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C M Armstrong

Publications and source records attributed to C M Armstrong.

At least 55 records · Page 3Linked to original sources
PubMed1988

Potassium channel "inactivation" induced by soft-glass patch pipettes.

We have studied the potassium currents of rat pituitary pars intermedia cells kept in primary culture using whole-cell recording with patch pipettes. The potassium current recorded with hard-glass pipettes is mainly carried by voltage-dependent channels that show slow inactivation in the presence of 0.5 mM internal EGTA. Fast "inactivation" of the potassium current is seen with patch pipettes fabricated from soft glass (soda glass or potash lead glass), and is probably caused by block of the potassium channels by di- or multivalent cations released from the glass.

Animals↗
PubMed1988

Fast-deactivating calcium channels in chick sensory neurons.

Whole-cell Ca and Ba currents were studied in chick dorsal root ganglion (DRG) cells kept 6-10 in culture. Voltage steps with a 15-microseconds rise time were imposed on the membrane using an improved patch-clamp circuit. Changes in membrane current could be measured 30 microseconds after the initiation of the test pulse. Currents through Ca channels were recorded under conditions that eliminate Na and K currents. Tail currents, associated with Ca channel closing, decayed in two distinct phases that were very well fitted by the sum of two exponentials. The time constants tau f and tau s were near 160 microseconds and 1.5 ms at -80 mV, 20 degrees C. The tail current components, called FD and SD (fast-deactivating and slowly deactivating), are Ca channel currents. They were greatly reduced when Mg2+ replaced all other divalent cations in the bath. The SD component inactivated almost completely as the test pulse duration was increased to 100 ms. It was suppressed when the cell was held at membrane potentials positive to -50 mV and was blocked by 100-200 microM Ni2+. This behavior indicates that the SD component was due to the closing of the low-voltage-activated (LVA) Ca channels previously described in this preparation. The FD component was fully activated with 10-ms test pulses to +20 mV at 20 degrees C, and inactivated to approximately 30% during 500-ms test pulses. It was reduced in amplitude by holding at -40 mV, but was only slightly reduced by micromolar concentrations of Ni2+. Replacement of Ca2+ with Ba2+ increased the FD tail current amplitudes by a factor of approximately 1.5. The deactivation kinetics did not change (a) as channels inactivated during progressively longer pulses or (b) when the degree of activation was varied. Further, tau f was affected neither by changing the holding potential nor by varying the test pulse amplitude. Lowering the temperature from 20 to 10 degrees C decreased tau f by a factor of 2.5. In all cases, the FD component was very well fitted by a single exponential. There was no indication of an additional tail component of significant size. Our findings indicate that the FD component is due to closing of a single class of Ca channels that coexist with the LVA Ca channel type in chick DRG neurons.

Animals↗
PubMed1987

External calcium ions are required for potassium channel gating in squid neurons.

The effects of calcium removal on the voltage-dependent potassium channels of isolated squid neurons were studied with whole cell patch-clamp techniques. When the calcium ion concentration was lowered from 10 to 0 millimolar (that is, no added calcium), potassium channel activity, identified from its characteristic time course, disappeared within a few seconds and there was a parallel increase in resting membrane conductance and in the holding current. The close temporal correlation of the changes in the three parameters suggests that potassium channels lose their ability to close in the absence of calcium and simultaneously lose their selectivity. If potassium channels were blocked by barium ion before calcium ion was removed, the increases in membrane conductance and holding current were delayed or prevented. Thus calcium is an essential cofactor in the gating of potassium channels in squid neurons.

Animals↗
PubMed1987

Supercharging: a method for improving patch-clamp performance.

Patch-clamp performance can be improved without altering the normal headstage configuration described by (Hamill, O. P., A. Marty, E. Neher, B. Sakmann, and F. J. Sigworth, 1981, Pfluegers Arch. Eur. J. Physiol., 391:85-100). The "supercharging" method permits resolution of such fast events as calcium and sodium tail currents. Digital computer modeling and analog electronic simulation were used to identify appropriate shapes for the command voltage and the voltage applied to a capacitor tied to the input of the headstage. The voltage command pulse consists of a step with a brief (5-15 microseconds) rectangular spike on its leading edge. Spike amplitude is a function of the membrane capacitance and the access resistance. The spike drives current through the access resistance and speeds charging of the membrane capacitance, making it possible to complete a voltage step within 5-15 microseconds. Clamping speed is independent of the electrode and feedback resistance over a wide range. The second function of the patch clamp amplifier is current measurement, and good time resolution requires suppression of the capacity transient. This can be accomplished by applying an appropriately shaped voltage to the small capacitor tied to the input of the headstage. Series resistance compensation for ionic current transients does not interfere with supercharging. Although the focus of this paper is on whole cell recording, the supercharging concept may prove useful for single channel and bilayer recording techniques.

Computer Simulation↗
PubMed1986

Properties of two types of calcium channels in clonal pituitary cells.

The calcium currents of GH3 cells have been studied using the whole cell variant of the patch-clamp technique. Under conditions that eliminate sodium and potassium currents, we observed inward currents that activated within a few milliseconds, and deactivated with two time constants, approximately 150 microseconds and 3 ms at -80 mV, 18-20 degrees C. The components are called FD and SD (fast deactivating and slow deactivating). Both components are calcium currents, and are greatly reduced when magnesium is substituted for most of the calcium in the bath. In addition to (a) their different rates of deactivation, the two components differ in a number of other properties. (b) The SD component inactivates almost completely, with a time constant of 23 ms at 20 mV, 19 degrees C. The FD component, on the other hand, shows little or no sign of inactivation, and is almost the same in amplitude from 10 to 100 ms. The components thus seem quite independent of each other, and must arise from two independent sets of channels. (c) The FD channels activate more rapidly than SD at 20 mV, by a factor of approximately 2 as is shown in several ways. (d) In 10 Ca or 10 Ba, the activation curve for SD channels is approximately 20 mV more negative than for FD or Na channels. (e) FD channels conduct barium ions more effectively than calcium by a ratio of approximately 2. (f) FD channels "wash out" within minutes after the patch electrode breaks into a cell, whereas SD channel current remains relatively stable. It is argued that SD channels, because of their negative activation threshold, are involved in electrical events near threshold, and that FD channels are best suited for calcium injection once a spike has been initiated.

Animals↗
PubMed1986

The role of calcium ions in the closing of K channels.

The effects of external Ca ion on K channel properties were studied in squid giant axons. Increasing the Ca concentration from 20 to 100 mM slowed K channel opening, and was kinetically equivalent to decreasing the depolarizing step by approximately 25 mV. The same Ca increase had a much smaller effect on closing kinetics, equivalent to making the membrane potential more negative by approximately mV. With regard to the conductance-voltage curve, this Ca increase was about equivalent to decreasing the depolarizing step by approximately 10 mV. The presence of K or Rb in the bath slowed closing kinetics and made the time course more complex: there were pronounced slow components in Rb and, to a lesser extent, in K. Increasing the Ca concentration strongly antagonized the slowing caused by Rb or K. Thus, Ca has a strong effect on closing kinetics only in the presence of these monovalent cations. Rb and K do not significantly alter opening kinetics, nor do they alter Ca's ability to slow opening kinetics. High Ca slightly affects the instantaneous I-V curve by selectively depressing inward current at negative voltages. The results imply that Ca has two actions on K channels, and in only one, the action on closing, does it compete with monovalent cations. We propose (a) that opening kinetics are slowed by binding of Ca to negatively charged parts of the gating apparatus that are at the external surface of the channel protein when the channel is closed; monovalent cations do not compete effectively in this action; (b) Ca (or possibly Mg) normally occupies closed channels and has a latching effect. External K or Rb competes with Ca for channel occupancy. Channels close sluggishly when occupied by a monovalent cation and tend to reopen. Thus, slow closing results from occupancy by K or Rb instead of Ca. The data are well fit by a model based on these ideas.

Animals↗
PubMed1985

Two distinct populations of calcium channels in a clonal line of pituitary cells.

The whole-cell variant of the patch clamp technique was used to study calcium channels in GH3 cells. Two distinct populations of calcium channels, first recognized from their closing kinetics, were observed. The slowly closing channels are activated in a relatively negative voltage range and are inactivated within 100 milliseconds. They conduct barium and calcium about equally well. The fast closing channels are activated at more positive voltages, are not inactivated during a 100-millisecond pulse, conduct barium in preference to calcium, and are activated slightly more rapidly than the slowly closing channels.

Animals↗
PubMed1984

Na and Ca channels in a transformed line of anterior pituitary cells.

The ionic conductances of GH3 cells, a transformed line from rat anterior pituitary, have been studied using the whole-cell variant of the patch-clamp technique (Hamill et al., 1981). Pipettes of very low resistance were used, which improved time resolution and made it possible to control the ion content of the cell interior, which equilibrated very rapidly with the pipette contents. Time resolution was further improved by using series resistance compensation and "ballistic charging" of the cell capacitance. We have identified and partially characterized at least three conductances, one carrying only outward current, and the other two normally inward. The outward current is absent when the pipette is filled with Cs+ instead of K+, and has the characteristics of a voltage-dependent potassium conductance. One of the two inward conductances (studied with Cs+ inside) has fast activation, inactivation and deactivation kinetics, is blocked by tetrodotoxin (TTX), and has a reversal potential at the sodium equilibrium potential. The other inward current activates more slowly and deactivates with a quick phase and a very slow phase after a short pulse. Either Ca++ or Ba++ serves as current carrier. During a prolonged pulse, current inactivates fairly completely if there is at least 5 mM Ca++ outside, and the amplitude of the current tails following the pulse diminishes with the time course of inactivation. When Ba++ entirely replaces Ca++ in the external medium, there is no inactivation, but deactivation kinetics of Ca channels vary as pulse duration increases: the slow phase disappears, the fast phase grows in amplitude. Inactivation (Ca++ outside) is unaltered by 50 mM EGTA in the pipette: inactivation cannot be the result of internal accumulation of Ca++.

Action Potentials↗
PubMed1983

Depolarizing response of rat parathyroid cells to divalent cations.

Membrane potentials were recorded from rat parathyroid glands continuously perfused in vitro. At 1.5 mM external Ca++, the resting potential averages -73 +/- 5 mV (mean +/- SD, n = 66). On exposure to 2.5 mM Ca++, the cells depolarize reversibly to a potential of -34 +/- 8 mV (mean +/- SD). Depolarization to this value is complete in approximately 2-4 min, and repolarization on return to 1.5 mM Ca++ takes about the same time. The depolarizing action of high Ca++ is mimicked by all divalent cations tested, with the following order of effectiveness: Ca++ greater than Sr++ greater than Mg++ greater than Ba++ for alkali-earth metals, and Ca++ greater than Cd++ greater than Mn++ greater than Co++ greater than Zn++ for transition metals. Input resistance in 1.5 mM Ca++ was 24.35 +/- 14 M omega (mean +/- SD) and increased by an average factor of 2.43 +/- 0.8 after switching to 2.5 mM Ca++. The low value of input resistance suggests that cells are coupled by low-resistance junctions. The resting potential in low Ca++ is quite insensitive to removal of external Na+ or Cl-, but very sensitive to changes in external K+. Cells depolarize by 61 mV for a 10-fold increase in external K+. In high Ca++, membrane potential is less sensitive to an increase in external K+ and is unchanged by increasing K+ from 5 to 25 mM. Depolarization evoked by high Ca++ may be slowed, but is unchanged in amplitude by removal of external Na+ or Cl-. Organic (D600) and inorganic (Co++, Cd++, and Mn++) blockers of the Ca++ channels do not interfere with the electrical response to Ca++ changes. Our results show remarkable parallels to previous observations on the control of parathormone (PTH) release by Ca++. They suggest an association between membrane voltage and secretion that is very unusual: parathyroid cells secrete when fully polarized, and secrete less when depolarized. The extraordinary sensitivity of parathyroid cells to divalent cations leads us to hypothesize the existence in their membranes of a divalent cation receptor that controls membrane permeability (possibly to K+) and PTH secretion.

Animals↗
PubMed1982

Evidence for a population of sleepy sodium channels in squid axon at low temperature.

We have studied the effects of temperature changes on Na currents in squid giant axons. Decreases in temperature in the 15-1 degrees C range decrease peak Na current with a Q10 of 2.2. Steady state currents, which are tetrodotoxin sensitive and have the same reversal potential as peak currents, are almost unaffected by temperature changes. After removal of inactivation by pronase treatment, steady state current amplitude has a Q10 of 2.3. Na currents generated at large positive voltages sometimes exhibit a biphasic activation pattern. The first phase activates rapidly and partially inactivates and is followed by a secondary slow current increase that lasts several milliseconds. Peak Na current amplitude can be increased by delivering large positive prepulses, an effect that is more pronounced at low temperatures. The slow activation phase is eliminated after a positive prepulse. The results are consistent with the hypothesis that there are two forms of the Na channel: (a) rapidly activating channels that completely inactivate, and (b) slowly activating "sleepy" channels that inactivate slowly if at all. Some fast channels are assumed to be converted to sleepy channels by cooling, possibly because of a phase transition in the membrane. The existence of sleepy channels complicates the determination of the Q10 of gating parameters and single-channel conductance.

Animals↗
PubMed1982

Slowing of sodium channel opening kinetics in squid axon by extracellular zinc.

The interaction of Zn ion on Na channels was studied in squid giant axons. At a concentration of 30 mM Zn2+ slows opening kinetics of Na channels with almost no alteration of closing kinetics. The effects of Zn2+ can be expressed as a "shift" of the gating parameters along the voltage axis, i.e., the amount of additional depolarization required to overcome the Zn2+ effect. In these terms the mean shifts caused by 30 mM Zn2+ were +29.5 mV for Na channel opening (on) kinetics (t1/2 on), +2 mV for closing (off) kinetics (tau off), and +8.4 mV for the gNa-V curve. Zn2+ does not change the shape of the instantaneous I-V curve for inward current, but reduces it in amplitude by a factor of or approximately 0.67. Outward current is unaffected. Effects of Zn2+ on gating current (measured in the absence of TTX) closely parallel its actions on gNa. On gating current kinetics are shifted by +27.5 mV, off kinetics by +6 mV, and the Q-V distribution by +6.5 mV. Kinetic modeling shows that Zn2+ slows the forward rate constants in activation without affecting backward rate constants. More than one of the several steps in activation must be affected. The results are not compatible with the usual simple theory of uniform fixed surface charge. They suggest instead that Zn2+ is attracted by a negatively charged element of the gating apparatus that is present at the outer membrane surface at rest, and migrates inward on activation.

Animals↗
PubMed1982

Divalent cations and the activation kinetics of potassium channels in squid giant axons.

The effects of external Zn+2 and other divalent cations on K channels in squid giant axons were studied. At low concentration (2 mM) Zn+2 slows opening kinetics without affecting closing kinetics. Higher concentrations (5-40 mM) progressively slow opening and speed channel closing to a lesser degree. In terms of "shifts," opening kinetics are strongly shifted to the right on the voltage axis, and off kinetics much less so. The shift of the conductance-voltage relation along the axis is intermediate. Zinc's kinetic effects show little sign of saturation at the highest concentration attainable. Zn does not alter the shape of the instantaneous current-voltage relation of open channels. Some other divalent cations have effects similar to Zn+2, Hg2+ being the most potent and Ca+2 the least. After treatment with Hg+2, which is irreversible, Zn+2 still slows opening kinetics, which suggests that each channel has at least two sites for divalent cation action. The results are not compatible with a simple theory of fixed, uniform surface charges. They suggest that external cations interact directly with a negatively charged element of the gating apparatus that moves inward from the membrane's outer surface during activation. Examination of normal kinetics shows that there is a slow step somewhere in the chain leading to channel opening. But the slowest step must not be the last one.

Animals↗
PubMed1982

Simulation of Na channel inactivation by thiazine dyes.

Some dyes of the methylene blue family serve as artificial inactivators of the sodium channels when present inside squid axons at a concentration of approximately 0.1 mM. The dyes restore a semblance of inactivation after normal inactivation has been destroyed by pronase. In fibers that inactivate normally, the dyes hasten the decay of sodium current. Many dye-blocked channels conduct transiently on exit of the dye molecule after repolarization to the holding potential. In contrast, normally inactivated channels do not conduct during recovery from inactivation. Kinetic evidence shows that inactivation of a dye-blocked channel is unlikely or impossible, which suggests that dye molecules compete with inactivation "particles" for the same site. In the absence of tetrodotoxin, the dyes do not affect the ON gating current unless the interpulse interval is very short. If sufficient equilibration time is allowed during a pulse, the initial amplitude of the OFF gating current is reduced to near zero. This suggests that a dye molecule is a Na channel completely blocks that channel's gating current, even the fraction that is resistant to normal inactivation. Dyes block INa and Ig with the same time course. This provides the strongest evidence to date that virtually all of recorded "gating current" is associated with Na channels. Tetrodotoxin greatly slows dissociation of dye molecules from Na channels and reduced gating current during both opening and closing of the channels.

Animals↗
PubMed1982

Block of squid axon K channels by internally and externally applied barium ions.

We have studied the interactions of Ba ion with K channels. Ba2+ blocks these channels when applied either internally or externally in millimolar concentrations. Periodic depolarizations enhance block with internal Ba2+, but diminish the block caused by external Ba2+. At rest, dissociation of Ba2+ from blocked channels is very slow, as ascertained by infrequent test pulses applied after washing Ba2+ form either inside or outside. The time constant for recovery from internal and external Ba2+ is the same. Frequent pulsing greatly shortens recovery time constant after washing away both Ba2+in and Ba2+out. Block by Ba2+ applied internally or externally is voltage dependent. Internal Ba2+ block behaves like a one-step reaction governed by a dissociation constant (Kd) that decreases e-fold/12 mV increase of pulse voltage: block deepens with more positive pulse voltage. For external Ba2+, Kd decreases e-fold/18 mV as holding potential is made more negative: block deepens with increasing negativity. Millimolar external concentrations of some cations can either lessen (K+) or enhance (NH+4, Cs+) block by external Ba2+. NH+4 apparently enhances block by slowing exist of Ba ions from the channels. Rb+ and Cs+ also slow clearing of Ba ions from channels. We think that (a) internally applied Ba2+ moves all the way through the channels, entering only when activation gates are open; (b) externally applied Ba2+ moves two-thirds of the way in, entering predominantly when activation gates are closed; (c) at a given voltage, Ba2+ occupies the same position in the channels whether it entered from inside or outside.

Animals↗
PubMed1981

Currents recorded through small areas of squid axon membrane with an internal virtual ground voltage clamp.

A new voltage-clamp apparatus for the squid axon has been implemented to enable recording of currents through small areas of axon membrane. The performance of this clamp was tested by recording total sodium currents from perfused axons (I total) and sodium currents from small membrane patches (I patch), which were recorded from inside the axon with an L-shaped pipette. The I patch records, although four orders of magnitude smaller than I total, were stable and showed normal kinetics and voltage dependence, and appeared to reflect the activation of a small population of normal sodium channels. The size of the current recorded from the patch was mainly a function of the tip diameter of the L-shaped pipette and of the shunt resistance between inside the pipette and the axoplasm.

Animals↗
PubMed1980

Interaction of barium ions with potassium channels in squid giant axons.

Blocking of potassium channels by internally and externally applied barium ions has been studied in squid giant axons. Internal Ba (3-5 mM) causes rapid decay or "inactivation" of potassium current (IK). The kinetics and degree of block are strongly voltage-dependent. Large positive voltages speed blocking and make it more profound. Raising the external potassium concentration (Ko) from 0 to 250 mM has the opposite effect: block is made slower and less severe. In contrast, for positive voltages block by the tetraethylammonium derivative 3-phenylpropyltriethylammonium ion is almost independent of Ko and voltage. Recovery from block by internal Ba has a rapid phase lasting a few milliseconds and a slow phase lasting approximately 5 min. Internal Ba causes a "hook" in the IK tails recorded on repolarizing the fiber in high potassium external medium. External Ba, on the other hand, blocks without much altering IK time-course. KD (the dissociation constant) for block by external Ba is a few millimolar, and depends on the internal potassium concentration, the holding potential, and other factors. A reaction scheme for Ba and K channels is presented, postulating that internal and external Ba reach the same point in the channel. Once there, Ba blocks and also stabilizes the closed conformation of the channel. The extreme stability of the Ba channel complex implies the existence of negative charge within the channel.

Animals↗