Brust-Mascher I, Webb W W
School of Applied and Engineering Physics, Cornell University, Ithaca, New York 14853, USA.
Biophys J. 1998 Oct;75(4):1669-78. doi: 10.1016/S0006-3495(98)77609-X.
Intracellular calcium waves in fish keratocytes are induced by the application of electric field pulses with amplitudes between 55 and 120 V/cm and full width at half-maximum of 65-100 ms. Calcium concentrations were imaged using two-photon excited fluorescence microscopy (Denk et al., 1990 Science. 248:73-76; Williams et al. 1994 FASEB J. 8:804-813) and the ratiometric calcium indicator indo-1. The applied electric field pulses induced waves with fast calcium rise times and slow decays, which nucleated in the lamellipodium at the hyperpolarized side of the cells and, less frequently, at the depolarized side. The effectiveness of wave generation was determined by the change induced in the membrane potential, which is about half the field strength times the cell width in the direction of the field. Stimulation of waves began at voltage drops across the cell above 150 mV and saturated at voltage drops above 300 mV, where almost all cells exhibited a wave. Waves were not induced in low-calcium media and were blocked by the nonselective calcium channel blockers cobalt chloride and verapamil, but not by specific organic antagonists of voltage-sensitive calcium channel conductance. Thapsigargin stopped wave propagation in the cell body, indicating that calcium release from intracellular stores is necessary. Thus a voltage pulse stimulates Ca2+ influx through calcium channels in the plasma membrane, and if the intracellular calcium concentration reaches a threshold, release from intracellular stores is induced, creating a propagating wave. These observations and the measured parameters (average velocity approximately 66 micron/s and average rise time approximately 68 ms) are consistent with a wave amplification model in which[equation, see text] determines the effective diffusivity of the propagating molecules, D approximately 300 micron2/s (Meyer, 1991. Cell. 64:675-678).
通过施加幅度在55至120V/cm之间且半高宽为65 - 100ms的电场脉冲可诱导鱼角膜细胞内的钙波。使用双光子激发荧光显微镜(登克等人,1990年《科学》。248:73 - 76;威廉姆斯等人,1994年《美国实验生物学会联合会杂志》。8:804 - 813)和比率型钙指示剂indo - 1对钙浓度进行成像。施加的电场脉冲诱导出具有快速钙上升时间和缓慢衰减的波,这些波在细胞超极化侧的片状伪足中产生,较少在去极化侧产生。波产生的有效性由膜电位诱导的变化决定,该变化约为场强乘以细胞在电场方向上宽度的一半。当细胞上的电压降超过150mV时开始刺激波产生,在电压降超过300mV时达到饱和,此时几乎所有细胞都表现出波。在低钙培养基中不会诱导出波,且波会被非选择性钙通道阻滞剂氯化钴和维拉帕米阻断,但不会被电压敏感性钙通道电导的特异性有机拮抗剂阻断。毒胡萝卜素会阻止波在细胞体中的传播,表明从细胞内储存库释放钙是必要的。因此,电压脉冲刺激Ca2+通过质膜中的钙通道流入,如果细胞内钙浓度达到阈值,就会诱导从细胞内储存库释放钙,从而产生传播波。这些观察结果和测量参数(平均速度约为66微米/秒,平均上升时间约为68毫秒)与波放大模型一致,其中[方程,见原文]决定了传播分子的有效扩散率,D约为300微米2/秒(迈耶,1991年。《细胞》。64:675 - 678)。