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Three-segment electrodiffusion probes for measuring velocity fields close to a wall
Authors:V. Sobolík  O. Wein  O. Gil  B. Tribollet
Affiliation:(1) Institute of Chemical Process Fundamentals, Czechoslovak Academy of Sciences, 165 02 Praha, 6 Suchdol, Czechoslovakia;(2) LP 14 of C.N.R.S., University of P. and M. Curie, Tour 22, 4 Place Jussieu, F-75252, Paris Cedex 05, France
Abstract:Three-segment electrodiffusion probes embedded in a wall allow to determine simultaneously the three kinematic parameters of flow close to the probe surface: the flow directiontheta, the wall shear rateq, and the normal velocity coefficientA,vz = –A z2. A well-controlled three-dimensional flow, generated by a rotating disk, was used to demonstrate the capabilities of this new kind of electrodiffusion probes by comparing experimental results with the prediction based on the well-known hydrodynamical theory.List of symbols A normal flow coefficient, Eq. (1) - A axis of the adjustment rod, Fig. 2 - c0 concentration of depolarizer (mol/m3) - D diffusivity of depolarizer (m2/s) - E correction of total current on normal flow effect - ex reference direction of the probe, Figs. 1 and 3 - F Faraday constant (F = 96,464 C/mol) - Fs normalized directional characteristic fors-th segment - fsm,gsm Fourier coefficients of directional characteristics, Eq. (4) and Table 3 - hm corrections of Fourier coefficients on normal flow effect, Eqs. (4) and (7) - is limiting diffusion current throughs-th segment (A) - itot(r) total current through the probe in dependence on its eccentricity (A) - K transport coefficient, Eqs. (3) and (5) - n number of electrons involved in redox reaction - O axis of the rotating disk, Fig. 2 - P centre of the probe, Fig. 2 - q magnitude of vectorial wall shear rate (s-1) - qx,qy components of vectorial wall shear rate - Q ratio of the currents in an eccentric and the central position of the probe, Eq. (15) - r radial coordinate, eccentricity of the probe - rA eccentricity of the adjustment rod (rA =Omacr Amacr, Fig. 2) - r, PHgr, z polar coordinates on the rotating disk - R effective radius of the probe (R = 0.337 mm) - S macroscopic area of the probe (S = 0.357 mm2) - x, y, z Cartesian coordinates moving with the probe - agr adjustment angle, Figs. 2 and 3 - beta angle included between local radius-vectoromacr ¯P of the probe and local direction of flow, Fig. 3 - theta angle included between reference directionex of the probe and local direction of flow, Fig. 3 - theta0 theoretical prediction oftheta, Eq. (11) - x0 theoretical prediction ofx, Eq. (14) - xexpx calculated from experimental data using Eq. (4) - v kinematic viscosity (m2/s) - sgr angle implied between gradient ofq and direction of flow, Eq. (8) - OHgr angular speed of the rotating disk (rad/s)
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