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

机译:心脏浦肯野纤维的强度—持续时间曲线:门限长度和电荷分布的影响

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摘要

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/Irh = [1 — exp (—t/τ)]-1.4. 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 τ.7. Liminal length was found by experiment and calculation to be about 0·1-0·2 λm 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.
机译:1.强度-长点刺激的绵羊心脏Purkinje纤维的激发持续时间曲线,其电荷分布沿纤维长度变化,其特征在于(a)一个相对于膜时间常数短的时间常数,( b)短时刺激的充电阈值明显下降,(c)电极在电流通过点测得的电压阈值明显上升(见Dominguez和Fozzard,1970)2。强度—从Purkinje纤维的较短部分中获得的持续时间曲线,其中在2-3毫秒后沿该部分的电荷分布相当均匀,具有较大的时间常数。3。对于长于建立电荷均匀性所需的2-3毫秒的刺激持续时间,通过拉比克希尔函数可以很好地拟合从较短的Purkinje纤维段获得的强度-持续时间曲线,I / Irh = [1-exp(-t /τ )] -1 .4。点激励长纤维和均匀充电的短纤维段的时间常数和视在电压阈值的差异可以用Rushton(1937)的极限长度概念来解释。最简单形式的边缘长度概念指出,必须将纤维的边缘长度提高到给定的电压阈值之上,以便产生传播的动作电位。5。这个概念预言,门槛长度越短,强度的时间常数就越短-点刺激长纤维的持续时间曲线6。该模型的另一个结论是,只有那些具有较长门襟长度的点刺激长纤维才会对刺激的电荷阈值保持恒定,约为0·2τ.7。通过实验和计算发现,心脏浦肯野纤维的束线长度约为0·1-0·2λm。8。点刺激的理论鱿鱼轴突和点刺激的浦肯野纤维之间在激发方面的行为差异可以通过假设理论鱿鱼轴突的极限长度比浦肯野纤维大几倍来解释。

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