mirror of
https://github.com/JuliaFEM/JuliaFEM.jl.git
synced 2026-10-01 22:09:20 +00:00
separated test from von mises and added MaterialModels namespace
This commit is contained in:
@@ -0,0 +1,123 @@
|
||||
module VonMisesTests
|
||||
|
||||
using PyPlot
|
||||
|
||||
macro R_str(s)
|
||||
s
|
||||
end
|
||||
|
||||
|
||||
using JuliaFEM.MaterialModels: hookeStiffnessTensor, calculate_stress!, State
|
||||
|
||||
function test_von_mises_basic()
|
||||
|
||||
steps = 1000
|
||||
strain_max = 0.003
|
||||
num_cycles = 3
|
||||
E = 200.0e3
|
||||
nu = 0.3
|
||||
ν = 0.3
|
||||
C = hookeStiffnessTensor(E, ν)
|
||||
|
||||
ϵ_tot = zeros(Float64, (steps, 6))
|
||||
ϵ_tot2 = zeros(Float64, (steps, 6))
|
||||
ϵ_tot3 = zeros(Float64, (steps, 6))
|
||||
|
||||
# Adding only strain in x-axis and counting for the poisson effect
|
||||
ϵ_tot[:, 1] = strain_max * sin(2 * pi * linspace(0, num_cycles, steps))
|
||||
ϵ_tot[:, 2] = strain_max * sin(2 * pi * linspace(0, num_cycles, steps)).*-ν
|
||||
ϵ_tot[:, 3] = strain_max * sin(2 * pi * linspace(0, num_cycles, steps)).*-ν
|
||||
ϵ_tot[:, 4] = strain_max / 10 * sin(2 * pi * linspace(0, num_cycles, steps))
|
||||
|
||||
ϵ_last = zeros(Float64, (6))
|
||||
ϵᵖ = zeros(Float64, (6))
|
||||
σ = zeros(Float64, (6, 1))
|
||||
σy = 200.0
|
||||
ss = Float64[]
|
||||
ee = Float64[]
|
||||
|
||||
eig_stress = zeros(Float64, (3, 3))
|
||||
eig_vals = zeros(Float64, (steps, 3))
|
||||
|
||||
function fill_tensor(a, b)
|
||||
a[1, 1] = b[1]
|
||||
a[2, 2] = b[2]
|
||||
a[3, 3] = b[3]
|
||||
|
||||
a[1, 2] = b[6]
|
||||
a[1, 3] = b[5]
|
||||
a[2, 3] = b[4]
|
||||
|
||||
a[2, 1] = b[6]
|
||||
a[3, 1] = b[5]
|
||||
a[3, 2] = b[4]
|
||||
end
|
||||
|
||||
mat = State(C, σy, zeros(Float64, 6), zeros(Float64, 6))
|
||||
|
||||
info("Starting calculation")
|
||||
tic()
|
||||
for i=1:steps
|
||||
ϵ_new = reshape(ϵ_tot[i, :, :], (6, 1))
|
||||
dϵ = ϵ_new - mat.ϵ
|
||||
calculate_stress!(dϵ, mat, Val{:vonMises})
|
||||
mat.ϵ += vec(dϵ)
|
||||
push!(ss, mat.σ[1])
|
||||
push!(ee, mat.ϵ[1])
|
||||
|
||||
fill_tensor(eig_stress, mat.σ)
|
||||
eig_vals[i, :] = sort(eigvals(eig_stress))
|
||||
end
|
||||
toc()
|
||||
# ================ Plotting =================== #
|
||||
n(θ, ϕ) = [sin(θ)*cos(ϕ)
|
||||
sin(θ)*sin(ϕ)
|
||||
cos(θ)]
|
||||
m(θ, ϕ, χ) = [-sin(ϕ)*cos(χ)-cos(θ)*cos(ϕ)*sin(χ)
|
||||
cos(ϕ)*cos(χ)-cos(θ)*sin(ϕ)*sin(χ)
|
||||
sin(θ)*sin(χ)]
|
||||
|
||||
w = [sqrt(2/3) * 200 * m(54.735 * pi / 180, 45 * pi/180, x) for x=0:0.15:(2*pi+0.1)]
|
||||
base_vec = [1 1 1] / sqrt(3)
|
||||
|
||||
for i=-5:5
|
||||
tt = [w[x] + vec(base_vec) + 50 * i for x=1:length(w)]
|
||||
x = map(x->tt[x][1], collect(1:length(w)))
|
||||
y = map(x->tt[x][2], collect(1:length(w)))
|
||||
z = map(x->tt[x][3], collect(1:length(w)))
|
||||
plot3D(x, y, z, color="blue")
|
||||
end
|
||||
|
||||
tt = [w[x] + vec(base_vec) + 50 * -5 for x=1:length(w)]
|
||||
x_start = map(x->tt[x][1], collect(1:length(w)))[1:5:end]
|
||||
y_start = map(x->tt[x][2], collect(1:length(w)))[1:5:end]
|
||||
z_start = map(x->tt[x][3], collect(1:length(w)))[1:5:end]
|
||||
|
||||
|
||||
tt = [w[x] + vec(base_vec) + 50 * 5 for x=1:length(w)]
|
||||
x_end = map(x->tt[x][1], collect(1:length(w)))[1:5:end]
|
||||
y_end = map(x->tt[x][2], collect(1:length(w)))[1:5:end]
|
||||
z_end = map(x->tt[x][3], collect(1:length(w)))[1:5:end]
|
||||
|
||||
for i=1:length(x_start)
|
||||
x = [x_start[i], x_end[i]]
|
||||
y = [y_start[i], y_end[i]]
|
||||
z = [z_start[i], z_end[i]]
|
||||
plot3D(x, y, z, color="blue")
|
||||
end
|
||||
|
||||
|
||||
info("Calculation finished")
|
||||
#PyPlot.plot(ee, ss)
|
||||
plot3D(eig_vals[:, 1], eig_vals[:, 2], eig_vals[:, 3], color="red")
|
||||
PyPlot.title("Stress path and von Mises yield surface")
|
||||
PyPlot.xlabel("Eig Stress 1")
|
||||
PyPlot.ylabel("Eig Stress 2")
|
||||
PyPlot.zlabel("Eig Stress 3")
|
||||
PyPlot.grid()
|
||||
PyPlot.show()
|
||||
end
|
||||
|
||||
test_von_mises_basic()
|
||||
|
||||
end
|
||||
Reference in New Issue
Block a user