Two-electrode voltage clamp

MC Marisol Sampedro Castañeda
EZ Edmar Zanoteli
RS Renata S Scalco
VS Vinicius Scaramuzzi
VC Vitor Marques Caldas
UR Umbertina Conti Reed
AS Andre Macedo Serafim da Silva
BO Benjamin O’Callaghan
RP Rahul Phadke
EB Enrico Bugiardini
RS Richa Sud
SM Samuel McCall
MH Michael G Hanna
HP Hanne Poulsen
RM Roope Männikkö
EM Emma Matthews
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Two-electrode voltage clamp is routinely used to characterize functional properties of Na+/K+-ATPase pumps (Horisberger and Kharoubi-Hess, 2002; Li et al., 2006; Poulsen et al., 2010; Vedovato and Gadsby, 2014; Hilbers et al., 2016). Data were collected with a GeneClamp 500B amplifier, Digidata 1200 digitizer and pCLAMP software (Molecular Devices) at room temperature. Currents were measured 2–4 days after injection in oocytes preincubated (>30 min) with a Na+-loading buffer (Poulsen et al., 2010), unless otherwise mentioned. Electrode resistance was 0.2–0.7 MΩ when filled with NaCl 3 M to allow fast voltage clamp. Currents were elicited with 200-ms test steps from −160 to +60 mV, at 20-mV increments, from a holding potential of −30 mV. Recordings were sampled at 5 kHz and filtered at 1 kHz. Ouabain 1 µM was included in all recording solutions to block endogenous pumps.

Transient sodium-dependent currents were recorded in 0 [K+]o (in mM: NaOH 115, sulphamic acid 110, MgCl2 1, CaCl2 0.5, BaCl2 5, HEPES 10, pH 7.4) with and without 10 mM ouabain, and isolated offline by subtraction. Scale was maximized to minimize signal clipping, and 10 traces were averaged to improve signal-to-noise ratio. The integral of transient ouabain-sensitive currents at −30 mV following the test voltage steps was plotted against test voltage and fitted to a Boltzmann function:

yielding the mid-point potential (V1/2), slope factor (dV) and top (A1) and bottom (A2) asymptotes. Total charge transfer, Qtot, represents the span of the Boltzmann fit (A1 − A2). Rate constants of Na+ binding/unbinding reactions derived from single (wild-type) or double (p.S779N) exponential fits to transient currents at the onset of the pulse. For p.S779N, the fast time constant, describing >90% of charge transfer, was analysed. Boltzmann fits to mean relaxation-voltage curves yielded the maximal forward and backward rate constants.

Leak currents were measured as the mean ouabain-sensitive currents in the last 50 ms of the test pulse. In some experiments, pH was altered or Na+ was replaced by NMDG+ as monovalent cation in a 3:1 ratio. In experiments with 145 mM Na+, 30 mM NaOH was added to 0 [K+]o solution. Reversal potential and slope conductance were obtained from linear fits to the current-voltage data.

Forward pumping activity was measured in various [K+]o concentrations before and after addition of 10 mM ouabain. Records were subtracted offline. In these experiments, extracellular NaOH was replaced with equimolar KOH. Concentration-response curves were fit with a Hill equation:

yielding [K+] EC50 values, Hill coefficient (h) and top (A1) and bottom (A2) asymptotes.

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