Detail publikačního výsledku

A Dynamic Mesh Method to Model Shape Change during Electrodeposition

KARIMI-SIBAKI, E.; KHARICHA, A.; ABDI,A.; WU, M.; LUDWIG, A.; BOHÁČEK, J.

Originální název

A Dynamic Mesh Method to Model Shape Change during Electrodeposition

Anglický název

A Dynamic Mesh Method to Model Shape Change during Electrodeposition

Druh

Článek WoS

Originální abstrakt

A novel dynamic mesh-based approach is proposed to simulate shape change of the deposit front during electrodeposition. Primary and secondary current distributions are computed. The proposed numerical model is tested on a two dimensional system for which analytical solutions was previously presented by Subramanian andWhite [J. Electrochem. Soc., 2002, C498-C505]. Firstly, calculations are carried out only in the electrolyte where the deposit front is considered to be the boundary of the computational domain. Secondly, a fully coupled simulation is carried out, and field structures such as electric potential and electric current density are computed both in the electrolyte and deposit. It is found that the deposit region must be included in calculations of primary current distribution as the magnitude of electric potential is inevitably non-zero at the deposit front during electrodeposition. However, the deposit front can be accurately tracked considering secondary current distribution with or without involving the deposit region in our calculations. All transient results are shown through animations in the supplemental materials. (c) 2019 The Electrochemical Society.

Anglický abstrakt

A novel dynamic mesh-based approach is proposed to simulate shape change of the deposit front during electrodeposition. Primary and secondary current distributions are computed. The proposed numerical model is tested on a two dimensional system for which analytical solutions was previously presented by Subramanian andWhite [J. Electrochem. Soc., 2002, C498-C505]. Firstly, calculations are carried out only in the electrolyte where the deposit front is considered to be the boundary of the computational domain. Secondly, a fully coupled simulation is carried out, and field structures such as electric potential and electric current density are computed both in the electrolyte and deposit. It is found that the deposit region must be included in calculations of primary current distribution as the magnitude of electric potential is inevitably non-zero at the deposit front during electrodeposition. However, the deposit front can be accurately tracked considering secondary current distribution with or without involving the deposit region in our calculations. All transient results are shown through animations in the supplemental materials. (c) 2019 The Electrochemical Society.

Klíčová slova

SIMULATION; DEPOSITION; TRANSPORT; SECONDARY; COPPER; FLOW

Klíčová slova v angličtině

SIMULATION; DEPOSITION; TRANSPORT; SECONDARY; COPPER; FLOW

Autoři

KARIMI-SIBAKI, E.; KHARICHA, A.; ABDI,A.; WU, M.; LUDWIG, A.; BOHÁČEK, J.

Rok RIV

2021

Vydáno

31.07.2019

Nakladatel

ELECTROCHEMICAL SOC INC

Místo

PENNINGTON

ISSN

0013-4651

Periodikum

JOURNAL OF THE ELECTROCHEMICAL SOCIETY

Svazek

166

Číslo

12

Stát

Spojené státy americké

Strany od

D521

Strany do

D529

Strany počet

9

URL