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. 1998 Dec 1;112(6):715–726. doi: 10.1085/jgp.112.6.715

Table I.

Effects of Zn2+ on the Forward (α) and Backward (β) Rates of Inactivation

[Zn2+] (μM) τ (s) I/Imax β (× 10−3 s−1) α (× 10−3 s−1) α1000
0 10 100 0 10 100 β0 β10 β100 β1000 α0 α10 α100
19.8°C  1093.3 344.7 75.5 0.2508 0.1271 0.0516 0.229 0.369 0.683 2.98      0.686     2.532       12.562 18.31
(0.2208) (0.0971) (0.0216) (0.202) (0.282) (0.286) 1.42      (0.713)        (2.619)      (12.959) 18.18
24.0°C 235.4      67.1 17.8 0.2213 0.0891 0.0391 0.940 1.328 2.197 2.34      3.308 13.575       53.983 16.32
(0.1913) (0.0591) (0.0091) (0.813) (0.881) (0.511) 0.63      (3.435) (14.022)       (55.669) 16.21
28.3°C 51.1       13.2  4.2 0.0908 0.0561 0.0378 1.777 4.250 9.000 5.06 17.792 71.508 229.095 12.88
(0.0608) (0.0261) (0.0078) (1.190) (1.977) (1.857) 1.56 (18.379) (73.781) (236.238) 12.85

The table lists the slow-gating relaxation time constant (τ) calculated from Fig. 5, the noninactivated current fraction (I/Imax) obtained from Fig. 7 C, the forward (α) and the backward (β) rates of inactivation at three different temperatures, and in 0, 10, and 100 μM Zn2+. β was calculated by dividing I/Imax by τ (Eq. 1), whereas α was obtained by subtracting β from 1/τ (Eq. 2). The numbers outside the parentheses were derived from original measured current without leak subtraction. The I/Imax values in parentheses were obtained by subtracting 0.03 from the original values outside parentheses and the α's and β's in parentheses were calculated accordingly.