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心脏浦肯野纤维的强度-时间曲线:阈长度和电荷分布的影响

Strength-duration curves in cardiac Purkinje fibres: effects of liminal length and charge distribution.

作者信息

Fozzard H A, Schoenberg M

出版信息

J Physiol. 1972 Nov;226(3):593-618. doi: 10.1113/jphysiol.1972.sp009999.

Abstract
  1. Strength-duration curves for excitation in long point-stimulated sheep cardiac Purkinje fibres, where the charge distribution varies along the length of the fibre, are characterized by (a) a time constant which is short relative to the membrane time constant, (b) an apparent fall in charge threshold for short duration stimuli, (c) an apparent rise in voltage threshold as measured by an electrode at the point of current passage (see Dominguez & Fozzard, 1970).2. Strength-duration curves obtained from shortened segments of Purkinje fibres, where the charge distribution along the segment is fairly uniform after 2-3 msec, have much larger time constants.3. For stimulus durations longer than the 2-3 msec necessary to establish charge uniformity, strength-duration curves obtained from shortened segments of Purkinje fibres were well fitted by the Lapicque-Hill equation, I/I(rh) = 1 - exp (-t/tau).4. The differences in the time constants and apparent voltage thresholds for point-stimulated long fibres and uniformly charged short fibre segments could be explained by the liminal length concept of Rushton (1937). The liminal length concept, in its simplest form, states that a liminal length of fibre must be raised above a given voltage threshold in order for a propagated action potential to be generated.5. This concept predicts that the shorter the liminal length, the shorter the time constant of strength-duration curves in point-stimulated long fibres.6. Another conclusion of the model is that only those point-stimulated long fibres with longer liminal lengths would have a constant charge threshold for stimuli of the order of 0.2 tau.7. Liminal length was found by experiment and calculation to be about 0.1-0.2 lambda(m) in cardiac Purkinje fibres.8. The differences in behaviour with regards to excitation between the point-stimulated theoretical squid axon and the point-stimulated Purkinje fibre may be explained by assuming that the liminal length of the theoretical squid axon is several times larger than that of the Purkinje fibre.
摘要
  1. 在长点刺激的绵羊心脏浦肯野纤维中,兴奋的强度-时间曲线的特点是:(a)时间常数相对于膜时间常数较短;(b)短持续时间刺激的电荷阈值明显下降;(c)在电流通过点处用电极测量时,电压阈值明显上升(见多明格斯和福扎德,1970年)。2. 从浦肯野纤维缩短段获得的强度-时间曲线,在2-3毫秒后沿段的电荷分布相当均匀,其时间常数要大得多。3. 对于刺激持续时间长于建立电荷均匀性所需的2-3毫秒,从浦肯野纤维缩短段获得的强度-时间曲线能很好地用拉皮克-希尔方程拟合,即I/I(rh)=1 - exp(-t/tau)。4. 点刺激的长纤维和均匀充电的短纤维段在时间常数和表观电压阈值上的差异可以用拉什顿(1937年)的阈长度概念来解释。阈长度概念最简单的形式是,为了产生传播的动作电位,纤维的阈长度必须升高到给定的电压阈值以上。5. 这个概念预测,阈长度越短,点刺激长纤维中强度-时间曲线的时间常数就越短。6. 该模型的另一个结论是,只有那些阈长度较长的点刺激长纤维,对于约0.2τ的刺激才有恒定的电荷阈值。7. 通过实验和计算发现,心脏浦肯野纤维的阈长度约为0.1-0.2λ(m)。8. 点刺激的理论乌贼轴突和点刺激的浦肯野纤维在兴奋行为上的差异,可以通过假设理论乌贼轴突的阈长度比浦肯野纤维的阈长度大几倍来解释。

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