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Query: UMLS:C0019829 (Hodgkin's disease)
 30,247 document(s) hit in 31,850,051 MEDLINE articles (0.00 seconds)

The inward sodium current in cardiac muscle is difficult to study by voltage clamp methods, so various indirect experimental measures have been used to obtain insight into its characteristics. These methods depend on the relationship between maximal upstroke velocity of the action potential (Vmax) and the sodium current (INa), usually defined in terms of the Hodgkin-Huxley model. These relationships were explored using an adaptation of this model to cardiac Purkinje fibers. In general Vmax corresponded to INa, and it could be used to determine the relationship of membrane potential to GNa, and h infinity. The results, however, depended on the method of stimulation of the action potential, and an optimal stimulation method was determined. A commonly used experimental technique called "membrane responsiveness" was shown to distort seriously the properties of steady-state gating inactivation that is supposed to measure. Estimation of the changes in maximal sodium conductance, such as those produced by tetrodotoxin (TTX), would be accurately measured. Some experimental results have indicated a voltage-dependent effect of TTX. Characteristics of the measures of TTX effect under those conditions were illustrated. In summary, calculations with a model of the cardiac Purkinje fiber action potential provide insight into the accuracy of certain experimental methods using maximal upstroke velocity as a measure of INa, and cast doubt on other experimental methods, such as membrane responsiveness.
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PMID:The relation of Vmax to INa, GNa, and h infinity in a model of the cardiac Purkinje fiber. 26 97

1. Sodium currents (INa) and asymmetrical displacement currents (ID) were measured in the same nerve fibres from Rana esculenta under similar conditions. 2. For exploring possible kinetic and steady state relations between INa and ID the following quantities were compared: (i) the activation of the sodium channels and (ii) the charge displacement of ID. 3. The delay of sodium activation increased after hyperpolarization. A corresponding effect on the displacement of charge was not observed. 4. Upon a small depolarization sodium activation rose slower than the displacement of charge, whereas at large depolarizations sodium activation reached a steady level before the charge displacement. 5. Upon repolarization to various levels between -52 and 12 mV relative to the resting potential, the ratio between the time constants of charge displacement and of sodium tail current varied between 3 and 1. 6. In the steady state the sodium activation was one half at about the same potential as the charge displacement but exhibited a clearly steeper voltage dependence. 7. Blocage of sodium channels with tetrodotoxin did not affect the asymmetrical displacement current. Replacing a part of external Na by tris did not alter the sodijm activation process. 8. The results indicate that the asymmetrical displacement of charge may reflect states of the gating mechanism in sodium channels but cannot be considered as a correlate of the Hodgkin Huxley m variable.
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PMID:Asymmetrical displacement current and its relation with the activation of sodium current in the membrane of frog myelinated nerve. 108 37

The origin of the action potential in neurones has yet to be answered satisfactorily for most cells. We present here a five-conductance model of the somatic membrane of the mature and intact sympathetic neurone studied in situ in the isolated rat superior cervical ganglion under two-electrode voltage-clamp conditions. The neural membrane hosts five separate types of voltage-dependent ionic conductances, which have been isolated at 37 degrees C by using simple manipulations such as conditioning-test protocols and external ionic pharmacological treatments. The total current could be separated into two distinct inward components: (1) the sodium current, INa, and (2) the calcium current, ICa; and three outward components: (1) the delayed rectifier, IKV, (2) the transient IA, and (3) the calcium-dependent IKCa. Each current has been kinetically characterized in the framework of the Hodgkin-Huxley scheme used for the squid giant axon. Continuous mathematical functions are now available for the activation and inactivation (where present) gating mechanisms of each current which, together with the maximum conductance values measured in the experiments, allow for a satisfactory reconstruction of the individual current tracings over a wide range of membrane voltage. The results obtained are integrated in a full mathematical model which, by describing the electrical behaviour of the neurone under current-clamp conditions, leads to a quantitative understanding of the physiological firing pattern. While, as expected, the fast inward current carried by Na+ contributes to the depolarizing phase of the action potential, the spike falling phase is more complex than previous explanations. IKCa, with a minor contribution from IKV, repolarizes the neurone only under conditions of low cell internal negativity. Their role becomes less pronounced in the voltage range negative to -60 mV, where membrane repolarization allows IA to deinactivate. In the spike arising from these voltage levels the membrane repolarization is mainly sustained by IA, which proves to be the only current sufficiently fast and large enough to recharge the membrane capacitor at the speed observed during activity. Different modes of firing coexist in the same neurone and the switching from one to another is fast and governed by the membrane potential level, which makes the selection between the different voltage-dependent channel systems. The neurone thus seems to be prepared to operate within a wide voltage range; the results presented indicate the basic factors underlying the different discrete behaviours.
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PMID:A five-conductance model of the action potential in the rat sympathetic neurone. 205 76

Gating currents (Ig) were recorded in single canine cardiac Purkinje cells at 10-12 degrees C. Ig characteristics corresponded closely to macroscopic INa characteristics and appeared to exhibit little contamination from other voltage-gated channels. Charge density predicted by peak INa was 0.14-0.22 fC micron -2 and this compared well with the measured value of 0.19 +/- 0.10 fC micron -2 (SD; n = 28). The charge-voltage relationship rose over a voltage similar to the peak INa conductance curve. The midpoints of the two relationships were not significantly different although the conductance curve was 1.5 +/- 0.3 (SD; n = 9) times steeper. Consistent with this observation, which predicted that a large amount of the gating charge would be associated with transitions close to the open state, an analysis of activation from Hodgkin-Huxley fits to the macroscopic currents showed that tau m corresponded well with a prominent component of Ig. Ig relaxations fitted two exponentials better than one over the range of voltages in which Na channels were activated. When the holding potential was hyperpolarized, relaxation of Ig during step depolarizations to 0 mV was prolonged but there was no substantial increase in charge, further suggesting that early closed-state transitions are less in charge, further suggesting that early closed-state transitions are less voltage dependent. The single cardiac Purkinje cell appears to be a good candidate for combining Ig and single-channel measurements to obtain a kinetic description of the cardiac Na channel.
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PMID:Gating currents associated with Na channels in canine cardiac Purkinje cells. 215 92

Action potentials, macroscopic ionic currents and single channel currents were recorded from growth cones of Aplysia right upper quadrant (r.u.q.) cells in culture, using the patch-clamp technique. Recordings were obtained from both intact growth cones and from growth cones that had been mechanically isolated from the rest of the neurone. In current-clamp mode, greater than half of the isolated growth cones display an all-or-none action potential when depolarized above 0 mV with outward current pulses. The remaining growth cones display only a graded depolarization that is unaffected by tetrodotoxin (TTX). In whole-cell voltage clamp almost all isolated growth cones display a rapidly activating and inactivating inward current followed by a delayed outward current in response to depolarizations positive to -20 mV. The rapid inward current reverses direction at around +70 to +80 mV and is completely suppressed by 100 microM-TTX, which suggests that this current is carried by the fast Hodgkin-Huxley sodium current channels. The delayed outward current appears to result from the activation of both the delayed rectifier potassium current, IK, and the calcium-activated potassium current, IC. The growth cones do not display any prominent early transient outward current, IA. The sodium current, INA, was studied in isolation by substituting caesium for potassium ions in the pipette solution. INa is half-inactivated at a holding potential of -36 mV, reaches half-maximal activation with a depolarization to 0 mV, and has a mean peak current density of 13 microA/cm2. The time course of inactivation is well described by a single exponential (tau = 3 ms at 0 mV). In cell-attached patches, a rapidly activating and inactivating inward current channel was recorded with an average unit conductance of 6.9 pS. The activation and inactivation parameters of the ensemble averaged current closely match the measured values from the macroscopic sodium current. At very positive potentials we recorded a voltage-dependent outward current channel with a conductance of around 35 pS. No significant inward calcium current was observed in whole-cell measurements and few single calcium channel currents were measured in cell-attached patches, suggesting a sparse distribution of calcium channels in the r.u.q. growth cones.
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PMID:Action potentials, macroscopic and single channel currents recorded from growth cones of Aplysia neurones in culture. 242 3

Mechanisms of electrolyte and fluid secretion in the hamster pancreatic acini were investigated by measurements of fluid and amylase secretion in vivo and in vitro, and membrane potential and resistance in vitro. Unlike mouse and rat pancreas the hamster pancreas secreted only a small amount of juice in response to acinar stimulants such as acetylcholine (ACh) and caerulein. The mean resting potential was -62 mV and the mean resting input resistance was 29 M omega. Ionophoretic application of ACh evoked membrane depolarization accompanied by a reduction in input resistance. The reversal potential for this ACh-evoked depolarization (EACh) was -11 mV. The EACh was shifted by changing extracellular K, Na and Cl concentration in a similar way to that of mouse pancreatic acinar cells. The relative permeability and current for K, Na and Cl at the EACh calculated by using the Goldman-Hodgkin-Katz equations were PK/PNa/PCl = 1/0.9/0.43 and IK/INa/ICl = 1/1.4/0.4 respectively (In the mouse Pk/PNa/PCl = 1/1.2/5 and Ik/INa/ICl = 1/2.3/1.3, Petersen et al. 1981). The results indicate that mechanisms of electrolyte and fluid secretion in hamster pancreatic acini are qualitatively similar to those in the mouse and rat pancreas. The less permeability of the acinar cell membrane to Cl ions in the hamster than in the mouse and rat appears to be associated with the fact that the acinar stimulant evokes a far smaller amount of fluid secretion in this species than in the mouse and rat.
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PMID:Fluid secretion and electrical properties of pancreatic acini of Syrian golden hamster. 243 10

Sodium currents, INa, were recorded from Xenopus laevis oocytes which had been injected with mRNA synthesized by in vitro transcription of the rat brain sodium channel II cDNA (Noda et al. 1986 a, b). Patch pipettes were used to apply depolarizing voltage steps and to record macroscopic sodium currents of between 50 and 750 pA from cell-attached patches of the oocyte membrane. With a combination of whole-cell and patch clamp recording, the properties of the implanted sodium channels could be studied in detail. They were analyzed according to the model of Hodgkin and Huxley (1952 a) assuming three activation gates. The activation of the sodium currents is characterized by an equilibrium potential of -29 mV and an apparent gating charge of 8.7 e0. At -64 mV half of the sodium currents were inactivated. From single-channel current recordings, an elementary sodium channel conductance of 19 pS and an average open time of 0.43 ms were obtained at -32 mV membrane potential and 16 degrees C. The single-channel and activation properties of rat brain sodium channel II are therefore comparable to those found in peripheral nerve and skeletal muscle, but inactivation occurs at less negative potentials. This could be a specific property of the brain sodium channels and may underlie the maintained inward sodium currents reported in brain neurones (French and Gage 1985).
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PMID:Patch clamp characterization of sodium channels expressed from rat brain cDNA. 243 40

1. Ganglion cells were dissociated from the enzyme-treated rat retina, identified with specific fluorescent labels, and maintained in vitro. Electrophysiological properties of solitary retinal ganglion cells were investigated with both conventional intracellular and patch-clamp recordings. Although comparable results were obtained for most measurements some important differences were noted. 2. The input resistance of solitary retinal ganglion cells was considerably higher when measured with 'giga-seal' suction pipettes than with conventional intracellular electrodes. Under current-clamp conditions with both intracellular and patch pipettes, these central mammalian neurones maintained resting potentials of about -60 mV and displayed action potentials followed by an after-hyperpolarization in response to small depolarizations. The membrane currents during this activity, analysed under voltage clamp with patch pipettes, consisted of five components: Na+ current (INa), Ca2+ current (ICa), and currents with properties similar to the delayed outward, the transient (A-type), and the Ca2+-activated K+ currents (IK, IA and IK(Ca), respectively). 3. Ionic substitution, pharmacological agents, and voltage-clamp experiments revealed that the regenerative currents were carried by both Na+ and Ca2+. 100 nM-1 microM-tetradotoxin (TTX) reversibly blocked the fast spikes carried by the presumptive INa, which under voltage-clamp analysis had classical Hodgkin-Huxley-type activation and inactivation. 4. Single-channel recordings of the Na+ current (iNa) permitted comparison of these 'microscopic' events with the 'macroscopic' whole-cell current (INa). The inactivation time constant (tau h) fitted to the averaged single-channel recordings of iNa in outside-out patches was slower than the tau h obtained during whole-cell recordings of INa. 5. In the presence of 1-40 microM-TTX and 20 mM-TEA, slow action potentials appeared in intracellular recordings and were probably mediated by Ca2+. The potentials were abrogated by 3 mM-Co2+ or 200 microM-Cd2+; conversely, increasing the extracellular Ca2+ concentration from 2.5 to 10-25 mM or substitution of 1 mM-Ba2+ for 2.5 mM-Ca2+ enhanced their amplitude. ICa was measured directly in whole-cell recordings with patch pipettes after blocking INa with extracellular 1 microM-TTX and K+ currents with intracellular 120-mM Cs+ and 20 mM-TEA. 6. During whole-cell recordings with patch electrodes, extracellular 20 mM-TEA suppressed IK and, to a lesser extent, IA. Extracellular 5 mM-4-AP or a pre-pulse of the membrane potential to -40 mV prior to stronger depolarization completely blocked IA.(ABSTRACT TRUNCATED AT 400 WORDS)
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PMID:Voltage-dependent conductances of solitary ganglion cells dissociated from the rat retina. 244 69

1. The properties of whole-cell Na+ currents (INa) were studied in immunocytochemically identified ovine gonadotrophs using the patch clamp technique. 2. Voltage recording under current clamp revealed that gonadotrophs did not fire spontaneously, and fired only a single action potential in response to a depolarizing current clamp step. 3. Under voltage clamp, INa was found to be sensitive to tetrodotoxin (TTX) and had an activation threshold of about -75 mV, with peak current occurring at -20 to -30 mV. 4. Using a two-pulse protocol a delay in the onset of inactivation was observed, suggesting that inactivation is dependent on and preceded by the activation phenomenon. 5. Kinetics of recovery from inactivation of the Na+ channels were studied with test pulses applied at various times after a depolarizing pre-pulse. Recovery from inactivation showed an initial delay, in contrast to the predictions of the Hodgkin-Huxley equations. 6. Recovery from inactivation was examined by using a repetitive pulse protocol, showing approximately 1 s is required for the channels to achieve a 95% recovery. 7. The steady-state inactivation (h infinity -V) curve was sigmoidal and fitted by a logistic growth curve model. The half-inactivation value of the Na+ current occurred at a membrane potential of -70 +/- 8 mV. 8. Noise power spectra derived from fluctuations of INa could be fitted with a single Lorentzian function, and the time constant value was slower at more depolarizing potentials. 9. The single-Na+-channel conductance was estimated from fluctuation analysis under conditions of reduced Na+ current amplitude by depolarizing pre-pulses. The single-channel conductance derived by the above method (approximately equal to 11 pS) corresponded to the single-channel conductance derived from single-channel current measurements using the outside-out version of the patch clamp technique (approximately equal to 13 pS). 10. Inactivation of INa was slowed by including 15 mM-iodate in the pipette. Ensemble fluctuation analysis of INa under these conditions was carried out using the steady state portion of the inactivation phase of the modified INa records, revealing a process best fitted by a double Lorentzian power spectrum, consistent with inactivation kinetics involving both a fast and a slow process. The time constant values correlated well with those obtained from a double-exponential fit to the decaying inactivation phase of the iodate-modified INa.(ABSTRACT TRUNCATED AT 400 WORDS)
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PMID:Characterization of voltage-gated sodium channels in ovine gonadotrophs: relationship to hormone secretion. 245 92

1. Membrane conductance parameters for the rat sympathetic neurone in vitro at 37 degrees C have been determined by two-electrode voltage-clamp analysis. The activation kinetics of two ionic currents, IA and IK(V), has been considered. Data for both currents are expressed in terms of Hodgkin-Huxley equations. 2. The isolated IA developed following third-order kinetics. The activation time constant, tau a, was estimated from the current time-to-peak and, for V less than or equal to -40 mV, from the IA tail current analysis upon membrane repolarization to various potentials. The maximum tau a occurred at -55 mV and varied from 0.26 to 0.82 ms in the range of potentials between -100 and +10 mV. The steady-state value of the variable a, corrected for inactivation, was evaluated in the voltage range from -60 to 0 mV; 14.4 mV are required to change a infinity e-fold. Steady-state gA was voltage dependent, increasing with depolarization to a maximum of 1.40 microS at +10 mV. 3. IK(V) was similarly analysed in isolation. The current proved to develop as a first-order process. tau n was determined by fitting a single exponential to the IK(V) rising phase and to the tail currents at the end of short depolarizing pulses. The bell-shaped voltage dependence of tau n exhibited a maximum (25.5 ms) at -30 mV, becoming minimal (1.8 ms) at -80 and +20 mV. The n infinity curve was obtained (n infinity = 0.5 at -6.54 mV; k = 8.91 mV). The mean maximum conductance, gK(V), was 0.33 microS per neurone at +10 mV. 4. Single spikes have been elicited by brief current pulses at membrane potentials from -40 to -100 mV under two-electrode current-clamp conditions in normal saline and in the presence of blockers of the ICa-IK(Ca) (Cd2+) and/or IK(V) (TEA, tetraethylammonium) systems. Spike repolarization was affected by the suppression of either current in the depolarized neurone, but was insensitive to both treatments when the spike arose from holding levels negative to -75 to -80 mV, indicating that at these membrane potentials the IA current mainly, if not exclusively, contributes to the action potential falling phase. 5. The basic features of the sympathetic neurone action potential were reconstructed by simulations based on present and previous voltage-clamp characterization of the IA, IK(V) and INa conductances.(ABSTRACT TRUNCATED AT 400 WORDS)
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PMID:The interactions between potassium and sodium currents in generating action potentials in the rat sympathetic neurone. 245 94


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