The Electrical Resistance and Capacitance of the Membranes of Nitella translucens

The resistance and capacitance of the membranes of Nitella translucenshave been measured by direct current and alternating currentmethods. Current of the order of 10^-7 amp. was injected intothe cell by means of a conventional Ag, AgCl_-3N KCl glass microelectrodeinserted into the vacuole of the cell. The change of potentialacross the membrane was recorded by two other internal microelectrodeswhich had been inserted into the cell at known distances fromthe current-injecting electrode. In the direct-current experimentsthe input current was in the form of a square pulse, while sinusoidalcurrents of frequency 25 cycles per second were used in thealternating current experiments. The cell was treated as a shortlength of coaxial cable and from the measurements the followingparameters could be obtained: the space constant (), the membraneresistance (R_m) and the membrane capacitance (C_m). The valuesof R_m ranged from 6.7 to 36 K ohm cm.² (mean of 21.4 K ohm cm.²)and those of ranged from 1.5 to 5.7 cm. (mean of 2.6 cm.).The capacitance value was about I µF cm.^-2 These results are discussed within the framework of our knowledgeof these parameters for other cells, particularly plant cells.The measured electrical resistance is shown to be at least tentimes less than the value estimated from the passive fluxesof the principal ions K, Na, and Cl. It is suggested that thisdiscrepancy, which is usually attributed to non-independentmovement of these ions, could be partially explained on electro-osmoticgrounds. The value of the capacitance is very close to thatwhich is usually obtained for other cell membranes. One exceptionallylow value for Nitella has been quoted in the literature. Thereason for the gross error in this particular measurement isgiven.     

Modulating Action of Hyperforin on the P-Type Calcium Channels in the Membranes of Rat Cerebellar Purkinje Neurons

A modulating action of hyperforin (an active compound of the extract from Hypericum perforatum) on a high-threshold component of the calcium current, sensitive to application of 100 nM -Aga-IVA toxin and identified as P current, was studied on freshly isolated Purkinje neurons with the use of a patch-clamp technique in the whole-cell configuration. It was shown that extracellular application of 0.8 M hyperforin caused a shift of the current-voltage (I-V) relationship of P current by -(8 ± 2) mV, slowdown of the activation kinetics, and a decrease in the amplitude of this current. The shift of the I-V relationship and slowdown of activation kinetics developed for less than 10 sec, while the P-current amplitude decreased for a much longer time (several minutes) and depended on the intracellular concentration of Ca²⁺ ions. -Aga-IVA toxin at the concentration of 100 nM completely blocked the recorded inward current in the presence of 0.8 M hyperforin. In experiments with intracellular perfusion of Purkinje neurons, we found that interaction of hyperforin with its binding site occurs at the external side of the cell membrane. The study of the mechanisms involved in the hyperforin-induced P-current modulation revealed that 1 mM GTPS (activating G_Ts proteins, as well as activating or blocking G_Ms proteins) or 1-2 mM GDPS (blocking G_Ts and G_Ms proteins) in the intracellular solution did not affect the hyperforin-induced modulation of P current. Hyperforin-induced Ca²⁺-independent shift of the I-V relationship and slowdown of the activation kinetics of P current were abolished in the presence of 0.5 M calmidazolium in the extracellular medium.     

Computed Membrane Currents in Cardiac Purkinje Fibers during Voltage Clamps

Recent measurements have indicated that some of the cardiac cell electrical capacitance is in series with a resistance. The computations of currents in a voltage clamp presented below show that, in this case, there is a danger that capacitive transient currents recorded during voltage clamp experiments may be confused with currents arising through rapid active membrane conductance changes. Secondly, a voltage clamp technique aimed at avoiding capacitive transients, namely the linear or ramp clamp, has recently been introduced. An attempt has been made here to evaluate the usefulness of ramp clamps in studying membrane electrical properties, by computing ramp clamp results and considering the difficulties in reconstructing the original model from these results. It is concluded that such a reconstruction is not feasible.     

Action Potentials in Lupinus angustifolius L. shoots

In Lupinus shoots electrical stimulus (DC) produces a voltagewave identical in character with the action potential in stimulatedsimple plant cells or in nerves. These action potentials wereregistered with a Kipp and Zonen Micrograph BD3, calomel electrodes,and an electrometer (input impedance, 10¹⁴ ). The wave form and its amplitude propagation velocity, pointof initiation, threshold value of the stimulus, and refractoryperiod were considered; the interdependence between these parametersand the magnitude and manner of application of the electricalstimulus are discussed. An analogy with Pflüger's laws was found.     

Changes in Cell Length During Action Potentials in Chara

Changes in cell length during excitation in Chara were recordedsimultaneously with extracellular action potentials. Cells stimulatedin artificial pond water (APW) gave a diphasic change in celllength ; that is, a transient shortening followed by a delayedextension. When a cell was stimulated 1–3 min after aprevious shortening, the extension phase was not evident, andthe amplitude of the shortening was always larger than the previousone. Cells stimulated in moist air gave shortenings with muchlarger amplitudes and much greater durations compared with thosein APW. From such marked differences in both amplitude and durationbetween the two types of shortening it is suggested that theshortening might be caused mainly by an osmotic water movementduring excitation. Net water loss during a single action potentialwas calculated from the cell shortening to be 1.076 nl cm^–2per impulse or 59800 pmol cm^–2 per impulse, which couldbe caused by a local enhancement of ionic concentration justoutside the plasmalemma of about 0.74 mN.     

Ionic Mechanisms for Electrical Heterogeneity between Rabbit Purkinje Fiber and Ventricular Cells

The intrinsic heterogeneity of electrical action potential (AP) properties between Purkinje fibers (PFs) and the ventricular wall, as well as within the wall, plays an important role in ensuring successful excitation of the ventricles. It can also be proarrhythmic due to nonuniform repolarization across the Purkinje-ventricular junction. However, the ionic mechanisms that underlie the marked AP differences between PFs and ventricular cells are not fully characterized. We studied such mechanisms by developing a new family of biophysically detailed AP models for rabbit PF cells and three transmural ventricular cell types. The models were based on and validated against experimental data recorded from rabbit at ionic channel, single cell, and tissue levels. They were then used to determine the functional roles of each individual ionic channel current in modulating the AP heterogeneity at the rabbit Purkinje-ventricular junction, and to identify specific currents responsible for the differential response of PFs and ventricular cells to pharmacological interventions.     

A Model for the Propagation of Action Potentials in Non-Uniformly Excitable Media

Electrophysiological properties of cardiac tissue change as a function of position. We define the "excitability" as the propagation velocity of an excitation pulse through the tissue, and study a simple FitzHugh-Nagumo (FHN) model of heart tissue whose excitability changes with position. The propagation velocity is shown to be a good continuous measure of the excitability for both limit cycle and excitable tissue. The influence of the spatial dependence of the excitability is examined for several normal and pathological situations. A novel transient effect is observed for a train of pulses propagating across an excitability step. Copyright 1999 Academic Press.     

A Dipole Model for Negative Steady-State Resistance in Excitable Membranes

A dipole model is presented for ion flow in excitable membranes. This model considers the membrane to be composed of two distinct regions: a polar region and a nonpolar region. Further, the construction of an electrodiffusive formalism which takes explicit account of the energy of partition required by an ion for passage from external fluid to nonpolar region is presented. In the polar region a cooperative effect is considered which produces a configurational transition of the polar group dependent only on membrane voltage. A resulting change in voltage drop across the polar group is brought about by this configurational transition. This gives rise to a negative steady-state resistance for the equimolar case, in reasonable agreement with observation. The theory, in addition, is in reasonable accord with nonequimolar ion flow, and provides an explanation for such effects as the following: the intercept of the voltage-current characteristic, the ion membrane concentrations inferred from electrodiffusion theories, and the effects of polyvalent cations     

Radiation Resistance of the Microflora Associated with Amniotic Membranes

Summary Amniotic membrane is widely used in the treatment of burn wounds and ulcers of various etiology. As it comes into contact with open wounds, it needs to be perfectly sterile to avoid the transmission of any disease. Accordingly, amniotic membrane needs to bear a high sterility assurance level (SAL). Conventionally, a radiation dose of 25 kGy is the generally accepted dose for sterilization. But to keep intact the biomechanical and other properties, it is sometimes proposed to use a lower dose without compromising an SAL of 10⁻⁶. The initial microbial contamination level and the radiation resistance of the contaminants determine the dose required for sterilization. The microbial species associated with the amniotic membrane from about 70 different batches were isolated. Twenty-two representative bacterial isolates were characterized and tested for survival in an incremental series of radiation doses from 0.5 to 5.0 kGy. The radiation decimal reduction dose (D₁₀) values for the strains were determined. Relatively higher D₁₀ values were recorded for the gram-positive isolates. The D₁₀ values of microbial isolates ranged from 0.16 to 1.3 kGy, and most resistant Bacillus strain had a D₁₀ value of 2.1 kGy. The radiation dose necessary to achieve an SAL of 10⁻⁶ was calculated based on the D₁₀values of the isolated strains. For a bioburden of 1000 Bacillus organism, the sterilization dose of 18.9 kGy is obtained. However, based on the experimental determination of D₁₀ of the radiation-resistant reference strain Bacillus pumilus, the adequate dose for radiation sterilization is found to be 19.8 kGy if bioburden level of 1000 is granted. The results substantiate that radiation dose of 25 kGy assures sterilization of amniotic membranes with bioburden level of 1000 colony forming units.     

Spontaneous All-or-Nothing Action Potentials in the Ciliate Bursaridium difficile

The electrical membrane properties and the swimming behaviour of the freshwater ciliate Bursaridium difficile were studied by current clamp recordings and video analysis. The resting membrane potential was –45 ± 6 mV (mean ± SD, n = 80), and the input resistance and membrane capacitance were 109 ± 42 megaohms (MΩ) (n = 63) and 457 ± 150 picofarads (pF) (n = 42), respectively. Based on an estimated surface area of 6.8 × 10^-4 cm², the corresponding specific membrane resistance and capacitance are 7.4 × 10⁴Ω× cm² and 0.7 μF/cm². Bursaridium difficile generates spontaneous, all-or-nothing action potentials with a well-defined threshold in normal medium. The spontaneous firing frequency was 0.22 ± 0.06 Hz (n = 80). The maximum rate of rise of the action potentials was less than 1 V/s, and they displayed a prolonged plateau phase (0.5–1 s). The action potentials were abolished in nominal Ca²⁺-free solution and are thus Ca²⁺-spikes. The swimming pattern of Bursaridium in homogeneous surroundings is composed of forward swimming periods interrupted by regular, short periods of backward swimming followed by a change in the forward swimming direction. The turning frequency corresponded to the spontaneous firing frequency, and only forward swimming was observed in nominal Ca²⁺-free solution. The periods of backward swimming activity are thus linked to the spontaneous action potentials.     

Multifocal Fluorescence Microscope for Fast Optical Recordings of Neuronal Action Potentials

In recent years, optical sensors for tracking neural activity have been developed and offer great utility. However, developing microscopy techniques that have several kHz bandwidth necessary to reliably capture optically reported action potentials (APs) at multiple locations in parallel remains a significant challenge. To our knowledge, we describe a novel microscope optimized to measure spatially distributed optical signals with submillisecond and near diffraction-limit resolution. Our design uses a spatial light modulator to generate patterned illumination to simultaneously excite multiple user-defined targets. A galvanometer driven mirror in the emission path streaks the fluorescence emanating from each excitation point during the camera exposure, using unused camera pixels to capture time varying fluorescence at rates that are ∼1000 times faster than the camera’s native frame rate. We demonstrate that this approach is capable of recording Ca²⁺ transients resulting from APs in neurons labeled with the Ca²⁺ sensor Oregon Green Bapta-1 (OGB-1), and can localize the timing of these events with millisecond resolution. Furthermore, optically reported APs can be detected with the voltage sensitive dye DiO-DPA in multiple locations within a neuron with a signal/noise ratio up to ∼40, resolving delays in arrival time along dendrites. Thus, the microscope provides a powerful tool for photometric measurements of dynamics requiring submillisecond sampling at multiple locations.     

Spatial Localization of Synapses Required for Supralinear Summation of Action Potentials and EPSPs

Although the supralinear summation of synchronizing excitatory postsynaptic potentials (EPSPs) and backpropagating action potentials (APs) is important for spike-timing-dependent synaptic plasticity (STDP), the spatial conditions of the amplification in the divergent dendritic structure have yet to be analyzed. In the present study, we simulated the coincidence of APs with EPSPs at randomly determined synaptic sites of a morphologically reconstructed hippocampal CA1 pyramidal model neuron and clarified the spatial condition of the amplifying synapses. In the case of uniform conductance inputs, the amplifying synapses were localized in the middle apical dendrites and distal basal dendrites with small diameters, and the ratio of synapses was unexpectedly small: 8-16% in both apical and basal dendrites. This was because the appearance of strong amplification requires the coincidence of both APs of 3-30 mV and EPSPs of over 6 mV, both of which depend on the dendritic location of synaptic sites. We found that the localization of amplifying synapses depends on A-type K+ channel distribution because backpropagating APs depend on the A-type K+ channel distribution, and that the localizations of amplifying synapses were similar within a range of physiological synaptic conductances. We also quantified the spread of membrane amplification in dendrites, indicating that the neighboring synapses can also show the amplification. These findings allowed us to computationally illustrate the spatial localization of synapses for supralinear summation of APs and EPSPs within thin dendritic branches where patch clamp experiments cannot be easily conducted.     

Conduction Velocity and Intracellular Action Potentials of the Tunicate Heart

The tubular heart of tunicates is composed of a single layer of myoendothelial cells. The direction of contraction reverses every few minutes. The conduction times in both directions are the same. Conduction velocity was greatest in the middle of the arms of the V-shaped heart and slowest in the apex. The greater the heart length, the greater was the conduction velocity. The Q₁₀ of conduction velocity was 2–2.3. Removal of the raphe which attaches the heart to the pericardium and removal of a line of undifferentiated cells opposite the raphe did not change the conduction velocity or prevent the heart from reversing the direction of conduction. The median resting potential of 42 cells was -71 mv and the median action potential was 75 mv. At 20°C the duration of the action potential was 1.2 sec and the maximal rate of depolarization was 3–10 v/sec. An increase in the beat frequency produced by electrically stimulating the heart decreased the resting potential, rate of rise, the duration, and the overshoot of the action potential. The shape of the action potential was sometimes different in the two directions of conduction. The electrophysiological evidence indicates only one cell type and suggests that the mode of the spread of excitation is by local current flow from cell to cell.     

Genesis of Epidermal Action Potentials in Cytokinesis Arrested Xenopus Embryos

When Xenopus embryos were treated continuously with cytochalasin B (3–10 μg/ml) from the 8 cell stage, cleavage arrested embryos in various degrees were observed. In 3–5 μg/ml cytochalasin B, cytokinesis was inhibited at the midblastula stage and pigment granules remained at the cell cortex of the animal pole. These cells showed epidermal like action potentials when the control embryos (St. 26/28) generated epidermal action potentials. In 5–7 μg/ml cytochalasin B, furrows, following their formation at early cleavage stages, regressed and no further cleavage from the 16 cell stage to morula stage took place. The pigment granules were dispersed throughout the interior of the cytoplasm. These cells showed no epidermal action potentials. Thus, it is considered that cytokinesis per sé , following the midblastula stage, is not a prerequisite for the genesis of epidermal action potentials, and that chronological times corresponding to the tailbud larva stage and a stable structure of the cellular cortex are required to bring about these potentials.     

Interaction of Horse Heart Cytochrome c with Lipid Bilayer Membranes: Effects on Redox Potentials

Cyclic voltammetry has been used to study the effects of interactions between horse cytochrome c and solid-supported planar lipid membranes, comprised of either egg phosphatidylcholine (PC) or PC plus 20 mol.% cardiolipin (CL), on the redox potential and the electrochemical electron transfer rate between the protein and a semiconductor electrode. Experiments were performed over a wide range of cytochrome c concentrations (0–440 M) at low (20 mM) and medium (160 mM) ionic strengths. Three types of electrochemical behavior were observed, which varied as a function of the experimental conditions. At very low cytochrome c concentration (0.1 M), and under conditions where electrostatic forces dominated the protein–lipid membrane interaction (i.e., low ionic strength with membranes containing CL), a redox potential (265 mV) and an electrochemical electron transfer rate constant (0.09s ^–1)were obtained which compare well with those measured in other laboratories using a variety of different chemical modifications of the working electrode. Two other electrochemical signals (not reported with chemically modified electrodes) were also observed to occur at higher cytochrome c concentrations with this membrane system, as well as with two other systems (membranes containing CL under medium ionic strength conditions, and PC only at low ionic strength). These involved positive shifts of the cytochrome c redox potential (by 40 and 60 mV) and large decreases in the electron transfer rate (to 0.03 and 0.003 s^–1). The observations can be rationalized in terms of a structural model of the cytochrome c–membrane interaction, in which association involves both electrostatic and hydrophobic forces and results in varying degrees of insertion of the protein into the hydrophobic interior of the membrane.     

Contraction and Action Potentials of Frog Heart Muscles Soaked in Sucrose Solution

Isolated auricles or ventricles from the frog continue to contract, either spontaneously or when stimulated, for from 2 to 4 hours after they are placed in isotonic sucrose solution. After the muscles stop contracting in sucrose solution, contractility is partially restored when the muscles are placed in chloride Ringer's. However, contractility is usually not restored if the muscles are placed in sulfate Ringer's. Ventricles soaked in sucrose solution at 4–7°C continue to contract for 12 to 24 hours and during the first few hours in sucrose solution the contractions often are enhanced. Several types of experiment indicate that the sucrose solution does replace the Ringer's in the extracellular space. Auricles and ventricles also continue to conduct action potentials, with an overshoot, for from 30 to 360 minutes after being placed in sucrose solution. Muscles soaked in sucrose until they are inexcitable rapidly recover in chloride Ringer's but often fail to recover in sulfate Ringer's. The results are discussed in relation to theories about the generation of the action potential in cardiac muscle, and the role of the extracellular fluid in contraction.     

Optical Mapping of Action Potentials and Calcium Transients in the Mouse Heart

The mouse heart is a popular model for cardiovascular studies due to the existence of low cost technology for genetic engineering in this species. Cardiovascular physiological phenotyping of the mouse heart can be easily done using fluorescence imaging employing various probes for transmembrane potential (V_m), calcium transients (CaT), and other parameters. Excitation-contraction coupling is characterized by action potential and intracellular calcium dynamics; therefore, it is critically important to map both V_m and CaT simultaneously from the same location on the heart^1-4. Simultaneous optical mapping from Langendorff perfused mouse hearts has the potential to elucidate mechanisms underlying heart failure, arrhythmias, metabolic disease, and other heart diseases. Visualization of activation, conduction velocity, action potential duration, and other parameters at a myriad of sites cannot be achieved from cellular level investigation but is well solved by optical mapping^1,5,6. In this paper we present the instrumentation setup and experimental conditions for simultaneous optical mapping of V_m and CaT in mouse hearts with high spatio-temporal resolution using state-of-the-art CMOS imaging technology. Consistent optical recordings obtained with this method illustrate that simultaneous optical mapping of Langendorff perfused mouse hearts is both feasible and reliable.     

Responses to Apical and Basolateral Application of Glutamate in Mouse Fungiform Taste Cells with Action Potentials

In taste bud cells, glutamate may elicit two types of responses, as an umami tastant and as a neurotransmitter. Glutamate applied to apical membrane of taste cells would elicit taste responses whereas glutamate applied to basolateral membrane may act as a neurotransmitter. Using restricted stimulation to apical or basolateral membrane of taste cells, we examined responses of taste cells to glutamate stimulation, separately. Apical application of monosodium glutamate (MSG, 0.3 M) increased firing frequency in some of mouse fungiform taste cells that evoked action potentials. These cells were tested with other basic taste compounds, NaCl (salty), saccharin (sweet), HCl (sour), and quinine (bitter). MSG-sensitive taste cells could be classified into sweet-best (S-type), MSG-best (M-type), and NaCl or other electrolytes-best (N- or E/H-type) cells. Furthermore, S- and M-type could be classified into two sub-types according to the synergistic effect between MSG and inosine-5′-monophosphate (S1, M1 with synergism; S2, M2 without synergism). Basolateral application of glutamate (100 μM) had almost no effect on the mean spontaneous firing rates in taste cells. However, about 10% of taste cells tested showed transient increases in spontaneous firing rates (>mean + 2 standard deviation) after basolateral application of glutamate. These results suggest the existence of multiple types of umami-sensitive taste cells and the existence of glutamate receptor(s) on the basolateral membrane of a subset of taste cells.