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2
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3
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Slow changes in membrane permeability and long-lasting action potentials in axons perfused with fluoride solutions.在用氟化物溶液灌注的轴突中,膜通透性的缓慢变化和持久的动作电位。
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本文引用的文献

1
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.
2
The dual effect of membrane potential on sodium conductance in the giant axon of Loligo.枪乌贼巨大轴突中膜电位对钠电导的双重作用。
J Physiol. 1952 Apr;116(4):497-506. doi: 10.1113/jphysiol.1952.sp004719.
3
Measurement of current-voltage relations in the membrane of the giant axon of Loligo.枪乌贼巨大轴突膜电流-电压关系的测量。
J Physiol. 1952 Apr;116(4):424-48. doi: 10.1113/jphysiol.1952.sp004716.
4
THE EFFECT OF DILUTING THE INTERNAL SOLUTION ON THE ELECTRICAL PROPERTIES OF A PERFUSED GIANT AXON.稀释内部溶液对灌流巨型轴突电特性的影响。
J Physiol. 1964 Apr;170(3):541-60. doi: 10.1113/jphysiol.1964.sp007348.
5
DEPENDENCE OF RESTING AND ACTION POTENTIALS ON INTERNAL POTASSIUM IN PERFUSED SQUID GIANT AXONS.灌注乌贼巨大轴突中静息电位和动作电位对细胞内钾离子的依赖性
J Physiol. 1963 Nov;169(1):91-115. doi: 10.1113/jphysiol.1963.sp007243.
6
Analysis of certain errors in squid axon voltage clamp measurements.鱿鱼轴突电压钳测量中某些误差的分析。
Biophys J. 1960 Nov;1(2):161-202. doi: 10.1016/s0006-3495(60)86882-8.
7
The action of calcium on the electrical properties of squid axons.钙对鱿鱼轴突电特性的作用。
J Physiol. 1957 Jul 11;137(2):218-44. doi: 10.1113/jphysiol.1957.sp005808.
8
A quantitative description of membrane current and its application to conduction and excitation in nerve.膜电流的定量描述及其在神经传导和兴奋中的应用。
J Physiol. 1952 Aug;117(4):500-44. doi: 10.1113/jphysiol.1952.sp004764.
9
The effect of internal sodium on the action potential in the presence of different internal anions.在存在不同细胞内阴离子的情况下,细胞内钠离子对动作电位的影响。
J Physiol. 1965 Dec;181(3):594-611. doi: 10.1113/jphysiol.1965.sp007785.
10
Slow changes in membrane permeability and long-lasting action potentials in axons perfused with fluoride solutions.在用氟化物溶液灌注的轴突中,膜通透性的缓慢变化和持久的动作电位。
J Physiol. 1970 Dec;211(3):707-28. doi: 10.1113/jphysiol.1970.sp009300.

与用氟化钠灌注的轴突中钠电导变化相关的速率常数。

Rate constants associated with changes in sodium conductance in axons perfused with sodium fluoride.

作者信息

Chandler W K, Meves H

出版信息

J Physiol. 1970 Dec;211(3):679-705. doi: 10.1113/jphysiol.1970.sp009299.

DOI:10.1113/jphysiol.1970.sp009299
PMID:5501057
原文链接:https://pmc.ncbi.nlm.nih.gov/articles/PMC1396074/
Abstract
  1. Membrane currents during step depolarizations were measured in axons which were perfused with 300 mM-NaF and placed in K-free artificial sea-water, -0.3-4 degrees C. The Na conductance was fitted by the modified Hodgkin-Huxley model, g(Na) = g(Na)m(3)(h(1) + h(2)). Changes in h(1) and h(2) were assumed to follow [Formula: see text] where x represents the inactive state.2. The rate constants and steady-state values for m were in agreement with the Hodgkin-Huxley equations except that the experimental relationship of m(infinity) (3) against V was shifted 10-15 mV in the negative direction. This discrepancy, which was not found in an experiment with choline sea-water, can be explained on the basis of a resistance in series with the membrane between the voltage measuring electrodes.3. At 0 degrees C the rate constants (in msec(-1)) associated with changes in h(1) and h(2) were fitted using the following equations: beta(h1) = 0.5/{exp [- (V + 32)/10] + D(1)exp (- V/V(1))}, alpha(h2) = pexp (V/V(2)), beta(h2) = pexp (V/V(2) - V/23.5) + pD(2), with the condition that at 0 mV, (alpha(h2) + beta(h2)) = p(D(2) + 2) = 0.55 msec(-1). The experiments gave average values D(1) = 3.6, V(1) = 240 mV, p = 0.08 msec(-1) and V(2) = 70 mV. The average value of g(Na) was 66 mmho/cm(2).4. At negative voltages where m(infinity) (3) against V is steep, the points for beta(h1) and alpha(h2)/beta(h2) from axons in Na sea-water were not fitted well by the above equations whereas data from an axon in choline sea-water were. These discrepancies can be explained on the basis of a series resistance.5. Measurements made at 16-17 degrees C indicated that g(Na) has a Q(10) of 1.6, tau(m) (-1) a Q(10) of 2.8 and beta(h1) a Q(10) of 3.5. The ratio alpha(h2)/beta(h2) was decreased relative to the value at 0 degrees C and could be fitted by using Q(10) = 0.6.6. Measurements made with 250 mM-NaF + 50 mM-KF inside gave rate constants which were very similar to those obtained with 300 mM-NaF. Perfusion with 300 mM-KF appeared to double the value of beta(h1), relative to that obtained with 300 mM-NaF, and to reduce alpha(h2)/beta(h2) by about half.7. The voltage dependence of alpha(h2) makes it likely that following depolarization recovery from the inactive state x occurs via x --> h(1) rather than x --> h(2) --> h(1).
摘要
  1. 在灌注了300 mM氟化钠并置于无钾人工海水中、温度为-0.3至4摄氏度的轴突中测量了阶跃去极化期间的膜电流。钠电导由修正的霍奇金-赫胥黎模型拟合,即g(Na)=g(Na)m³(h₁+h₂)。假设h₁和h₂的变化遵循[公式:见原文],其中x代表失活状态。

  2. m的速率常数和稳态值与霍奇金-赫胥黎方程一致,只是m(∞)³与V的实验关系在负方向上偏移了10至15 mV。这种差异在胆碱海水实验中未发现,可基于电压测量电极之间与膜串联的电阻来解释。

  3. 在0摄氏度时,与h₁和h₂变化相关的速率常数(单位为毫秒⁻¹)使用以下方程拟合:β(h₁)=0.5/{exp[- (V + 32)/10]+D₁exp(- V/V₁)},α(h₂)=pexp(V/V₂),β(h₂)=pexp(V/V₂ - V/23.5)+pD₂,条件是在0 mV时,(α(h₂)+β(h₂))=p(D₂ + 2)=0.55毫秒⁻¹。实验得出的平均值为D₁ = 3.6,V₁ = 240 mV,p = 0.08毫秒⁻¹,V₂ = 70 mV。g(Na)的平均值为66毫姆欧/平方厘米。

  4. 在m(∞)³对V陡峭的负电压下,来自钠海水中轴突的β(h₁)和α(h₂)/β(h₂)的数据点不能很好地用上述方程拟合,而来自胆碱海水中轴突的数据则可以。这些差异可基于串联电阻来解释。

  5. 在16至17摄氏度下进行的测量表明,g(Na)的Q₁₀为1.6,τm⁻¹的Q₁₀为2.8,β(h₁)的Q₁₀为3.5。α(h₂)/β(h₂)的比值相对于0摄氏度时的值有所降低,并且可以用Q₁₀ = 0.6来拟合。

  6. 内部灌注250 mM氟化钠+50 mM氟化钾时得到的速率常数与用300 mM氟化钠时得到的非常相似。相对于用300 mM氟化钠时得到的值,灌注300 mM氟化钾似乎使β(h₁)的值增加了一倍,并使α(h₂)/β(h₂)降低了约一半。

  7. α(h₂)的电压依赖性使得去极化后从失活状态x恢复可能通过x→h₁而不是x→h₂→h₁发生。