Effects of membrane polarization on sarcoplasmic calcium release in skeletal muscle

Calcium release from the sarcoplasmic reticulum was investigated in voltage-clamped, tetrodotoxin-treated frog skeletal muscle fibres injected with arsenazo III. Short (5 ms) depolarizing pulses (test pulses) produced a transient change in arsenazo III absorption, signalling an increase in intracellular calcium in concentration (calcium transient). Conditioning subthreshold depolarizations, which preceded the test pulse, potentiated the calcium transient triggered by the test pulse. Conditioning hyperpolarizations, applied either before or after the test pulse, inhibited the calcium transient. These effects of conditioning polarizations on the calcium transient may explain similar effects of subthreshold polarizations on muscle contraction that have previously been reported. The potentiating effect of subthreshold depolarizations was observed only when the test pulse was short (5 ms). The potentiating effect develops at -48 mV with a time constant of about 7 ms at 6.5 degrees C; this seems to be slower than that predicted by the potential spread from the surface along the tubular system. Thus, part of the effect could arise from the coupling process between tubular depolarization and calcium release.     

Soliton-Like Regimes and Excitation Pulse Reflection (Echo) in Homogeneous Cardiac Purkinje Fibers: Results of Numerical Simulations

On the basis of numerical simulations of the partial McAllister-Noble-Tsien equations quantitatively describing the dynamics of electrical processes in conductive cardiac Purkinje fibers we reveal unusual – soliton-like – regimes of interaction of nonlinear excitation pulses governing the heart contraction rhythm: reflection of colliding pulses instead of their annihilation. The phenomenological mechanism of the reflection effects is that in a narrow (but finite) range of the system parameters the traveling pulse presents a doublet consisting of a high-amplitude leader followed by a low-amplitude subthreshold wave. Upon collisions of pulses the leaders are annihilated, but subthreshold waves summarize becoming superthreshold and initiating two novel echo-pulses traveling in opposite directions. The phenomenon revealed presents an analogy to the effect of reflection of colliding nerve pulses, predicted recently, and can be of use in getting insight into the mechanisms of heart rhythm disturbances.     

Changes in membrane characteristics of heart muscle during inhibition

Membrane characteristics were studied in isolated muscle strands from auricles of frogs using the "square pulse" technique. Changes in the time course and spatial spread of subthreshold electrotonic potentials were measured. If acetylcholine is applied in concentrations which cause slowing or stoppage of the heart beat, the following changes are produced: (a) the length constant (λ) of the membrane is reduced, (b) the time constant is shortened. The effects are reversible and increase with acetylcholine concentration. The membrane changes caused by acetylcholine dimmish with time. It is concluded that during acetylcholine inhibition, as well as during vagal inhibition, the conductance of the muscle membrane is increased. Appreciable changes in the resting membrane potential need not accompany inhibition.     

Temporal interaction between single spikes and complex spike bursts in hippocampal pyramidal cells

Cortical pyramidal cells fire single spikes and complex spike bursts. However, neither the conditions necessary for triggering complex spikes, nor their computational function are well understood. CA1 pyramidal cell burst activity was examined in behaving rats. The fraction of bursts was not reliably higher in place field centers, but rather in places where discharge frequency was 6-7 Hz. Burst probability was lower and bursts were shorter after recent spiking activity than after prolonged periods of silence (100 ms-1 s). Burst initiation probability and burst length were correlated with extracellular spike amplitude and with intracellular action potential rising slope. We suggest that bursts may function as "conditional synchrony detectors," signaling strong afferent synchrony after neuronal silence, and that single spikes triggered by a weak input may suppress bursts evoked by a subsequent strong input.     

Control of swimming in the hydrozoan jellyfish Aequorea aequorea: direct activation of the subumbrella

The epithelial cells that overlie the inner nerve ring of the hydrozoan jellyfish Aequorea aequorea were investigated ultrastructurally and electrophysiologically. The structurally unspecialized epithelial cells are interconnected by gap junctions and are electrically active during swimming as a single, long-duration action potential was recorded during each swim contraction. Intercellular electrical- and dye-coupling was demonstrated within the epithelial region extending into the velum and subumbrellar regions. Excitatory post-synaptic potentials were recorded from epithelial cells following swim motorneuron spikes with a short latency. Psps were up to 60 mV in amplitude and, when triggered in bursts, showed summation provided the interpulse interval was less than 25-35 ms. The initial gap in each of a series of bursts showed facilitation with the first few swim contractions following a period of inactivity. In actively swimming medusae, psp amplitude was relatively constant. The reversal potential for epithelial psp was estimated at between 0 and +20 mV. Spontaneous psps spread throughout the epithelial region electronically, but the amplitude decrease with conducting distance was less than that for current pulses injected into individual epithelial cells. This presumably represents the effect of widespread synaptic activation of epithelial cells via multiple input sites throughout the inner nerve ring as opposed to point-source input in current injection experiments. During a radial response, action potential amplitude was decreased and rise time increased due to decremental conduction through the inhibited region. It is postulated that conduction of a full action potential requires that electrotonic current spread from adjacent, active epithelial cells occur in synchrony with synaptic input from swim motoneurons.     

Auditory nerve and interneurone responses to natural sounds in several species of cicadas

ABSTRACT. The calling and courtship songs of 17-year cicadas and of Say's cicadas differ both in the sound frequency spectrum and in temporal pattern. Multiunit recordings with hook electrodes from the whole auditory nerve show that the hearing organs are especially sensitive to transient stimuli occurring in natural sounds. Artificially produced clicks elicit bursts of spikes synchronized among various primary sensory fibres. These fibres respond to natural calling and courtship songs with a specificity dependent on carrier frequency, rhythm and transient content of the sound, following sound pulses (i.e. tymbal actions) up to repetition rates of 200 Hz. An ascending, plurisegmental interneurone was characterized by intracellular recording and simultaneously stained with cobalt. Its main arborization spatially overlaps the anterior part of the sensory auditory neuropile, and the axon was traced as far as the prothoracic ganglion. Direct input from primary auditory fibres was suggested by latency measurements. Intracellular recordings from such neurons in different species show distinct auditory input, with phasic-tonic spike responses to tones. In general, the interneurone response is more species-specific to calling than to courtship songs, and the preferential response to the conspecific calling song is based primarily upon sound frequency content.     

Electrical Properties of the Pacemaker Neurons in the Heart Ganglion of a Stomatopod, Squilla oratoria

In the Squilla heart ganglion, the pacemaker is located in the rostral group of cells. After spontaneous firing ceased, the electrophysiological properties of these cells were examined with intracellular electrodes. Cells respond to electrical stimuli with all-or-none action potentials. Direct stimulation by strong currents decreases the size of action potentials. Comparison with action potentials caused by axonal stimulation and analysis of time relations indicate that with stronger currents the soma membrane is directly stimulated whereas with weaker currents the impulse first arises in the axon and then invades the soma. Spikes evoked in a neuron spread into all other neurons. Adjacent cells are interconnected by electrotonic connections. Histologically axons are tied with the side-junction. B spikes of adjacent cells are blocked simultaneously by hyperpolarization or by repetitive stimulation. Experiments show that under such circumstances the B spike is not directly elicited from the A spike but is evoked by invasion of an impulse or electrotonic potential from adjacent cells. On rostral stimulation a small prepotential precedes the main spike. It is interpreted as an action potential from dendrites.     

The inner life of bursts

In the thalamus, bursts and single spikes are elicited by distinct visual stimuli, suggesting distinct visual functions. In this issue of Neuron, Wang et al. make use of intracellular recordings of thalamic neurons in vivo to provide a clear, detailed explanation of how natural stimuli are converted into a neural code that uses both bursts and single spikes.     

Stem Extension Rate in Light-Grown Plants : Effects of Photo- and Thermoperiodic Treatments on the Endogenous Circadian Rhythm in Chenopodium rubrum

Low temperature pulses have two effects on the circadian rhythm exhibited by stem extension rate of green Chenopodium rubrum plants. First, low temperature pulses have the same effect on the phasing of the rhythm as a dark period interrupting continuous light. Second, low temperature pulses stimulate stem extension rate during the 10 hours immediately following the end of the pulse. A difference in temperature between soil and air increases this effect. In any case, it is the change in temperature which is essential and not a specific temperature. Effects of light and temperature on phasing and amplitude of the rhythm explain why the maximal stem growth is observed under normal photo-thermoperiodic conditions, i.e. a high temperature during the photoperiod and a low temperature during the dark period.     

Initiation and abolition of the action potential of a single node of Ranvier

1. Using single node preparations of the bull frog or the toad, observations were made on the variation of the voltage across the nodal membrane under various experimental conditions. 2. The time constant of the variation in the membrane voltage caused by a long subthreshold rectangular pulse was of the order of 0.1 msec. 3. The action potential was initiated when the potential inside the node was raised stimulating pulses above a threshold level of approximately 15 mv. for a node in normal Ringer; it was greater in a relatively refractory node and in a partially narcotized node. 4. The variation of the membrane voltage caused by long stimulating pulses of subrheobasic strengths was in general proportional to the strength of the applied pulse. A non-linear behavior of the membrane voltage was observed with barely subthreshold stimulating pulses. 5. The early portion of the action potential of a node was not modified by a direct current which was strong enough to produce measurable potential changes (IR drops) across the resting membrane. 6. A strong pulse of inward current applied to the node during activity abolished the portion of the action potential following the pulse in all-or-none manner. 7. There was no refractory period after a response abolished in its early phase. Following a response abolished later, the recovery in the spike height started from the level of the action potential at the time of abolition. 8. Initiation and abolition of action potentials at a single node are interpreted as "transitions" between the two "equilibrium potential levels" at the node.     

Demonstration of spontaneous and stretch induced urinary bladder EMG in the living rabbit

Spontaneous bladder EMG was recorded in the living rabbit from an isovolumetric bladder without chemical or electrical stimulation. Mechanical intervention, either by lifting the bladder out of the abdomen or by rapid filling, resulted in stretch induced bladder EMG. A self made epoxy resin electrode device that embedded 32 EMG recording electrodes in a matrix like pattern, each electrode Ag/AgCl, d = 0.6 mm with an interdistance of 2.3 mm, was used for registration. The recorder used a common average reference technique and a sample frequency of 400 Hz. A signal bandwidth of 0.05 to 108 Hz was available for analysis. Spontaneous EMG consisted of single spikes and bursts (2-20 spikes), but not of continuous activity. The shape of spikes was triphasic. Single spikes appeared with and without burst activity. Small (2-5 spikes) and large bursts (6-20 spikes) were discerned; small bursts not necessarily propagated across electrodes, large bursts did and were able to organize, suggesting that they were under short neuron system control. Spontaneous EMG was probably related to both contraction and relaxation. Stretch induced EMG was characterised by continuous activity on all electrodes, spikes that followed each other immediately, slowly fading away. The spikes had an elongated third phase when compared to the shape of spontaneous activity. Highest activity and amplitudes were found after lifting the bladder out of the abdomen and placing it on the electrode device. A concept is put forward in which the continuous activity is not unequivocally related to muscle shortening, but where the current stress and strain situation of the bladder tissue can cause a muscle fibre elongation upon the appearance of electrical activity. The EMG activity found was in many aspects similar to results of a previous study using mortalized rabbits. Artifact sources like the heart, respiration, or local movement between electrode and bladder could easily be identified due to the new experimental methodology used.     

Electrophysiological properties of human oviduct smooth muscle cells in dissociated cell culture.

Intracellular recordings were made from human oviduct smooth muscle maintained in cell culture. Solitary cells isolated from one another and cells in contact with one another retained electrical properties of smooth muscle in vivo. Membrane potential of solitary cells and connected cells was -35 mV. Connected cells formed electrotonic junctions which transmitted current from one cell to another. This current spread was responsible for differences in input resistance and time constant in solitary cells, 66 Momega and 96 msec, compared to connected cells, 26 Momega and 56 msec. All cells expressed delayed rectification to depolarizing current pulses. Some cells generated action potentials spontaneously or in response to intracellular current pulses. Action potentials were abolished by cobalt or by EGTA. Slow wave potentials, 5 . 20 mV in amplitude, occurred continuously once every 15 to 45 seconds in connected cells.     

Pacemaker Potentials for the Periodic Burst Discharge in the Heart Ganglion of a Stomatopod, Squilla oratoria

From somata of the pacemaker neurons in the Squilla heart ganglion, pacemaker potentials for the spontaneous periodic burst discharge are recorded with intracellular electrodes. The electrical activity is composed of slow potentials and superimposed spikes, and is divided into four types, which are: (a) "mammalian heart" type, (b) "slow generator" type, (c) "slow grower" type, and (d) "slow deficient" type. Since axons which are far from the somata do not produce slow potentials, the soma and dendrites must be where the slow potentials are generated. Hyperpolarization impedes generation of the slow potential, showing that it is an electrically excitable response. Membrane impedance increases on depolarization. Brief hyperpolarizing current can abolish the plateau but brief tetanic inhibitory fiber stimulation is more effective for the abolition. A single stimulus to the axon evokes the slow potential when the stimulus is applied some time after a previous burst. Repetitive stimuli to the axon are more effective in eliciting the slow potential, but the depolarization is not maintained on continuous stimulation. Synchronization of the slow potential among neurons is achieved by: (a) the electrotonic connections, with periodic change in resistance of the soma membrane, (b) active spread of the slow potential, and (c) synchronization through spikes.     

Circadian rhythm in endogenous nerve activity in the eye of Musca dornestica L.

The frequency of occurrence of endogenous bursts of spikes was monitored by external electrode placed on the surface of housefly eyes in darkness. In LD 16:8 the frequency of these bursts showed an entrained rhythm, with a c. 10-fold change in level from rest to active periods. The rate began to increase in anticipation of dawn. The free-running period in DD was c. 21 h and in LL, 16–17 h. The active/rest ratio was 1.0 in DD and 2.5 in LL, the active phase being 10.4 h in DD and 12.3 h in LL. In these respects the rhythm conforms to Aschoff's rule. In groups of flies, the entrained rhythm was apparently lost 4–6 days after transfer from LD to LL, because the individual flies' rhythms changed from the 24 h entrained state to the LL, free-running state at differing rates, leading to asynchrony. After four cycles the phase angles in a sample of ten flies differed by 120 (8 h). In contrast, when flies were transferred from LD to DD, the phase angle variation did not differ markedly, even after 9 days, from that of entrained flies. The findings are discussed in terms of Truman's (1972) clock types.     

Sub-MHz bursts of nanosecond pulses excite neurons at paradoxically low electric field thresholds without membrane damage

Neuromodulation applications of nanosecond electric pulses (nsEP) are hindered by their low potency to elicit action potentials in neurons. Excitation by a single nsEP requires a strong electric field which injures neurons by electroporation. We bypassed the high electric field requirement by replacing single nsEP stimuli with high-frequency brief nsEP bursts. In hippocampal neurons, excitation thresholds progressively decreased at nsEP frequencies above 20–200 kHz, with up to 20–30-fold reduction at sub-MHz and MHz rates. For a fixed burst duration, thresholds were determined by the duty cycle, irrespective of the specific nsEP duration, rate, or number of pulses per burst. For 100-μs bursts of 100-, 400-, or 800-ns pulses, the threshold decreased as a power function when the duty cycle exceeded 3–5 %. nsEP bursts were compared with single “long” pulses whose duration and amplitude matched the duration and the time-average amplitude of the burst. Such pulses deliver the same electric charge as bursts, within the same time interval. High-frequency nsEP bursts excited neurons at the time-average electric field 2–3 times below the threshold for a single long pulse. For example, the excitation threshold of 139 ± 14 V/cm for a single 100-μs pulse decreased to 57 ± 8 V/cm for a 100-μs burst of 100-ns, 0.25-MHz pulses (p < 0.001). Applying nsEP in bursts reduced or prevented the loss of excitability in multiple stimulation attempts. Stimulation by high-frequency nsEP bursts is a powerful novel approach to excite neurons at paradoxically low electric charge while also avoiding the electroporative membrane damage.     

Calcium bursts induced by nanosecond electric pulses

We report here real-time imaging of calcium bursts in human lymphocytes exposed to nanosecond, megavolt-per-meter pulsed electric fields. Ultra-short (less than 30 ns), high-field (greater than 1 MV/m), electric pulses induce increases in cytosolic calcium concentration and translocation of phosphatidylserine (PS) to the outer layer of the plasma membrane in Jurkat T lymphoblasts. Pulse-induced calcium bursts occur within milliseconds and PS externalization within minutes. Caspase activation and other indicators of apoptosis follow these initial symptoms of nanosecond pulse exposure. Pulse-induced PS translocation is observed even in the presence of caspase inhibitors. Ultra-short, high-field, electroperturbative pulse effects differ substantially from those associated with electroporation, where pulses of a few tens of kilovolts-per-meter lasting a few tens of microseconds open pores in the cytoplasmic membrane. Nanosecond pulsed electric fields, because their duration is less than the plasma membrane charging time, develop voltages across intracellular structures without porating the cell.     

Non-synaptic interaction between neurons in molluscs

1. Isolated pedal ganglia of the pteropodial mollusc, Clione limacina, generate a locomotory rhythm. In 30% of the pedal ganglia preparations the locomotory rhythm was not regular, i.e. the locomotor generator worked in “bursts” alternating with periods of low activity.2. The “locomotor bursts” were caused by spontaneous activation of command neurons located in the pedal ganglia.3. A single neuron was extracted from burst-generating preparations by means of the intracellular microelectrode and then its soma was put back, into the initial place between the ganglion cells. Twenty-five percent of the isolated neurons renewed the bursts-related changes in their activity after the insertion into the ganglion. The neurons which were originally excited during the “locomotor bursts” continued to be excited after isolation, while those which were inhibited continued to be inhibited during the bursts.4. It is suggested that the command neurons controlling the locomotor generator can exert action on the target cells in the absence of morphological synapses.     

Electrically triggered all-or-none Ca(2)+-liberation during action potential in the giant alga Chara.

Electrically triggered action potentials in the giant alga Chara corallina are associated with a transient rise in the concentration of free Ca(2)+ in the cytoplasm (Ca(2)+(cyt)). The present measurements of Ca(2)+(cyt) during membrane excitation show that stimulating pulses of low magnitude (subthreshold pulse) had no perceivable effect on Ca(2)+(cyt). When the strength of a pulse exceeded a narrow threshold (suprathreshold pulse) it evoked the full extent of the Ca(2)+(cyt) elevation. This suggests an all-or-none mechanism for Ca(2)+ mobilization. A transient calcium rise could also be induced by one subthreshold pulse if it was after another subthreshold pulse of the same kind after a suitable interval, i.e., not closer than a few 100 ms and not longer than a few seconds. This dependency of Ca(2)+ mobilization on single and double pulses can be simulated by a model in which a second messenger is produced in a voltage-dependent manner. This second messenger liberates Ca(2)+ from internal stores in an all-or-none manner once a critical concentration (threshold) of the second messenger is exceeded in the cytoplasm. The positive effect of a single suprathreshold pulse and two optimally spaced subthreshold pulses on Ca(2)+ mobilization can be explained on the basis of relative velocity for second messenger production and decomposition as well as the availability of the precursor for the second messenger production. Assuming that inositol-1,4,5,-trisphosphate (IP(3)) is the second messenger in question, the present data provide the major rate constants for IP(3) metabolism.     

Efficient inhibition of bursts by bursts in the auditory system of crickets

In crickets, auditory information about ultrasound is carried bilaterally to the brain by the AN2 neurons. The ON1 neuron provides contralateral inhibitory input to AN2, thereby enhancing bilateral contrast between the left and right AN2s, an important cue for sound localization. We examine how the structures of the spike trains of these neurons affect this inhibitory interaction. As previously shown for AN2, ON1 responds to salient peaks in stimulus amplitude with bursts of spikes. Spike bursts, but not isolated spikes, reliably signal the occurrence of specific features of the stimulus. ON1 and AN2 burst at similar times relative to the amplitude envelope of the stimulus, and bursts are more tightly time-locked to stimulus feature than the isolated spikes. As a consequence, spikes that, in the absence of contralateral inhibition, would occur within AN2 bursts are more likely to be preceded by spikes in ON1 (mainly also in bursts) than are isolated AN2 spikes. This leads to a large decrease in the burst rate of the inhibited AN2. We conclude that the match in coding properties of ON1 and AN2 allows contralateral inhibition to be most efficient for those portions of the response that carry the behaviourally relevant information, i.e. for bursts. Electronic supplementary material The online version of this article (doi:) contains supplementary material, which is available to authorized users.     

On the electrotonic spread in cardiac muscle of the mouse

As an appropriate model which can simulate the cardiac working muscle with respect to the passive electrical spread, a lattice whose sides have linear cable properties is presented, and the passive potential spread on the model is mathematically analyzed in the fiber direction. Distribution of electrotonic potential in the fiber direction was measured with a pair of intracellular microelectrodes in the cardiac muscle fiber of mouse. By employing “pencil type” microelectrodes potential distribution in the transverse direction within a fiber was also measured. This transverse effect was differentiated from the longitudinal potential distribution. A tonically applied potential at any point of a cell interior spreads continuously in a manner described by a Bessel function. Using appropriate electrical and morphological parameters the experimental results proved to fit the curve obtained from numerical calculation on the model. The apparent length constant obtained for smaller distances (less than 100 μ) from the current source was 70 μ, and it increases as the distance becomes larger. At a point inside the fiber the resistance to the extracellular fluid ranged from 200 to 600 KΩ. The influence of coupling resistance between current and recording electrodes on the measurement of electrotonic potential was examined for small interelectrode distance.