Gene/Protein Disease Symptom Drug Enzyme Compound
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Query: UMLS:C0019829 (Hodgkin's disease)
 30,247 document(s) hit in 31,850,051 MEDLINE articles (0.00 seconds)

1. Voltage- and time-dependent outward currents were recorded from relaxed enzymatically isolated smooth muscle cells from the rabbit left descending coronary artery using a single pipette voltage clamp technique. The calcium-activated potassium current was blocked by inclusion of EGTA in the pipette solution and CdCl2 in the extracellular bath. 2. Outward currents were elicited with depolarizing voltage steps to potentials positive to -20 mV. Long (5 s) voltage steps revealed slow inactivation of the current with a time constant of nearly 3 s at +60 mV. Potassium was identified as the predominant charge carrier by reversal potential measurements in potassium substitution experiments. 3. The results of kinetic analyses compared favourably with the Hodgkin-Huxley model for a delayed rectifier with some deviations. The sigmoid current onset was best fitted by raising the activation variable (n) to the second power. Deactivation tail currents were consistently found to be comprised of two exponential components. The kinetics of activation and deactivation were strongly voltage-dependent from -80 to +60 mV. 4. Envelope of tails experiments showed that the scaled tail current amplitudes followed the kinetic behaviour of current activation. The contribution of each of the two exponential tail components was also measured in these experiments. They did not reveal kinetically separable currents, nor were they differentially altered by 4-aminopyridine (4-AP), tetraethylammonium (TEA), or elevated [K+]o. 5. The steady-state voltage-dependence curves for both activation and inactivation were well fitted by a Boltzmann distribution with V1/2 = -5.60 mV and k = -8.66 mV for n infinity act and V1/2 = -24.20 mV and k = 5.16 mV for n infinity act. Super-imposition of the two curves revealed a 'window' of voltage where channels are available for activation without completely inactivating. 6. Neither of the commonly used potassium channel blockers, TEA or 4-AP, were particularly effective blockers of IK, reducing current by only 50-70% at an extracellular concentration of 10 mM. TEA block was mildly voltage-dependent and was more effective in reducing current towards the end of a 500 ms depolarization. 4-AP, on the other hand, demonstrated considerable voltage-dependence and preferentially reduced early currents. 7. Outward currents recorded from guinea-pig and human coronary artery myocytes under the same conditions as in the rabbit cell experiments displayed similar characteristics.(ABSTRACT TRUNCATED AT 400 WORDS)
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PMID:A voltage-dependent potassium current in rabbit coronary artery smooth muscle cells. 191 87

1. Whole-cell and patch-clamp techniques (Hamill, Marty, Neher, Sakmann & Sigworth, 1981) have been used to make quantitative measurements of the transient inward sodium current (INa) in single cells from bullfrog atrium. This preparation is particularly suitable for the study of INa: (i) the current density is relatively low, (ii) the cells lack a transverse tubule system, (iii) isolated myocytes can be maintained at reduced temperatures (approximately 8-12 degrees C); therefore kinetics can be studied quantitatively. 2. INa was pharmacologically and kinetically isolated from other transmembrane currents by blocking ICa with CdCl2 (0.2-0.5 mM) or LaCl3 (5 x 10(-6) M), and by using only relatively short voltage-clamp depolarizations which did not activate IK (the delayed rectifier). 3. The voltage dependence of INa in bullfrog atrium is similar to that in amphibian node of Ranvier or fast skeletal muscle. The threshold for activation is approximately -50 mV. The peak of the INa vs. membrane potential relation is near -5 to -10 mV. The reversal potential in 'normal' (115 mM-Na+) Ringer solution is +59.0 mV (S.D. +/- 3.4, n = 10). Reduction of external Na+ concentration to one-third of normal resulted in an approximately -27 mV shift of the reversal potential, close to that expected for a highly Na+-selective conductance. 4. Steady-state inactivation of INa (h infinity), measured with a conventional two-pulse voltage-clamp protocol, spanned the membrane potential range from -90 to -50 mV. The potential dependence of h infinity was well described by a single Boltzmann function with half-inactivation at -71 mV and maximum slope of 6.0 mV. 5. Steady-state activation of INa (m infinity) was determined from fits of INa records to a Hodgkin-Huxley model. The potential dependence of m infinity was fitted to a Boltzmann function with half-activation at -33 mV and maximum slope of 9.5 mV. Thus at temperatures around 10 degrees C there was very little overlap of the m infinity and h infinity curves, and only very small steady-state 'window' currents are predicted. 6. The activation time constant, tau m, had a 'bell-shaped' dependence on membrane potential. The peak value of tau m was about 4.2 ms, at a membrane potential of -35 mV (9 degrees C). 7. The time course of inactivation of INa was consistently better described by the sum of two exponentials than by one exponential.(ABSTRACT TRUNCATED AT 400 WORDS)
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PMID:Sodium current in single cells from bullfrog atrium: voltage dependence and ion transfer properties. 245 Oct 6