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The theory showed that the wave was controlled by the driving work difference of the two PFs.
So the driving work difference Δw (Fig. 5b) should also be averaged over time to evaluate the wave velocity from equation (6).
For the whole system, the energy generated by the driving work difference Δw = w2−w1 equaled the energy dissipated viscously by the PF.
To obtain the wave velocity from equation (1), the driving work difference w2−w1 and the equilibrium jump frequency κ0 should be obtained in advance.
The driving work difference between PF2 and PF1, which drove the wave, was obtained from w2 and w1 illustrated above (Fig. 5a).
All the forces that induced the driving work of the PF were contained into the disjoining pressure39, which could be obtained directly from MD results.
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