Eiran Kochavi, Yoram Oren, Abraham Tamir, Tuvia Kravchik BENGURION UNIVERSITY OF THE NEGEV, FACULTY - PowerPoint PPT Presentation

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Eiran Kochavi, Yoram Oren, Abraham Tamir, Tuvia Kravchik BENGURION UNIVERSITY OF THE NEGEV, FACULTY

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Title: Eiran Kochavi, Yoram Oren, Abraham Tamir, Tuvia Kravchik BENGURION UNIVERSITY OF THE NEGEV, FACULTY


1
Eiran 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

2
The 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.

3
The 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.

4
The experimental system
5
Results
  • 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.

6
Results
  • Mass transfer coefficients decrease by increasing
    the nozzle-electrode distance. However, the
    influence is more pronounced at smaller distances

7
Scheme 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).

11

Concentration profile of impinging jet
over a submerged sphere electrode

12
Flow vectors map of impinging jet over a
submerged sphere electrode

13
Theoretical 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

14
Comparison between Experimental and Theoretical
limiting currents
15
PHOENICS characteristics
  • PHOENICS X11 Version 2.1.3
  • Operating system UNIX
  • Convergence
  • The number of iterations - 2000

16
PHOENICS 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

17
CONCLUSIONS
  • 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.

18
RECOMMENDATIONS
  • 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.
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