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Electrodeposition Modeling Using Coupled Phase-Field And Lattice Boltzmann Approach

Author

Listed:
  • D. V. PATIL

    (The CUNY Energy Institute, Department of Chemical Engineering, City College of New York, 140th Street and Convent Avenue, New York, NY 10031, USA)

  • K. N. PREMNATH

    (Department of Mechanical Engineering, University of Colorado Denver, 1200 Larimer Street, Campus Box 112, PO Box 173364 Denver, CO 80217-3364, USA)

  • D. DESAI

    (The CUNY Energy Institute, Department of Chemical Engineering, City College of New York, 140th Street and Convent Avenue, New York, NY 10031, USA)

  • SANJOY BANERJEE

    (The CUNY Energy Institute, Department of Chemical Engineering, City College of New York, 140th Street and Convent Avenue, New York, NY 10031, USA)

Abstract

In this paper, a coupled phase-field (PF) and lattice Boltzmann method (LBM) is presented to model the multiphysics phenomenon involving electro-chemical deposition. The deposition (or dissolution) of the electrode is represented using variations of an order-parameter. The time-evolution of an order-parameter is proportional to the variation of a Ginzburg–Landau free-energy functional. Further, the free-energy densities of the two phases are defined based on a dilute or an ideal solution approximation. An efficient LBM is used to obtain the converged electro-static potential field for each physical time-step of the evolution of the PF variable. The coupled approach demonstrates the applicability of the LBM in a multiphysics scenario. The numerical validation for the coupled approach is performed by the simulation of the electrodeposition process ofCufromCuSO4solution.

Suggested Citation

  • D. V. Patil & K. N. Premnath & D. Desai & Sanjoy Banerjee, 2014. "Electrodeposition Modeling Using Coupled Phase-Field And Lattice Boltzmann Approach," International Journal of Modern Physics C (IJMPC), World Scientific Publishing Co. Pte. Ltd., vol. 25(01), pages 1-8.
  • Handle: RePEc:wsi:ijmpcx:v:25:y:2014:i:01:n:s0129183113400184
    DOI: 10.1142/S0129183113400184
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