Table 4.

Model parameters

Channel domain Transition Forward rate Reverse rate 
DI L689I A↔I1 1.11E-04 4.45E-04 
 I1↔I2 3.97E-05 2.24E-05 
 I2↔I3 3.33E-04 9.48E-01 
DII L689I A↔I1 4.91E-05 3.56E-04 
 I1↔I2 4.79E-05 3.03E-05 
 I2↔I3 6.19E-09 4.91E-02 
DIII L689I A↔I1 2.18E-04 4.63E-04 
 I1↔I2 3.82E-05 2.38E-05 
 I2↔I3 2.97E-04 3.55E-03 
DIV L689I A↔I1 2.13E-04 3.99E-04 
 I1↔I2 1.83E-05 2.27E-05 
 I2↔I3 4.88E-04 9.91E-01 
Channel domain Transition Forward rate Reverse rate 
DI L689I A↔I1 1.11E-04 4.45E-04 
 I1↔I2 3.97E-05 2.24E-05 
 I2↔I3 3.33E-04 9.48E-01 
DII L689I A↔I1 4.91E-05 3.56E-04 
 I1↔I2 4.79E-05 3.03E-05 
 I2↔I3 6.19E-09 4.91E-02 
DIII L689I A↔I1 2.18E-04 4.63E-04 
 I1↔I2 3.82E-05 2.38E-05 
 I2↔I3 2.97E-04 3.55E-03 
DIV L689I A↔I1 2.13E-04 3.99E-04 
 I1↔I2 1.83E-05 2.27E-05 
 I2↔I3 4.88E-04 9.91E-01 

The discrete-state Markov models used in Fig. 8 in our companion paper (Silva and Goldstein, 2013) are parameterized for the forward and reverse rate transitions between states A and I1, states I1 and I2, and states I2 and I3 for the L689I mutation in each of the voltage-sensor domains.

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