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https://github.com/JuliaFEM/JuliaFEM.jl.git
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Merge branch 'master' of git://github.com/JuliaFEM/JuliaFEM.jl into HEAD
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using ForwardDiff
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using NLsolve
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function outer_prod(a, b)
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out = zeros(3,3,3,3)
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for i=1:3
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for j=1:3
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for k=1:3
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for l=1:3
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out[i, j, k, l] = a[i, j] * b[k, l]
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end
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end
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end
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end
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out
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end
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function double_contr(a, b)
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out = zeros(3, 3)
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for i=1:3
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for j=1:3
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for k=1:3
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for l=1:3
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out[i, j] += a[i,j,k,l] * b[k, l]
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end
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end
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end
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end
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out
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end
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"""
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Symmetric fourth order identity tensor
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Definition can be found from:
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http://www.ce.berkeley.edu/~sanjay/ce231mse211/symidentity.pdf
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"""
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function identity_tensor_symm_4th_order()
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my_kron(i,j) = i == j ? 1 : 0
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II = zeros(Float64, (3, 3, 3, 3))
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for i=1:3
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for j=1:3
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for k=1:3
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for l=1:3
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v1 = my_kron(i, k)
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v2 = my_kron(j, l)
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v3 = my_kron(i, l)
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v4 = my_kron(j, k)
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II[i,j,k,l] = 0.5 * (v1*v2 + v3*v4)
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end
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end
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end
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end
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II
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end
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"""
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Fourth order stiffness tensor
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C = λ * I ⊗ I + 2 * μ * II
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Definition: https://en.wikipedia.org/wiki/Hooke's_law
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Literature from tensors and vectors
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# http://www.iith.ac.in/~ashok/Maths_Lectures/Tutorial/VectTensColMat.pdf
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# https://en.wikipedia.org/wiki/Tensor_product
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# http://www.math.psu.edu/yzheng/m597k/m597kL11.pdf
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"""
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function stiffnessTensor(youngs_modulus, poissons_ratio, ::Type{Val{:isotropic}})
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E = youngs_modulus
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v = poissons_ratio
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I = eye(3)
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II = identity_tensor_symm_4th_order()
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mu = E/(2*(1+v))
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lambda = E*v/((1+v)*(1-2*v))
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return lambda * outer_prod(I, I) + 2 * mu * II
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end
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"""
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Create a isotropic Hooke material matrix C
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More information: http://www.efunda.com/formulae/solid_mechanics/mat_mechanics/hooke_isotropic.cfm
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https://en.wikipedia.org/wiki/Hooke's_law
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http://www.ce.berkeley.edu/~sanjay/ce231mse211/symidentity.pdf
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Parameters
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----------
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E: Float
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Elastic modulus
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ν: Float
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Poisson constant
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Returns
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-------
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Array{Float64, (6,6)}
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"""
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function stiffnessTensor(E, ν)
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a = 1 - ν
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b = 1 - 2*ν
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c = 1 + ν
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multiplier = E / (b * c)
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return Float64[a ν ν 0 0 0;
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ν a ν 0 0 0;
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ν ν a 0 0 0;
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0 0 0 b 0 0;
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0 0 0 0 b 0;
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0 0 0 0 0 b].*multiplier
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end
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type State
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C :: Array{Float64, 2}
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σ_y :: Float64
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σ :: Array{Float64, 1}
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ϵ :: Array{Float64, 1}
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end
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# using vectors with double contradiction
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# http://www-2.unipv.it/compmech/teaching/available/const_mod/const_mod_mat-review_notation.pdf
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M = [1 0 0 0 0 0;
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0 1 0 0 0 0;
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0 0 1 0 0 0;
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0 0 0 2 0 0;
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0 0 0 0 2 0;
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0 0 0 0 0 2;]
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"""
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Equivalent tensile stress.
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More info can be found from: https://en.wikipedia.org/wiki/Von_Mises_yield_criterion
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Section: Reduced von Mises equation for different stress conditions
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Parameters
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----------
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σ: Array{Float64, 6}
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Stress in Voigt notation
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Returns
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-------
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Float
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"""
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function σₑ(σ)
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s = σ[1:6] - 1/3 * sum([σ[1], σ[2], σ[3]]) * [1 1 1 0 0 0]'
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return sqrt(3/2 * s' * M * s)[1]
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end
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"""
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Von Mises Yield criterion
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More info can be found from: http://csm.mech.utah.edu/content/wp-content/uploads/2011/10/9tutorialOnJ2Plasticity.pdf
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Parameters
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----------
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σ: Array{Float64, 6}
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Stress in Voigt notation
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k: Float64
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Material constant, Yield limit
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Returns
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-------
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Float
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"""
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function vonMisesYield(σ, k)
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σₑ(σ) - k
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end
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"""
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Function for NLsolve. Inside this function are the equations which we want to find root.
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Ψ is the yield function below. Functions defined here:
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dσ - C (dϵ - dλ*dΨ/dσ) = 0
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σₑ(σ) - k = 0
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Parameters
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----------
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params: Array{Float64, 7}
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Array containing values from solver
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dϵ: Array{Float64, 6}
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Strain rate vector in Voigt notation
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C: Array{Float64, (6, 6)}
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Material tensor
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k: Float
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Material constant, yield limit
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Δt: Float
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time increment
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σ_begin:Array{Float64, 6}
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Stress vector in Voigt notation
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Returns
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-------
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Array{Float64, 7}, return values for solver
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"""
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function vonMisesRoot(params, dϵ, C, σ_y, σ_begin)
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# Creating wrapper for gradient
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yield_wrap(pars) = vonMisesYield(pars, σ_y)
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dfdσ = ForwardDiff.gradient(yield_wrap)
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# Stress rate
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dσ = params[1:6]
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σ_tot = [vec(σ_begin); 0.0] + params
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# Calculating plastic strain rate
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dϵp = params[end] * dfdσ(σ_tot)
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# Calculating equations
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function_1 = dσ - C * (dϵ - dϵp[1:6])
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function_2 = yield_wrap(σ_tot)
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[vec(function_1); function_2]
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end
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"""
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Stress for ideal plastic von Mises material model
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Parameters
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----------
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dϵ: Array{Float64, 6}
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Strain rate vector in Voigt notation
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Δt: Float
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time increment
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σ: Array{Float64, 6}
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Last stress vector in Voigt notation
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C: Array{Float64, (6, 6)}
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Material tensor
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k: Float
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Material constant, yield limit
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Returns
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-------
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Tuple
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Plastic strain rate dϵᵖ and new stress vector σ
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"""
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function calculate_stress!(dϵ, mat::State, ::Type{Val{:vonMises}})
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σ = mat.σ
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C = mat.C
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σ_y = mat.σ_y
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# Test stress
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σ_tria = σ + C * dϵ
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# Calculating and checking for yield
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yield = vonMisesYield(σ_tria, σ_y)
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if yield > 0
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# Yielding happened
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# Creating functions for newton: xₙ₊₁ = xₙ - df⁻¹ * f and initial values
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initial_guess = [vec(σ_tria - σ); 0.1]
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f(σ_) = vonMisesRoot(σ_, dϵ, C, σ_y, σ)
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df = ForwardDiff.jacobian(f)
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# Calculating root
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result = nlsolve(not_in_place(f, df), initial_guess).zero
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mat.σ += result[1:6]
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else
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mat.σ = vec(σ_tria)
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end
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end
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