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51849121397
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In all of the metadynamics runs that we have performed, we have chosen as the collective variable the distance between the WVI ion and the O atom of a nearby water molecule. We have done one simulation for each of the following processes: (i) WO3(OH, H2O → [WO3(OH)(H2O, The parameters used in this run are k, 0.2 au and M, 10 amu. The height of the hills (W) is 0.31 kcal mol-1, their perpendicular width (Δs⊥) 0.1, and the deposition rate (Δt) 0.0144 ps. The estimated error (ε) in the computation of the free energy is 1 kcal mol-1. The total simulation time (ttotal) was 9 ps, ii, WO3(OH)(H 2O, → WO3OH, H 2O. k, 0.2 au, M, 10 amu, W, 0.19 kcal mol -1, Δs⊥, 0.1
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total = 5 ps.
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44
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51849122304
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Different metadynamics runs were performed. One for each of the following processes: (i) WO2(OH)2, H2O → [WO 2(OH)2(H2O, Same parameters as those for the previous metadynamics, except W, 0.19 kcal mol-1 and ttotal, 25 ps, ii, WO2(OH)2(H 2O, → WO2(OH)2, H2O. Same parameters as those for (i, except ttotal, 17 ps, iii, WO2(OH)2(H2O, H2O → [WO2(OH)2(H2O)2, Same parameters as those for (i, except ttotal, 9 ps, iv, WO 2(OH)2(H2O)2] → [WO 2(OH)2(H2O, H2O. Same parameters as those for i, except W, 0.25 kcal mol-1 and t total, 6 ps
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total = 6 ps.
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45
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51849142104
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total = 5 ps.
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total = 5 ps.
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Poblet, J.M.7
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