Movement of labelled decamethonium in muscle fibres of the rat

High acetylcholine concentrations cause rapid inactivation before fast desensitization in nicotinic acetylcholine receptors from Torpedo

By using both a 3 to 4 ms quenched-86Rb+ flux assay and native acetylcholine receptor (AChR) rich electroplaque vesicles on which 50-60% of acetylcholine activation sites were blocked with alpha-BTX, we determined apparent rates of agonist-induced inactivation in AChR from Torpedo under conditions where measured flux response was directly proportional to initial 86Rb+ influx rate. Inactivation kinetics with acetylcholine in both the activating range (10 microM-10 mM) and the self-inhibiting range (15-100 mM) were measured at 4 degrees C. In the presence of 10 microM-1 mM acetylcholine, inactivation is characterized by a single exponential rate constant, kd (fast desensitization). Plots of kd vs. acetylcholine concentration display maximum kds [kd(max)] of 6.6-8.0 s-1, half-maximal kd at 102 +/- 16 microM, and a Hill coefficient of 1.6 +/- 0.3, closely paralleling the initial ion flux response of AChR. Thus, fast desensitization probably occurs from a doubly-liganded preopen state or the open channel state. In the self-inhibiting acetylcholine concentration range, inactivation is biphasic. A "rapid inactivation" phase is complete within 30 ms, followed by fast desensitization at a rate close to kd(max). Both the rate and extent of rapid inactivation increase with acetylcholine concentration, indicating that acetylcholine binds to its self-inhibition site with apparent kon approximately equal to 10(3) M-1s-1 and koff approximately equal to 40 s-1. This slow kon suggests either hindered access to the inhibitory allosteric site or that a fast binding step is followed by a slower conformational change leading to channel inhibition. Overall, our data suggest that acetylcholine binds preferentially to its inhibitory site when the receptor is in the open-channel conformation and that fast desensitization can occur from all multiple-liganded states.

The permeability of the endplate channel to organic cations in frog muscle

The relative permeability of endplate channels to many organic cations was determined by reversal-potential criteria. Endplate currents induced by iontophoretic "puffs" of acetylcholine were studied by a Vaseline gap, voltage clamp method in cut muscle fibers. Reversal potential changes were measured as the NaCl of the bathing medium was replaced by salts of organic cations, and permeability ratios relative to Na+ ions were calculated from the Goldman-Hodgkin-Katz equation. 40 small monovalent organic cations had permeability ratios larger than 0.1. The most permeant including NH4+, hydroxylamine, hydrazine, methylamine, guanidine, and several relatives of guanidine had permeability ratios in the range 1.3--2.0. However, even cations such as imidazole, choline, tris(hydroxymethyl)aminomethane, triethylamine, and glycine methylester were appreciably permeant with permeability ratios of 0.13--0.95. Four compounds with two charged nitrogen groups were also permeant. Molecular models of the permeant ions suggest that the smallest cross-section of the open pore must be at least as large as a square, 6.5 A x 6.5 A. Specific chemical factors seem to be less important than access or friction in determining the ionic selectivity of the endplate channel.

The extracellular compartments of frog skeletal muscle

1. Detailed studies of solute efflux from frog sartorius muscle and single muscle fibres were carried out in order to characterize a 'special region' (Harris, 1963) in the extracellular space of muscle and determine whether this 'special region' is the sarcoplasmic reticulum. 2. The efflux of radioactive Na, Cl, glusose, 3-O-methylglucose, xylose, glycine, leucine, cycloleucine, Rb, K, inulin (mol. wt. 5000) and dextran (mol. wt. 17,000) from previously loaded muscles was studied. In all cases except dextran the curve had three components, a rapid (A) component which could be equated with efflux from the extracellular space proper, a slow (C) component representing cellular solute and an intermediate (B) component. The distribution space for the B component was 8% of muscle volume in summer frogs and 12% in winter frogs and appeared to be equal for all compounds studied. We tested the hypothesis that the B component originated from the sarcoplasmic reticulum. 3. The C component was missing from the dextran curves. Both dextran and inulin entered the compartment of origin of the B component (compartment B) to the same extent as small molecules. 4. For all compounds studies, the efflux rate constant for the A component could be predicted from the diffusion coefficient. For the B component the efflux rate constant was 6--10 times slower than that for the A component but was still proportional to the diffusion coefficient for the solute in question. 5. When Na and sucrose efflux from single fibres was followed, a B component was usually observed. The average distribution space for this component was small, averaging 1.5% of fibre volume. There was no difference between the average efflux rate constants for Na and sucrose. 6. In an appendix, the constraints placed on the properties of a hypothetical channel between the sarcoplasmic reticulum and the T-system by the linear electrical parameters of frog skeletal muscle are derived. It is shown that the conductance of such a channel must be less than 0.06 x 10(-3) mohs/cm2 of fibre membrane. 7. The conductance between compartment B and the extracellular space can be calculated from the efflux rate constants for Na, K and Cl. The value obtained was 5 x 10(-3) mhos/cm2 of fibre membrane or 100 times the limiting value for the conductance of the T-SR junction. 8. The finding that there is a B component in the efflux curves for large molecular weight substances like inulin and dextran and the small size of the B component in efflux curves from single muscle fibres indicate that the 'speical region' of the extra-cellular space of frog muscle is not the sarcoplasmic reticulum. This conclusion is confirmed by a calculation of the conductance between the B compartment and the extracellular space. The value obtained is incompatible with predicted electrical properteis of the SR-T-tubule junction...

Sodium entry in rat diaphragm induced by depolarizing drugs

1. An increased uptake of labelled sodium was found in the end-plate region of rat diaphragm following brief exposure to solution containing (24)Na plus carbachol (100 muM), with a wash in inactive saline. Tetrodotoxin (0.1 muM) was also present. Comparable results were obtained with decamethonium and suberyldicholine.2. With carbachol (100 muM) the influx of labelled sodium at the end-plate region was increased by a factor of at least three as compared with that at the end of the fibres.3. After entry the labelled sodium spread along the fibres with an apparent diffusion coefficient which was half that expected in the external solution.4. The dose-response curve for the effect of carbachol gave a half-maximal value of 72 muM.5. In muscles depolarized by potassium methyl sulphate the effect of carbachol on the entry of sodium was reduced although demonstrable.6. The entry of labelled sodium at the end-plate was maintained during prolonged exposure to carbachol (100 muM) or decamethonium (100 muM).7. The rate of entry of (24)Na obtained with carbachol, after corrections for the wash, was estimated as 1.5 x 10(3) ions channel(-1) sec(-1), measured over a period of 15 sec.8. Labelled decamethonium and labelled carbachol also accumulated at the end-plate region. After extrapolation to allow for the effects of the wash the entry of decamethonium when expressed as a clearance (pl. mg(-1) sec(-1)) was comparable to that of sodium, as expected if decamethonium and sodium enter through the same channels.