Hepatic capacitance vessel responses to bilateral carotid occlusion in anesthetized cats.
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UNLABELLED: Efficient on-line digitization is the prerequisite for computerized analysis of the electrical phenomena occurring during defibrillation. Conventional hardware presently provides only limited time resolution. The performance of various digitization rates for recording of voltage, current, and calculation of derived quantities like impedance, energy, and defibrillator capacitance was investigated. It was assessed both experimentally and by computer simulation of a trapezoidal discharge (of 9 msec duration into a constant resistive load of 50 omega with a defibrillator capacitance of 132 microF). The accuracy achieved with different digitization rates is given. For example, an accuracy of 1% for analog-digital conversion for impedance calculation during this kind of DC shock requires a sampling rate of 8 kHz without, and a rate of 1 kHz with linear interpolation to correct for the hardware dependent error due to sequential sampling. CONCLUSION: Highly efficient analog-digital conversion of delivered voltage and current during DC shocks is available within the limits of conventional inexpensive hardware.
Membrane electrical properties, component ionic conductances and excitability characteristics of extensor digitorum longus muscle from 3-4, 16 and 29 months old rats were measured "in vitro". Fiber diameter, membrane resistance (Rm) and membrane capacitance, increased with aging, and the increase was significant at 29 months. The increase of Rm was mostly due to a decrease of chloride conductance (GC1), whereas potassium conductance (GK) increased only slightly, at 16 and 29 months. Due to the lowered GC1, the latency of action potential increased at both ages with a consequent prolongation of the duration of action potential. Nevertheless, a decrease in the firing capability was recorded in the aged fibers. Our results indicate, that during aging, the most affected parameter of skeletal muscle fibers is GC1, although changes of this passive conductance alone cannot entirely account for the changes in the excitability characteristics recorded.
The current-voltage steady-state characteristics, cyclic voltammograms and capacitance-voltage steady-state relationships of bilayer lipid membranes made from dioleoylphosphatidylcholine or its mixtures with dolichyl-12 phosphate have been studied. Sustained fluctuations of the capacitance of dolichyl phosphate modified bilayers under applied voltage were observed. The results suggest that the dynamics of dolichyl phosphate molecules in membranes can be regulated by transmembrane electrical potential.
A method of stabilizing the membrane potential of a small area of cardiac muscle membrane and the limitations of this method are described. Tiny bundles or strands, approximately 80 mum in diameter, of electrically interconnected fibers from the ventricles of rabbit hearts were used in a double sucrose gap. Current records associated with step changes in voltage were complicated by two capacitive surges of current of nodal and nonnodal origin and large "leakage" currents of nonnodal origin resulting mainly from the multifibered nature of the preparation and emphasized by the method. The transient, inward membrane currents in response to moderate depolarizing steps in command potential had the same duration as the upstroke of the action potential. In good runs, currents were smooth and free from notches. These initial currents behaved qualitatively like the initial sodium currents in squid axon and in other excitable membranes. A fraction of the initial sodium current persisted at least as long as 300 ms. The relationship between peak initial current and voltage was graded and linear in the positive direction. In the negative region the relationship was often very steep, indicating insufficient voltage control of all the membranes despite the squareness of the voltage record. Other indications of inadequacy of control could occur and thus even with this optimum preparation of cardiac muscle it was not feasible to analyze quantitatively either the initial or the prolonged sodium currents.
The capacitive photoelectric current responses of the halorhodopsins from Halobacterium salinarum (shR) and from Natronobacterium pharaonis (phR) were studied using membrane fragments adsorbed onto a thin polyester film. The electric current of shR was not much affected by ionic strength or cations present in the medium (Na+, K+, Li+, Mg2+, or Ca2+), but was greatly influenced by the Cl- concentration. It increased biphasically as the Cl- concentration increased from 0 to 5 M, then decreased and almost vanished at around 10 or 12 M. Apparent Kd's of about 0.1 and 6 M were deduced for the Kd of Cl- uptake sites. We had to assume a sigmoidal increase of Cl- binding with a Hill coefficient of about 8 at the cytoplasmic, Cl- release site(s). The half-maximum Cl- concentration for the sigmoidal binding was about 7.5 M. The electric current of phR had a maximum around 30 mM Cl- and biphasically decreased at higher Cl- concentrations. The apparent Kd for the Cl- uptake site was 5 mM. The biphasic decrease in the transport activity was explained by assuming a sum of simple hyperbolic type binding (Kd = 0.2 M) and sigmoidally increasing binding with a Hill coefficient of 10 on the cytoplasmic side. The half-maximum concentration of the latter cooperative binding was 5.6 M. This great difference between the apparent affinity of the release site of shR and that of phR can explain the previously reported difference between the Cl- dependency of their photocycles. These results also suggest that there may be multiple Cl- binding sites in the Cl- transport pathway. A simple sequence of Cl- transport steps based on a multiion channel model is proposed.
We perform low-temperature electrical transport measurements on gated, quasi-2D graphite quantum dots. In devices with low contact resistances, we use longitudinal and Hall resistances to extract carrier densities of 9.2-13 x 10(12) cm(-2) and mobilities of 200-1900 cm(2)/V.s. In devices with high resistance contacts, we observe Coulomb blockade phenomena and infer the charging energies and capacitive couplings. These experiments demonstrate that electrons in mesoscopic graphite pieces are delocalized over nearly the whole graphite piece down to low temperatures.
A computer model of the aorta and its branches was made based on a simulation of an electrical transmission line using T elements. The model represented the aorta, with branches to the arms and legs and a branch to the head. The values for the capacitance and inductance of each T element could be specified, and a linearly increasing left ventricular pressure was used to drive the model. Transmission line equations were used to select values for the components, and an attempt was made to simulate the results of measurements of blood velocity in the aorta and peripheral arteries of normal subjects. The values obtained with the model showed a close relation to those in experimental studies. The results support the hypothesis that the arterial bed can be well represented by a "lossless" branched transmission line, with impedances matched at each branch and terminated with resistances that give a reflection coefficient of 0.5. A driving function, in which a linearly increasing left ventricular pressure provided a transient input to an aortic root of relatively low impedance, gave the best simulation of the experimental results.
High frequency current is used in surgery for cutting the tissue and stopping bleeding. Its usage is more frequent in endoscopic than open surgery. "Polarity" (monopolar and bipolar) marks the number of the electrical poles on the application place. Monopolar current has been used more often. With its usage thermal injuries are possible: coagulation outside of the laparoscopic view, direct coupling, capacitive coupling, sparking, skin combustion, activity on the heart rhythm. Because of these complications, the bipolar current is more and more in usage, which reduces the number of complications or avoids them completely. Many bipolar instruments are available today. Bipolar hook for endoscopic surgery is a new instrument which unites the good characteristics of the hook and bipolar current.
Dielectrophoresis and electrorotation are commonly used to measure dielectric properties and membrane electrical parameters of biological cells. We have derived quantitative relationships for several critical points, defined in Fig. A 1, which characterize the dielectrophoretic spectrum and the electrorotational spectrum of a cell, based on the single-shell model (Pauly, H., and H.P. Schwan, 1959. Z. Naturforsch. 14b:125-131; Sauer, F.A. 1985. Interactions between Electromagnetic Field and Cells. A. Chiabrera, C. Nicolini, and H.P. Schwan, editors. Plenum Publishing Corp., New York. 181-202). To test these equations and to obtain membrane electrical parameters, a technique which allowed simultaneous measurements of the dielectrophoresis and the electrorotation of single cells in the same chamber, was developed and applied to the study of Neurospora slime and the Myeloma Tib9 cell line. Membrane electrical parameters were determined by the dependence of the first critical frequency of dielectrophoresis (fct1) and the first characteristic frequency of electrorotation (fc1) on the conductivity of the suspending medium. Membrane conductances of Neurospora slime and Myeloma also were found to be 500 and 380 S m-2, respectively. Several observations indicate that these cells are more complex than that described by the single-shell model. First, the membrane capacities from fct1 (0.81 x 10(-2) and 1.55 x 10(-2) F m-2 for neurospora slime and Myeloma, respectively) were at least twice those derived from fc1. Second, the electrorotation spectrum of Myeloma cells deviated from the single-shell like behavior. These discrepancies could be eliminated by adapting a three-shell model (Furhr, G., J. Gimsa, and R. Glaser. 1985. Stud. Biophys. 108:149-164). Apparently, there was more than one membrane relaxation process which could influence the lower frequency region of the beta-dispersion. fct1 of Myeloma in a medium of given external conductivity were found to be similar for most cells, but for some a dramatically increased fct1 was recorded. Model analysis suggested that a decrease in the cytoplasmatic conductivity due to a drastic ion loss in a cell could cause this increase in fct1. Model analysis also suggested that the electrorotation spectrum in the counter-field rotation range and fc1 would be more sensitive to conductivity changes of the cytoplasmic fluid and to the influence of internal membranes than would fct1, although the latter would be sensitive to changes in capacitance of the cytoplasmic membranes.
Many investigators assert that the ion-conducting pathway of the Na channel is a water-filled pore. This assertion must be reevaluated to clear the way for more productive approaches to channel gating. The hypothesis of an aqueous pore leaves the questions of voltage-dependent gating and ion selectivity unexplained because a column of water can neither serve as a switch nor provide the necessary selectivity. The price of believing in an aqueous pore therefore is a futile search for separate ad hoc mechanisms for gating and selectivity. The fallacy is to assume that only water is available to carry ions rapidly, ignoring the role of the glycoprotein, which can form an elastomeric phase with water. The elastomer is a state of matter, neither liquid nor solid, in which the molecules of a liquid are threaded together with cross-linked polymer chains; it supports fast ion motion (Owen, 1989). An alternative hypothesis for channel gating, based on condensed-state materials science, already exists (Leuchtag, 1988, 1991a). The ferroelectric-superionic transition hypothesis (FESITH) postulates that the Na channel exists in a metastable ordered (closed) state at resting potential and, on threshold depolarization, undergoes a reversible order-disorder phase transition to a less-ordered, ion-conducting (open) state. The ordered state is ferroelectric; the disordered state is a fast ion conductor selective for Li+ and Na+. The basis of the voltage dependence is elevation of transition temperature with electric field, well established in ferroelectrics. FESITH is consistent with single-channel transitions, gating currents, heat and cold block, and other phenomena observed at channel or membrane level. An implication of FESITH, the Curie-Weiss law, has been shown to explain existing data on membrane capacitance versus temperature in squid axon (Leuchtag, 1991c). Only on the basis of a clear understanding of function can we expect new structural data on the Na-channel glycoprotein to generate realistic structure-function models at the molecular level.
Weakly electric fish orient at night by employing active electrolocation. South American and African species emit electric signals and perceive the consequences of these emissions with epidermal electroreceptors. Objects are detected by analyzing the electric images which they project onto the animal's electroreceptive skin surface. Electric images depend on size, distance, shape, and material of objects and on the morphology of the electric organ and the fish's body. It is proposed that the mormyrid Gnathonemus petersii possesses two electroreceptive "foveae" at its Schnauzenorgan and its nasal region, both of which resemble the visual fovea in the retina of many animals in design, function, and behavioral use. Behavioral experiments have shown that G. petersii can determine the resistive and capacitive components of an object's complex impedance in order to identify prey items during foraging. In addition, fish can measure the distance and three-dimensional shape of objects. In order to determine object properties during active electrolocation, the fish have to determine at least four parameters of the local signal within an object's electric image: peak amplitude, maximal slope, image width, and waveform distortions. A crucial parameter is the object distance, which is essential for unambiguous evaluation of object properties.
This study aimed at establishment of adequate evaluation of intestinal viability before release of the strangulated intestine by measuring electrical properties. In rats a 20-cm segment of the distal ileum and mesentery was strangulated. The intestine was strangulated for 0, 2, 15, 45, 90, and 120 min. The conductance and capacitance obtained by impedance analyzer were used to calculate tan(delta)m in the strangulated intestine. ATP was measured as well. In another experiment, after various periods of strangulation, tan(delta)m was measured just before release of the strangulation. Rats were divided into Group A (survived for 7 days) and Group D (died within 7 days). There was a positive correlation between tan(delta)m and ATP levels (P < 0.01). And tan(delta)m was significantly greater in Group A than in Group D (P < 0.05). There were no deaths at a tan(delta)m value of 2.36 or more and no survivors at a tan(delta)m of less than 2.20 except for one rat. These results suggested that tan(delta)m may be a useful index of the viability of the strangulated intestine before reperfusion.
The abdominal circulation contains a high proportion of the total blood volume and this can change either passively in response to changes in vascular distending pressure or actively (termed a capacitance response) to changes in sympathetic nervous activity. The liver is the largest abdominal organ and this study was designed to evaluate its potential contribution to overall vascular capacitance and compliance. In chloralose anaesthetized dogs, the liver was vascularly isolated, perfused through the portal vein and hepatic artery at either constant pressures or constant flows and drained from the hepatic veins at constant pressure. Changes in vascular resistance were assessed from changes in inflow pressures or flows and hepatic blood volume was determined by differences between net inflow and outflow. During constant flow perfusion the change in hepatic volume (capacitance change) in response to supramaximal stimulation of sympathetic nerves at 16 Hz was (mean +/- S.E.M.) -2.40 +/- 0.61 ml (kg body weight)-1. This response was not significantly different during constant pressure perfusion. The changes in portal venous and hepatic arterial pressures during stimulation at constant flow perfusion were +0.67 +/- 0.13 and +4.92 +/- 0.67 kPa, respectively. The compliance of the liver, assessed as the change in volume to a change in hepatic venous pressure, was +5.44 +/- 0.18 ml kg-1 kPa-1. These results indicate that the liver has a major capacitance role, comparable to that of the canine spleen and, in addition, is highly compliant. No evidence was found to suggest that a sphincter on the hepatic outflow exists. Assuming similar responses occur in humans, who do not possess a large contractile spleen, the liver would be the most important controllable blood reservoir in the body.
Simple and composite membranes have been prepared from 2% collodion solutions containing different amounts of polystyrenesulfonic acid (PSSA). Various membrane parameters such as water content, electrolyte uptake, exchange capacity, and permselectivity of these membranes have been determined. The resistance and capacitance of simple membranes have been measured as functions of both external electrolyte concentration and internal fixed charge density. The impedance characteristics of composite membranes also have been determined and discussed in terms of the resistance and capacitance characteristics of simple membranes from which the composite structures have been formed.
A series of pulse procedures was used to distinguish experimentally between a 'capacitative' (Schneider & Chandler, 1973) and a 'resistive' (Matthias, Levis & Eisenberg, 1980) model of 'charge movements' in skeletal muscle. A general condition describing the conservation of charge in a non-linear capacitor that was used as the basis for the experiments is derived in the Appendix. It was shown that earlier criteria concerning equality of 'on' and 'off' charge in response to large steps are insufficient to exclude resistive models. However, the capacitative, but not the resistive model successfully explained results bearing on charge conservation assessed through pulse procedures involving: (i) small, 10 mV voltage steps from a series of prepulse voltages, (ii) voltage steps to a fixed potential from a series of hyperpolarized voltages, (iii) pulse sequences incorporating a 'staircase' of voltage steps. It is concluded that the earlier use of 'on' and 'off' equality in response to large voltage steps is insufficient to exclude a resistive basis for the non-linear transient. However pulse procedures explicitly designed to distinguish the two models give results consistent with a capacitative model for the non-linear charge and at variance with a resistive one.
1. Intracellular recordings were obtained from thirty-eight rat supraoptic nucleus (s.o.n.) neurosecretory neurones in perfused hypothalamic explants. Changes in membrane potential and conductance were monitored following application of gamma-aminobutyric acid (GABA), and related agonists and antagonists. 2. GABA depressed action potential discharge of all of thirty-five s.o.n. neurones tested and induced either membrane hyperpolarization or depolarization. Neurones that displayed membrane hyperpolarization in response to lower GABA concentrations (30-300 microM) demonstrated a biphasic membrane voltage change with a later depolarizing phase as a response to higher concentrations (up to 3000 microM). 3. GABA (10-3000 microM) induced a prominent concentration-dependent increase in membrane conductance in all neurones. The critical slope for the log-log plot of [GABA] vs. GABA-induced membrane conductance was 1.7, indicating co-operativity in the GABA receptor-induced conductance change. 4. Muscimol (0.3-30 microM) potently mimicked all the effects of GABA. Bicuculline (1-100 microM) antagonized the effects of GABA and muscimol in a competitive manner. 5. Glycine and taurine (1-10 mM) had weak effects, although comparatively similar to those of GABA. These actions were blocked both by bicuculline (100 microM) and by strychnine (1 microM). At higher concentrations (greater than 10 microM), strychnine also antagonized the actions of GABA. 6. In recordings with potassium-acetate-filled micropipettes, the reversal potential of hyperpolarizing membrane voltage responses to GABA was -72.5 +/- 1.5 mV in close agreement (+/- 5 mV) with the reversal potential of inhibitory post-synaptic potentials (i.p.s.p.s) recorded in the same neurones. Depolarizing responses to GABA reversed polarity at -50 +/- 1.6 mV. In recordings with KCl-filled micropipettes, voltage responses to GABA were always depolarizing and reversed near -40.0 +/- 4.3 mV. Similarly, reduction of the concentration of chloride ions in the perfusion medium from 134 to 10.4 mM induced a positive shift of the GABA reversal potential by 40-50 mV. 7. From measurements of input resistance (Rin) and cell time constant (tau O), input capacitance (Cin; representing total membrane capacitance) was calculated as 78.9 +/- 2.1 pF. During responses to GABA or muscimol, decreased Rin was accompanied by a linearly related decrease in tau o indicating that these substances had no effect on the membrane capacitance of s.o.n. neurones.(ABSTRACT TRUNCATED AT 400 WORDS)
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