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Numerical Simulation of MHD Jet flows

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free surface plasma facing components (PFCs) jet flow, droplet and film curtain ... of the upper half part generally balances those of the lower half part, so the ... – PowerPoint PPT presentation

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Title: Numerical Simulation of MHD Jet flows


1
Numerical Simulation of MHD Jet flows
Kang Weishan
Southwestern Institute of Physics Chengdu,
610064, P R China
2
Outline
  • Introduction
  • Simplified Model
  • Numerical Simulation
  • Conclusion

3
1. Introduction
  • free surface plasma facing components (PFCs)
  • jet flow, droplet and film curtain

4
Advantages of free surface
  • to withstand high plasma heat flux and ion flux
  • to extract heat efficiently
  • to improve thermal power conversion efficiencies
    significantly
  • continuously renewable surface, to enhance
    diverter lifetime

5
2. Simplified Model
2.1 Governing equations
  • conservation of mass
  • conservation of momentum
  • conservation of charge
  • Ohms law

6
2.2 Schematic of jet flow
boundary layer
core zone
7
2.3 Analyses of induced electrical current and
potential
_
_


In x-y plane
  • MHD effect on a jet flow can be broken into
    two parts
  • in X-axle direction electromagnetic (EM) force
    tend to drag the flow, which leads to a shorter
    range distance and a lager radius of the jet flow
  • in Y-axle direction EM force of the upper half
    part generally balances those of the lower half
    part, so the jet flow can keep stable and cross
    section is flatten

8
2.4 The cross-section of the jet flow is flatten
by EM force
9
3. Numerical Simulation
  • The MHD effect is reflected in an additional term
    of Lorentz force in the momentum equation which
    is derived from the Ohms law by solving the
    electrical potential equation
  • Volume of Fluid (VOF), which is used to track the
    interface between the phases and suited for free
    surface issues

10
3.1 Geometry and mesh of the computational model
11
3.2 Numerical result (1)
Induced electrical potential distribution in x-y
plane
12
3.2 Numerical result (2)
Induced electrical potential distribution in
cross-section
13
3.2 Numerical result (3)
x-component velocity distribution
14
3.2 Numerical result (4)
y-component velocity distribution
15
3.2 Numerical result (5)
z-component velocity distribution
16
4. Conclusions
  • A jet flow under the gradient magnetic field can
    keep its shape stable due to EM force on its
    direction and the compressed EM force on its
    cross section
  • Theres a decrease in the length of the range
    distance and an increase in the radius of the
    flow with the augment of the value of the
    magnetic field.
  • Theres an increase in the length of the range
    distance of the flow with the augment of the
    value of the initial inlet velocity.

17
Thank you !
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