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骨骼肌中电荷运动的介电成分。

Dielectric components of charge movements in skeletal muscle.

作者信息

Huang C L

出版信息

J Physiol. 1981;313:187-205. doi: 10.1113/jphysiol.1981.sp013658.

Abstract
  1. Voltage clamp experiments measured transients from 10 mV steps applied about different membrane potentials, VT. Their analysis employed the Fourier transform relationship between dielectric spectra of permittivity as a function of frequency, and the step transient admittance, as well as established methods. 2. The membrane capacitance measured between -85 mV and about -50 mV rose monotonically and was associated with simple decaying transients in both 'on' and 'off' steps. At more depolarized potentials the capacitance increased sharply and was associated with a charging current of complex form, before falling again beyond the transition potential. 3. Step-transient responses for dielectric analysis were sampled in the above voltage range. Dielectric spectra of the non-linear transients were obtained by subtracting Fourier transforms of transients at VC = -85 mV from test transforms at VT. 4. The imaginary transform coefficients represent a spectrum of dielectric loss against frequency. These showed two non-linear components. The q beta component formed a broad peak, when charge movements were simple monotonic decays. A sharp low-frequency q gamma peak became superimposed at particular voltages when charge-movement kinetics became complex. 5. In contrast, 'off' transients were simple monotonic relaxations. Their transforms showed only one dielectric loss peak, whose frequency was relatively voltage-independent when q gamma occurred in 'on' transforms. 6. Both altering holding potential from VH = -85 to -50 mV and adding 1 mM-tetracaine to the bathing solution reduced the dependence of capacitance on voltage. The non-linear polarization currents became simple monotonic relaxations at both the beginning and end of the voltage step. 7. It is concluded that charge movements are composed of at least two components: q beta, and the tetracaine and voltage-inactivated q gamma. Any causal relationship between q beta and q gamma and the membrane processes they might underlie would be expected to be complex.
摘要
  1. 电压钳实验测量了在不同膜电位VT施加10 mV阶跃时的瞬变情况。其分析采用了介电常数的介电谱(作为频率的函数)与阶跃瞬变电纳之间的傅里叶变换关系,以及既定方法。2. 在 -85 mV至约 -50 mV之间测量的膜电容单调上升,并且在“开启”和“关闭”阶跃中均与简单的衰减瞬变相关。在更正极化的电位下,电容急剧增加,并与复杂形式的充电电流相关,然后在超过转变电位后再次下降。3. 在上述电压范围内对用于介电分析的阶跃瞬变响应进行采样。通过从VT处的测试变换中减去VC = -85 mV时瞬变的傅里叶变换,获得非线性瞬变的介电谱。4. 虚数变换系数表示介电损耗随频率的谱。这些显示出两个非线性成分。当电荷运动为简单的单调衰减时,qβ成分形成一个宽峰。当电荷运动动力学变得复杂时,一个尖锐的低频qγ峰在特定电压下叠加出现。5. 相比之下,“关闭”瞬变是简单的单调弛豫。它们的变换仅显示一个介电损耗峰,当qγ出现在“开启”变换中时,其频率相对与电压无关。6. 将保持电位从VH = -85 mV改变为 -50 mV以及向浴液中添加1 mM丁卡因,均降低了电容对电压的依赖性。在电压阶跃的开始和结束时,非线性极化电流均变为简单的单调弛豫。7. 得出的结论是,电荷运动至少由两个成分组成:qβ,以及丁卡因和电压失活的qγ。qβ和qγ与它们可能构成基础的膜过程之间的任何因果关系预计都很复杂。

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