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2
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本文引用的文献

1
POTENTIAL, IMPEDANCE, AND RECTIFICATION IN MEMBRANES.膜的电位、阻抗和整流。
J Gen Physiol. 1943 Sep 20;27(1):37-60. doi: 10.1085/jgp.27.1.37.
2
MEMBRANE POTENTIAL OF THE SQUID GIANT AXON DURING CURRENT FLOW.鱿鱼巨大轴突在电流流动时的膜电位。
J Gen Physiol. 1941 Mar 20;24(4):551-63. doi: 10.1085/jgp.24.4.551.
3
Space Charge Regions in Fixed Charge Membranes and the Associated Property of Capacitance.固定电荷膜中的空间电荷区域及其相关电容特性。
Biophys J. 1962 Mar;2(2 Pt 1):179-98. doi: 10.1016/s0006-3495(62)86848-9.
4
The effect of sodium ions on the electrical activity of giant axon of the squid.钠离子对鱿鱼巨大轴突电活动的影响。
J Physiol. 1949 Mar 1;108(1):37-77. doi: 10.1113/jphysiol.1949.sp004310.
5
Branching dendritic trees and motoneuron membrane resistivity.分支树突状结构与运动神经元膜电阻
Exp Neurol. 1959 Nov;1:491-527. doi: 10.1016/0014-4886(59)90046-9.
6
AN ELECTROGENIC SODIUM PUMP IN SNAIL NERVE CELLS.蜗牛神经细胞中的一种生电钠泵。
Comp Biochem Physiol. 1965 Jan;14:167-83. doi: 10.1016/0010-406x(65)90017-4.
7
THE RUBIDIUM AND POTASSIUM PERMEABILITY OF FROG MUSCLE MEMBRANE.青蛙肌肉膜的铷和钾通透性
J Physiol. 1964 Dec;175(1):134-59. doi: 10.1113/jphysiol.1964.sp007508.
8
[ELECTRICAL CHARACTERISTICS OF THE SURFACE MEMBRANE OF GIANT NERVE CELLS OF HELIX POMATIA].[圆田螺巨神经细胞表面膜的电学特性]
Fiziol Zh SSSR Im I M Sechenova. 1963 Dec;49:1468-74.
9
Membrane potential transients and membrane time constant of motoneurons.运动神经元的膜电位瞬变和膜时间常数
Exp Neurol. 1960 Oct;2:503-32. doi: 10.1016/0014-4886(60)90029-7.
10
[Anode opening excitations of single Ranvier nodes].[单个郎飞结的阳极开口激发]
Pflugers Arch Gesamte Physiol Menschen Tiere. 1958;267(5):524-31. doi: 10.1007/BF00361739.

温度和离子对软体动物神经元电流-电压关系及电学特性的影响。

The effects of temperature and ions on the current-voltage relation and electrical characteristics of a molluscan neurone.

作者信息

Marmor M F

出版信息

J Physiol. 1971 Nov;218(3):573-98. doi: 10.1113/jphysiol.1971.sp009634.

DOI:10.1113/jphysiol.1971.sp009634
PMID:5133949
原文链接:https://pmc.ncbi.nlm.nih.gov/articles/PMC1331602/
Abstract
  1. Current-voltage relations were generated in the Anisodoris giant neurone (G cell) by either current pulses or slow biphasic current ramps.2. Inward-going rectification occurred during hyperpolarization at warm temperatures (10-15 degrees C), but not at cold temperatures (0-5 degrees C) or in the absence of external K.3. Replacing external K with Rb eliminated inward-going rectification in the warm, but produced it in the cold. The removal of external Na, Cl or Ca had no effect upon inward-going rectification.4. At cold temperatures the I-V relation was linear when generated by current pulses, but was non-linear in accordance with the constant field hypothesis when generated by current ramps.5. A high conductance state developed when the membrane was hyperpolarized beyond a critical potential (approximately - 130 mV in the cold, and - 110 mV in the warm) which was dependent upon external Ca, but not upon K, Na or Cl.6. Hysteresis was observed in the ramp-generated I-V relation whenever the cell was polarized into the high conductance state.7. Rectification and the high conductance state appear to involve different mechanisms within the membrane. However, both are dependent upon absolute membrane potential and not the resting potential.8. The axonal-somatic conductance ratio for the G cell was calculated to be between 2 and 10.9. The membrane time constant (200-100 msec) and specific resistance (0.1-1.5 x 10(6) Omega cm(2)) varied with temperature, membrane potential, and external ions in a manner that correlated with changes in the shape of the I-V relation. In addition, the resistance was dependent upon external Ca.10. The K permeability (P(K)), measured during inhibition of inwardgoing rectification, was independent of temperature and membrane potential. However, P(Na) increased with warming.11. The specific capacitance was calculated to be 0.5-1.0 muF/cm(2). The capacitance increased slightly with warming, but was independent of membrane potential and unaffected by reductions in external K or Na.
摘要
  1. 通过电流脉冲或缓慢的双相电流斜坡在异鳃海兔巨神经元(G细胞)中产生电流-电压关系。

  2. 在温暖温度(10 - 15摄氏度)下超极化期间出现内向整流,但在寒冷温度(0 - 5摄氏度)下或无外部钾时不出现。

  3. 用铷替代外部钾消除了温暖时的内向整流,但在寒冷时产生了内向整流。去除外部钠、氯或钙对内向整流没有影响。

  4. 在寒冷温度下,由电流脉冲产生时I-V关系是线性的,但由电流斜坡产生时根据恒定场假说是非线性的。

  5. 当膜超极化超过临界电位(寒冷时约为 - 130 mV,温暖时约为 - 110 mV)时会出现高电导状态,这取决于外部钙,而不取决于钾、钠或氯。

  6. 每当细胞极化到高电导状态时,在斜坡产生的I-V关系中观察到滞后现象。

  7. 整流和高电导状态似乎涉及膜内不同机制。然而,两者都取决于绝对膜电位而非静息电位。

  8. G细胞的轴突-胞体电导比经计算在2到10之间。

  9. 膜时间常数(200 - 100毫秒)和比电阻(0.1 - 1.5×10⁶欧姆·厘米²)随温度、膜电位和外部离子而变化,其方式与I-V关系形状的变化相关。此外,电阻取决于外部钙。

  10. 在抑制内向整流期间测量的钾渗透率(P(K))与温度和膜电位无关。然而,P(Na)随温度升高而增加。

  11. 比电容经计算为0.5 - 1.0微法/厘米²。电容随温度升高略有增加,但与膜电位无关,且不受外部钾或钠减少的影响。