Membrane capacitance in frog cut twitch fibers mounted in a double vaseline-gap chamber.

In experiments on cut muscle fibers mounted in a double Vaseline-gap chamber, electrical measurements are usually made by measuring the voltage V1(t) in one end pool and by passing current I2(t) from the other end pool to the central pool, which is usually clamped to earth potential. The voltage in the current-passing end pool is denoted by V2(t). This article describes how the value of the holding current, Ih, and the values of delta V2(infinity)/delta V1(infinity) and delta I2(infinity)/delta V1(infinity) that are associated with a small change in V1(t) can be used to estimate the linear cable parameters rm, ri, and re in a cut fiber that has been equilibrated with a Cs-containing internal solution. rm, ri, and re represent, respectively, the resistance of the plasma membranes, the internal longitudinal resistance, and the external longitudinal resistance under the Vaseline seals, all for a unit length of fiber. The apparent capacitance, Capp, of the preparation is defined to equal integral of infinity 0 delta I2,tr(t) dt/delta V1(infinity), in which delta I2,tr(t) represents the transient component of current that is associated with a change in V1(t) of amplitude delta V1(infinity). A method is described to estimate cm, the capacitance of the plasma membranes per unit length of fiber, from Capp and the values of rm, ri, and re. In experiments carried out with a tetraethylammonium chloride (TEA.Cl) solution at 13-14 degrees C in the central pool, cm remained stable for as long as 3-4 h. The values of cm, 0.19 microF/cm on average, and their variation with fiber diameter are similar to published results from intact fibers. This article also describes the different pathways that are taken by the current that flows from the current-passing end pool to the central pool. Approximately two-thirds of delta I2,tr(t) flows across the capacitance of the plasma membranes in the central-pool region. The rest flows either across plasma membranes that are under the two Vaseline seals or directly from the current-passing end pool to the central pool, across the external longitudinal resistance under the Vaseline seal. [There is also a current that flows directly from the voltage-measuring end pool to the central pool but this does not contribute to delta I2,tr(t).]

Effects of manganese chloride, verapamil, and hypoxia on the rate-dependent increase in internal longitudinal resistance of rabbit myocardium

The effects of high rates of stimulation on the internal longitudinal restivity (Ri) and conduction velocity (θ) were studied on rabbit papillary muscle preparations using a silicon-oil chamber. Increasing the rate from 75 to 150/min caused Ri to rise and θ to decrease. The maximum rate of depolarization and action potential duration were also decreased. At a rate of 300/min the effects were more pronounced. Blockade of the slow inward current (Isi) and of the Na–Ca exchange by MnCl2 (5 mmol/L) did not prevent rate-induced changes in these variables. Verapamil (0.02 mmol/L) was also ineffective. Hypoxia [Formula: see text] at 75/min induced changes in Ri and θ which were similar to those recorded at 150/min under aerobic conditions. The effects of high rates of stimulation were potentiated under hypoxia. From the present results it is suggested that Isi and the Na–Ca exchange are not the main determinants of the rate-induced increase in Ri, which could be determined by other intracellular Ca-release mechanisms or by a decrease in myoplasmic pH.Key words: intercellular coupling, conduction velocity, calcium channel blockers.

A method for measurement of internal longitudinal resistance in papillary muscle

We have modified the original Weidmann method for the measurement of internal longitudinal resistance in ventricular muscle by using air rather than silicon oil to insulate guinea pig papillary muscles and by omitting the tetrodotoxin inactivation of a portion of the preparation and have examined the requirements necessary for the theoretical assumptions to be satisfied by this or similar preparations. We found a homogeneous depolarization wavefront beyond about 1 mm from the stimulating electrodes. The adequacy of the interelectrode spacing was identified by a discrete plateau in the extracellular potential recording. The extracellular resistance in this preparation was sensitive to changes in the volume of the extracellular compartment, which we manipulated by changing inflow and outflow rates, and to changes in total ionic content of the superfusate. Our results establish the essential nature of maintaining constant flow rates and total ionic content and suggest that changes in volume and ionic content of a restricted extracellular space could conceivably influence conduction in vivo.