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jgs |
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#test_advect.py Gauss |
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from esys.escript import * |
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import esys.finley |
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from esys.linearPDEs import LinearPDE |
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from esys.linearPDEs import AdvectivePDE |
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import os |
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def classical_lhs(): |
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####################### FINLEY UPWINDING HARDCODED ################# |
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global surfacePDE |
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surfacePDE = LinearPDE(mesh) |
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A = Tensor(0.0, Function(mesh)) |
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for j in range(2): |
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for l in range(2): |
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A[j,l] = velocity[j] * velocity[l] * cte * dt |
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B = velocity * cte |
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C = dt * velocity |
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D=1.0 |
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surfacePDE.setValue(A=A, B=B, C=C, D=D) |
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def classical_rhs(): |
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####################### FINLEY UPWINDING HARDCODED ################# |
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X = velocity * cte * gauss_tronc_old |
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Y = gauss_tronc_old |
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surfacePDE.setValue(X=X, Y=Y) |
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def finley_upwd_lhs(): |
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####################### FINLEY UPWINDING ################# |
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global surfacePDE |
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surfacePDE = AdvectivePDE(mesh) |
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C = dt * velocity |
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D=1.0 |
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surfacePDE.setValue(C=C, D=D) |
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def finley_upwd_rhs(): |
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####################### FINLEY UPWINDING ################# |
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Y = gauss_tronc_old |
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surfacePDE.setValue(Y=Y) |
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def taylor_galerkin_lhs(): |
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####################### TAYLOR - GALERKIN ################# |
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global surfacePDE |
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surfacePDE = LinearPDE(mesh) |
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surfacePDE.setValue(D=1.0) |
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def taylor_galerkin_rhs(): |
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####################### TAYLOR - GALERKIN ################# |
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X = Vector(0.0, Function(mesh)) |
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for i in range(2): |
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for j in range(2): |
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X[i] -= (dt**2)/2.0*velocity[i]*velocity[j]*grad(gauss_tronc_old)[j] |
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Y = gauss_tronc_old*Scalar(1.0, Function(mesh)) |
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for j in range(2): |
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Y -= dt*velocity[j]*grad(gauss_tronc_old)[j] |
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surfacePDE.setValue(X=X, Y=Y) |
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############ start of main code ######################## |
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dt = 0.5 |
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t_step = 1 |
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mesh = esys.finley.Rectangle(l0=4.0, l1=2.0, order=1, n0=60, n1=30) |
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if os.path.exists("results/sylvain/dist_error.dat"): |
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os.unlink("results/sylvain/dist_error.dat") |
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xx = mesh.getX()[0] |
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yy = mesh.getX()[1] |
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gauss = (160*(xx-0.25)**4 - 320*(xx-0.25)**3 + 160*(xx-0.25)**2 )*( 160*(yy-0.5)**4 - 320*(yy-0.5)**3 + 160*(yy-0.5)**2) |
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mask_tronc = (xx-0.25).wherePositive()*(1.25-xx).wherePositive()*(yy-0.5).wherePositive()*(1.5-yy).wherePositive() |
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gauss_tronc_new = gauss*mask_tronc |
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reference = Lsup(gauss_tronc_new) |
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gauss_tronc_new.saveDX("results/sylvain/gauss.%2.2i.dx" % 0) |
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h = Lsup(mesh.getSize()) |
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coeff = 0.3 |
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v_adim = coeff*h/dt |
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cte = h/(2.0*v_adim) |
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t_step_end = 2.0/(coeff*h) |
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velocity = Vector(0.0, Function(mesh)) |
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velocity[0] = v_adim |
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velocity.saveDX("results/sylvain/velocity_field.dx") |
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taylor_galerkin_lhs() |
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q = mesh.getX()[0].whereZero() + (4.0-mesh.getX()[0]).whereZero() + mesh.getX()[1].whereZero() + (2.0-mesh.getX()[1]).whereZero() |
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surfacePDE.setValue(q=q) |
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while (t_step <= t_step_end): |
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gauss_tronc_old = gauss_tronc_new |
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taylor_galerkin_rhs() |
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gauss_tronc_new = surfacePDE.getSolution() |
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gauss_tronc_old.saveDX("results/sylvain/gauss.%2.2i.dx" % t_step) |
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print "integral of f", integrate(gauss_tronc_new*Scalar(1.0, Function(mesh))) |
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dist = v_adim*dt*t_step |
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error = 100*abs(Lsup(gauss_tronc_new)-reference)/reference |
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File1 = file("results/sylvain/dist_error.dat", "a", 1) |
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File1.write("%e %e\n" % (dist, error)) |
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File1.close() |
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t_step = t_step + 1 |