Opening rate of acetylcholine receptor channels.

The nicotinic acetylcholine (ACh) receptor is responsible for rapid conversion of chemical signals to electrical signals at the neuromuscular junction. Because the receptor and its ion channel are components of a single transmembrane protein, the time between ACh binding and channel opening can be minimized. To determine just how quickly the channel opens, we made rapid (100-400 microseconds) applications of 0.1-10 mM ACh to outside-out, multichannel membrane patches from BC3H-1 cells, while measuring the onset of current flow through the channels at 11 degrees C. Onset time is steeply dependent upon ACh concentration when channel activation is limited by binding of ACh (0.1-1 mM). At +50 mV, the 20-80% onset time reaches a plateau near 110 microseconds above 5 mM ACh as channel opening becomes rate limiting. Thus, we calculate the opening rate, beta = 12/ms, without reference to specific channel activation schemes. At -50 mV, the combination of a rapid, voltage-dependent block of channels by ACh with a finite solution exchange time distorts onset. To determine opening rate at -50 mV, we determine the kinetic parameters of block from "steady-state" current and noise analyses, assume a sequential model of channel activation/block, and numerically simulate current responses to rapid perfusion of ACh. Using this approach, we find beta = 15/ms. In contrast to the channel closing rate, the opening rate is relatively insensitive to voltage.     

Properties of single cardiac Na channels at 35 degrees C

Single Na channel currents were recorded in cell-attached patches of mouse ventricular myocytes with an improved patch clamp technique. Using patch pipettes with a pore diameter in the range of 200 nm, seals with a resistance of up to 4 T omega were obtained. Under those conditions, total noise could be reduced to levels as low as 0.590 pA rms at 20 kHz band width. At this band width, properties of single- channel Na currents were studied at 35 degrees C. Six out of a total of 23 patches with teraohm seals contained channel activity and five of these patches contained one and only one active channel. Amplitude histograms excluding transition points showed heterogenous distributions of levels. In one patch, part of the openings was approximately Gaussian distributed at different potentials yielding a slope conductance of 27 pS. The respective peak open probability at -10 mV was 0.26. The mean open time was determined at voltages between -60 and -10 mV by evaluation of the distribution of the event-related gaps in the center of the baseline noise to be approximately 40 microseconds at -60 mV and 50-74 microseconds between -50 and -10 mV. It is concluded that single cardiac Na channels open at 35 degrees C frequently with multiple levels and with open times in the range of several tens of microseconds.     

On the kinetics of large-conductance glutamate-receptor ion channels in rat cerebellar granule neurons

Ion channels activated by glutamate, aspartate, and N-methyl-D-aspartate (NMDA) have been investigated in outside-out patches from cultured cerebellar granule neurons of the rat. Openings of these channels occur in bursts, within which the individual openings are separated by brief shuttings or gaps. The shut-time distributions obtained with each agonist were fitted with four exponential components. The briefest two components were considered as 'gaps within bursts'. Their mean time-constants were: glutamate, 58.0 microseconds and 592 microseconds; aspartate, 31.3 microseconds and 644 microseconds; NMDA, 40.5 microseconds and 903 microseconds. Distributions of burst durations were fitted with three exponential components. The mean time-constants obtained for the longest two components were: glutamate, 1.33 ms and 10.5 ms; aspartate, 2.15 ms and 10.3 ms; NMDA, 2.42 ms and 10.5 ms. Evidence is given that these two components of burst duration reflect the gating kinetics of 50 pS openings and not the fact that each agonist produces openings to more than one conductance level. Not only do openings occur in bursts, but these bursts were observed to occur in clusters, which can be hundreds of milliseconds long. We discuss the relation between the kinetics of single-channel openings observed in patches and the spectral components detected in whole-cell current noise.     

The role of intrinsic neuronal properties in the encoding of auditory information in the cochlear nuclei.

It is now possible to relate the intrinsic electrical properties of particular cells in the cochlear nuclei of mammals with their biological function. In the layered dorsal cochlear nucleus, information concerning the location of a sound source seems to be contained in the spatial pattern of activation of a population of neurons. In the unlayered, ventral cochlear nucleus, however, neurons carry information in their temporal firing patterns. The voltage-sensitive conductances that make responses to synaptic current brief enable bushy cells to convey signals from the auditory nerve to the superior olivary complex with a temporal precision of at least 120 microseconds.     

Rapid charge translocation by the cardiac Na(+)-Ca2+ exchanger after a Ca2+ concentration jump.

The kinetics of Na(+)-Ca2+ exchange current after a cytoplasmic Ca2+ concentration jump (achieved by photolysis of DM-nitrophen) was measured in excised giant membrane patches from guinea pig or rat heart. Increasing the cytoplasmic Ca2+ concentration from 0.5 microM in the presence of 100 mM extracellular Na+ elicits an inward current that rises with a time constant tau 1 < 50 microseconds and decays to a plateau with a time constant tau 2 = 0.65 +/- 0.18 ms (n = 101) at 21 degrees C. These current signals are suppressed by Ni2+ and dichlorobenzamil. No stationary current, but a transient inward current that rises with tau 1 < 50 microseconds and decays with tau 2 = 0.28 +/- 0.06 ms (n = 53, T = 21 degrees C) is observed if the Ca2+ concentration jump is performed under conditions that promote Ca(2+)-Ca2+ exchange (i.e., no extracellular Na+, 5 mM extracellular Ca2+). The transient and stationary inward current is not observed in the absence of extracellular Ca2+ and Na+. The application of alpha-chymotrypsin reveals the influence of the cytoplasmic regulatory Ca2+ binding site on Ca(2+)-Ca2+ and forward Na(+)-Ca2+ exchange and shows that this site regulates both the transient and stationary current. The temperature dependence of the stationary current exhibits an activation energy of 70 kj/mol for temperatures between 21 degrees C and 38 degrees C, and 138 kj/mol between 10 degrees C and 21 degrees C. For the decay time constant an activation energy of 70 kj/mol is observed in the Na(+)-Ca2+ and the Ca(2+)-Ca2+ exchange mode between 13 degrees C and 35 degrees C. The data indicate that partial reactions of the Na(+)-Ca2+ exchanger associated with Ca2+ binding and translocation are very fast at 35 degrees C, with relaxation time constants of about 6700 s-1 in the forward Na(+)-Ca2+ exchange and about 12,500 s-1 in the Ca(2+)-Ca2+ exchange mode and that net negative charge is moved during Ca2+ translocation. According to model calculations, the turnover number, however, has to be at least 2-4 times smaller than the decay rate of the transient current, and Na+ inward translocation appears to be slower than Ca2+ outward movement.     

Voltage clamp of the cardiac sodium current at 37 degrees C in physiologic solutions.

The cardiac sodium current was studied in guinea pig ventricular myocytes using the cell-attached patch voltage clamp at 37 degrees C in the presence of 145 mM external sodium concentration. When using large patch pipettes (access resistance, 1-2 M omega), the capacity current transient duration was typically 70 microseconds for voltage clamp steps up to 150 mV. At 37 degrees C the maximum inward sodium current peaked in approximately 200 microseconds after the onset of a clamp step and at this strong depolarization, less than 10% of the sodium current developed during the capacity transient. The sodium current developed smoothly and the descending limb of the current-voltage relationship usually spanned a range of 40 mV. Moreover, currents reduced by inactivation of sodium channels could be scaled to superimpose on the maximum current. Current tails elicited by deactivation followed a monoexponential time course that was very similar for currents of different sizes. Data obtained over a range of temperatures (15 degrees-35 degrees C) showed that the steady-state inactivation and conductance-voltage curves were shifted to more negative voltages at lower temperatures. These results demonstrate the feasibility of investigating the sodium current of mammalian cardiac cells at 37 degrees C in normal physiological solutions.     

Selective labeling and rotational diffusion of the ADP/ATP translocator in the inner mitochondrial membrane

Submitochondrial particles were labeled with the triplet probe eosin-5-maleimide (EMA) after pretreatment with N-ethylmaleimide. On sodium dodecyl sulfate-polyacrylamide gels, eosin fluorescence occurred in a single band of Mr approximately 30,000. The labeled band was identified as the ADP/ATP translocator, since EMA binding was completely inhibited by carboxyatractylate. Furthermore, the EMA-labeled polypeptide had the same molecular weight as the purified carboxyatractylate-bound translocator and the purified EMA-labeled translocator. Rotational diffusion of the translocator around the membrane normal in submitochondrial particles was measured by observing flash-induced absorption anisotropy of EMA. The translocator rotates with a time constant which varied from approximately 240 microseconds at 5 degrees C to approximately 100 microseconds at 37 degrees C. However, it is likely that only a fraction of the translocator rotates, the remainder being immobile over the measurement time of 500 microseconds. The mobile fraction of the translocator decreased with decrease in temperature. The observed fluorescence anisotropy of 0.24 indicates that EMA undergoes subnanosecond rapid wobbling in the binding site of the ADP/ATP translocator.     

Cell-attached patch clamp study of the electropermeabilization of amphibian cardiac cells.

Potential gradients imposed across cell or lipid membranes break down the insulating properties of these barriers if an intensity and time-dependent threshold is exceeded. Potential gradients of this magnitude may occur throughout the body, and in particular in cardiac tissue, during clinical defibrillation, ablation, and electrocution trauma. To study the dynamics of membrane electropermeabilization a cell-attached patch clamp technique was used to directly control the potential across membrane patches of single ventricular cells enzymatically isolated from frog (Rana pipiens) hearts. Ramp waveshapes were used to reveal rapid membrane conductance changes that may have otherwise been obscured using rectangular waveshapes. We observed a step increase (delta t less than 30 microseconds) or breakdown in membrane conductance at transmembrane potential thresholds of 0.6-1.1 V in response to 0.1-1.0 kV/s voltage ramps. Conductance kinetics on a sub-millisecond time scale indicate that breakdown is preceded by a period of instability during which the noise and amplitude of the membrane conductance begin to increase. In some cells membrane breakdown was observed to be fully reversible when using an intershock interval of 1 min (20-23 degrees C). These findings support energetic models of membrane electropermeabilization which describe the formation of membrane pores (or growth of existing pores) to a conducting state (instability), followed by a rapid expansion of these pores when the energy barrier for the formation of hydrophilic pores is overcome (breakdown).     

Kinetic constants of the acetylcholine (ACh) receptor reaction deduced from the rise in open probability after steps in ACh concentration.

Outside-out patches of enzymatically dissociated adult and denervated mouse muscle fibers were superfused repetitively by pulses of acetylcholine (ACh) containing solution. Up to 300 channels opened simultaneously 300 microseconds after the beginning of a 1,000 microM ACh pulse corresponding to a peak current i of almost -1 nA. Single responses to ACh were averaged and the concentration dependence of i and of the rise time tr from 0.1 i to 0.9 i was measured. In adult receptors, i increased proportional to the second to third power of ACh concentration, whereas in embryonic-type receptors it was proportional to the first to the second power. tr increased from approximately 0.3 ms at 1,000 microM ACh to a plateau value of approximately 5 ms for adult and of approximately 10 ms for embryoniclike receptors at concentrations less than 10 microM ACh. The concentration dependence of i and tr was simulated using the standard model of ACh binding with different combinations of rate constants and two and three binding sites for ACh. The calculated curves were compared to the measurements and a set of well fitting rate constants was determined for adult and embryoniclike receptors. Three binding sites for ACh were necessary to fit the dose response for i for adult receptors. A method for deriving rate constants in a model of ACh-receptor interaction is described that avoids analysis of open-closed kinetics of single channels, which in rapid systems, as the ones studied here, are at the limit of the frequency response of the current measurement.     

Primary and secondary electron donors in photosystem II of chloroplasts. Rates of electron transfer and location in the membrane.

Absorption changes at 820 or 515 nm after a short laser flash were studied comparatively in untreated chloroplasts and in chloroplasts in which oxygen evolution is inhibited. In chloroplasts pre-treated with Tris, the primary donor of Photosystem II (P-680) is oxidized by the flash it is re-reduced in a biphasic manner with half-times of 6 microseconds (major phase) and 22 microseconds. After the second flash, the 6 microseconds phase is nearly absent and P-680+ decays with half-times of 130 microseconds (major phase) and 22 microseconds. Exogenous electron donors (MnCl2 or reduced phenylenediamine) have no direct influence on the kinetics of P-680+. In untreated chloroplasts the 6 and 22 microseconds phases are of very small amplitude, either at the 1st, 2nd or 3rd flash given after dark-adaptation. They are observed, however, after incubation with 10 mM hydroxylamine. These results are interpreted in terms of multiple pathways for the reduction of P-680+: a rapid reduction (less than 1 microseconds) by the physiological donor D1; a slower reduction (6 and 22 microseconds) by donor D'1, operative when O2 evolution is inhibited; a back-reaction (130 microseconds) when D'1 is oxidized by the pre-illumination in inhibited chloroplasts. In Tris-treated chloroplasts the donor system to P-680+ has the capacity to deliver only one electron. The absorption change at 515 nm (electrochromic absorption shift) has been measured in parallel. It is shown that the change linked to Photosystem II activity has nearly the same magnitude in untreated chloroplasts or in chloroplasts treated with hydroxylamine or with Tris (first and subsequent flashes). Thus we conclude that all the donors (P-680, D1, D'1) are located at the internal side of the thylakoid membrane.     

Gating current kinetics in Myxicola giant axons. Order of the back transition rate constants.

Gating current, Ig, was recorded in Myxicola axons with series resistance compensation and higher time resolution than in previous studies. Ig at ON decays as two exponentials with time constants, tau ON-F and tau ON-S, very similar to squid values. No indication of an additional very fast relaxation was detected, but could be still unresolved. Ig at OFF also displays two exponentials, neither reflecting recovery from charge immobilization. Deactivation of the two I(ON) components may proceed with well-separated exponentials at -100 mV. INa tail currents at OFF also display two exponentials plus a third very slow relaxation of 5-9% of the total tail current. The very slow component is probably deactivation of a very small subpopulation of TTX sensitive channels. A -100 mV, means for INa tail component time constants (four axons) are 76 microseconds (range: 53-89 microseconds) and 344 microseconds (range: 312-387 microseconds), and for IOFF (six axons) 62 microseconds (range: 34-87 microseconds) and 291 microseconds (range: 204-456 microseconds) in reasonable agreement. INa ON activation time constant, tau A, is clearly slower than tau ON-F at all potentials. Except for the interval -30 to -15 mV, tau A is clearly faster than tau ON-S, and has a different dependency on potential. tau ON-S is several fold smaller than tau h. Computations with a closed2----closed1----open activation model indicated Na tail currents are consistent with a closed1----open rate constant greater than the closed2----closed1.     

On the slowly rising phase of the sodium gating current in the squid giant axon.

High-resolution records of the sodium gating current in the squid giant axon demonstrate the existence of a slowly rising phase that is first apparent at pulse potentials slightly below zero, and becomes increasingly pronounced at more positive potentials. At +80 mV the current reaches its peak with a delay of 30 microseconds at 10 degrees C. It is suggested that this current is generated by the first two steps labelled R-->P and P-->A in the S4 units of all four domains of the series-parallel gating system, activating the channel before its opening by the third steps A-->B in domains I, II and III in conjunction with hydration. The kinetics of the slowly rising phase can only be explained by the incorporation of an appropriate degree of voltage-dependent cooperativity between the S4 voltage-sensors for their two initial transitions.     

Sodium and gating current time shifts resulting from changes in initial conditions

The sodium and gating currents of the squid giant axon elicited by a depolarizing pulse are delayed, with little change in shape, as a result of a hyperpolarizing prepulse. The delays are almost completely saturated, at approximately 45 microseconds, for prepulses to -140 mV. At 8 degrees C they develop with time constants of between 60 and 180 microseconds for prepulses in the -130- to -150-mV range. There is a correlation between the extra charge moved during the gating current and the increase in the time delay of the sodium current as the magnitude of the hyperpolarizing prepulse is increased. These results strengthen the conclusion that the gating current is indeed closely associated with the process of sodium channel opening and provide information concerning the kinetics of the early steps, which are hidden in ionic current measurements. The main features of the gating and sodium current time shifts and the correlation between charge movement and time shifts are duplicated by a sequential six-state model for sodium activation.     

Sodium current in voltage clamped internally perfused canine cardiac Purkinje cells.

Study of the excitatory sodium current (INa) intact heart muscle has been hampered by the limitations of voltage clamp methods in multicellular preparations that result from the presence of large series resistance and from extracellular ion accumulation and depletion. To minimize these problems we voltage clamped and internally perfused freshly isolated canine cardiac Purkinje cells using a large bore (25-microns diam) double-barreled flow-through glass suction pipette. Control of [Na+]i was demonstrated by the agreement of measured INa reversal potentials with the predictions of the Nernst relation. Series resistance measured by an independent microelectrode was comparable to values obtained in voltage clamp studies of squid axons (less than 3.0 omega-cm2). The rapid capacity transient decays (tau c less than 15 microseconds) and small deviations of membrane potential (less than 4 mV at peak INa) achieved in these experiments represent good conditions for the study of INa. We studied INa in 26 cells (temperature range 13 degrees-24 degrees C) with 120 or 45 mM [Na+]o and 15 mM [Na+]i. Time to peak INa at 18 degrees C ranged from 1.0 ms (-40 mV) to less than 250 microseconds (+ 40 mV), and INa decayed with a time course best described by two time constants in the voltage range -60 to -10 mV. Normalized peak INa in eight cells at 18 degrees C was 2.0 +/- 0.2 mA/cm2 with [Na+]o 45 mM and 4.1 +/- 0.6 mA/cm2 with [Na+]o 120 mM. These large peak current measurements require a high density of Na+ channels. It is estimated that 67 +/- 6 channels/micron 2 are open at peak INa, and from integrated INa as many as 260 Na+ channels/micron2 are available for opening in canine cardiac Purkinje cells.     

Properties of the fusion pore that forms during exocytosis of a mast cell secretory vesicle

During exocytosis, secretory vesicles of mast cells generate a current transient that marks the opening of the fusion pore, the first aqueous connection that forms between the vesicle lumen and the cell exterior. By recording and analyzing such current transients, we have tracked the conductance of the fusion pore over the first millisecond of its existence. The first opening of the pore occurs rapidly, generally within 100 microseconds at 23 degrees C. The electric conductance of the pore is a few hundred picosiemens at first, but gradually increases over the subsequent milliseconds. Evidently the pore opens abruptly and then dilates. The initial conductance of the pore suggests a diameter comparable to that of a large ion channel. From an analysis of "capacitance flicker" we infer that a pore can increase its diameter severalfold and still close again completely. This suggests that several early events in membrane fusion are reversible.     

Kinetics of homomeric GluR6 glutamate receptor channels.

We studied the kinetics of the unedited version of rat GluR6 glutamate (glu) receptor channels, GluR6Q, in outside-out patches using a system for submillisecond solution exchange. Half-maximum activation of the channels was reached with approximately 0.5 microM glu. The maximum slope of the double-logarithmic plot of the peak current versus glu was approximately 1.3, indicating that at least two binding steps are necessary to open the channels. Currents in response to a pulse of 10 microM glu had a short rise time (10-90% of peak current) of approximately 220 microseconds at approximately 20 degrees C. The rise time increased with falling glu concentration, reaching approximately 6.0 ms with 10 microM glu. In the continued presence of glu, the channels desensitized, and this desensitization can be described with a single time constant of approximately 7.0 ms for a pulse of 10 microM glu. The steady-state current in response to a long pulse of 10 microM glu was below 1/280th of the peak current. The time constant of desensitization was found to be independent of concentration between 30.0 and 0.3 microM glu, but to be increased for lower concentrations. After a short pulse of 1 ms duration and 10 or 0.3 microM glu, currents decayed with a time constant of approximately 2.5 ms. Recovery from desensitization after a pulse took approximately 5 s, and the half-time of recovery was approximately 2.2 s. Continuous application of low concentrations of glutamate reduced the peak currents in response to a pulse of 10 microM glu markedly. Fifty percent response reduction was observed in the continuous presence of approximately 0.3 microM glu. Our results for homomeric GluR6 agree with a cyclical reaction scheme developed for completely desensitizing, glu-activated channels on crayfish muscles.     

Survival value of Slifer's Patches for locusts at a high temperature

Normal male locusts with functional Slifer's Patches had longer effective activity and overall survival times than others with covered abdominal patches, at 55°C in dry air but not in wet air. It is concluded that in hot, dry conditions the patches constitute an emergency cooling system which aids survival by localised rapid transpiration. It is suggested that selective cooling of vulnerable organs is more important than the whole-body temperature. Evaporation from other parts of the body does not contribute significantly to the survival time. Even above the transition temperature of the normal cuticle, the patches may be the only important site of evaporative cooling because of their specialisation for rapid transmission of water through the integument.     

Diffusion cannot govern the discharge of neurotransmitter in fast synapses.

In the present work we show that diffusion cannot provide the observed fast discharge of neurotransmitter from a synaptic vesicle during neurotransmitter release, mainly because it is not sufficiently rapid nor is it sufficiently temperature-dependent. Modeling the discharge from the vesicle into the cleft as a continuous point source, we have determined that discharge should occur in 50-75 microseconds, to provide the observed high concentrations of transmitter at the critical zone.     

Effect of Temperature on the Distribution of Membrane Particles in Streptococcus faecalis as Seen by the Freeze-Fracture Technique

When cells of Streptococcus faecalis ATCC 9790 were incubated at temperatures above 10 C before being frozen for freeze-fracture, a random distribution of particles was observed on the outer fracture face of the freeze-cleaved cell membrane. However, when cells were incubated below 10 C before freezing, particleless patches were seen on this membrane surface. The size of the patches produced on chilling could be increased by centrifugation or by storing the chilled cells overnight at about 3 C. Patch formation appeared readily reversible, since the medium and large patches that formed on chilling could not be observed in cells warmed for 10 s at 25 C. However, during the transition from the patch to patchless state, smaller patches not seen in the chilled cells were observed. This suggested that the smaller patches might have been intermediate forms produced by the fragmentation of larger patches on warming.