Table 1.
List of simulations for WT KcsA with different opening degrees of inner gate
Traj IDPDBaIntracellular gatebRuntime (ns)Protonated residuesIon concentration (mM)
3F7Vc Fully open (23 Å) 1,600 H25,E71,E120,H124 200 
3F7Vc Fully open (23 Å) 340 H25,E71,E120,H124 150 
3F7Vc Fully open (23 Å) 1,130 H25,E71,E120,H124 150 
3F7Vc Fully open (23 Å) 450 H25,E71,E120 200 
5VK6d Fully open (22 Å) 10,000 H25,E71,E118,H124 150 
3FB6 Partially open (16 Å) 500 H25,E71,E118 200 
3FB6 Partially open (16 Å) 1,000 H25,E71,E120,H124 200 
3FB6 Partially open (16 Å) 1,200 E71,E118 200 
3FB5 Partially open (14 Å) 1,000 H25,E71,E120,H124 200 
10 3FB5 Partially open (14 Å) 1,000 H25,E71 200 
11 1K4C Closed (11 Å) 1,500 E71 200 
12 3FB6e Partially open (17.5 Å) 110 H25,E71,E120 1,000 
13 3F7Ve Fully open (23 Å) 190 H25,E71,E120,H124 1,000 
Traj IDPDBaIntracellular gatebRuntime (ns)Protonated residuesIon concentration (mM)
3F7Vc Fully open (23 Å) 1,600 H25,E71,E120,H124 200 
3F7Vc Fully open (23 Å) 340 H25,E71,E120,H124 150 
3F7Vc Fully open (23 Å) 1,130 H25,E71,E120,H124 150 
3F7Vc Fully open (23 Å) 450 H25,E71,E120 200 
5VK6d Fully open (22 Å) 10,000 H25,E71,E118,H124 150 
3FB6 Partially open (16 Å) 500 H25,E71,E118 200 
3FB6 Partially open (16 Å) 1,000 H25,E71,E120,H124 200 
3FB6 Partially open (16 Å) 1,200 E71,E118 200 
3FB5 Partially open (14 Å) 1,000 H25,E71,E120,H124 200 
10 3FB5 Partially open (14 Å) 1,000 H25,E71 200 
11 1K4C Closed (11 Å) 1,500 E71 200 
12 3FB6e Partially open (17.5 Å) 110 H25,E71,E120 1,000 
13 3F7Ve Fully open (23 Å) 190 H25,E71,E120,H124 1,000 
a

This is the crystal structure used as the initial conformation in MD simulations.

b

The cross-subunit distance (shown in parentheses) between the Cα atoms of Thr112 of diagonally opposed monomer was used as an indicator for the opening degree of the inner gate in the initial conformation.

c

To produce an open-conductive model from the 3F7V structure, which displays a constricted filter, the 2.0-Å resolution x-ray structure 1K4C was used as a template, and the filter was aligned to the channel using the backbone atoms of residues 65–74 and 80–84. The backbone atoms of the filter residues 74–80 have been restrained to maintain the conductive conformation in the initial phase of MD simulations. Video 1 shows the conformational transition in Traj-1 (0–800 ns).

d

An alternative open-conductive model based on the open-conductive crystal structure 5VK6 for mutant E71A. In the initial conformation of this simulation, residue 71 was mutated back to Glu as the WT. In addition, the original disulfide bonds in the crystal structure were removed by mutating all of the relevant residues back to WT.

e

These simulations were performed to test the permeability of partially opening inner gate. To collect enough sample within limited time, the ion concentration is higher than other simulations, and these are the only two trajectories with external electric field (300 mV). In addition, the initial conformations of Traj-12 and Traj-13 were snapshots, respectively, from Traj-6 and Traj-1, and the inner gate was restrained as 17.5 Å and 23 Å through the whole trajectory.

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