Correct Boundary Condition for an Open Atmosphere? #29893
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Setting the temperature would not influence the result if it were very far from the heat source. Right now it seems close, and will impose a strong decrease in the temperature to meet this boundary condition.
This sets the heat flux to 0. This is in effect imposing a symmetry of the system, which is also not realistic. I think the right solution for temperature is no boundary condition on the right and top, letting the INSFVEnergyAdvection kernel advect energy through those boundaries. Can you get the flow equations to converge with a fixed temperature profile (using an exodus restart from the current T profile for example) |
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Question
Hello,
I revisited one of my early MOOSE practice problems about natural circulation flow from a heated wall (constant temperature), and open to the atmosphere. This problem was taken from Bergman and Lavine Heat and Mass Transfer Textbook:
I defined my mesh as a simple 2D rectangle, where the left boundary represents the heated wall, the bottom boundary represents the ground, and the right and top boundaries represent ambient air. I had to compute the heat rate coming off the wall to compare it to the one from the textbook. However, the value I computed was less than the textbook's example: ~ 232.42 Watts < 1108.24 Watts. I'm not sure if I computed the heat rate wrong or if I set my boundary conditions incorrectly. Currently I have a dirichlet boundary condition on the right and top boundaries of 296 Kelvin, but I don't think that represents ambient air accurately. I tried to use an outflow condition with INSFVMomentumAdvectionOutflowBC for velocity and FVNeumann for the temperature both set to 0, but the solve was unstable and didn't converge.
Additional information
Mesh size and type: 30x30
Reynolds number:
Discretization (finite element CG/DG, finite volume, etc): finite volume
Models (turbulence, porous media, etc): natural circulation
Solver method (fully coupled, segregated, multiapps, etc):
Base input you started from:
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