Mass transfer at rotating cone electrodes |
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Authors: | A F S Afshar D R Gabe B Sewell |
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Affiliation: | (1) IPTME, Loughborough University of Technology, LE11 3TU Loughborough, UK;(2) Twickenham Plating Group PLC, Colne Rd., TW1 4JR Twickenham, Middlesex, UK;(3) Present address: S. G. Owen Co. Ltd., Lodge Farm Industrial Estate, NN5 7UF Northampton, UK |
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Abstract: | Upright and inverted rotating cone electrodes (apex half angle 52°) have been studied using electrodeposition of copper from an acid electrolyte (Sc=1770) by means of limiting current mass transport techniques. The behaviour suggests that it is appropriate to regard these electrodes as modified disc electrodes. The upright rotating cone electrode exhibits a flow transition atRe=1×105. In laminar flowSh=4.5Re
0.48 and in turbulent flowSh=0.04Re
0.95. The inverted rotating cone electrode exhibits a flow transition atRe=6×104. In laminar flowSh=4.5Re
0.45 and in turbulent flowSh=0.04Re
0.88. The data have been interpreted in terms of a coating thickness affected by throwing power effects and the use of a conical cathode cell for control of high speed electrodeposition processes is indicated.Nomenclature
A
electrode area (cm2)
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C
b
concentration (of bulk solution) (mol cm–3)
- c
concentration difference (mol cm–3)
-
D
diffusion coefficient (cm2 s–1)
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f/2
friction factor
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F
Faraday's constant (96485 A s mol–1)
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i
L
limiting current density (A cm–2)
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J
mass transfer flux (mol s–1 cm–2)
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K
L
mass transfer coefficient (cm s–1)
-
l
slant height of the cone (cm)
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U
peripheral velocity (cm s–1)
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x
local condition coordinate (cm)
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z
no. of electrons
-
apex half-angle of cone
-
angular velocity (rad s–1)
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wall shear stress (dyn cm–2)
-
kinematic viscosity (cm2 s–1)
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Re
Reynolds number=Ud/v
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Sc
Schmidt number=v/D
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Sh
Sherwood number=K
L
d/D |
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Keywords: | |
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