Title: Eiran Kochavi, Yoram Oren, Abraham Tamir, Tuvia Kravchik BENGURION UNIVERSITY OF THE NEGEV, FACULTY
1Eiran Kochavi, Yoram Oren, Abraham Tamir, Tuvia
KravchikBEN-GURION UNIVERSITY OF THE NEGEV,
FACULTY OF ENGINEERING SCIENCES, DEPARTMENT OF
CHEMICAL ENGINEERING, BEER-SHEVA, ISRAEL
- MASS TRANSFER TO SPHERE AND HEMISPHERE ELCTRODES
BY IMPINGING JET
2The goals of this work
- Characterization of mass transfer rates to
sphere and hemisphere electrodes, under impinging
jet of solution. - Characterization of mass transfer with both
electrodes in two systems submerged in the
electrolyte solution and unsubmerged. - Development of theoretical model that
characterizes the system of impinging jet to
electrodes.
3The goals of this work (cond)
- Comparison between experimental and theoretical
limiting currents - Prediction of flow and concentration profiles at
complex geometry system by using numerical
simulation program (PHOENICS) with the proper
boundary conditions.
4The experimental system
5Results
- Mass transfer coefficients increased as we
increased the linear velocity of the electrolyte
jet at the nozzle exit - Mass transfer coefficients for the submerged
hemisphere electrode, are higher than the
coefficients for a sphere electrode.
6Results
- Mass transfer coefficients decrease by increasing
the nozzle-electrode distance. However, the
influence is more pronounced at smaller distances
7Scheme of solution domain
8 Theoretical model and PHOENICS settings
- The grid distribution was divided into two
sections (in Y-axis) - 1- Near the electrode surface (20 cells) the
distribution was according to a power-law
expanding grid - 2- In the electrolyte bulk (20 cells) the
distribution was according to a uniform grid
9 Theoretical model and PHOENICS settings
(contd)
- The model employed a 41x37 grid cells (BFC) in
the y-z plane. - The cells region was divided into two frames
- 1- zone where the solution flows out of the
nozzle. The method of the interpolation of
internal points was transfinite (TRANS)
10 Theoretical model and PHOENICS
settings(contd)
- 2- zone where the solution impinging the
electrode and flows over it to the outlet. The
method of the interpolation of internal points
was Laplace-like equation (LAP).
11Concentration profile of impinging jet
over a submerged sphere electrode
12Flow vectors map of impinging jet over a
submerged sphere electrode
13Theoretical results for impinging jet on a
submerged sphere electrode
- At the impingement zone we observed a sharp
concentration profile that is influenced by jet
impingement on the electrode surface. - Because of the vortex (at the flow vectors map)
on the electrode sides we observed the
concentration profile to become wider along Z-axis
14Comparison between Experimental and Theoretical
limiting currents
15PHOENICS characteristics
- PHOENICS X11 Version 2.1.3
- Operating system UNIX
- Convergence
- The number of iterations - 2000
16PHOENICS characteristics
- Relaxation
- The Relaxation factors for the variables
- P1(pressure) linear relaxation (LINRLX)- 0.01
- C1(mass fraction of ferricyanid ion) linear
relaxation (LINRLX) - 0.01 - C2 (mass fraction of water)linear relaxation
(LINRLX) - 0.01 - V1(velocity vector in Y-axis) false-time-step
relaxation (FALSDT) - 110-5 - W1(velocity vector in Z-axis) false-time-step
relaxation (FALSDT) - 110-6
17CONCLUSIONS
- 1. Using a numerical simulation code (PHOENICS),
enables us to develop a method to predict the
theoretical limiting current values - 2. Calculated limiting currents from the
concentration field distribution, were in a good
agreement (0.5-10 ) by comparison to
experimental results.
18RECOMMENDATIONS
- 1. Development of theoretical model for submerged
hemisphere electrode and compare the results with
the experimental one - 2. Developments of theoretical model for
unsubmerged sphere and hemisphere electrode, and
compare the results with the experimental one.