经检查了两种常见的实验条件:(1)当背景 K(+)电导呈线性时;和(2)当这种 K(+)电导高度非线性并表现出明显的内向整流时。在 K(+)电导呈线性的情况下,细胞膜和膜片钳之间的密封电阻中的“漏”电流总是使 E(m) 去极化。我们的计算证实,当密封电阻至少比目标细胞的输入电阻大 5 倍时,就可以准确表征 E(m)。在主要背景电流包括明显非线性 K(+)电导(由于内向整流)的情况下测量 E(m)会产生复杂且有些违背直觉的结果。实际上,当非线性、内向整流的 K(+)电导与密封电流相互作用时,细胞的静息膜电位至少有两个可能的稳定值。这种双稳态行为已在多种小型哺乳动物细胞中报告,包括来自心脏、内皮细胞、平滑肌和骨骼的细胞。我们对这两种常见实验情况的理论处理提供了有用的机制见解,并提出了实用的方法,可以最小化这些显著限制及其影响。