Hartmann Flow
Item | Value/Name |
---|---|
Mesh | Simple block mesh for a simple plate |
Discritisation | Governing equations: continuity equation, The Cauchy momentum equation, and the Ampère's law |
Physical parameters | ρ(mass density of fluid)=1 [kg/m3] ν(kinematic viscosity)=1 [m2/s] μ(magnetic permeability)=1 [kg⋅m⋅s-2⋅A-2, or N/A2] σ(electric conductivity)=1 [kg-1⋅m-3⋅s3⋅A2, or S/m, or (Ωm)-1] |
Initial values | B(magnetic field)=(0, 20, 0) [T] and uniform p(kinematic pressure)=(0) [m2s-2] U(flow velocity)=(0) [m/s] |
Solver | mhdFoam |
1. Pre-Processing
Item | Value |
---|---|
Size of one cell | (x:0.2, y:0.05, z:0.1) [m] |
Number of cells | (x:100, y:40, z:1) |
2. Settings
See the Summary of the case (above) for the physical parameters.
3. Simulation
The following table shows the control parameters for performing a simulation.
Item | Value |
---|---|
Start time [seconds] | 0 |
End time [seconds] | 4 |
Time step (Δt) [seconds] | 0.005 |
The simulation is governed by several equations (see the Summary of the case above and the sheet below).
According to the sheet above, the following results on p (pressure, precisely kinematic pressure) and U (flow velocity) are the properties of fluid.
4. Post-Processing
The magnetic field reaches the equilibrium state around at Time=2.0 sec.
5. Analysis
In this case, most of the physical parameters are not realistic.
5.1 Hartmann Number
The ratio between fluid viscosity (ν) and magnetic viscosity (η)