scholarly journals Na/K pump current in aggregates of cultured chick cardiac myocytes.

1990 ◽  
Vol 95 (1) ◽  
pp. 61-76 ◽  
Author(s):  
J R Stimers ◽  
N Shigeto ◽  
M Lieberman
Keyword(s):  
Steady State ◽  
Cardiac Myocytes ◽  
Pump Current ◽  
Cardiac Cells ◽  
Hill Coefficient ◽  
Published Data ◽  
Free Solution ◽  
Embryonic Chick ◽  
Current Voltage ◽  
Current Voltage Relationship

Spontaneously beating aggregates of cultured embryonic chick cardiac myocytes, maintained at 37 degrees C, were voltage clamped using a single microelectrode switching clamp to measure the current generated by the Na/K pump (Ip). In resting, steady-state preparations an ouabain-sensitive current of 0.46 +/- 0.03 microA/cm2 (n = 22) was identified. This current was not affected by 1 mM Ba, which was used to reduce inward rectifier current (IK1) and linearize the current-voltage relationship. When K-free solution was used to block Ip, subsequent addition of Ko reactivated the Na/K pump, generating an outward reactivation current that was also ouabain sensitive. The reactivation current magnitude was a saturating function of Ko with a Hill coefficient of 1.7 and K0.5 of 1.9 mM in the presence of 144 mM Nao. The reactivation current was increased in magnitude when Nai was increased by lengthening the period of time that the preparation was exposed to K-free solution prior to reactivation. When Nai was raised by 3 microM monensin, steady-state Ip was increased more than threefold above the resting value to 1.74 +/- 0.09 microA/cm2 (n = 11). From these measurements and other published data we calculate that in a resting myocyte: (a) the steady-state Ip should hyperpolarize the membrane by 6.5 mV, (b) the turnover rate of the Na/K pump is 29 s-1, and (c) the Na influx is 14.3 pmol/cm2.s. We conclude that in cultured embryonic chick cardiac myocytes, the Na/K pump generates a measurable current which, under certain conditions, can be isolated from other membrane currents and has properties similar to those reported for adult cardiac cells.

Simulation of Na/K Pump Current-Voltage Relationship

1992 ◽  
Vol 671 (1 Ion-Motive AT) ◽  
pp. 449-451 ◽  
Author(s):  
X.-Y. LIU ◽  
T. A. KINARD ◽  
J. R. STIMERS
Keyword(s):  
Pump Current ◽  
Current Voltage ◽  
Current Voltage Relationship ◽  
Voltage Relationship

scholarly journals Steady-state current-voltage relationship of the Na/K pump in guinea pig ventricular myocytes.

1989 ◽  
Vol 94 (3) ◽  
pp. 511-537 ◽  
Author(s):  
D C Gadsby ◽  
M Nakao
Keyword(s):  
Steady State ◽  
Guinea Pig ◽  
Rate Constants ◽  
Ventricular Myocytes ◽  
Pump Current ◽  
Membrane Current ◽  
Negative Slope ◽  
Current Voltage ◽  
State Cycle ◽  
External K

Whole-cell currents were recorded in guinea pig ventricular myocytes at approximately 36 degrees C before, during, and after exposure to maximally effective concentrations of strophanthidin, a cardiotonic steroid and specific inhibitor of the Na/K pump. Wide-tipped pipettes, in combination with a device for exchanging the solution inside the pipette, afforded reasonable control of the ionic composition of the intracellular solution and of the membrane potential. Internal and external solutions were designed to minimize channel currents and Na/Ca exchange current while sustaining vigorous forward Na/K transport, monitored as strophanthidin-sensitive current. 100-ms voltage pulses from the -40 mV holding potential were used to determine steady-state levels of membrane current between -140 and +60 mV. Control experiments demonstrated that if the Na/K pump cycle were first arrested, e.g., by withdrawal of external K, or of both internal and external Na, then neither strophanthidin nor its vehicle, dimethylsulfoxide, had any discernible effect on steady-state membrane current. Further controls showed that, with the Na/K pump inhibited by strophanthidin, membrane current was insensitive to changes of external [K] between 5.4 and 0 mM and was little altered by changing the pipette [Na] from 0 to 50 mM. Strophanthidin-sensitive current therefore closely approximated Na/K pump current, and was virtually free of contamination by current components altered by the changes in extracellular [K] and intracellular [Na] expected to accompany pump inhibition. The steady-state Na/K pump current-voltage (I-V) relationship, with the pump strongly activated by 5.4 mM external K and 50 mM internal Na (and 10 mM ATP), was sigmoid in shape with a steep positive slope between about 0 and -100 mV, a less steep slope at more negative potentials, and an extremely shallow slope at positive potentials; no region of negative slope was found. That shape of I-V relationship can be generated by a two-state cycle with one pair of voltage-sensitive rate constants and one pair of voltage-insensitive rate constants: such a two-state scheme is a valid steady-state representation of a multi-state cycle that includes only a single voltage-sensitive step.

scholarly journals [Na] and [K] dependence of the Na/K pump current-voltage relationship in guinea pig ventricular myocytes.

1989 ◽  
Vol 94 (3) ◽  
pp. 539-565 ◽  
Author(s):  
M Nakao ◽  
D C Gadsby
Keyword(s):  
Guinea Pig ◽  
Ventricular Myocytes ◽  
Pump Current ◽  
Hill Coefficient ◽  
Independent Manner ◽  
Current Voltage ◽  
Voltage Dependent ◽  
Scale Down ◽  
Na Ions ◽  
The Right

Na/K pump current was determined between -140 and +60 mV as steady-state, strophanthidin-sensitive, whole-cell current in guinea pig ventricular myocytes, voltage-clamped and internally dialyzed via wide-tipped pipettes. Solutions were designed to minimize all other components of membrane current. A device for exchanging the solution inside the pipette permitted investigation of Na/K pump current-voltage (I-V) relationships at several levels of pipette [Na] [( Na]pip) in a single cell; the effects of changes in external [Na] [( Na]o) or external [K] [( K]o) were also studied. At 50 mM [Na]pip, 5.4 mM [K]o, and approximately 150 mM [Na]o, Na/K pump current was steeply voltage dependent at negative potentials but was approximately constant at positive potentials. Under those conditions, reduction of [Na]o enhanced pump current at negative potentials but had little effect at positive potentials: at zero [Na]o, pump current was only weakly voltage dependent. At 5.4 mM [K]o and approximately 150 mM [Na]o, reduction of [Na]pip from 50 mM scaled down the sigmoid pump I-V relationship and shifted it slightly to the right (toward more positive potentials). Pump current at 0 mV was activated by [Na]pip according to the Hill equation with best-fit K0.5 approximately equal to 11 mM and Hill coefficient nH approximately equal to 1.4. At zero [Na]o, reduction of [Na]pip seemed to simply scale down the relatively flat pump I-V relationship: Hill fit parameters for pump activation by [Na]pip at 0 mV were K0.5 approximately equal to 10 mM, nH approximately equal to 1.4. At 50 mM [Na]pip and high [Na]o, reduction of [K]o from 5.4 mM scaled down the sigmoid I-V relationship and shifted it slightly to the right: at 0 mV, K0.5 approximately equal to 1.5 mM and nH approximately equal to 1.0. At zero [Na]o, lowering [K]o simply scaled down the flat pump I-V relationships yielding, at 0 mV, K0.5 approximately equal to 0.2 mM, nH approximately equal to 1.1. The voltage-independent activation of Na/K pump current by both intracellular Na ions and extracellular K ions, at zero [Na]o, suggests that neither ion binds within the membrane field. Extracellular Na ions, however, seem to have both a voltage-dependent and a voltage-independent influence on the Na/K pump: they inhibit outward Na/K pump current in a strongly voltage-dependent fashion, with higher apparent affinity at more negative potentials (K0.5 approximately equal to 90 mM at -120 mV, and approximately 170 mM at -80 mV), and they compete with extracellular K ions in a seemingly voltage-independent manner.(ABSTRACT TRUNCATED AT 400 WORDS)

1S,3R-ACPD Induces a Region of Negative Slope Conductance in the Steady-State Current-Voltage Relationship of Hippocampal Pyramidal Cells

1997 ◽  
Vol 77 (1) ◽  
pp. 221-228 ◽  
Author(s):  
Anita Lüthi ◽  
Beat H. Gähwiler ◽  
Urs Gerber
Keyword(s):  
Steady State ◽  
Reversal Potential ◽  
Pyramidal Cells ◽  
Resting Potential ◽  
Negative Slope ◽  
Inward Current ◽  
Current Voltage ◽  
Steady State Current ◽  
Current Voltage Relationship ◽  
Voltage Relationship

Lüthi, Anita, Beat H. Gähwiler, and Urs Gerber. 1 S,3 R-ACPD induces a region of negative slope conductance in the steady-state current-voltage relationship of hippocampal pyramidal cells. J. Neurophysiol. 77: 221–228, 1997. Synaptic responses mediated by metabotropic glutamate receptors (mGluRs) display a marked voltage-dependent increase in amplitude when neurons are moderately depolarized beyond membrane potential. We have investigated the basis for this apparent nonlinear behavior by activatingmGluRs with 1 S,3 R-1-aminocyclopentane-1,3-dicarboxylate(1 S,3 R-ACPD; 10 μM) in CA3 pyramidal cells from rat hippocampal slice cultures with the use of the single-electrode voltage-clamp technique. Under control conditions, cells depolarized from resting potential by 10–20 mV responded with delayed outwardly rectifying currents due to activation of voltage- and Ca2+-dependent K+ conductances. In contrast, in the continuous presence of 1 S,3 R-ACPD, small depolarizations (10–20 mV) induced a delayed inward current. The steady-state current-voltage relationship for this response displayed a region of negative slope conductance at potentials between −55 and −40 mV. The reversal potential of the corresponding 1 S,3 R-ACPD-sensitive tail currents (−93.0 ± 2.2 mV, mean ± SE) was close to the potassium reversal potential, consistent with an mGluR-mediated suppression of K+ current. When external K+ concentration was increased to 8 mM, there was a positive shift in reversal potential to −76.9 ± 5.1 mV. The depolarization-induced inward current in the presence of 1 S,3 R-ACPD was blocked by Ba2+ (1 mM). The response was not dependent on changes in intracellular Ca2+ concentration and was insensitive to bath-applied Cs+ (1 mM), ruling out a contribution of Ca2+-dependent currents or the inward rectifier I Q. Furthermore, the effect of 1 S,3 R-ACPD was not mimicked by inhibiting afterhyperpolarizing current and M current with low-Ca2+ saline (0.5 mM Ca2+, 10 mM Mg2+) containing 10 mM tetraethylammonium chloride. A comparison of the responses induced by 1 S,3 R-ACPD and N-methyl-d-aspartate showed that both induce an inward current with small depolarizations from resting potential but with different kinetics and Mg2+ sensitivity. These results indicate that the suppression of K+ currents in response to activation of mGluRs is markedly voltage dependent, increasing at depolarized potentials and decreasing at hyperpolarized potentials. The negative slope conductance at membrane voltages positive to resting potential may underlie the amplification of mGluR-mediated responses when the membrane potential approaches action potential threshold.

scholarly journals Voltage Dependence of the Apparent Affinity for External Na+ of the Backward-Running Sodium Pump

2001 ◽  
Vol 117 (4) ◽  
pp. 315-328 ◽  
Author(s):  
Paul De Weer ◽  
David C. Gadsby ◽  
R.F. Rakowski
Keyword(s):  
Steady State ◽  
Sodium Pump ◽  
Channel Model ◽  
Pump Current ◽  
Hill Coefficient ◽  
Access Channel ◽  
Electrogenic Sodium Pump ◽  
The Difference ◽  
Loligo Pealei ◽  
The Hill

The steady-state voltage and [Na+]o dependence of the electrogenic sodium pump was investigated in voltage-clamped internally dialyzed giant axons of the squid, Loligo pealei, under conditions that promote the backward-running mode (K+-free seawater; ATP- and Na+-free internal solution containing ADP and orthophosphate). The ratio of pump-mediated 42K+ efflux to reverse pump current, Ipump (both defined by sensitivity to dihydrodigitoxigenin, H2DTG), scaled by Faraday's constant, was −1.5 ± 0.4 (n = 5; expected ratio for 2 K+/3 Na+ stoichiometry is −2.0). Steady-state reverse pump current-voltage (Ipump-V) relationships were obtained either from the shifts in holding current after repeated exposures of an axon clamped at various Vm to H2DTG or from the difference between membrane I-V relationships obtained by imposing Vm staircases in the presence or absence of H2DTG. With the second method, we also investigated the influence of [Na+]o (up to 800 mM, for which hypertonic solutions were used) on the steady-state reverse Ipump-V relationship. The reverse Ipump-V relationship is sigmoid, Ipump saturating at large negative Vm, and each doubling of [Na+]o causes a fixed (29 mV) rightward parallel shift along the voltage axis of this Boltzmann partition function (apparent valence z = 0.80). These characteristics mirror those of steady-state 22Na+ efflux during electroneutral Na+/Na+ exchange, and follow without additional postulates from the same simple high field access channel model (Gadsby, D.C., R.F. Rakowski, and P. De Weer, 1993. Science. 260:100–103). This model predicts valence z = nλ, where n (1.33 ± 0.05) is the Hill coefficient of Na binding, and λ (0.61 ± 0.03) is the fraction of the membrane electric field traversed by Na ions reaching their binding site. More elaborate alternative models can accommodate all the steady-state features of the reverse pumping and electroneutral Na+/Na+ exchange modes only with additional assumptions that render them less likely.

scholarly journals Apparent affinity of the Na/K pump for ouabain in cultured chick cardiac myocytes. Effects of Nai and Ko.

1991 ◽  
Vol 98 (4) ◽  
pp. 815-833 ◽  
Author(s):  
J R Stimers ◽  
S Liu ◽  
M Lieberman
Keyword(s):  
Cardiac Myocytes ◽  
Pump Current ◽  
State Distribution ◽  
Isolated Cells ◽  
Intact Cells ◽  
Apparent Affinity ◽  
Current Voltage ◽  
Wide Range ◽  
Order Of Magnitude ◽  
Hank’S Solution

The measured apparent affinity (K0.5) of the Na/K pump for ouabain has been reported to vary over a wide range. In a previous report we found that changing Nai could alter apparent affinity by at least an order of magnitude and that the model presented predicted this variability. To increase our understanding of this variability, isolated cells or two- to three-cell clusters of cardiac myocytes from 11-d embryonic chick were used to measure the effects of Nai and Ko on the K0.5 of the Na/K pump for ouabain. Myocytes were whole-cell patch clamped and Na/K pump current (Ip) was measured in preparations exposed to a Ca-free modified Hank's solution (HBSS) that contained 1 mM Ba, 10 mM Cs, and 0.1 mM Cd. Under these conditions there are no Ko-sensitive currents other than Ip because removal of Ko in the presence of ouabain had no effect on the current-voltage (I-V) relation. The I-V relation for Ip showed that in the presence of 5.4 mM Ko and 51 mM Nai, Ip has a slight voltage dependence, decreasing approximately 30% from 0 to -130 mV. Increasing Nai in the patch pipette from 6 to 51 mM (Ko = 5.4 mM) caused Ip to increase from 0.46 +/- 0.07 (n = 5) to 1.34 +/- 0.08 microA/cm2 (n = 13) with a K0.5 for Nai of 17.4 mM and decreased the K0.5 for ouabain from 18.5 +/- 1.8 (n = 4) to 3.1 +/- 0.4 microM (n = 3). Similarly, varying Ko between 0.3 and 10.8 mM (Nai = 24 mM) increased Ip from 0.13 +/- 0.01 (n = 5) to 0.90 +/- 0.05 microA/cm2 (n = 5) with a K0.5 for Ko of 1.94 mM and increased K0.5 for ouabain from 0.56 +/- 0.14 (n = 3-6) to 10.0 +/- 1.1 microM (n = 6). All of these changes are predicted by the model presented. A qualitative explanation of these results is that Nai and Ko interact with the Na/K pump to shift the steady-state distribution of the Na/K pump molecules among the kinetic states. This shift in state distribution alters the probability that the Na/K pump will be in the conformation that binds ouabain with high affinity, thus altering the apparent affinity. In intact cells, the measured apparent affinity represents a combination of all the rate constants in the model and does not equate to simple first-order binding kinetics.(ABSTRACT TRUNCATED AT 400 WORDS)

scholarly journals Independent Versus Coupled Inactivation in Sodium Channels

1998 ◽  
Vol 111 (3) ◽  
pp. 451-462 ◽  
Author(s):  
Nenad Mitrovic ◽  
Alfred L. George ◽  
Richard Horn
Keyword(s):  
Steady State ◽  
Peak Current ◽  
Recovery From Inactivation ◽  
Current Voltage ◽  
Steady State Inactivation ◽  
Kinetics Of ◽  
Current Voltage Relationship ◽  
Hyperpolarizing Shift ◽  
S4 Segment ◽  
Positively Charged

The voltage sensor of the sodium channel is mainly comprised of four positively charged S4 segments. Depolarization causes an outward movement of S4 segments, and this movement is coupled with opening of the channel. A mutation that substitutes a cysteine for the outermost arginine in the S4 segment of the second domain (D2:R1C) results in a channel with biophysical properties similar to those of wild-type channels. Chemical modification of this cysteine with methanethiosulfonate-ethyltrimethylammonium (MTSET) causes a hyperpolarizing shift of both the peak current–voltage relationship and the kinetics of activation, whereas the time constant of inactivation is not changed substantially. A conventional steady state inactivation protocol surprisingly produces an increase of the peak current at −20 mV when the 300-ms prepulse is depolarized from −190 to −110 mV. Further depolarization reduces the current, as expected for steady state inactivation. Recovery from inactivation in modified channels is also nonmonotonic at voltages more hyperpolarized than −100 mV. At −180 mV, for example, the amplitude of the recovering current is briefly almost twice as large as it was before the channels inactivated. These data can be explained readily if MTSET modification not only shifts the movement of D2/S4 to more hyperpolarized potentials, but also makes the movement sluggish. This behavior allows inactivation to have faster kinetics than activation, as in the HERG potassium channel. Because of the unique properties of the modified mutant, we were able to estimate the voltage dependence and kinetics of the movement of this single S4 segment. The data suggest that movement of modified D2/S4 is a first-order process and that rate constants for outward and inward movement are each exponential functions of membrane potential. Our results show that D2/S4 is intimately involved with activation but plays little role in either inactivation or recovery from inactivation.

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