316 lines
13 KiB
Fortran
316 lines
13 KiB
Fortran
!--------------------------------------------------------------------------------------------------
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!> @author Franz Roters, Max-Planck-Institut für Eisenforschung GmbH
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!> @author Philip Eisenlohr, Max-Planck-Institut für Eisenforschung GmbH
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!> @author Martin Diehl, Max-Planck-Institut für Eisenforschung GmbH
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!> @brief material subroutine for isotropic plasticity
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!> @details Isotropic Plasticity which resembles the phenopowerlaw plasticity without
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!! resolving the stress on the slip systems. Will give the response of phenopowerlaw for an
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!! untextured polycrystal
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!--------------------------------------------------------------------------------------------------
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submodule(phase:plastic) isotropic
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type :: tParameters
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real(pReal) :: &
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M, & !< Taylor factor
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dot_gamma_0, & !< reference strain rate
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n, & !< stress exponent
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h_0, &
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h, & !< hardening pre-factor
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h_ln, &
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xi_inf, & !< maximum critical stress
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a, &
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c_1, &
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c_4, &
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c_3, &
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c_2
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logical :: &
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dilatation
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character(len=pStringLen), allocatable, dimension(:) :: &
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output
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end type tParameters
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type :: tIsotropicState
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real(pReal), pointer, dimension(:) :: &
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xi
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end type tIsotropicState
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!--------------------------------------------------------------------------------------------------
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! containers for parameters and state
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type(tParameters), allocatable, dimension(:) :: param
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type(tIsotropicState), allocatable, dimension(:) :: state
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contains
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!--------------------------------------------------------------------------------------------------
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!> @brief Perform module initialization.
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!> @details reads in material parameters, allocates arrays, and does sanity checks
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!--------------------------------------------------------------------------------------------------
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module function plastic_isotropic_init() result(myPlasticity)
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logical, dimension(:), allocatable :: myPlasticity
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integer :: &
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ph, &
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Nmembers, &
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sizeState, sizeDotState
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real(pReal) :: &
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xi_0 !< initial critical stress
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character(len=:), allocatable :: &
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refs, &
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extmsg
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type(tDict), pointer :: &
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phases, &
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phase, &
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mech, &
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pl
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myPlasticity = plastic_active('isotropic')
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if (count(myPlasticity) == 0) return
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print'(/,1x,a)', '<<<+- phase:mechanical:plastic:isotropic init -+>>>'
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print'(/,a,i0)', ' # phases: ',count(myPlasticity); flush(IO_STDOUT)
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print'(/,1x,a)', 'T. Maiti and P. Eisenlohr, Scripta Materialia 145:37–40, 2018'
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print'( 1x,a)', 'https://doi.org/10.1016/j.scriptamat.2017.09.047'
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phases => config_material%get_dict('phase')
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allocate(param(phases%length))
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allocate(state(phases%length))
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extmsg = ''
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do ph = 1, phases%length
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if (.not. myPlasticity(ph)) cycle
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associate(prm => param(ph), stt => state(ph))
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phase => phases%get_dict(ph)
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mech => phase%get_dict('mechanical')
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pl => mech%get_dict('plastic')
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print'(/,1x,a,i0,a)', 'phase ',ph,': '//phases%key(ph)
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refs = config_listReferences(pl,indent=3)
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if (len(refs) > 0) print'(/,1x,a)', refs
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#if defined (__GFORTRAN__)
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prm%output = output_as1dString(pl)
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#else
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prm%output = pl%get_as1dString('output',defaultVal=emptyStringArray)
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#endif
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xi_0 = pl%get_asFloat('xi_0')
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prm%xi_inf = pl%get_asFloat('xi_inf')
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prm%dot_gamma_0 = pl%get_asFloat('dot_gamma_0')
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prm%n = pl%get_asFloat('n')
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prm%h_0 = pl%get_asFloat('h_0')
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prm%h = pl%get_asFloat('h', defaultVal=3.0_pReal) ! match for fcc random polycrystal
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prm%M = pl%get_asFloat('M')
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prm%h_ln = pl%get_asFloat('h_ln', defaultVal=0.0_pReal)
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prm%c_1 = pl%get_asFloat('c_1', defaultVal=0.0_pReal)
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prm%c_4 = pl%get_asFloat('c_4', defaultVal=0.0_pReal)
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prm%c_3 = pl%get_asFloat('c_3', defaultVal=0.0_pReal)
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prm%c_2 = pl%get_asFloat('c_2', defaultVal=0.0_pReal)
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prm%a = pl%get_asFloat('a')
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prm%dilatation = pl%get_asBool('dilatation',defaultVal = .false.)
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!--------------------------------------------------------------------------------------------------
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! sanity checks
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if (xi_0 < 0.0_pReal) extmsg = trim(extmsg)//' xi_0'
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if (prm%dot_gamma_0 <= 0.0_pReal) extmsg = trim(extmsg)//' dot_gamma_0'
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if (prm%n <= 0.0_pReal) extmsg = trim(extmsg)//' n'
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if (prm%a <= 0.0_pReal) extmsg = trim(extmsg)//' a'
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if (prm%M <= 0.0_pReal) extmsg = trim(extmsg)//' M'
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!--------------------------------------------------------------------------------------------------
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! allocate state arrays
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Nmembers = count(material_ID_phase == ph)
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sizeDotState = size(['xi'])
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sizeState = sizeDotState
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call phase_allocateState(plasticState(ph),Nmembers,sizeState,sizeDotState,0)
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deallocate(plasticState(ph)%dotState) ! ToDo: remove dotState completely
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!--------------------------------------------------------------------------------------------------
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! state aliases and initialization
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stt%xi => plasticState(ph)%state(1,:)
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stt%xi = xi_0
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plasticState(ph)%atol(1) = pl%get_asFloat('atol_xi',defaultVal=1.0_pReal)
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if (plasticState(ph)%atol(1) < 0.0_pReal) extmsg = trim(extmsg)//' atol_xi'
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end associate
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!--------------------------------------------------------------------------------------------------
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! exit if any parameter is out of range
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if (extmsg /= '') call IO_error(211,ext_msg=trim(extmsg))
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end do
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end function plastic_isotropic_init
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!--------------------------------------------------------------------------------------------------
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!> @brief Calculate plastic velocity gradient and its tangent.
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!--------------------------------------------------------------------------------------------------
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module subroutine isotropic_LpAndItsTangent(Lp,dLp_dMp,Mp,ph,en)
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real(pReal), dimension(3,3), intent(out) :: &
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Lp !< plastic velocity gradient
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real(pReal), dimension(3,3,3,3), intent(out) :: &
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dLp_dMp !< derivative of Lp with respect to the Mandel stress
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real(pReal), dimension(3,3), intent(in) :: &
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Mp !< Mandel stress
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integer, intent(in) :: &
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ph, &
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en
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real(pReal), dimension(3,3) :: &
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Mp_dev !< deviatoric part of the Mandel stress
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real(pReal) :: &
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dot_gamma, & !< strainrate
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norm_Mp_dev, & !< norm of the deviatoric part of the Mandel stress
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squarenorm_Mp_dev !< square of the norm of the deviatoric part of the Mandel stress
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integer :: &
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k, l, m, n
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associate(prm => param(ph), stt => state(ph))
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Mp_dev = math_deviatoric33(Mp)
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squarenorm_Mp_dev = math_tensordot(Mp_dev,Mp_dev)
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norm_Mp_dev = sqrt(squarenorm_Mp_dev)
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if (norm_Mp_dev > 0.0_pReal) then
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dot_gamma = prm%dot_gamma_0 * (sqrt(1.5_pReal) * norm_Mp_dev/(prm%M*stt%xi(en)))**prm%n
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Lp = dot_gamma * Mp_dev/norm_Mp_dev
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forall (k=1:3,l=1:3,m=1:3,n=1:3) &
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dLp_dMp(k,l,m,n) = (prm%n-1.0_pReal) * Mp_dev(k,l)*Mp_dev(m,n) / squarenorm_Mp_dev
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forall (k=1:3,l=1:3) &
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dLp_dMp(k,l,k,l) = dLp_dMp(k,l,k,l) + 1.0_pReal
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forall (k=1:3,m=1:3) &
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dLp_dMp(k,k,m,m) = dLp_dMp(k,k,m,m) - 1.0_pReal/3.0_pReal
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dLp_dMp = dot_gamma * dLp_dMp / norm_Mp_dev
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else
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Lp = 0.0_pReal
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dLp_dMp = 0.0_pReal
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end if
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end associate
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end subroutine isotropic_LpAndItsTangent
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!--------------------------------------------------------------------------------------------------
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!> @brief Calculate inelastic velocity gradient and its tangent.
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!--------------------------------------------------------------------------------------------------
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module subroutine plastic_isotropic_LiAndItsTangent(Li,dLi_dMi,Mi,ph,en)
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real(pReal), dimension(3,3), intent(out) :: &
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Li !< inleastic velocity gradient
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real(pReal), dimension(3,3,3,3), intent(out) :: &
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dLi_dMi !< derivative of Li with respect to Mandel stress
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real(pReal), dimension(3,3), intent(in) :: &
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Mi !< Mandel stress
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integer, intent(in) :: &
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ph, &
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en
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real(pReal) :: &
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tr !< trace of spherical part of Mandel stress (= 3 x pressure)
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integer :: &
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k, l, m, n
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associate(prm => param(ph), stt => state(ph))
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tr=math_trace33(math_spherical33(Mi))
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if (prm%dilatation .and. abs(tr) > 0.0_pReal) then ! no stress or J2 plasticity --> Li and its derivative are zero
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Li = math_I3 &
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* prm%dot_gamma_0 * (3.0_pReal*prm%M*stt%xi(en))**(-prm%n) &
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* tr * abs(tr)**(prm%n-1.0_pReal)
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forall (k=1:3,l=1:3,m=1:3,n=1:3) dLi_dMi(k,l,m,n) = prm%n / tr * Li(k,l) * math_I3(m,n)
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else
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Li = 0.0_pReal
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dLi_dMi = 0.0_pReal
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end if
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end associate
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end subroutine plastic_isotropic_LiAndItsTangent
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!--------------------------------------------------------------------------------------------------
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!> @brief Calculate the rate of change of microstructure.
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!--------------------------------------------------------------------------------------------------
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module function isotropic_dotState(Mp,ph,en) result(dotState)
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real(pReal), dimension(3,3), intent(in) :: &
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Mp !< Mandel stress
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integer, intent(in) :: &
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ph, &
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en
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real(pReal), dimension(plasticState(ph)%sizeDotState) :: &
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dotState
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real(pReal) :: &
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dot_gamma, & !< strainrate
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xi_inf_star, & !< saturation xi
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norm_Mp !< norm of the (deviatoric) Mandel stress
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associate(prm => param(ph), stt => state(ph), dot_xi => dotState(1))
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norm_Mp = merge(sqrt(math_tensordot(Mp,Mp)), &
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sqrt(math_tensordot(math_deviatoric33(Mp),math_deviatoric33(Mp))), &
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prm%dilatation)
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dot_gamma = prm%dot_gamma_0 * (sqrt(1.5_pReal) * norm_Mp /(prm%M*stt%xi(en))) **prm%n
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if (dot_gamma > 1e-12_pReal) then
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if (dEq0(prm%c_1)) then
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xi_inf_star = prm%xi_inf
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else
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xi_inf_star = prm%xi_inf &
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+ asinh( (dot_gamma / prm%c_1)**(1.0_pReal / prm%c_2))**(1.0_pReal / prm%c_3) &
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/ prm%c_4 * (dot_gamma / prm%dot_gamma_0)**(1.0_pReal / prm%n)
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end if
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dot_xi = dot_gamma &
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* ( prm%h_0 + prm%h_ln * log(dot_gamma) ) &
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* sign(abs(1.0_pReal - stt%xi(en)/xi_inf_star)**prm%a *prm%h, 1.0_pReal-stt%xi(en)/xi_inf_star)
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else
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dot_xi = 0.0_pReal
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end if
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end associate
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end function isotropic_dotState
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!--------------------------------------------------------------------------------------------------
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!> @brief Write results to HDF5 output file.
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!--------------------------------------------------------------------------------------------------
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module subroutine plastic_isotropic_result(ph,group)
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integer, intent(in) :: ph
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character(len=*), intent(in) :: group
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integer :: o
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associate(prm => param(ph), stt => state(ph))
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outputsLoop: do o = 1,size(prm%output)
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select case(trim(prm%output(o)))
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case ('xi')
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call result_writeDataset(stt%xi,group,trim(prm%output(o)), &
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'resistance against plastic flow','Pa')
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end select
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end do outputsLoop
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end associate
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end subroutine plastic_isotropic_result
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end submodule isotropic
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