Sharma Vinod, Tung Leslie
Department of Biomedical Engineering, The Johns Hopkins University, 720 Rutland Avenue, Baltimore, MD 21205, USA.
J Physiol. 2002 Jul 15;542(Pt 2):477-92. doi: 10.1113/jphysiol.2001.013197.
Changes in transmembrane voltage (V(m)) of cardiac cells during electric field stimulation have a complex spatial- and time-dependent behaviour that differs significantly from electrical stimulation of space-clamped membranes by current pulses. A multisite optical mapping system was used to obtain 17 or 25 microm resolution maps of V(m) along the long axis of guinea-pig ventricular cells (n = 57) stained with voltage-sensitive dye (di-8-ANEPPS) and stimulated longitudinally with uniform electric field (2, 5 or 10 ms, 3-62 V cm(-1)) pulses (n = 201). The initial polarizations of V(m) responses (V(mr)) varied linearly along the cell length and reversed symmetrically upon field reversal. The remainder of the V(m) responses had parallel time courses among the recording sites, revealing a common time-varying signal component (V(ms)). V(ms) was depolarizing for pulses during rest and hyperpolarizing for pulses during the early plateau phase. V(ms) varied in amplitude and time course with increasing pulse amplitude. Four types of plateau response were observed, with transition points between the different responses occurring when the maximum polarization at the ends of the cell reached values estimated as 60, 110 and 220 mV. Among the cells that had a polarization change of > 200 mV at their ends (for fields > 45 V cm(-1)), some (n = 17/25) had non-parallel time courses among V(m) recordings of the various sites. This implied development of an intracellular field (E(i)) that was found to increase exponentially with time (tau = 7.2 +/- 3.2 ms). Theoretical considerations suggest that V(ms) represents the intracellular potential (phi(i)) as well as the average polarization of the cell, and that V(mr) is the manifestation of the extracellular potential gradient resulting from the field stimulus. For cells undergoing field stimulation, phi(i) acts as the cellular physiological state variable and substitutes for V(m), which is the customary variable for space-clamped membranes.
在电场刺激期间,心脏细胞跨膜电压(V(m))的变化具有复杂的空间和时间依赖性行为,这与通过电流脉冲对空间钳制膜进行电刺激有显著差异。使用多部位光学映射系统获取了用电压敏感染料(di-8-ANEPPS)染色的豚鼠心室细胞(n = 57)沿长轴的17或25微米分辨率的V(m)图谱,并用电场均匀(2、5或10毫秒,3 - 62伏/厘米(-1))脉冲进行纵向刺激(n = 201)。V(m)反应(V(mr))的初始极化沿细胞长度呈线性变化,并在电场反转时对称反转。V(m)反应的其余部分在记录部位之间具有平行的时间进程,揭示了一个共同的随时间变化的信号成分(V(ms))。对于静息期的脉冲,V(ms)是去极化的,而对于早期平台期的脉冲,V(ms)是超极化的。V(ms)的幅度和时间进程随脉冲幅度增加而变化。观察到四种类型的平台反应,当细胞两端的最大极化达到估计为60、110和220毫伏的值时,不同反应之间出现转变点。在其两端极化变化> 200毫伏的细胞中(对于电场> 45伏/厘米(-1)),一些(n = 17/25)在各个部位的V(m)记录之间具有非平行的时间进程。这意味着细胞内电场(E(i))的发展,发现其随时间呈指数增加(时间常数τ = 7.2 +/- 3.2毫秒)。理论考虑表明,V(ms)代表细胞内电位(φ(i))以及细胞的平均极化,并且V(mr)是由场刺激产生的细胞外电位梯度的表现。对于接受场刺激的细胞,φ(i)作为细胞生理状态变量,替代了V(m),而V(m)是空间钳制膜的常用变量。