TY - JOUR
T1 - Theory of microscopic electrodeposition under a uniform parallel magnetic field - 1. Nonequilibrium fluctuations of magnetohydrodynamic (MHD) flow
AU - Morimoto, Ryoichi
AU - Miura, Miki
AU - Sugiyama, Atsushi
AU - Miura, Makoto
AU - Oshikiri, Yoshinobu
AU - Mogi, Iwao
AU - Takagi, Satoshi
AU - Yamauchi, Yusuke
AU - Aogaki, Ryoichi
N1 - Funding Information:
This work was performed in part at the Queensland node of the Australian National Fabrication Facility, a company established under the National Collaborative Research Infrastructure Strategy to provide nano- and micro-fabrication facilities for Australia's researchers.
Publisher Copyright:
© 2019 Elsevier B.V.
PY - 2019/9/1
Y1 - 2019/9/1
N2 - Nonequilibrium fluctuations of concentration, velocity and so on are formulated for electrode reactions including electrodeposition under a uniform magnetic field parallel to electrode surface. In electrodeposition, nonequilibrium fluctuations occur on the both sides of the electrode surface and solution; on the electrode-surface side, three-dimensional (3D) and two-dimensional (2D) nucleation proceed under the control of symmetrical and asymmetrical nonequilibrium fluctuations, respectively. On the solution side, a characteristic laminar flow called magnetohydrodynamic (MHD) flow with microscopic convection flows called micro-MHD flows are induced, so that the fluctuations on the solution side are described as Fourier components of complex 2D plane waves traveling with the MHD flow. The fluctuations on the electrode-surface side are interfered with the micro-MHD flows, yielding characteristic 3D and 2D nuclei. In Part 1 of the present paper, the amplitudes of the micro-MHD flows and concentration fluctuation on the solution side are first established independent of the fluctuations on the electrode-surface side.
AB - Nonequilibrium fluctuations of concentration, velocity and so on are formulated for electrode reactions including electrodeposition under a uniform magnetic field parallel to electrode surface. In electrodeposition, nonequilibrium fluctuations occur on the both sides of the electrode surface and solution; on the electrode-surface side, three-dimensional (3D) and two-dimensional (2D) nucleation proceed under the control of symmetrical and asymmetrical nonequilibrium fluctuations, respectively. On the solution side, a characteristic laminar flow called magnetohydrodynamic (MHD) flow with microscopic convection flows called micro-MHD flows are induced, so that the fluctuations on the solution side are described as Fourier components of complex 2D plane waves traveling with the MHD flow. The fluctuations on the electrode-surface side are interfered with the micro-MHD flows, yielding characteristic 3D and 2D nuclei. In Part 1 of the present paper, the amplitudes of the micro-MHD flows and concentration fluctuation on the solution side are first established independent of the fluctuations on the electrode-surface side.
KW - Instability
KW - Magnetic field
KW - Micro-MHD effect
KW - Micro-MHD flow
KW - Nonequilibrium fluctuation
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U2 - 10.1016/j.jelechem.2019.113254
DO - 10.1016/j.jelechem.2019.113254
M3 - Article
AN - SCOPUS:85068542092
SN - 1572-6657
VL - 848
JO - Journal of Electroanalytical Chemistry
JF - Journal of Electroanalytical Chemistry
M1 - 113254
ER -