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examples/shells/dynamics/composite/free_vibration/reddy_chao_examples.jl
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""" | ||
Vibration analysis of cross-ply square plate | ||
Reference values: ? [Hz] | ||
From: J.N. REDDY and W.C. CHAO | ||
A COMPARISON OF CLOSED-FORM AND FINITE-ELEMENT SOLUTIONS | ||
OF THICK LAMINATED ANISOTROPIC RECTANGULAR PLATES, | ||
Nuclear Engineering and Design 64 (1981) 153-167 153 | ||
""" | ||
module reddy_chao_examples | ||
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using Arpack | ||
using FinEtools | ||
using FinEtools.AlgoBaseModule: solve_blocked!, matrix_blocked | ||
using FinEtools.MeshExportModule.VTKWrite: vtkwrite | ||
using FinEtoolsDeforLinear | ||
using FinEtoolsFlexStructures.FESetShellT3Module: FESetShellT3 | ||
using FinEtoolsFlexStructures.FEMMShellT3FFModule | ||
using FinEtoolsFlexStructures.RotUtilModule: initial_Rfield, update_rotation_field! | ||
using VisualStructures: plot_nodes, plot_midline, render, plot_space_box, plot_midsurface, space_aspectratio, save_to_json | ||
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function _execute(formul, n, visualize) | ||
# Material I | ||
E_1 = E_2 | ||
E = 207*phun("GPa") | ||
nu = 0.3; | ||
rho= 7850*phun("KG/M^3"); | ||
L0 = 2.54 * phun("m") | ||
B0 = 1.27 * phun("m") | ||
thickness = 12.7*phun("mm"); | ||
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# Report | ||
@info "Mesh: $n elements per side" | ||
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tolerance = B0/n/1000 | ||
X = [0.0 0.0 0.0; | ||
B0 0.0 0.0; | ||
B0 B0 0.0; | ||
B0 2*B0 0.0; | ||
0.0 2*B0 0.0; | ||
0.0 B0 0.0; | ||
] | ||
l2fens = FENodeSet(X); | ||
conn = [1 2; 6 3; 5 4; 2 3; 3 4; 5 6; 6 1] | ||
l2fes = FESetL2(conn); | ||
nLayers = 5 | ||
ex = function (x, k) | ||
x[3] += k*L0/nLayers | ||
x | ||
end | ||
fens,fes = Q4extrudeL2(l2fens, l2fes, nLayers, ex); # Mesh | ||
fens, fes = Q4toT3(fens, fes) | ||
for r in 1:n | ||
fens, fes = T3refine(fens, fes) | ||
end | ||
@show count(fens) | ||
vtkwrite("dbcs.vtu", fens, fes) | ||
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mater = MatDeforElastIso(DeforModelRed3D, rho, E, nu, 0.0) | ||
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sfes = FESetShellT3() | ||
accepttodelegate(fes, sfes) | ||
femm = formul.make(IntegDomain(fes, TriRule(1), thickness), mater) | ||
associate = formul.associategeometry! | ||
stiffness = formul.stiffness | ||
mass = formul.mass | ||
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# Construct the requisite fields, geometry and displacement | ||
# Initialize configuration variables | ||
geom0 = NodalField(fens.xyz) | ||
u0 = NodalField(zeros(size(fens.xyz,1), 3)) | ||
Rfield0 = initial_Rfield(fens) | ||
dchi = NodalField(zeros(size(fens.xyz,1), 6)) | ||
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# Apply EBC's | ||
# simple support | ||
l1 = selectnode(fens; box = Float64[-Inf Inf -Inf Inf 0.0 0.0], inflate = tolerance) | ||
for i in [1, 2, 3, 4, 5, 6] | ||
setebc!(dchi, l1, true, i) | ||
end | ||
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applyebc!(dchi) | ||
numberdofs!(dchi); | ||
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# Assemble the system matrix | ||
associategeometry!(femm, geom0) | ||
K = stiffness(femm, geom0, u0, Rfield0, dchi); | ||
M = mass(femm, geom0, dchi); | ||
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K_ff = matrix_blocked(K, nfreedofs(dchi), nfreedofs(dchi))[:ff] | ||
M_ff = matrix_blocked(M, nfreedofs(dchi), nfreedofs(dchi))[:ff] | ||
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# Solve | ||
OmegaShift = 0.0*2*pi | ||
neigvs = 4 | ||
d, v, nconv = eigs(K_ff+OmegaShift*M_ff, M_ff; nev=neigvs, which=:SM, explicittransform=:none) | ||
d[:] = d .- OmegaShift; | ||
fs = real(sqrt.(complex(d)))/(2*pi) | ||
@show fs | ||
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# Visualization | ||
if visualize | ||
U = v[:, 4] | ||
scattersysvec!(dchi, (L0/4)/maximum(abs.(U)).*U) | ||
update_rotation_field!(Rfield0, dchi) | ||
plots = cat(plot_space_box([[0 0 0]; [L0 L0 L0]]), | ||
#plot_nodes(fens), | ||
plot_midsurface(fens, fes; x = geom0.values, u = dchi.values[:, 1:3], R = Rfield0.values); | ||
dims = 1) | ||
pl = render(plots) | ||
end | ||
nothing | ||
end | ||
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function test_convergence() | ||
formul = FEMMShellT3FFModule | ||
@info "Double Cell Box Vibration" | ||
for n in [1, 2, 3, 4] | ||
_execute(formul, n, false) | ||
end | ||
return true | ||
end | ||
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function allrun() | ||
println("#####################################################") | ||
println("# test_convergence ") | ||
test_convergence() | ||
return true | ||
end # function allrun | ||
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@info "All examples may be executed with " | ||
println("using .$(@__MODULE__); $(@__MODULE__).allrun()") | ||
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end # module | ||
nothing |