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. 2010 Sep;136(3):273–282. doi: 10.1085/jgp.200910398

Table I.

Biophysical properties of heteromeric Kv1 channels

Parameters Adjacent Kv1.1-1.1-1.2-1.2 Reverse adjacent Kv1.2-1.2-1.1-1.1 Diagonal Kv1.1-1.2-1.1-1.2 Reverse diagonal Kv1.2-1.1-1.2-1.1
τact at 0 mV (ms) 1.9 ± 0.1 (3) 2.3 ± 0.6 (3) 1.4 ± 0.1 (3) 1.3 ± 0.1 (4)
τinact1 at 0 mV (ms) 540 ± 2 (5) 529 ± 50 (4) 306 ± 34 (3)a 341 ± 17 (4)a
τinact2 at 0 mV 6,200 ± 500 (5) 5,053 ± 596 (4) 3,586 ± 485 (3) 4,372 ± 404 (4)
V 1/2 (mV) −17 ± 1 (9) −18 ± 1 (14) −22 ± 1 (7)a −21 ± 1 (10)a
Slope (k) 11 ± 1 (9) 12 ± 1 (14) 11 ± 1 (7) 10 ± 1 (10)

Values (mean ± SEM) for activation and inactivation were derived by fitting to single- and double-exponential functions, respectively. V1/2 and slope k were calculated from Boltzmann equation fitting of the gk-V plots.

a

Significant difference from adjacent constructs (P < 0.05; Mann-Whitney U test).