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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 anatomy and physiology of the Drosophila larval neuromuscular junction were studied. 2. The dependence of muscle resting potentials on [K+]o and [Na+]o follows the Goldman-Hodgkin-Katz equation (PNa/PK=0-23). Chloride ions distribute passively across the membrane. 3. The mean specific membrane resistance of muscle fibres is 4-3 X 10(3) omega cm2, and the mean specific membrane capacitance is 7-1 muF/cm2. The muscle fibre is virtually isopotential. 4. Transmitter release is quantal. Both the miniature excitatory junctional potential and the evoked release follow the Poisson distribution. 5. Transmitter release depends on approximately the fourth power of [Ca2+]o. If Sr2+ replaces Ca2+, it depends on approximately the fourth power of [Sr2+]o. Mg2+ reduces transmitter release without altering the fourth power dependence on [Ca2+]o.
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PMID:Properties of the larval neuromuscular junction in Drosophila melanogaster. 1 39

Teorell's fixed charge theory for membrane ion permeability was utilized to calculate specific ionic permeabilities from measurements of membrane potential, conductance, and specific ionic transference numbers. The results were compared with the passive ionic conductances calculated from the branched equivalent circuit membrane model of Hodgkin Huxley. Ionic permeabilities for potassium, sodium, and chloride of crayfish (Procambarus clarkii) medial giant axons were examined over an external pH range from 3.8 to 11.4. Action potentials were obtained over this pH range. Failures occurred below pH 3.8 during protonation of membrane phospholipid phosphate and carboxyl, and above pH 11.4 from calcium precipitation. In general, chloride permeability increases with membrane protonation, while cation permeability decreases. At pH 7.0, PK = 1.33 X 10(-5), PCl = 1.49 X 10(-6), PNa = 1.92 X 10(-8) cm/s. PK: PCl: PNa = 693:78:1. PCl is zero above pH 10.6 and is opened predominately by protonation of epsilon-amino, and partially by tyrosine and sulfhydryl groups from pH 10.6 to 9. PK is activated in part by ionization of phospholipid phosphate and carboxyl around pH 4, then further by imidazole from pH 5 to 7, and then predominately from pH 7 to 9 by most probably phosphatidic acid. PNa permeability parallels that of potassium from pH 5 to 9.4. Below pH 5 and above pH 9.4, PNa increases while PK decreases. Evidence was obtained that these ions possibly share common passive permeable channels. The data best support the theory of Teorell, that membrane fixed charges regulate permiability and that essentially every membrane ionizable group appears involved in various amounts in ionic permeability control.
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PMID:Ionic permeability of K, Na, and Cl in crayfish nerve. Regulation by membrane fixed charges and pH. 1 19

Voltage-clamp currents and resting membrane potential of squid giant axons have been studied at extracellular pH varying between 4 and 10. The membrane currents, analyzed according to the Hodgkin-Huxley equations, showed that sodium permeability, PNa(E), and potassium conductance gK(E), curves were shifted toward positive voltages by different amounts and slightly depressed as the external pH was lowered. Under the same conditions, taum(E) and taun(E) were found to be enhanced and shifted to a larger extent in the same direction. The rate constants alpham and alphan were shifted substantially toward positive voltages, but betam and betan changed hardly at all. The shift of the alpham(E) curve was analyzed in terms of a fixed surface charge model; it indicates that unspecific negative groups with an approximate pKa of 4.5 are located in the vicinity of sodium active sites with an average charge separation of 8 A. A similar figure is obtained for the potassium system from the shift of the alphan(E) curve.
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PMID:Action of extracellular pH on Na+ and K+ membrane currents in the giant axon of Loligo vulgaris. 3 97

Human IgD present in the serum of normal individuals or of patients with Hodgkin's disease (having high IgD concentrations) was characterized and compared with five IgD myeloma proteins. IgD was isolated using a highly specific anti-delta insoluble immunoabsorbent from which the bound material was eluted with sodium dodecyl sulphate (SDS) or urea. The latter reagent could be removed by extensive dialysis, thus making possible the renaturation of the eluted molecules. The purity of the IgD thus isolated was confirmed by antigenic analysis. Both kappa and lambda light chain determinants were present on serum IgD, although lambda light chain was predominant with a ratio over the kappa chain of 2:1. SDS-polyacrylamide slab gel electrophoresis analysis revealed two different molecular forms of serum IgD, one (IgD) migrating identically to monoclonal IgD, the other (IgD2) having a faster mobility. The difference between the two molecules was entirely, due to the different sizes of their constituent delta chains. Peptide mapping of the two chains (delta1 and delta2 respectively) and of the delta chain of an IgD myeloma protein was carried out using 125I-labelled material. The three molecules displayed a high degree of homology, the delta2 chain differing by the presence of three characteristic extra peptides. The significance of these extra peptides is discussed in the light of the peptide mapping technique employed.
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PMID:Characterization of IgD. I. Isolation of two molecular forms from human serum. 8 32

The encoder region in receptors and neurons is represented by the inhomogeneous origin of the axon. The axon diameter and the excitability are in fact space-dependent. For the analysis the soma is described by a system with concentrated parameters followed by an inhomogeneous axon. The membrane properties are approximated by the slightly modified Hodgkin-Huxley equations. The assumption that the space-dependence of the excitability originates in variations of the conductance value for sodium ions accounts for a number of experimental results. The influence of other membrane parameters upon the mechanism of impulse generation and transmission has also been analysed.
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PMID:[Modelling of biological encoding mechanisms as a system with distributed parameters]. 17 22

1. Miniature end-plate currents (m.e.p.c.s) were recorded from mouse diaphragm using a point voltage-clamp. The relation between m.e.p.c. amplitude and membrane potential was determined in bathing solutions of varied composition. 2. In solution containing normal sodium the relation between m.e.p.c. height and membrane potential (Im.e.p.c./Vm relation) was always linear, at least in the range +30 to -100 mV; the reversal potential (Vr) at which Im.e.p.c. was zero was close to 0. The slope of the Im.e.p.c./Vm line varied little between junctions (coefficient of variation about 20%) and was about 50 nS, or 1nA per 20 mV. The Im.e.p.c./Vm relation was not altered by withdrawal of Ca2+, addition of ethanol, or substitution of NO-3 or SO2-(4) for Cl-. 3. Alteration of K+ concentration in the bathing medium, in the range 10 to 1 mM, had no apparent effect on the Im.e.p.c./Vm relation. 4. Reduction of Na+ concentration, with isosmotic substitution of sucrose, caused rapid alteration of the Im.e.p.c./Vm relation, which became rectifying, with a slope at negative Vm less than at positive Vm. Vr was shifted in the negative direction. Quantitatively these changes were close to those predicted by the Goldman-Hodgkin-Katz formulation for permeation of monovalent ions through a membrane with constant field. 5. In solution with low Na+ (2 mM) and partial substitution of K+ for Na+, the Im.e.p.c./Vm relation was indistinguishable from that in solutions with Na" as the predominant extracellular cation. With complete substitution of K+ for Na+ the Im.e.p.c./Vm relation was a little less steep (at negative Vm) than in Na+ solution and Vr was shifted slightly in the negative direction. 6. With substitution of NH+4 for Na+, the Im.e.p.c./Vm relation was little changed (about 10% steeper at negative Vm). With substitution of Li+ for Na+, the Im.e.p.c./Vm relation remained linear, but was made less steep, at positive as well as negative Vm, and Vr was shifted slightly in the positive direction. 7. These results indicate that the permeability change associated with generation of the m.e.p.c. (i.e., evoked by a quantum of transmitter) corresponds to the opening of a single species of membrane channel that allows the free movement of K+, Na+, NH+4, AND Li+ ions along their electrochemical gradients. The channel discriminates little between these ions. The apparent order of permeability is Li+ greater than NH+4 greater than Na+ greater than or equal to K+. The apparent permeability per channel corresponds to that expected for channels of about 6.4 A diameter, 100 A length, and ionic mobility the same as in dilute solution.
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PMID:A voltage-clamp study of the permeability change induced by quanta of transmitter at the mouse end-plate. 21 56

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. The concentrations of sodium, potassium and chloride in frog and bovine lenses showed a normal intracellular ion distribution with the sum of the internal cations approximately equal to the external sum. In the cephalopod lens, however, the sum inside was much lower than that outside.2. The membrane potentials of frog, Sepiola and bovine lenses were -63, -63 and -23 mV respectively. A comparison of the electrical data with the Nernst potentials predicted from ion concentration data indicated that sodium and chloride ions as well as potassium contributed to the membrane potential in frog and bovine. In contrast, the membrane and Nernst potentials for potassium were equal in Sepiola.3. Substituting potassium for sodium in the external medium depolarized lens potentials in all three species. Estimates of the relative permeabilities of sodium, potassium and chloride were obtained by fitting the Goldman-Hodgkin-Katz equation to the potential data.4. The potassium permeability was determined directly by (42)K efflux measurements and values of 2.99, 9.83 and 3.13 (x (-8) m sec(-1)) were obtained for frog, Sepiola and bovine lenses respectively.5. The effect of raising external potassium on the efflux rate constant was determined and there was reasonable agreement between experiment and theory (Kimizuka-Koketsu) in frog and bovine lenses, but the Sepiola data indicated that the potassium permeability decreased by a factor of 2.6 when the external potassium was raised from 10 to 120 mM-K+.6. The measured specific conductances, obtained using two internal micro-electrodes, were 7.7, 15.9 and 9.9 (Sm(-2)) for frog, cephalopod and bovine lenses respectively. These data compare with computed values (Kimizuka-Koketsu theory) of 7.5, 14.1 and 17.2 (Sm(-2)).7. The effect of increasing external potassium on the conductance was also tested and there was good agreement between experiment and theory (assuming constant permeabilities) only in the amphibian lens. However, when the cephalopod data were corrected assuming a 2.6-fold decrease in P(K) for a twelvefold increase in potassium, then there was excellent agreement between experiment and theory.8. The bovine measured conductances were much lower than the theoretical values throughout the range of external potassium concentrations and several explanations were proposed to account for the discrepancies.
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PMID:A comparison of ion concentrations, potentials and conductances of amphibian, bovine and cephalopod lenses. 30

1. Kinetics of inactivation of sodium channels in myelinated nerve from Rana pipiens were studied at 4.5 degrees C using the voltage clamp technique of Dodge & Frankenhaeuser (1958).2. Potassium currents were blocked by cutting the internodes in 20 mM-TEA-Cl + 100 mM-KCl and by adding 12 mM-TEA-Cl to the external Ringer. Leakage and capacitative currents were subtracted electronically.3. Kinetics of recovery from inactivation of the sodium channels were studied by inactivating the channels with a large depolarizing prepulse and allowing the channels to recover at different potentials; the extent of recovery was measured by applying a test pulse at various times after the prepulse.4. Kinetics of development of inactivation were studied by two different methods. The first was to measure the decay of sodium current under a maintained depolarization. The second method was to measure the decay of the peak sodium current in a test pulse as a function of time after the onset of a maintained depolarization. These two methods yielded similar results for the kinetics of inactivation development.5. Contrary to expectations of the Hodgkin-Huxley formalism, the time course of recovery from and development of inactivation is not strictly exponential. Rather, recovery from complete inactivation shows an initial delay which depends on recovery potentials. Development of inactivation at a fixed potential exhibits at least two exponentials.6. The steady-state inactivation curve h(infinity)(E) is asymmetrical and is fitted better by 1/[1+exp (A(1)E+B(1)) +exp (A(2)E+B(2))] than by 1/[1+exp (AE+B)].7. Most of the above kinetic observation on inactivation can be fitted by the following modification of the h system of the Hodgkin-Huxley formalism: [Formula: see text]8. In the analysis it was not necessary to modify the concept of two separate processes, activation and inactivation, governing the opening and closing of the sodium channels.
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PMID:Inactivation of sodium channels: second order kinetics in myelinated nerve. 30 88

1. Voltage-clamp studies were carried out on single rabbit myelinated nerve fibres at 14 degrees C with the method of Dodge & Frankenhaeuser (1958). 2. A method was developed to allow the ionic currents through the modal membrane to be calibrated exactly under voltage-clamp conditions by measuring the resistance of the internode through which the current was injected. 3. The ionic currents in a rabbit node of Ranvier can be resolved into two components, a sodium current and a leak current. Potassium current is almost entirely absent. 4. The sodium currents in rabbit nodes were fitted by the Hodgkin-Huxley model using m2h kinetics. The kinetics of sodium currents in a rabbit node differ from that in a frog node under similar experimental conditions in two respects: (a) inactivation is faster, tau h for rabbit being 2-3 times smaller around -50 mV; (b) the P(Na) (E) curve for mammal is shifted 10-15 mV in the hyperpolarizing direction. 5. From the kinetics of sodium current, the non-propagating rabbit action potential was reconstructed at 14 degrees C. The transient inward sodium current is responsible for the fast initial depolarization phase of the action potential, while the repolarizing phase is accounted for by leak alone. The computed shape of the action potential was in good agreement with the experimentally obtained action potential. 6. At 14 degrees C, frog and rabbit nodes with similar diameters have similar measured gNa values.
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PMID:A quantitative description of membrane currents in rabbit myelinated nerve. 31 74


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