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

We have examined the problem of obtaining relationships between the type of stable solutions of the Hodgkin-Huxley type system, the values of its parameters and a constant applied current (I). As variable parameters of the system the maximal Na+(-gNa), K+(-gK) conductances and shifts (Gm, Gh, Gn) of the voltage-dependences have been chosen. To solve this problem it is sufficient to find points belonging to the boundary, partitioning the parameter space of the system into the regions of the qualitatively different types of stable solutions (steady states and stable periodic oscillations). Almost all over the physiological range of I, a type of stable solution is determined by the type of steady state (stable or unstable). Using this fact, the approximate solution of this problem could be obtained by analyzing the spectrum of eigenvalues of the Jacobian matrix for the linearized system. The families of the plan sections of the boundary have been constructed in the three-parameter spaces (I, -gNa, -gK), (I, Gm, Gh), (I, Gm, Gn).
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PMID:Partition of the Hodgkin-Huxley type model parameter space into the regions of qualitatively different solutions. 131 1

The influence of giga-seal formation on the properties of the Na+ channels within the covered membrane patch was investigated with a whole-cell pipette and a patch pipette applied to the same cell. Current kinetics, current/voltage relation and channel densities were determined in three combinations: (i) voltage-clamping and current recording with the whole-cell pipette, (ii) voltage-clamping with the whole-cell pipette and current recording with the patch pipette and, (iii) voltage-clamping and current recording with the patch pipette. The Hodgkin-Huxley (1952) parameters tau m and tau h were smaller for the patch currents than for the whole cell, and the h infinity curve was shifted in the negative direction. The channel density was of the order of 10 times smaller. All effects were independent of the extracellular Ca2+ concentration. The capacitive current generated in the patch by the whole-cell Na+ current and its effect on the transmembrane voltage of the patch were evaluated. The kinetic parameters of the Na+ channels in the patch did not depend on whether the voltage was clamped with the whole-cell pipette or the patch pipette. Thus, the results are not due to spurious voltage.
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PMID:Giga-seal formation alters properties of sodium channels of human myoballs. 131 48

1. Na+ currents expressed in astrocytes cultured from spinal cord were studied by whole cell patch-clamp recording. Two subtypes of astrocytes, pancake and stellate cells, were morphologically differentiated and showed expression of Na+ channels at densities that are unusually high for glial cells (2-8 channels/microns2) and comparable to cultured neurons. 2. Na+ currents in stellate and pancake astrocytes were comparable to neuronal Na+ currents with regard to Na(+)-current activation (tau m) and inactivation (tau h) time constants, which were equally fast in both astrocyte types. However, they differed with respect to voltage dependence of activation, and current-voltage (I-V) curves were approximately 10 mV more positive in stellate cells (-11.1 +/- 5.6 mV, mean +/- SD) than in pancake cells (19.7 +/- 4.5 mV). Steady-state activation (m infinity curves) was 16 mV more negative in pancake (mean V1/2 = -48.8 mV) than in stellate cells (mean V1/2 = -32.7 mV). 3. Steady-state inactivation (h infinity curves) of Na+ currents was distinctly different in the two astrocyte types. In stellate astrocytes h infinity curves had midpoints close to -65 mV (-64.6 +/- 6.5 mV), similar to most cultured neurons. In pancake astrocytes h infinity-curves were approximately 25 mV more negative, with midpoints close to -85 mV (84.5 +/- 9.5 mV). 4. The two forms of Na+ currents were additionally distinguishable by their sensitivity to tetrodotoxin (TTX). Na+ currents in stellate astrocytes were highly TTX sensitive [half-maximal inhibition (Kd) = 5.7 nM] whereas Na+ currents in pancake astrocytes were relatively TTX resistant, requiring 100- to 1,000-fold higher concentrations for blockage (Kd = 1,007 nM). 5. Na+ currents were fit by the Hodgkin-Huxley (HH) model. In pancake astrocytes, as in squid gigant axons, Na(+)-current kinetics could be well described with an m3h model, whereas in stellate astrocytes Na+ currents were better described with higher-order power terms for activation (m). On average, best fits were obtained using an m4h model. 6. Pancake astrocytes were capable of generating action-potential (AP)-like responses under current clamp whereas stellate astrocytes were not. The h infinity curve for APs shows that membrane potentials more negative than -70 mV are required to allow these responses to occur.(ABSTRACT TRUNCATED AT 400 WORDS)
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PMID:Ion channels in spinal cord astrocytes in vitro. II. Biophysical and pharmacological analysis of two Na+ current types. 133 55

1. Dissociated neurones from embryonic rat hypothalamus were grown for several weeks in culture where they formed complex networks. These synaptically coupled networks were capable of generating synchronized bursting activity. Voltage-activated membrane currents were studied in these neurones using a patch clamp in the whole-cell configuration. 2. Outward currents were carried by K+ ions and consisted of an inactivating and a non-inactivating component. These components were similar to the transient K+ current (IA) and the delayed rectifier current (IK) reported in neurones from the postnatal rat hypothalamus. Application of Zn2+ (1 mM) blocked the transient component completely while reducing the non-inactivating component by only approximately 20%. 3. Inward currents were carried by Na+ and Ca2+ ions. Rapidly activating transient Na+ currents were activated at approximately -25 mV. TTX entirely blocked these currents at low concentration (300 nM). Voltage sensitivity of the Na+ conductance was 5.8 mV per e-fold change with half-maximal activation occurring at -8 mV. Na+ current kinetics could be well described by the Hodgkin-Huxley model (m3h). 4. With depolarizing pulses from a holding potential of -80 mV two Ca2+ current components with different ranges of activation were identified. Low voltage-activated (LVA, T-type) Ca2+ currents were activated at approximately -50 mV. High voltage-activated (HVA; also called L- or N-type) Ca2+ currents were observed at membrane potentials more positive to approximately -30 mV. LVA Ca2+ currents were observed in hypothalamic neurones that had developed a network of dendritic processes in the course of several weeks in culture. Activation and inactivation time constants of LVA Ca2+ currents were 15-25 ms and 30-100 ms (-30 to -45 mV). In contrast to HVA Ca2+ currents, no LVA Ca2+ currents were seen in neuronal somata obtained from the network cultures by mechanical dissociation. This suggests that most of the LVA Ca2+ channels are located on the dendritic tree rather than on the soma membrane. 5. HVA Ca2+ currents were maximal between 0 and +10 mV (external [Ca2+] = 5 mM). The time-to-peak was in the range of 1.7-5.4 ms (+30 to -10 mV). Tail currents following repolarization decayed monoexponentially with a time constant of approximately 210 microseconds. During 500 ms depolarizations, 90% of the current inactivated. The time course of inactivation showed two time constants of approximately 40 and approximately 700 ms.(ABSTRACT TRUNCATED AT 400 WORDS)
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PMID:Ionic currents in cultured rat hypothalamic neurones. 133 25

The Hodgkin-Huxley equation for electrogenesis in the voltage clamped squid giant axon was used to predict the effect of altering maximal Na+ conductance (gNa+max) on the repetitive firing process. The main finding was that increasing gNa+max, without changing any other membrane parameter, reduced the threshold current required to evoke repetitive firing. That is, it rendered the membrane hyperexcitable. Threshold for evoking single action potentials was also affected, but much less so. Other consequences of increasing gNa+max were a decrease in the minimum sustainable rhythmic firing frequency (mRFF), a monotonic increase in firing frequency at any given suprathreshold stimulus intensity, an increase in the current value at which intense depolarizing stimuli block rhythmogenesis, an increase in the maximal sustainable firing frequency using intense currents (MRFF), and the consequent expansion of the dynamic range for stimulus encoding. Thus, the control of gNa+max through the regulation of Na+ channel synthesis and membrane incorporation at sites of rhythmogenesis (e.g. axon hillock-initial segment region, or peripheral sensory endings) is a potential regulatory mechanism for neuronal excitability and stimulus encoding.
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PMID:Na+ conductance and the threshold for repetitive neuronal firing. 133 24

1. Voltage signals of about 1 mV evoked in photoreceptors of the drone honey bee by shallow modulation of a background illumination of an intensity useful for behaviour are thought to be amplified by voltage-dependent Na+ channels. To elucidate the roles of the various membrane conductances in this amplification we have studied the effects of the Na+ channel blocker tetrodotoxin (TTX) and various putative K+ channel blockers on the membrane potential, Vm. 2. Superfusion of a slice of retina with 0.5-10 mM-4-aminopyridine (4-AP) depolarized the membrane and, in fifty of sixty-three cells induced repetitive action potentials. Ionophoretic injection of tetraethylammonium produced similar effects. 3. In order to measure the depolarization caused by 4-AP, action potentials were prevented by application of TTX: 4-AP was applied when the membrane was depolarized to different levels by light. 4-AP induced an additional depolarization at all membrane potentials tested (-64 to -27 mV). We conclude that there are 4-AP-sensitive K+ channels that are open at constant voltage over this range. 4. 4-AP slowed down the recovery phase of the action potential induced by a light flash by a factor that ranged from 0.51 to 0.16. This reduction could be accounted for by the reduction in a voltage-independent K+ conductance estimated from the steady-state depolarization. 5. After the voltage-gated Na+ channels had been blocked by TTX, exposure to 4-AP further changed the amplitude of the response to a small (approximately 10%) decremental light stimulus. The change was an increase when the background illumination brought Vm to potentials more negative than about -40 mV; it was a decrease when Vm > -40 mV. The data could be fitted by a circuit representation of the membrane with a light-activated conductance and a K+ conductance (EK = -66 mV) that was partly blocked by 4-AP. The voltage range studied was from -52 to -27 mV; neither conductance in the model was voltage dependent. 6. The responses to small changes in light intensity in the absence of TTX were mimicked by a model. We conclude that a voltage-dependent Na+ conductance described by the Hodgkin-Huxley equations can amplify small voltage changes in a cell membrane that is also capable of generating action potentials; the magnitude of the K+ conductance is critical for optimization of signals while avoiding membrane instability.
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PMID:Membrane conductances involved in amplification of small signals by sodium channels in photoreceptors of drone honey bee. 133 99

1. The ionic dependence of current through the 3',5'-cyclic guanosine monophosphate (cyclic GMP)-activated channels of salamander rods was studied in excised inside-out membrane patches from isolated outer segments. Voltage-clamp experiments on transducing rods were performed so that the channels in intact cells could be compared with those in excised patches. 2. The reversal potential of the cyclic GMP-induced patch current was close to the Na+ equilibrium potential when the concentration of NaCl on the cytoplasmic surface of a patch was varied at constant external NaCl concentration. Fitting the Goldman-Hodgkin-Katz equation indicated that the apparent ratio of permeabilities for Na+ and Cl- was at least 50. This confirms a previous report that the channel's Na+ permeability is much larger than its Cl- permeability. 3. Na+ currents through the channel did not obey the independence principle. The outward patch current at large positive potential began to saturate with increasing concentrations of internal Na+, as if permeation required Na+ to bind to a site with an apparent dissociation constant around 180 mM. 4. In symmetrical NaCl solutions containing very low concentrations of divalent cations the current-voltage relation measured from excised patches 50 microseconds after switching the voltage showed mild outward rectification. By 1 ms the rectification was more pronounced. The rectification at 50 microseconds is attributed to voltage dependence of Na+ permeation. The additional rectification at later times is attributed to voltage dependence of the channel's probability of being open, depolarization favouring the open state. 5. In symmetrical Mg2+ solutions the cyclic GMP-induced patch currents were smaller and the outward rectification was more pronounced. 6. Addition of Mg2+ or Ca2+ to an internal Na+ solution blocked the cyclic GMP-induced Na+ current through the channels, as if by occupying a single binding site with an affinity in the 0.1-2 mM range. Block by Mg2+ was voltage dependent, suggesting that the binding site was within the channel's transmembrane electric field. Raising the Mg2+ concentration on the external surface of the patch increased the apparent dissociation constant of block by internal Mg2+, as expected if external and internal Mg2+ compete for the same binding site. 7. Block by internal Ca2+ had an opposite and weaker voltage dependence than block by internal Mg2+. 8. In symmetrical solutions containing both Na+ and Mg2+ the outward rectification was more pronounced than in solutions containing Na+ alone. In solutions thought to be close to physiological the outward patch current increased e-fold for a depolarization of 24-30 mV.(ABSTRACT TRUNCATED AT 400 WORDS)
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PMID:Cation interactions within the cyclic GMP-activated channel of retinal rods from the tiger salamander. 138 54

We study two different two-dimensional reductions of the Hodgkin-Huxley equations. We show that they display the same qualitative bifurcation scheme as the original equations but overestimate the current range where periodic emission occurs. This is essentially due to the assumption that the evolution of the sodium activation variable m is instantaneous with respect to the dynamics of the variables h and n, an hypothesis that breaks down at high values of the injected current. To prove this point we compare the current-amplitude relation, the current-frequency relation, and the shapes of individual spikes for the two reduced models to the results obtained for the original Hodgkin-Huxley model and for a three-dimensional model with instantaneous sodium activation. We show that a more satisfying agreement with the original Hodgkin-Huxley equations is obtained if we modify the evolution equation for the potential by incorporating the prominent features of the dynamics of m.
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PMID:Two and three dimensional reductions of the Hodgkin-Huxley system: separation of time scales and bifurcation schemes. 139 Nov 18

Membrane potential of the isolated outer hair cells (OHCs) from the guinea pig cochlea was measured using conventional microelectrodes filled with 200 mM KCl. The resting membrane potential during superfusion with the standard physiological saline solution containing 3.5 mM K+ was -47.3 +/- 1.4 mV (N = 72), which was higher than those previously reported for isolated OHCs studied by using microelectrodes. Addition of ouabain (10(-5)-10(-3) M), the specific Na+, K+ ATPase inhibitor, depolarized the cell slowly and progressively, indicating the presence of low but definite Na+, K+ ATPase activity in the plasma membrane of OHCs. The magnitude of membrane potential was mainly dependent on the extracellular K+ concentration ([K+]O). A ten-fold increase of [K+]O depolarized the membrane potential by 49.6 +/- 1.0 mV (N = 58). A decrease of [Na+]O to one tenth of the control hyperpolarized the membrane potential by about 2 mV. Decreasing extracellular Cl- from 131.3 mM to 27.5 mM did not cause a significant change in the membrane potential. Using the Goldman-Hodgkin-Katz equation, assuming a negligible contribution of Cl- to the membrane potential and total monovalent cat ion concentration of the cytosol similar to the extracellular fluid, we calculated the permeability ratio of K+ versus Na+ to 131 +/- 19 and intracellular K+ concentration to 33.3 +/- 1.9 mM.
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PMID:Membrane potential measurement in isolated outer hair cells of the guinea pig cochlea using conventional microelectrodes. 142 66

In this study, the expression of the novel intermediate filament protein Restin in human tissues was analyzed. Restin expression was studied by immunohistochemistry using polyclonal and monoclonal antibodies. Restin was not detected in normal tissues, a range of B- and T-cell non-Hodgkin's lymphomas, and nonlymphoid tumors. However, Restin was present in Reed-Sternberg cells and variants thereof in Hodgkin's disease, with the exception of the lymphocyte-predominant, paragranuloma subtype. Restin was also highly expressed in anaplastic large-cell lymphoma (so-called Ki-1 lymphoma). As expected, Restin was also expressed in Hodgkin cell lines L428, L428KSA, Co, and KM-H2 and the anaplastic large-cell lymphoma cell line Karpas 299, which was confirmed by sodium dodecyl sulfate-polyacrylamide gel electrophoresis and Western blotting, as well as Northern blotting. The presence of Restin in both Hodgkin's disease and anaplastic large-cell lymphoma is intriguing and might indicate a role of this structural protein in the pathogenesis of both conditions.
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PMID:Expression of the novel intermediate filament-associated protein restin in Hodgkin's disease and anaplastic large-cell lymphoma. 145 Apr 14


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