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. 1998 Feb 1;111(2):313–342. doi: 10.1085/jgp.111.2.313

Table III.

Parameter Estimates for Scheme 3+2′

Partial charge WT's rate at 0 mV V2's rate at 0 mV
e0 s−1 s−1
For S0↔ S1, S1↔ S2, and S2↔ S3
qa 1 = 0.47 a 1(0) = 1650 (c = 1.3) a 1(0) = 1450 (c)
qb 1 = −0.52 b 1(0) = 450 (1/c) b 1(0) = 450 (1/c)
qa 2 = 0.08 a 2(0) = 4900 a 2(0) = 4270
qb 2 = −0.52 b 2(0) = 960 b 2(0) = 960
qa 3 = 0.08 a 3(0) = 7920 a 3(0) = 6980
qb 3 = −0.52 b 3(0) = 1560 b 3(0) = 1560
For the transitions near the open state
q αN-1 = 0.75  αN-1(0) = 7000      αN-1(0) = 3800
q βN-1 = −0.30  βN-1(0) = 340      βN-1(0) = 19000
q αN = 0.18   αN(0) = 7000 αN(0) = 3800
q βN = −0.52   βN(0) = 240 βN(0) = 650
qc = 0.2 c(0) = 7 c(0) = 17
qd = 0.0 d(0) = 600 d(0) = 600
qe 1 = 0.0    e 1(0) = 230 e 1(0) = 400
qf 1 = 0.20    f 1(0) = 3500 f 1(0) = 3500
qe 2 = 0.0    e 2(0) = 600 e 2(0) = 600
qf 2 = 0.0    f 2(0) = 7000 f 2(0) = 7000

The parameter c reflects a small amount of cooperative interaction, which has been introduced into S0↔ S1, as shown in Scheme I.