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https://github.com/JuliaFEM/JuliaFEM.jl.git
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dce7472cda
`Analysis` is basically doing same than `Solver` before, but has a slighly simpler structure and is more general.
208 lines
6.9 KiB
Julia
208 lines
6.9 KiB
Julia
# This file is a part of JuliaFEM.
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# License is MIT: see https://github.com/JuliaFEM/JuliaFEM.jl/blob/master/LICENSE.md
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using JuliaFEM
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using JuliaFEM.Preprocess
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using JuliaFEM.Postprocess
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using JuliaFEM.Testing
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#= this has nothing to do here
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@testset "calculate cross-sectional properties" begin
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mesh_file = @__DIR__() * "/testdata/primitives.med"
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mesh = aster_read_mesh(mesh_file, "CYLINDER_20_TET4")
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# calculate cross-sectional properties A and Iₓ
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fixed1 = Problem(Dirichlet, "left support", 3, "displacement")
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fixed1.elements = create_elements(mesh, "FACE1")
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A = calculate_area(fixed1)
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info("cross-section area: $A")
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# real area is π
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@test isapprox(A, pi; rtol=0.1)
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Xc = calculate_center_of_mass(fixed1)
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info("center of mass: $Xc")
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@test isapprox(Xc, [0.0, 0.0, 0.0]; atol=1.0e-12)
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I = calculate_second_moment_of_mass(fixed1)
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info("moments:")
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info(I)
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I_expected = zeros(3, 3)
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I_expected[2,2] = I_expected[3,3] = pi/4
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rtol = norm(I[2,2]-I_expected[2,2]) / max(I[2,2],I_expected[2,2])
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info("I rtol = $rtol")
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@test isapprox(I, I_expected; rtol = 0.2)
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end
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=#
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#=
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test subjects:
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- calculate cross-sectional properties
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- modal analysis with known solution
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Fixed-fixed solution is ωᵢ = λᵢ²√(EI/ρA) , where λᵢ = cosh(λᵢℓ)cos(λᵢℓ)
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1: 4.730040744862704
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2: 7.853204624095838
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3: 10.995607838001671
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Youngs modulus is tuned such that lowest eigenfrequency matches 1.0
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5 lowest eigenfrequencies using Code Aster and Tet4 elements:
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numéro fréquence (HZ) norme d'erreur
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1 1.19789E+00 2.20137E-12
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2 1.20179E+00 1.99034E-12
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3 3.07391E+00 3.29226E-13
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4 3.08812E+00 2.91550E-13
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5 4.87370E+00 2.95986E-13
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5 lowest eigenfrequencies using Code Aster and Tet10 elements:
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numéro fréquence (HZ) norme d'erreur
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1 9.65942E-01 1.54950E-11
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2 9.66160E-01 1.62712E-11
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3 2.52127E+00 2.06544E-12
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4 2.52187E+00 1.77970E-12
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5 3.48584E+00 9.96170E-13
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[1] De Silva, Clarence W. Vibration: fundamentals and practice. CRC press, 2006, p.355
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=#
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@testset "long rod natural frequencies" begin
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mesh_file = @__DIR__() * "/testdata/primitives.med"
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mesh = aster_read_mesh(mesh_file, "CYLINDER_20_TET10")
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# for (id, coords) in mesh.nodes
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# mesh.nodes[id][1] *= 5.0
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# end
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body = Problem(Elasticity, "rod", 3)
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body.elements = create_elements(mesh, "CYLINDER")
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#E = 50475.44814745859
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E = 50475.5
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rho = 1.0
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update!(body.elements, "youngs modulus", E)
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update!(body.elements, "poissons ratio", 0.3)
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update!(body.elements, "density", rho)
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# calculate cross-sectional properties A and Iₓ
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fixed1 = Problem(Dirichlet, "left support", 3, "displacement")
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fixed1.elements = create_elements(mesh, "FACE1")
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update!(fixed1.elements, "displacement 1", 0.0)
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update!(fixed1.elements, "displacement 2", 0.0)
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update!(fixed1.elements, "displacement 3", 0.0)
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fixed2 = Problem(Dirichlet, "right support", 3, "displacement")
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fixed2.elements = create_elements(mesh, "FACE2")
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update!(fixed2.elements, "displacement 1", 0.0)
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update!(fixed2.elements, "displacement 2", 0.0)
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update!(fixed2.elements, "displacement 3", 0.0)
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A = calculate_area(fixed1)
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info("cross-section area: $A")
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# using SALOME / SMESH, A = 2.82843
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# real area is π
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@test isapprox(A, pi; rtol=0.1)
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Xc = calculate_center_of_mass(fixed1)
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info("center of mass: $Xc")
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#@test isapprox(Xc, [0.0, 0.0, 0.0]; atol=1.0e-5)
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I = calculate_second_moment_of_mass(fixed1)
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info("moments:")
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info(I)
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I_expected = zeros(3, 3)
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r = 1.0
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I_expected[2,2] = I_expected[3,3] = pi/4*r^2
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rtol = norm(I[2,2]-I_expected[2,2]) / max(I[2,2],I_expected[2,2])
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info("I rtol = $rtol")
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@test isapprox(I, I_expected; rtol = 0.2)
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#=
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# apply transform Tx + b, in this case move cross-section to
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# xy-plane from yz-plane, i.e.
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# x₁ = y₂
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# y₁ = z₂
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T = [
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0.0 1.0 0.0
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0.0 0.0 1.0]
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b = [0.0, 0.0]
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X 1 = first(cross_section)("geometry", [1/3, 1/3], 0.0)
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apply_affine_transform!(cross_section, T, b)
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X2 = first(cross_section)("geometry", [1/3, 1/3], 0.0)
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info("X1 = $X1, X2 = $X2")
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@test isapprox(T*X1+b, X2)
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=#
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c = sqrt(E*I[2,2]/(rho*A))
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info("c = $c")
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# analytical solution is
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l = 20.0
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r = 1.0
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la = 4.730040744862704/l
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# semi-analytical (c numerical)
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freq_sa = (c*la^2)/(2*pi)
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info("freq_sa = $freq_sa")
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A = pi*r^2
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I = pi/4*r^4
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c = sqrt(E*I/(rho*A))
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info("c analytical = $c")
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freq_a = (c*la^2)/(2*pi)
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info("freq_a = $freq_a")
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solver = Solver(Modal, body, fixed1, fixed2)
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solver.properties.nev = 5
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solver()
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freqs_jf = sqrt.(solver.properties.eigvals)/(2.0*pi)
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# with Tet4 elements
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#freqs_ca = [1.19789E+00, 1.20179E+00, 3.07391E+00, 3.08813E+00, 4.87370E+00]
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# with Tet10 elements
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freqs_ca = [9.65942E-01, 9.66160E-01, 2.52127E+00, 2.52187E+00, 3.48584E+00]
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# looks that juliafem results are more close to 1.0, maybe different integration order
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rtol1 = norm(freq_sa - freqs_jf[1])/max(freq_sa, freqs_jf[1])
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rtol2 = norm(freq_a - freqs_jf[1])/max(freq_a, freqs_jf[1])
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info("rtol 1 = $rtol1, rtol 2 = $rtol2")
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passed = true
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for (f1, f2) in zip(freqs_jf, freqs_ca)
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rtol = norm(f1-f2) / max(f1,f2)
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@printf "JF: %8.5e | CA: %8.5e | rtol: %8.5e\n" f1 f2 rtol
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passed &= (rtol < 3.0e-2)
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end
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@test rtol2 < 3.5e-2
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@test passed
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#=
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result = XDMF()
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for (i, freq) in enumerate(freqs)
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isapprox(freq, 0.0) && continue
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info("$i freq: $freq")
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xdmf_new_result!(result, body, freq)
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xdmf_save_field!(result, body, freq, "displacement"; field_type="Vector")
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end
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xdmf_save!(result, "/tmp/rod_nf.xmf")
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=#
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end
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@testset "eigenvalues of cube (tet4)" begin
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meshfile = @__DIR__() * "/testdata/primitives.med"
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mesh = aster_read_mesh(meshfile, "CUBE_TET4")
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cube = Problem(mesh, Elasticity, "CUBE", 3)
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update!(cube.elements, "youngs modulus", 10000.0)
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update!(cube.elements, "poissons ratio", 0.3)
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update!(cube.elements, "density", 10.0)
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sym23 = create_elements(mesh, "FACE231")
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update!(sym23, "displacement 1", 0.0)
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sym13 = create_elements(mesh, "FACE131")
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update!(sym13, "displacement 2", 0.0)
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sym12 = create_elements(mesh, "FACE121")
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update!(sym12, "displacement 3", 0.0)
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bcs = Problem(Dirichlet, "bcs", 3, "displacement")
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bcs.elements = [sym23; sym13; sym12]
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solver = Solver(Modal)
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solver.properties.nev = 5
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push!(solver, cube, bcs)
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solver()
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freqs_jf = sqrt.(solver.properties.eigvals)/(2.0*pi)
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freqs_ca = [3.73724E+00, 3.73724E+00, 4.93519E+00, 6.59406E+00, 7.65105E+00]
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for (f1, f2) in zip(freqs_jf, freqs_ca)
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rtol = norm(f1-f2) / max(f1,f2)
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@printf "JF: %8.5e | CA: %8.5e | rtol: %8.5e\n" f1 f2 rtol
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@test rtol < 1.0e-5
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end
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end
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