Division of Physics, Office of Science and Engineering Laboratories, Center for Devices and Radiological Health, Food and Drug Administration, Silver Spring, Maryland, USA.
Biophys J. 2013 Jan 8;104(1):268-78. doi: 10.1016/j.bpj.2012.11.007.
The measurement, quantitative analysis, theory, and mathematical modeling of transmembrane potential and currents have been an integral part of the field of electrophysiology since its inception. Biophysical modeling of action potential propagation begins with detailed ionic current models for a patch of membrane within a distributed cable model. Voltage-clamp techniques have revolutionized clinical electrophysiology via the characterization of the transmembrane current gating variables; however, this kinetic information alone is insufficient to accurately represent propagation. Other factors, including channel density, membrane area, surface/volume ratio, axial conductivities, etc., are also crucial determinants of transmembrane currents in multicellular tissue but are extremely difficult to measure. Here, we provide, to our knowledge, a novel analytical approach to compute transmembrane currents directly from experimental data, which involves high-temporal (200 kHz) recordings of intra- and extracellular potential with glass microelectrodes from the epicardial surface of isolated rabbit hearts during propagation. We show for the first time, to our knowledge, that during stable planar propagation the biphasic total transmembrane current (I(m)) dipole density during depolarization was ∼0.25 ms in duration and asymmetric in amplitude (peak outward current was ∼95 μA/cm(2) and peak inward current was ∼140 μA/cm(2)), and the peak inward ionic current (I(ion)) during depolarization was ∼260 μA/cm(2) with duration of ∼1.0 ms. Simulations of stable propagation using the ionic current versus transmembrane potential relationship fit from the experimental data reproduced these values better than traditional ionic models. During ventricular fibrillation, peak I(m) was decreased by 50% and peak I(ion) was decreased by 70%. Our results provide, to our knowledge, novel quantitative information that complements voltage- and patch-clamp data.
跨膜电位和电流的测量、定量分析、理论和数学建模自电生理学诞生以来一直是其不可或缺的组成部分。动作电位传播的生物物理建模始于分布式电缆模型中膜片的详细离子电流模型。电压钳技术通过对跨膜电流门控变量的特征化,彻底改变了临床电生理学;然而,这种动力学信息本身不足以准确表示传播。其他因素,包括通道密度、膜面积、表面积/体积比、轴向电导率等,也是多细胞组织中跨膜电流的关键决定因素,但极难测量。在这里,我们提供了一种新颖的分析方法,从实验数据中直接计算跨膜电流,这涉及到使用玻璃微电极从离体兔心的心外膜表面在传播过程中进行高时间(200 kHz)的细胞内和细胞外电位记录。我们首次表明,在稳定的平面传播期间,去极化期间双相总跨膜电流(I(m))偶极子密度持续约 0.25 ms,幅度不对称(峰值外向电流约为 95 μA/cm(2),峰值内向电流约为 140 μA/cm(2)),去极化期间的峰值内向离子电流(I(ion))约为 260 μA/cm(2),持续时间约为 1.0 ms。使用从实验数据拟合的离子电流与跨膜电位关系的稳定传播模拟更好地再现了这些值,优于传统的离子模型。在心室颤动期间,I(m)峰值降低了 50%,I(ion)峰值降低了 70%。我们的结果提供了新颖的定量信息,补充了电压和膜片钳数据。