class ExplicitIsotropicElectroMechanics_108(Material):
""" Electromechanical model in terms of internal energy
W(C,D) = W_mn(C) + 1/2/eps_2/J (FD0*FD0)
W_mn(C) = u1*C:I+u2*G:I - 2*(u1+2*u2)*lnJ + lamb/2*(J-1)**2
"""
def __init__(self, ndim, **kwargs):
mtype = type(self).__name__
super(ExplicitIsotropicElectroMechanics_108,
self).__init__(mtype, ndim, **kwargs)
# REQUIRES SEPARATELY
self.nvar = self.ndim + 1
self.energy_type = "internal_energy"
self.legendre_transform = LegendreTransform()
self.nature = "nonlinear"
self.fields = "electro_mechanics"
if self.ndim == 2:
self.H_VoigtSize = 5
elif self.ndim == 3:
self.H_VoigtSize = 9
# LOW LEVEL DISPATCHER
self.has_low_level_dispatcher = True
# self.has_low_level_dispatcher = False
def KineticMeasures(self, F, ElectricFieldx, elem=0):
from Florence.MaterialLibrary.LLDispatch._ExplicitIsotropicElectroMechanics_108_ import KineticMeasures
D, stress = KineticMeasures(self, np.ascontiguousarray(F),
ElectricFieldx)
return D, stress, None
def Hessian(self,
StrainTensors,
ElectricDisplacementx,
elem=0,
gcounter=0):
mu1 = self.mu1
mu2 = self.mu2
lamb = self.lamb
eps_2 = self.eps_2
I = StrainTensors['I']
J = StrainTensors['J'][gcounter]
b = StrainTensors['b'][gcounter]
D = ElectricDisplacementx.reshape(self.ndim, 1)
Dx = D.reshape(self.ndim)
DD = np.dot(D.T, D)[0, 0]
C_mech = 2.*mu2/J*(2*einsum('ij,kl',b,b) - einsum('ik,jl',b,b) - einsum('il,jk',b,b)) +\
2.*(mu1+2.*mu2)/J*( einsum("ik,jl",I,I)+einsum("il,jk",I,I) ) + \
lamb*(2.*J-1.)*einsum("ij,kl",I,I) - lamb*(J-1)*( einsum("ik,jl",I,I)+einsum("il,jk",I,I) )
C_elect = 1./eps_2*(0.5*DD*(einsum('ik,jl',I,I) + einsum('il,jk',I,I) + einsum('ij,kl',I,I) ) - \
einsum('ij,k,l',I,Dx,Dx) - einsum('i,j,kl',Dx,Dx,I))
self.elasticity_tensor = C_mech + C_elect
self.coupling_tensor = 1. / eps_2 * (einsum('ik,j', I, Dx) + einsum(
'i,jk', Dx, I) - einsum('ij,k', I, Dx))
self.dielectric_tensor = 1. / eps_2 * I
# TRANSFORM TENSORS TO THEIR ENTHALPY COUNTERPART
E_Voigt, P_Voigt, C_Voigt = self.legendre_transform.InternalEnergyToEnthalpy(
self.dielectric_tensor, self.coupling_tensor,
self.elasticity_tensor)
# BUILD HESSIAN
factor = -1.
H1 = np.concatenate((C_Voigt, factor * P_Voigt), axis=1)
H2 = np.concatenate((factor * P_Voigt.T, E_Voigt), axis=1)
H_Voigt = np.concatenate((H1, H2), axis=0)
return H_Voigt
def CauchyStress(self,
StrainTensors,
ElectricDisplacementx,
elem=0,
gcounter=0):
mu1 = self.mu1
mu2 = self.mu2
lamb = self.lamb
eps_2 = self.eps_2
I = StrainTensors['I']
J = StrainTensors['J'][gcounter]
b = StrainTensors['b'][gcounter]
D = ElectricDisplacementx.reshape(self.ndim, 1)
DD = np.dot(D.T, D)[0, 0]
trb = trace(b)
if self.ndim == 2:
trb += 1.
simga_mech = 2.0*mu1/J*b + \
2.0*mu2/J*(trb*b - np.dot(b,b)) -\
2.0*(mu1+2*mu2)/J*I +\
lamb*(J-1.)*I
sigma_electric = 1. / eps_2 * (np.dot(D, D.T) - 0.5 * DD * I)
sigma = simga_mech + sigma_electric
return sigma
def ElectricDisplacementx(self,
StrainTensors,
ElectricFieldx,
elem=0,
gcounter=0):
D = self.legendre_transform.GetElectricDisplacement(
self, StrainTensors, ElectricFieldx, elem, gcounter)
# SANITY CHECK FOR IMPLICIT COMPUTATUTAION OF D
# eps_2 = self.eps_2
# E = ElectricFieldx.reshape(self.ndim,1)
# D_exact = eps_2*E
# D = D_exact
return D
def Permittivity(self,
StrainTensors,
ElectricDisplacementx,
elem=0,
gcounter=0):
eps_2 = self.eps_2
I = StrainTensors['I']
self.dielectric_tensor = 1. / eps_2 * I
# Negative definite inverse is needed due to Legendre transform
return -eps_2 * I
def ElectrostaticMeasures(self, F, ElectricFieldx, elem=0):
from Florence.MaterialLibrary.LLDispatch._IsotropicElectroMechanics_108_ import KineticMeasures
D, _, H_Voigt = KineticMeasures(self, np.ascontiguousarray(F),
ElectricFieldx)
# H_Voigt = np.linalg.inv(np.ascontiguousarray(H_Voigt[:,-self.ndim:,-self.ndim:]))
H_Voigt = np.ascontiguousarray(H_Voigt[:, -self.ndim:, -self.ndim:])
return D, None, H_Voigt
class IsotropicElectroMechanics_201(Material):
"""Electromechanical model in terms of internal energy
W(C,D) = W_mn(C) + 1/2/eps_1 (FD0*FD0)
W_mn(C) = u1*C:I+u2*G:I - 2*(u1+2*u2)*lnJ + lamb/2*(J-1)**2
"""
def __init__(self, ndim, **kwargs):
mtype = type(self).__name__
super(IsotropicElectroMechanics_201,
self).__init__(mtype, ndim, **kwargs)
# REQUIRES SEPARATELY
self.nvar = self.ndim + 1
self.energy_type = "internal_energy"
self.legendre_transform = LegendreTransform()
self.nature = "nonlinear"
self.fields = "electro_mechanics"
if self.ndim == 2:
self.H_VoigtSize = 5
elif self.ndim == 3:
self.H_VoigtSize = 9
# LOW LEVEL DISPATCHER
self.has_low_level_dispatcher = False
def Hessian(self,
StrainTensors,
ElectricDisplacementx,
elem=0,
gcounter=0):
mu1 = self.mu1
mu2 = self.mu2
lamb = self.lamb
eps_1 = self.eps_1
I = StrainTensors['I']
J = StrainTensors['J'][gcounter]
b = StrainTensors['b'][gcounter]
D = ElectricDisplacementx.reshape(self.ndim, 1)
Dx = D.reshape(self.ndim)
DD = np.dot(D.T, D)[0, 0]
self.elasticity_tensor = 2.*mu2/J*(2*einsum('ij,kl',b,b) - einsum('ik,jl',b,b) - einsum('il,jk',b,b)) +\
2.*(mu1+2.*mu2)/J*( einsum("ik,jl",I,I)+einsum("il,jk",I,I) ) + \
lamb*(2.*J-1.)*einsum("ij,kl",I,I) - lamb*(J-1)*( einsum("ik,jl",I,I)+einsum("il,jk",I,I) )
self.coupling_tensor = J / eps_1 * (einsum('ik,j', I, Dx) +
einsum('i,jk', Dx, I))
self.dielectric_tensor = J / eps_1 * I
# TRANSFORM TENSORS TO THEIR ENTHALPY COUNTERPART
E_Voigt, P_Voigt, C_Voigt = self.legendre_transform.InternalEnergyToEnthalpy(
self.dielectric_tensor, self.coupling_tensor,
self.elasticity_tensor)
# BUILD HESSIAN
factor = -1.
H1 = np.concatenate((C_Voigt, factor * P_Voigt), axis=1)
H2 = np.concatenate((factor * P_Voigt.T, E_Voigt), axis=1)
H_Voigt = np.concatenate((H1, H2), axis=0)
return H_Voigt
def CauchyStress(self,
StrainTensors,
ElectricDisplacementx,
elem=0,
gcounter=0):
mu1 = self.mu1
mu2 = self.mu2
lamb = self.lamb
eps_1 = self.eps_1
I = StrainTensors['I']
J = StrainTensors['J'][gcounter]
b = StrainTensors['b'][gcounter]
D = ElectricDisplacementx.reshape(self.ndim, 1)
if self.ndim == 2:
trb = trace(b) + 1
else:
trb = trace(b)
simga_mech = 2.0*mu1/J*b + \
2.0*mu2/J*(trb*b - np.dot(b,b)) -\
2.0*(mu1+2*mu2)/J*I +\
lamb*(J-1)*I
sigma_electric = J / eps_1 * np.dot(D, D.T)
sigma = simga_mech + sigma_electric
return sigma
def ElectricDisplacementx(self,
StrainTensors,
ElectricFieldx,
elem=0,
gcounter=0):
D = self.legendre_transform.GetElectricDisplacement(
self, StrainTensors, ElectricFieldx, elem, gcounter)
# SANITY CHECK FOR IMPLICIT COMPUTATUTAION OF D
# I = StrainTensors['I']
# J = StrainTensors['J'][gcounter]
# E = ElectricFieldx.reshape(self.ndim,1)
# eps_1 = self.eps_1
# D_exact = eps_1/J*E
# # print np.linalg.norm(D - D_exact)
# return D_exact
return D
class IsotropicElectroMechanics_102(Material):
"""Electromechanical model in terms of internal energy
W(C,D0) = W_neo(C) + 1/2/eps_1/J (FD0*FD0)
"""
def __init__(self, ndim, **kwargs):
mtype = type(self).__name__
super(IsotropicElectroMechanics_102,
self).__init__(mtype, ndim, **kwargs)
# REQUIRES SEPARATELY
self.nvar = self.ndim + 1
self.energy_type = "internal_energy"
self.legendre_transform = LegendreTransform()
self.nature = "nonlinear"
self.fields = "electro_mechanics"
if self.ndim == 2:
self.H_VoigtSize = 5
elif self.ndim == 3:
self.H_VoigtSize = 9
# LOW LEVEL DISPATCHER
self.has_low_level_dispatcher = False
def Hessian(self,
StrainTensors,
ElectricDisplacementx,
elem=0,
gcounter=0):
mu = self.mu
lamb = self.lamb
eps_1 = self.eps_1
I = StrainTensors['I']
J = StrainTensors['J'][gcounter]
b = StrainTensors['b'][gcounter]
D = ElectricDisplacementx.reshape(self.ndim, 1)
Dx = D.reshape(self.ndim)
DD = np.dot(D.T, D)[0, 0]
C_mech = lamb*(2.*J-1.)*einsum("ij,kl",I,I) + \
(mu/J - lamb*(J-1))*( einsum("ik,jl",I,I)+einsum("il,jk",I,I) )
C_elect = 1./eps_1*(0.5*DD*(einsum('ik,jl',I,I) + einsum('il,jk',I,I) + einsum('ij,kl',I,I) ) - \
einsum('ij,k,l',I,Dx,Dx) - einsum('i,j,kl',Dx,Dx,I))
self.elasticity_tensor = C_mech + C_elect
self.coupling_tensor = 1. / eps_1 * (einsum('ik,j', I, Dx) + einsum(
'i,jk', Dx, I) - einsum('ij,k', I, Dx))
self.dielectric_tensor = 1. / eps_1 * I
# TRANSFORM TENSORS TO THEIR ENTHALPY COUNTERPART
E_Voigt, P_Voigt, C_Voigt = self.legendre_transform.InternalEnergyToEnthalpy(
self.dielectric_tensor, self.coupling_tensor,
self.elasticity_tensor)
# BUILD HESSIAN
factor = -1.
H1 = np.concatenate((C_Voigt, factor * P_Voigt), axis=1)
H2 = np.concatenate((factor * P_Voigt.T, E_Voigt), axis=1)
H_Voigt = np.concatenate((H1, H2), axis=0)
return H_Voigt
def CauchyStress(self,
StrainTensors,
ElectricDisplacementx,
elem=0,
gcounter=0):
mu = self.mu
lamb = self.lamb
eps_1 = self.eps_1
I = StrainTensors['I']
J = StrainTensors['J'][gcounter]
b = StrainTensors['b'][gcounter]
D = ElectricDisplacementx.reshape(self.ndim, 1)
DD = np.dot(D.T, D)[0, 0]
return 1.0 * mu / J * (b - I) + lamb * (J - 1) * I + 1 / eps_1 * (
np.dot(D, D.T) - 0.5 * DD * I)
def ElectricDisplacementx(self,
StrainTensors,
ElectricFieldx,
elem=0,
gcounter=0):
D = self.legendre_transform.GetElectricDisplacement(
self, StrainTensors, ElectricFieldx, elem, gcounter)
# SANITY CHECK
# eps_1 = self.eps_1
# D_exact = eps_1*ElectricFieldx.reshape(self.ndim,1)
# print np.linalg.norm(D_exact - D)
# return D_exact
return D
class IsotropicElectroMechanics_100(Material):
"""Simplest electromechanical model with no coupling in terms of internal energy
W(C,D0) = W_neo(C) + 1/2/eps_1* (D0*D0)
"""
def __init__(self, ndim, **kwargs):
mtype = type(self).__name__
super(IsotropicElectroMechanics_100,
self).__init__(mtype, ndim, **kwargs)
# REQUIRES SEPARATELY
self.nvar = self.ndim + 1
self.energy_type = "internal_energy"
self.legendre_transform = LegendreTransform()
self.nature = "nonlinear"
self.fields = "electro_mechanics"
if self.ndim == 2:
self.H_VoigtSize = 5
elif self.ndim == 3:
self.H_VoigtSize = 9
# LOW LEVEL DISPATCHER
self.has_low_level_dispatcher = False
def Hessian(self,
StrainTensors,
ElectricDisplacementx,
elem=0,
gcounter=0):
mu = self.mu
lamb = self.lamb
eps_1 = self.eps_1
I = StrainTensors['I']
J = StrainTensors['J'][gcounter]
b = StrainTensors['b'][gcounter]
D = ElectricDisplacementx.reshape(self.ndim, 1)
Dx = D.reshape(self.ndim)
DD = np.dot(D.T, D)[0, 0]
self.elasticity_tensor = lamb*(2.*J-1.)*einsum("ij,kl",I,I) + \
(mu/J - lamb*(J-1))*( einsum("ik,jl",I,I)+einsum("il,jk",I,I) )
self.coupling_tensor = np.zeros((self.ndim, self.ndim, self.ndim))
self.dielectric_tensor = J / eps_1 * np.linalg.inv(b)
# TRANSFORM TENSORS TO THEIR ENTHALPY COUNTERPART
E_Voigt, P_Voigt, C_Voigt = self.legendre_transform.InternalEnergyToEnthalpy(
self.dielectric_tensor, self.coupling_tensor,
self.elasticity_tensor)
# BUILD HESSIAN
factor = -1.
H1 = np.concatenate((C_Voigt, factor * P_Voigt), axis=1)
H2 = np.concatenate((factor * P_Voigt.T, E_Voigt), axis=1)
H_Voigt = np.concatenate((H1, H2), axis=0)
return H_Voigt
def CauchyStress(self,
StrainTensors,
ElectricDisplacementx,
elem=0,
gcounter=0):
mu = self.mu
lamb = self.lamb
I = StrainTensors['I']
J = StrainTensors['J'][gcounter]
b = StrainTensors['b'][gcounter]
return 1.0 * mu / J * (b - I) + lamb * (J - 1) * I
def ElectricDisplacementx(self,
StrainTensors,
ElectricFieldx,
elem=0,
gcounter=0):
D = self.legendre_transform.GetElectricDisplacement(
self, StrainTensors, ElectricFieldx, elem, gcounter)
# SANITY CHECK FOR IMPLICIT COMPUTATUTAION OF D
# I = StrainTensors['I']
# J = StrainTensors['J'][gcounter]
# b = StrainTensors['b'][gcounter]
# E = ElectricFieldx.reshape(self.ndim,1)
# eps_1 = self.eps_1
# D_exact = eps_1/J*np.dot(b,E)
# # print np.linalg.norm(D - D_exact)
# return D_exact
# print D
return D
class IsotropicElectroMechanics_107(Material):
"""Electromechanical model in terms of internal energy
W(C,D0) = W_mn(C) + 1/2/eps_1 (D0*D0) + 1/2/eps_2/J (FD0*FD0) + W_reg(C,D0)
W_mn(C) = u1*C:I+u2*G:I - 2*(u1+2*u2+6*mue)*lnJ + lamb/2*(J-1)**2 + mue*(C:I)**2
W_reg(C,D_0) = 2/eps_e/mue (F:F)(FD0*FD0) + 1/mu/eps_e**2*(FD0*FD0)**2
"""
def __init__(self, ndim, **kwargs):
mtype = type(self).__name__
super(IsotropicElectroMechanics_107, self).__init__(mtype, ndim, **kwargs)
# REQUIRES SEPARATELY
self.nvar = self.ndim+1
self.energy_type = "internal_energy"
self.legendre_transform = LegendreTransform()
self.nature = "nonlinear"
self.fields = "electro_mechanics"
if self.ndim == 2:
self.H_VoigtSize = 5
elif self.ndim == 3:
self.H_VoigtSize = 9
# LOW LEVEL DISPATCHER
self.has_low_level_dispatcher = True
# self.has_low_level_dispatcher = False
def KineticMeasures(self,F,ElectricFieldx, elem=0):
from Florence.MaterialLibrary.LLDispatch._IsotropicElectroMechanics_107_ import KineticMeasures
return KineticMeasures(self,np.ascontiguousarray(F), ElectricFieldx)
def Hessian(self,StrainTensors,ElectricDisplacementx,elem=0,gcounter=0):
mu1 = self.mu1
mu2 = self.mu2
mue = self.mue
lamb = self.lamb
eps_1 = self.eps_1
eps_2 = self.eps_2
eps_e = self.eps_e
I = StrainTensors['I']
J = StrainTensors['J'][gcounter]
b = StrainTensors['b'][gcounter]
D = ElectricDisplacementx.reshape(self.ndim,1)
Dx = D.reshape(self.ndim)
DD = np.dot(D.T,D)[0,0]
D0D = np.dot(D,D.T)
if self.ndim==2:
trb = trace(b) + 1
else:
trb = trace(b)
C_mech = 2.*mu2/J*(2*einsum('ij,kl',b,b) - einsum('ik,jl',b,b) - einsum('il,jk',b,b)) +\
2.*(mu1+2.*mu2+6*mue)/J*( einsum("ik,jl",I,I)+einsum("il,jk",I,I) ) + \
lamb*(2.*J-1.)*einsum("ij,kl",I,I) - lamb*(J-1)*( einsum("ik,jl",I,I)+einsum("il,jk",I,I) ) +\
8.*mue/J*einsum('ij,kl',b,b)
C_elect = 1./eps_2*(0.5*DD*(einsum('ik,jl',I,I) + einsum('il,jk',I,I) + einsum('ij,kl',I,I) ) - \
einsum('ij,k,l',I,Dx,Dx) - einsum('i,j,kl',Dx,Dx,I))
# REGULARISATION TERMS
C_reg = 8.*J/eps_e*( einsum('ij,k,l',b,Dx,Dx) + einsum('i,j,kl',Dx,Dx,b) ) + \
8.*J**3/mue/eps_e**2*einsum('i,j,k,l',Dx,Dx,Dx,Dx)
self.elasticity_tensor = C_mech + C_elect + C_reg
self.coupling_tensor = 1./eps_2*(einsum('ik,j',I,Dx) + einsum('i,jk',Dx,I) - einsum('ij,k',I,Dx)) + \
8*J/eps_e*einsum('ij,k',b,Dx) + 4*J/eps_e*trb*( einsum('ik,j',I,Dx) + einsum('i,jk',Dx,I) ) +\
4.*J**3/mue/eps_e**2*DD* ( einsum('ik,j',I,Dx) + einsum('i,jk',Dx,I) ) + 8.*J**3/mue/eps_e**2*einsum('i,j,k',Dx,Dx,Dx)
self.dielectric_tensor = J/eps_1*np.linalg.inv(b) + 1./eps_2*I + \
4.*J/eps_e*trb*I + \
8.*J**3/mue/eps_e**2*(D0D + 0.5*DD*I)
# TRANSFORM TENSORS TO THEIR ENTHALPY COUNTERPART
E_Voigt, P_Voigt, C_Voigt = self.legendre_transform.InternalEnergyToEnthalpy(self.dielectric_tensor,
self.coupling_tensor, self.elasticity_tensor)
# BUILD HESSIAN
factor = -1.
H1 = np.concatenate((C_Voigt,factor*P_Voigt),axis=1)
H2 = np.concatenate((factor*P_Voigt.T,E_Voigt),axis=1)
H_Voigt = np.concatenate((H1,H2),axis=0)
return H_Voigt
def CauchyStress(self,StrainTensors,ElectricDisplacementx,elem=0,gcounter=0):
mu1 = self.mu1
mu2 = self.mu2
mue = self.mue
lamb = self.lamb
eps_2 = self.eps_2
eps_e = self.eps_e
I = StrainTensors['I']
J = StrainTensors['J'][gcounter]
b = StrainTensors['b'][gcounter]
D = ElectricDisplacementx.reshape(self.ndim,1)
DD = np.dot(D.T,D)[0,0]
D0D = np.dot(D,D.T)
if self.ndim==2:
trb = trace(b) + 1
else:
trb = trace(b)
sigma_mech = 2.0*mu1/J*b + \
2.0*mu2/J*(trb*b - np.dot(b,b)) -\
2.0*(mu1+2*mu2+6*mue)/J*I +\
lamb*(J-1)*I +\
4.*mue/J*trb*b
sigma_electric = 1./eps_2*(D0D - 0.5*DD*I)
# REGULARISATION TERMS
sigma_reg = 4.*J/eps_e*(DD*b + trb*D0D) + \
4.0*J**3/mue/eps_e**2*DD*D0D
sigma = sigma_mech + sigma_electric + sigma_reg
return sigma
def ElectricDisplacementx(self,StrainTensors,ElectricFieldx,elem=0,gcounter=0):
D = self.legendre_transform.GetElectricDisplacement(self, StrainTensors, ElectricFieldx, elem, gcounter)
return D
def Permittivity(self,StrainTensors,ElectricDisplacementx,elem=0,gcounter=0):
mu1 = self.mu1
mu2 = self.mu2
mue = self.mue
lamb = self.lamb
eps_1 = self.eps_1
eps_2 = self.eps_2
eps_e = self.eps_e
I = StrainTensors['I']
J = StrainTensors['J'][gcounter]
b = StrainTensors['b'][gcounter]
D = ElectricDisplacementx.reshape(self.ndim,1)
Dx = D.reshape(self.ndim)
DD = np.dot(D.T,D)[0,0]
D0D = np.dot(D,D.T)
if self.ndim==2:
trb = trace(b) + 1
else:
trb = trace(b)
self.dielectric_tensor = J/eps_1*np.linalg.inv(b) + 1./eps_2*I + \
4.*J/eps_e*trb*I + \
8.*J**3/mue/eps_e**2*(D0D + 0.5*DD*I)
# TRANSFORM TENSORS TO THEIR ENTHALPY COUNTERPART
H_Voigt = -np.linalg.inv(self.dielectric_tensor)
return H_Voigt
def ElectrostaticMeasures(self,F,ElectricFieldx, elem=0):
from Florence.MaterialLibrary.LLDispatch._IsotropicElectroMechanics_107_ import KineticMeasures
D, _, H_Voigt = KineticMeasures(self,np.ascontiguousarray(F), ElectricFieldx)
H_Voigt = np.ascontiguousarray(H_Voigt[:,-self.ndim:,-self.ndim:])
return D, None, H_Voigt
class IsotropicElectroMechanics_109(Material):
""" Electromechanical model in terms of internal energy
W(C,D) = W_mn(C) + 1/2/eps_2/J (FD0*FD0)
W_mn(C) = u1*C:I+u2*G:I - 2*(u1+2*u2)*lnJ + lamb/2*(J-1)**2
"""
def __init__(self, ndim, **kwargs):
mtype = type(self).__name__
super(IsotropicElectroMechanics_109, self).__init__(mtype, ndim, **kwargs)
# REQUIRES SEPARATELY
self.nvar = self.ndim+1
self.energy_type = "internal_energy"
self.legendre_transform = LegendreTransform()
self.nature = "nonlinear"
self.fields = "electro_mechanics"
if self.ndim == 2:
self.H_VoigtSize = 5
elif self.ndim == 3:
self.H_VoigtSize = 9
# LOW LEVEL DISPATCHER
self.has_low_level_dispatcher = True
# self.has_low_level_dispatcher = False
def KineticMeasures(self,F,ElectricFieldx, elem=0):
from Florence.MaterialLibrary.LLDispatch._IsotropicElectroMechanics_109_ import KineticMeasures
return KineticMeasures(self,np.ascontiguousarray(F), ElectricFieldx)
def Hessian(self,StrainTensors,ElectricDisplacementx,elem=0,gcounter=0):
mu_v = self.mu_v
mu1 = self.mu1
mu2 = self.mu2
lamb = self.lamb
eps_2 = self.eps_2
I = StrainTensors['I']
J = StrainTensors['J'][gcounter]
b = StrainTensors['b'][gcounter]
D = ElectricDisplacementx.reshape(self.ndim,1)
Dx = D.reshape(self.ndim)
DD = np.dot(D.T,D)[0,0]
C_mech = 2.*mu2/J*(2*einsum('ij,kl',b,b) - einsum('ik,jl',b,b) - einsum('il,jk',b,b)) +\
2.*(mu1+2.*mu2)/J*( einsum("ik,jl",I,I)+einsum("il,jk",I,I) ) + \
lamb*(2.*J-1.)*einsum("ij,kl",I,I) - lamb*(J-1)*( einsum("ik,jl",I,I)+einsum("il,jk",I,I) )
C_elect = 1./eps_2*(0.5*DD*(einsum('ik,jl',I,I) + einsum('il,jk',I,I) + einsum('ij,kl',I,I) ) - \
einsum('ij,k,l',I,Dx,Dx) - einsum('i,j,kl',Dx,Dx,I))
# C_linear = self.H_Voigt
C_linear = H_Voigt = lamb*einsum('ij,kl',I,I)+mu_v*(einsum('ik,jl',I,I)+einsum('il,jk',I,I))
self.elasticity_tensor = C_mech + C_elect + C_linear
self.coupling_tensor = 1./eps_2*(einsum('ik,j',I,Dx) + einsum('i,jk',Dx,I) - einsum('ij,k',I,Dx))
self.dielectric_tensor = 1./eps_2*I
# TRANSFORM TENSORS TO THEIR ENTHALPY COUNTERPART
E_Voigt, P_Voigt, C_Voigt = self.legendre_transform.InternalEnergyToEnthalpy(self.dielectric_tensor,
self.coupling_tensor, self.elasticity_tensor)
# BUILD HESSIAN
factor = -1.
H1 = np.concatenate((C_Voigt,factor*P_Voigt),axis=1)
H2 = np.concatenate((factor*P_Voigt.T,E_Voigt),axis=1)
H_Voigt = np.concatenate((H1,H2),axis=0)
return H_Voigt
def CauchyStress(self,StrainTensors,ElectricDisplacementx,elem=0,gcounter=0):
mu_v = self.mu_v
mu1 = self.mu1
mu2 = self.mu2
lamb = self.lamb
eps_2 = self.eps_2
I = StrainTensors['I']
J = StrainTensors['J'][gcounter]
b = StrainTensors['b'][gcounter]
strain = StrainTensors['strain'][gcounter]
D = ElectricDisplacementx.reshape(self.ndim,1)
DD = np.dot(D.T,D)[0,0]
trb = trace(b)
if self.ndim==2:
trb += 1.
simga_mech = 2.0*mu1/J*b + \
2.0*mu2/J*(trb*b - np.dot(b,b)) -\
2.0*(mu1+2*mu2)/J*I +\
lamb*(J-1.)*I
sigma_electric = 1./eps_2*(np.dot(D,D.T) - 0.5*DD*I)
# CHECK IF THIS IS NECESSARY
if self.ndim == 3:
tre = trace(strain)
elif self.ndim == 2:
tre = trace(strain) + 1
# USE FASTER TRACE FUNCTION
sigma_linear = 2.*mu_v*strain + lamb*tre*I
sigma = simga_mech + sigma_electric + sigma_linear
return sigma
def ElectricDisplacementx(self,StrainTensors,ElectricFieldx,elem=0,gcounter=0):
D = self.legendre_transform.GetElectricDisplacement(self, StrainTensors, ElectricFieldx, elem, gcounter)
# SANITY CHECK FOR IMPLICIT COMPUTATUTAION OF D
# I = StrainTensors['I']
# J = StrainTensors['J'][gcounter]
# b = StrainTensors['b'][gcounter]
# E = ElectricFieldx.reshape(self.ndim,1)
# eps_1 = self.eps_1
# eps_2 = self.eps_2
# inverse = np.linalg.inv(J/eps_1*np.linalg.inv(b) + 1./eps_2*I)
# D_exact = np.dot(inverse,E)
# print np.linalg.norm(D - D_exact)
# return D_exact
return D