The current density during battery operation is often assumed uniform across the entire electrode surface. This may be valid for conformal solid/liquid interfaces; however, solid/solid interfaces generally have imperfect contacts. By introducing the contact area ratio, γ, to the electrochemical model, it can be demonstrated clearly that the effective current density scales linearly with the 1/γ and the overpotential scales exponentially with contact area loss, 1-γ.The calculation of surface contact area must consider the multi-length-scale nature of surface roughness. Assuming surface roughness is self-affine, Bo Persson’s multiscale contact mechanics model for elastic materials can be used for the cathode/solid electrolyte interface to predict the necessary pressure to maintain the original contact area. [1]However, the most challenging process is Li-stripping, as the vacancy generated by each Li atom removed from the interfaces can accumulate and generate voids, reducing the contact area. However, under an applied stack pressure, the self-affine property will reach a steady state interface contact ratio (γo.) in different length scales. Thus, we proposed a coupled atomistic-and-continuum model, which will capture Li striping and vacancy hopping and accumulation near the Li/SE interface with Density Functional Theory (DFT) informed Kinetic Monte Carlo (KMC) simulations and predict the macroscopic contact area evolution according to the macroscopic creep law with finite element simulations (FEM). The creep rate will be mapped to preferred forward hopping rates for all the Li atoms at the atomic scale. Solving these models iteratively leads to a steady contact area ratio (γo.). Generally, lithiophilic interface requires less stack pressure to maintain a flat surface while a higher stack pressure is needed at lithiophobic interfaces to accelerate Li vacancy diffusion into the bulk and maintain a flat surface. This critical stack pressure needs to be high enough to alter the Li forward-and-backward hopping barriers at the interface. This predictive multiscale simulation scheme was able to combine multiple chemical-mechanical effects during Li stripping morphology evolution. [2,3] [1] Hong-Kang Tian and Yue Qi, Electrochem. Soc. 2017, 164, E3512[2] T. Yang and Y. Qi, Chem. Mat. 2021, 33, 2814-2823[3] Feng, C.T. Yang, and Y. Qi, J. Electrochem. Soc. 2022, 169, 090526