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Leigh D. Plant, Peter N. Bowers, Qianyong Liu, Thomas Morgan, Tingting Zhang, Matthew W. State, Weidong Chen, Rick A. Kittles, Steve A.N. Goldstein
Published in Volume 116, Issue 2
J Clin Invest. 2006; 116(2):430–435 doi:10.1172/JCI25618
Abstract | Full text | PDF | Supplemental material
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Figure 2

Y1103 channels show a change in inactivation gating at low pH. Whole-cell currents in HEK-293 cells expressing SCN5A S1103 (open squares) or SCN5A Y1103 (filled squares). Top: Sample traces with S1103 channels. Arrows indicate points of measure. Scale bar: 1 nA. Filter and sampling frequencies were 5 and 20 kHz, respectively. (A) Normalized conductance/voltage (G/Gmax) relationships for S1103 and Y1103 channels show no change with a shift of internal pH (pHi) from pH 7.4 to pH 6.7 (n = 4–13). Curves fitted to a Boltzmann relationship (y = 1/{1 + exp[V – V1/2/Vs]}, where Vs is slope factor). Inset: Current/voltage relationships. Values for V1/2 are reported in Supplemental Table 3. (B) Y1103 channels showed a shift in voltage-dependent steady-state inactivation at pHi 6.7, whereas S1103 channels did not. Normalized peak current values (I/Imax) are plotted against prepulse potential (mV). Curves fitted as in A. At pH 6.7, V1/2 for S1103 is –84 + 1 mV (n = 7) and for Y1103 is –77 + 2 mV (n = 8; P < 0.05; 2-population Student’s t test). Values are mean ± SEM. (C) Time constants for recovery from inactivation were the same for S1103 and Y1103 channels at physiological pH but were speeded when Y1103, but not S1103, was exposed to pHi 6.7 (n = 11). Curves are exponential fits to the recovery time course, I(t)/Imax = Af[1 – exp(–t/τf)] + As[1 – exp(–t/τs)], where A is the amplitude of fast (f) and slow (s) components and t is time. Values for τ are reported in Supplemental Table 3.