The stability and growth or dissolution of a single surface nanobubble on a chemically patterned surface are studied by Molecular Dynamics (MD) simulations of binary mixtures consisting of Lennard-Jones (LJ) particles. Our simulations reveal how pinning of the three-phase contact line on the surface can lead to the stability of the surface nanobubble, provided that the concentration of the dissolved gas is oversaturated. We have performed equilibrium simulations of surface nanobubbles at different gas oversaturation levels . The equilibrium contact angle is found to follow the theoretical result of Lohse and Zhang (Phys. Rev. E 2015, 91, 031003®), namely $\sin\theta_e = \zeta L/L_cL_c = 4\gamma/P_0\gammaP_0\zeta<0$ the surface nanobubble dissolves and the dissolution dynamics shows a “stick-jump” behaviour of the three-phase contact line.

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