2015-05-28 22:32:23 +05:30
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!--------------------------------------------------------------------------------------------------
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!> @author Pratheek Shanthraj, Max-Planck-Institut für Eisenforschung GmbH
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!> @brief material subroutine incorporating kinematics resulting from thermal expansion
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!> @details to be done
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!--------------------------------------------------------------------------------------------------
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module kinematics_thermal_expansion
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2019-05-15 02:42:32 +05:30
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use prec
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2019-05-17 02:44:47 +05:30
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use IO
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use config
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use debug
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use math
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use lattice
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use material
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2020-02-28 14:55:07 +05:30
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2019-02-23 01:07:41 +05:30
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implicit none
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private
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integer, dimension(:), allocatable :: kinematics_thermal_expansion_instance
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type :: tParameters
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real(pReal) :: &
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T_ref
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real(pReal), dimension(3,3,3) :: &
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expansion = 0.0_pReal
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end type tParameters
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type(tParameters), dimension(:), allocatable :: param
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public :: &
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kinematics_thermal_expansion_init, &
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kinematics_thermal_expansion_initialStrain, &
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kinematics_thermal_expansion_LiAndItsTangent
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2015-05-28 22:32:23 +05:30
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contains
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!--------------------------------------------------------------------------------------------------
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!> @brief 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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subroutine kinematics_thermal_expansion_init
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2020-02-29 02:14:40 +05:30
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integer :: Ninstance,p,i
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real(pReal), dimension(:), allocatable :: &
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temp
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2020-01-10 05:58:32 +05:30
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write(6,'(/,a)') ' <<<+- kinematics_'//KINEMATICS_thermal_expansion_LABEL//' init -+>>>'; flush(6)
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Ninstance = count(phase_kinematics == KINEMATICS_thermal_expansion_ID)
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if (iand(debug_level(debug_constitutive),debug_levelBasic) /= 0) &
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write(6,'(a16,1x,i5,/)') '# instances:',Ninstance
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allocate(kinematics_thermal_expansion_instance(size(config_phase)), source=0)
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allocate(param(Ninstance))
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do p = 1, size(config_phase)
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kinematics_thermal_expansion_instance(p) = count(phase_kinematics(:,1:p) == KINEMATICS_thermal_expansion_ID)
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if (all(phase_kinematics(:,p) /= KINEMATICS_thermal_expansion_ID)) cycle
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associate(prm => param(kinematics_thermal_expansion_instance(p)), &
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config => config_phase(p))
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prm%T_ref = config%getFloat('reference_temperature', defaultVal=0.0_pReal)
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! read up to three parameters (constant, linear, quadratic with T)
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temp = config%getFloats('thermal_expansion11')
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prm%expansion(1,1,1:size(temp)) = temp
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temp = config%getFloats('thermal_expansion22',defaultVal=[(0.0_pReal, i=1,size(temp))],requiredSize=size(temp))
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prm%expansion(2,2,1:size(temp)) = temp
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temp = config%getFloats('thermal_expansion33',defaultVal=[(0.0_pReal, i=1,size(temp))],requiredSize=size(temp))
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prm%expansion(3,3,1:size(temp)) = temp
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do i=1, size(prm%expansion,3)
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prm%expansion(1:3,1:3,i) = lattice_symmetrize33(prm%expansion(1:3,1:3,i),config%getString('lattice_structure'))
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enddo
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end associate
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enddo
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end subroutine kinematics_thermal_expansion_init
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2015-07-23 21:29:25 +05:30
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!--------------------------------------------------------------------------------------------------
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!> @brief report initial thermal strain based on current temperature deviation from reference
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!--------------------------------------------------------------------------------------------------
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2019-02-13 04:05:22 +05:30
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pure function kinematics_thermal_expansion_initialStrain(homog,phase,offset)
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integer, intent(in) :: &
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phase, &
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homog, &
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offset
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real(pReal), dimension(3,3) :: &
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kinematics_thermal_expansion_initialStrain !< initial thermal strain (should be small strain, though)
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associate(prm => param(kinematics_thermal_expansion_instance(phase)))
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kinematics_thermal_expansion_initialStrain = &
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(temperature(homog)%p(offset) - prm%T_ref)**1 / 1. * prm%expansion(1:3,1:3,1) + & ! constant coefficient
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(temperature(homog)%p(offset) - prm%T_ref)**2 / 2. * prm%expansion(1:3,1:3,2) + & ! linear coefficient
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(temperature(homog)%p(offset) - prm%T_ref)**3 / 3. * prm%expansion(1:3,1:3,3) ! quadratic coefficient
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end associate
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2015-07-24 20:17:18 +05:30
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end function kinematics_thermal_expansion_initialStrain
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2015-07-23 21:29:25 +05:30
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2019-02-23 01:07:41 +05:30
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2015-05-28 22:32:23 +05:30
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!--------------------------------------------------------------------------------------------------
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!> @brief contains the constitutive equation for calculating the velocity gradient
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!--------------------------------------------------------------------------------------------------
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2018-12-31 01:28:38 +05:30
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subroutine kinematics_thermal_expansion_LiAndItsTangent(Li, dLi_dTstar, ipc, ip, el)
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integer, intent(in) :: &
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ipc, & !< grain number
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ip, & !< integration point number
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el !< element number
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real(pReal), intent(out), dimension(3,3) :: &
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Li !< thermal velocity gradient
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real(pReal), intent(out), dimension(3,3,3,3) :: &
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dLi_dTstar !< derivative of Li with respect to Tstar (4th-order tensor defined to be zero)
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2019-05-17 02:44:47 +05:30
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integer :: &
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phase, &
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homog
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real(pReal) :: &
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T, TDot
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2019-06-14 13:07:01 +05:30
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phase = material_phaseAt(ipc,el)
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homog = material_homogenizationAt(el)
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T = temperature(homog)%p(thermalMapping(homog)%p(ip,el))
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TDot = temperatureRate(homog)%p(thermalMapping(homog)%p(ip,el))
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associate(prm => param(kinematics_thermal_expansion_instance(phase)))
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Li = TDot * ( &
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prm%expansion(1:3,1:3,1)*(T - prm%T_ref)**0 & ! constant coefficient
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+ prm%expansion(1:3,1:3,2)*(T - prm%T_ref)**1 & ! linear coefficient
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+ prm%expansion(1:3,1:3,3)*(T - prm%T_ref)**2 & ! quadratic coefficient
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) / &
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(1.0_pReal &
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+ prm%expansion(1:3,1:3,1)*(T - prm%T_ref)**1 / 1. &
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+ prm%expansion(1:3,1:3,2)*(T - prm%T_ref)**2 / 2. &
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+ prm%expansion(1:3,1:3,3)*(T - prm%T_ref)**3 / 3. &
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)
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end associate
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dLi_dTstar = 0.0_pReal
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2015-05-28 22:32:23 +05:30
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end subroutine kinematics_thermal_expansion_LiAndItsTangent
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end module kinematics_thermal_expansion
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