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Boundary conditions for vortex particle passing through a square domain |
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August 18, 2017, 09:47 |
Boundary conditions for vortex particle passing through a square domain
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Case
I am trying to simulate a single vortex particle which convects along with the freestream velocity through a free-surface square domain. Initially the particle is outside of the domain, so I simulate the particle approaching, entering, travelling through, exiting and distancing from the domain. Approach For this case the analytical solution for the velocity and pressure are known in closed-form. So I can compute the velocity and pressure at any given point in space and instance in time. I would like to use the analytical solution to impose boundary conditions. Results and problem Previously, I had good results for a case where the particle passes the domain from the outside (so it never enters or exits the domain). In this case I used the analytical solution to impose a non-uniform Dirichlet b.c. for the velocity on all four sides. This worked well, but for the case where the particle passes through the domain I get wiggles along the side at which the particle exits the domain. Question What type of boundary condition(s) could I use for this case? Notes Analytical solution: The velocity equals the freestream velocity plus the induction by the particle. The pressure is calculated via Bernoulli's principle. u = uInf + Gamma/(2*pi*r^2)*(1 - exp(-0.5*(r/e)^2))*ry v = vInf - Gamma/(2*pi*r^2)*(1 - exp(-0.5*(r/e)^2))*rx p = pInf + 0.5*[(uInf*uInf + vInf*vInf) - (u*u + v*v)] uInf = freestream velocity in x direction vInf = freestream velocity in y direction pInf = freestream pressure Gamma = particle strength e = particle core radius r = Euclidean distance between particle and point of evaluation rx = x component of r ry = y component of r ps: The analytical solution is NaN at r = 0. I have ensured that r never becomes 0 by positioning the particle such that it never coincides with a cell center or face center. |
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Tags |
boundary conditions, non-uniform bc, potential flow, unsteady b.c. |
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