Space-Clamp Problems When Voltage Clamping Neurons Expressing Voltage-Gated Conductances

2008 ◽  
Vol 99 (3) ◽  
pp. 1127-1136 ◽  
Author(s):  
Dan Bar-Yehuda ◽  
Alon Korngreen

The voltage-clamp technique is applicable only to spherical cells. In nonspherical cells, such as neurons, the membrane potential is not clamped distal to the voltage-clamp electrode. This means that the current recorded by the voltage-clamp electrode is the sum of the local current and of axial currents from locations experiencing different membrane potentials. Furthermore, voltage-gated currents recorded from a nonspherical cell are, by definition, severely distorted due to the lack of space clamp. Justifications for voltage clamping in nonspherical cells are, first, that the lack of space clamp is not severe in neurons with short dendrites. Second, passive cable theory may be invoked to justify application of voltage clamp to branching neurons, suggesting that the potential decay is sufficiently shallow to allow spatial clamping of the neuron. Here, using numerical simulations, we show that the distortions of voltage-gated K+ and Ca2+ currents are substantial even in neurons with short dendrites. The simulations also demonstrate that passive cable theory cannot be used to justify voltage clamping of neurons due to significant shunting to the reversal potential of the voltage-gated conductance during channel activation. Some of the predictions made by the simulations were verified using somatic and dendritic voltage-clamp experiments in rat somatosensory cortex. Our results demonstrate that voltage-gated K+ and Ca2+ currents recorded from branching neurons are almost always severely distorted.

1990 ◽  
Vol 64 (4) ◽  
pp. 1077-1088 ◽  
Author(s):  
P. A. Rutecki ◽  
F. J. Lebeda ◽  
D. Johnston

1. The epileptiform discharges in the CA3 region of the rat hippocampal slice produced by bath application of the potassium channel blocker tetraethylammonium (TEA) were investigated. The effects of a convulsant (5 mM) and subconvulsant (0.5 mM) concentration of TEA on the mossy fiber-evoked synaptic currents were studied by the use of voltage-clamp techniques to determine whether TEA, like 4-aminopyridine (4-AP), another potassium channel blocker and convulsant, increased both inhibitory and excitatory components of the synaptic response. 2. At extracellular potassium concentrations of 2.5 mM, TEA (5 mM) was found to produce spontaneously occurring epileptiform discharges that could be recorded extracellularly. The intracellular correlate of the epileptiform discharge, the paroxysmal depolarizing shift (PDS), could be reversed in polarity by depolarizing the membrane and was associated with a large increase in membrane conductance. These results suggest that a synaptically mediated potential underlies the generation of the epileptiform discharge. 3. The reversal potential for the PDS was dependent on the time, relative to the extracellularly recorded field discharge, at which the measurement was made. In current clamp the mean reversal potential of the PDS measured at the midpoint of the extracellular discharge was -3.3 +/- 2.9 (SE) mV (n = 9). The reversal potential of the PDS was considerably more negative when measured either before or after the midpoint of the extracellular discharge, suggesting the presence of an inhibitory synaptic component. In voltage clamp similar results were obtained and a large conductance change was found to be associated with the PDS. These results suggest that the synaptic conductance associated with the PDS has both inhibitory and excitatory components. 4. TEA increased significantly the mossy fiber-evoked, early-inhibitory conductance. A convulsant concentration (5 mM) increased the conductance measured 15 ms after the stimulus from 39.7 +/- 8.7 to 87.2 +/- 8.0 nS (n = 6). The reversal potential associated with the conductance depolarized from -68.3 +/- 3.4 to -58.3 +/- 4.0 mV after 5 mM TEA. A subconvulsant concentration of TEA (0.5 mM) also increased the conductance of the mossy fiber-evoked response at 15 ms after the stimulus from 49.5 +/- 3.1 to 63.1 +/- 6.1 nS (n = 4) without an associated shift in reversal potential. 5. The late-inhibitory component of the mossy fiber-evoked response, when present, was increased by 5 mM TEA and unchanged by 0.5 mM TEA. 6. The excitatory mossy fiber-evoked synaptic current was studied in the presence of picrotoxin and was found to be increased and prolonged by 5 mM TEA.(ABSTRACT TRUNCATED AT 400 WORDS)


2008 ◽  
Vol 99 (2) ◽  
pp. 1020-1031 ◽  
Author(s):  
Magnus J. E. Richardson ◽  
Gilad Silberberg

Accurate measurement of postsynaptic potential amplitudes is a central requirement for the quantification of synaptic strength, dynamics of short-term and long-term plasticity, and vesicle-release statistics. However, the intracellular voltage is a filtered version of the underlying synaptic signal and so a method of accounting for the distortion caused by overlapping postsynaptic potentials must be used. Here a voltage-deconvolution technique is demonstrated that defilters the entire voltage trace to reveal an underlying signal of well-separated synaptic events. These isolated events can be cropped out and reconvolved to yield a set of isolated postsynaptic potentials from which voltage amplitudes may be measured directly—greatly simplifying this common task. The method also has the significant advantage of providing a higher temporal resolution of the dynamics of the underlying synaptic signal. The versatility of the method is demonstrated by a variety of experimental examples, including excitatory and inhibitory connections to neurons with passive membranes and those with activated voltage-gated currents. The deconvolved current-clamp voltage has many features in common with voltage-clamp current measurements. These similarities are analyzed using cable theory and a multicompartment cell reconstruction, as well as direct comparison to voltage-clamp experiments.


1993 ◽  
Vol 70 (6) ◽  
pp. 2584-2595 ◽  
Author(s):  
P. Branchereau ◽  
J. Champagnat ◽  
M. Denavit-Saubie

1. Ionic conductances controlled by type A and type B cholecystokinin (CCK) receptors were studied in neurons of the rat nucleus tractus solitarius (NTS) and dorsal motor nucleus of the vagus (DMNV), using intracellular and whole-cell patch clamp recordings in current or voltage clamp configuration during bath application of agonists (CCK8, CCK4, BC 264) and antagonists. 2. CCKA receptor-related inhibition was associated with a membrane hyperpolarization and a decrease in input resistance that developed 2-6 min after the arrival of drug into the extracellular medium. These effects were induced by 5 nM CCK8 but not BC 264 and they were blocked by the CCKA antagonist, L-364,718, but not by the CCKB antagonist, L-365,260. 3. CCKA receptor-related inhibition was generated by a potassium current that reversed at a reversal potential E(rev) of -73 +/- 1 (mean +/- SE) mV with bathing potassium concentration [K+]o = 6 mM and at -88 +/- 1 with [K+]o = 3 mM, in agreement with the Nernst equation for potassium ions. 4. CCKB receptor-related excitation was associated with a membrane depolarization and an increase of the input resistance induced by the following agonists at threshold concentrations: CCK8 (0.2 nM) > or = BC 264 (0.4 nM) > CCK4 (10.9 nM). The increase of input resistance was abolished by L-365,260 and was maintained after blockade of the CCKA current by L-364,718. 5. CCKB receptor-related excitation, in the neurons (30% of cases) in which clear response reversal was observed, appeared to be generated by a decrease of a potassium conductance. Responses showed a reversal potential E(rev) of -68 +/- 4 mV with [K+]o = 6 mM and -89 +/- 1 mV with [K+]o = 3 mM, verifying predictions from the Nernst equation applied to potassium ions. However, in 70% of cases, clear reversal was not observed at membrane potentials negative to the theoretical potassium equilibrium potential EK. 6. In voltage clamp studies, CCK8 induced a 181 +/- 17 pA inward current associated with a 26 +/- 4% decrease in the instantaneous current (I(ins)) generated by hyperpolarizing voltage steps. This effect on I(ins) was demonstrated in the absence of effects on the outward noninactivating potassium current (IM) and on the inward noninactivating cationic current (IQ). 7. CCKB receptor-mediated excitation was not suppressed by cobalt, a blocker of calcium currents, and was not associated with a change of the calcium-dependent potassium current (IK(Ca)).(ABSTRACT TRUNCATED AT 400 WORDS)


2018 ◽  
Vol 114 (3) ◽  
pp. 477a
Author(s):  
Zakany Florina ◽  
Ferenc Papp ◽  
Gyorgy Panyi ◽  
Zoltan Varga

1986 ◽  
Vol 55 (6) ◽  
pp. 1115-1135 ◽  
Author(s):  
D. G. Owen ◽  
M. Segal ◽  
J. L. Barker

Current and voltage-clamp recordings were made at room temperature from cultured mouse spinal neurons using conventional two-electrode voltage-clamp techniques and electrodes filled with either 3 M KCl, 3 M CsCl, or 3 M Cs2SO4. In the presence of tetraethylammonium and tetrodotoxin, “fast” (rapidly rising and falling) action potentials (FAP) of variable duration were recorded in most neurons. “Slow” (slowly rising and falling) depolarizing potentials (SDP) occurred in 23% of the cells, when using KCl-filled electrodes, and in 82% of the cells with CsCl-filled electrodes. The SDP was frequently preceded by an FAP, although in some cells activation of the SDP occurred before the FAP threshold was reached and in a graded fashion. Both the FAP and SDP were abolished by Cd2+ and other Ca2+ antagonists. In cells exhibiting SDPs, voltage-clamp analysis revealed a sustained (noninactivating) inward current (Isin) during depolarizing steps to potentials more positive than -45 mV. Repolarizing steps resulted in slowly decaying inward tail currents (Itail). Both Isin and Itail were abolished in solutions nominally free of Cao2+, or containing Ca2+-channel antagonists. Bao2+ did not support Isin. The data indicated a U-shaped activation curve for Isin, peaking at about -10 mV. Activation of Isin occurred exponentially with a time constant of approximately 140 ms at -23 mV, becoming faster at more depolarized potentials (ca. 50 ms at -2 mV). Deactivation was slow, giving rise to tail currents lasting seconds. In some cases deactivation could be described by a single exponential process, although frequently the kinetics were more complex. Deactivation was faster at hyperpolarized potentials and sensitive to extracellular ([Ca2+]o), duration of activating voltage steps, and the degree of activation of Isin. Using CsCl-filled electrodes, the reversal potential (Erev) for Isin was -1.7 mV (SEM 3.5 mV, n = 20). Erev always corresponded to the reversal potential for gamma-aminobutyric acid-evoked currents in the same cell. In experiments in which Cs2SO4-filled electrodes were used, Erev was estimated to be -44 mV (SEM 2.3 mV, n = 9). Neither complete substitution of Nao+ with choline ions nor elevation of [K+]o 10-fold significantly affected the estimated Erev. However, substitution of Cl0- with isethionate or methanesulphonate increased the amplitude of inward currents (recorded with CsCl-filled electrodes) and shifted Erev to more depolarized potentials. The results indicate that Cl- are the primary charge carriers for this current and that Cai2+ is required for its activation, leading us to identify it as ICl(Ca).(ABSTRACT TRUNCATED AT 400 WORDS)


1999 ◽  
Vol 82 (5) ◽  
pp. 2415-2427 ◽  
Author(s):  
M. S. Yeoman ◽  
P. R. Benjamin

We have used a combination of current-clamp and voltage-clamp techniques to characterize the electrophysiological properties of enzymatically dissociated Lymnaea heart ventricle cells. Dissociated ventricular muscle cells had average resting membrane potentials of −55 ± 5 mV. When hyperpolarized to potentials between −70 and −63 mV, ventricle cells were capable of firing repetitive action potentials (8.5 ± 1.2 spikes/min) that failed to overshoot 0 mV. The action potentials were either simple spikes or more complex spike/plateau events. The latter were always accompanied by strong contractions of the muscle cell. The waveform of the action potentials were shown to be dependent on the presence of extracellular Ca2+ and K+ ions. With the use of the single-electrode voltage-clamp technique, two types of voltage-gated K+ currents were identified that could be separated by differences in their voltage sensitivity and time-dependent kinetics. The first current activated between −50 and −40 mV. It was relatively fast to activate (time-to-peak; 13.7 ± 0.7 ms at +40 mV) and inactivated by 53.3 ± 4.9% during a maintained 200-ms depolarization. It was fully available for activation below −80 mV and was completely inactivated by holding potentials more positive than −40 mV. It was completely blocked by 5 mM 4-aminopyridine (4-AP) and by concentrations of tetraethylammonium chloride (TEA) >10 mM. These properties characterize this current as a member of the A-type family of voltage-dependent K+ currents. The second voltage-gated K+ current activated at more depolarized potentials (−30 to −20 mV). It activated slower than the A-type current (time-to-peak; 74.1 ± 3.9 ms at +40 mV) and showed little inactivation (6.2 ± 2.1%) during a maintained 200-ms depolarization. The current was fully available for activation below −80 mV with a proportion of the current still available for activation at potentials as positive as 0 mV. The current was completely blocked by 1–3 mM TEA. These properties characterize this current as a member of the delayed rectifier family of voltage-dependent K+ currents. The slow activation rates and relatively depolarized activation thresholds of the two K+ currents are suggestive that their main role is to contribute to the repolarization phase of the action potential.


1998 ◽  
Vol 80 (1) ◽  
pp. 262-269 ◽  
Author(s):  
John A. White ◽  
Ruby Klink ◽  
Angel Alonso ◽  
Alan R. Kay

White, John A., Ruby Klink, Angel Alonso, and Alan R. Kay. Noise from voltage-gated ion channels may influence neuronal dynamics in the entorhinal cortex. J. Neurophysiol. 80: 262–269, 1998. Neurons of the superficial medial entorhinal cortex (MEC), which deliver neocortical input to the hippocampus, exhibit intrinsic, subthreshold oscillations with slow dynamics. These intrinsic oscillations, driven by a persistent Na+ current and a slow outward current, may help to generate the theta rhythm, a slow rhythm that plays an important role in spatial and declarative learning. Here we show that the number of persistent Na+ channels underlying subthreshold oscillations is relatively small (<104) and use a physiologically based stochastic model to argue that the random behavior of these channels may contribute crucially to cellular-level responses. In acutely isolated MEC neurons under voltage clamp, the mean and variance of the persistent Na+ current were used to estimate the single channel conductance and voltage-dependent probability of opening. A hybrid stochastic-deterministic model was built by using voltage-clamp descriptions of the persistent and fast-inactivating Na+ conductances, along with the fast and slow K+ conductances. All voltage-dependent conductances were represented with nonlinear ordinary differential equations, with the exception of the persistent Na+ conductance, which was represented as a population of stochastic ion channels. The model predicts that the probabilistic nature of Na+ channels increases the cell's repertoire of qualitative behaviors; although deterministic models at a particular point in parameter space can generate either subthreshold oscillations or phase-locked spikes (but rarely both), models with an appropriate level of channel noise can replicate physiological behavior by generating both patterns of electrical activity for a single set of parameters. Channel noise may contribute to higher order interspike interval statistics seen in vitro with DC current stimulation. Models with channel noise show evidence of spike clustering seen in brain slice experiments, although the effect is apparently not as prominent as seen in experimental results. Channel noise may contribute to cellular responses in vivo as well; the stochastic system has enhanced sensitivity to small periodic stimuli in a form of stochastic resonance that is novel (in that the relevant noise source is intrinsic and voltage-dependent) and potentially physiologically relevant. Although based on a simple model that does not include all known membrane mechanisms of MEC stellate cells, these results nevertheless imply that the stochastic nature of small collections of molecules may have important effects at the cellular and network levels.


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