2016-01-09 01:15:20 +05:30
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!--------------------------------------------------------------------------------------------------
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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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2018-12-30 22:41:03 +05:30
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!> @author Martin Diehl, Max-Planck-Institut für Eisenforschung GmbH
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2018-12-30 16:03:27 +05:30
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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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2016-01-09 01:15:20 +05:30
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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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2021-01-27 01:22:48 +05:30
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submodule(phase:plastic) isotropic
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2020-02-14 11:47:30 +05:30
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2019-05-17 02:26:48 +05:30
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type :: tParameters
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2019-03-28 03:12:02 +05:30
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real(pReal) :: &
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2019-03-28 03:39:45 +05:30
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M, & !< Taylor factor
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2019-03-28 11:09:07 +05:30
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dot_gamma_0, & !< reference strain rate
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2019-03-28 03:12:02 +05:30
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n, & !< stress exponent
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2020-09-22 18:32:24 +05:30
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h_0, &
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2021-06-22 02:52:51 +05:30
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h, & !< hardening pre-factor
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2019-03-28 11:09:07 +05:30
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h_ln, &
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2019-03-28 03:39:45 +05:30
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xi_inf, & !< maximum critical stress
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2019-03-28 03:12:02 +05:30
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a, &
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2019-03-28 03:39:45 +05:30
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c_1, &
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c_4, &
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c_3, &
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2020-03-15 00:33:57 +05:30
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c_2
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2019-03-28 03:12:02 +05:30
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logical :: &
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dilatation
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2020-02-14 11:47:30 +05:30
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character(len=pStringLen), allocatable, dimension(:) :: &
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output
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2019-03-28 03:12:02 +05:30
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end type tParameters
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2020-02-14 11:47:30 +05:30
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2019-05-17 02:26:48 +05:30
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type :: tIsotropicState
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2019-03-28 03:12:02 +05:30
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real(pReal), pointer, dimension(:) :: &
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2021-07-04 12:21:53 +05:30
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xi
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2019-03-28 03:12:02 +05:30
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end type tIsotropicState
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2017-09-19 05:12:27 +05:30
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2019-01-13 21:33:49 +05:30
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!--------------------------------------------------------------------------------------------------
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! containers for parameters and state
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2021-05-24 20:50:33 +05:30
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type(tParameters), allocatable, dimension(:) :: param
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2022-02-04 04:10:25 +05:30
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type(tIsotropicState), allocatable, dimension(:) :: state
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2018-12-30 22:41:03 +05:30
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2016-01-09 01:15:20 +05:30
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contains
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!--------------------------------------------------------------------------------------------------
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2020-02-14 11:47:30 +05:30
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!> @brief Perform module initialization.
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2016-01-09 01:15:20 +05:30
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!> @details reads in material parameters, allocates arrays, and does sanity checks
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!--------------------------------------------------------------------------------------------------
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2020-09-14 00:30:34 +05:30
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module function plastic_isotropic_init() result(myPlasticity)
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2019-05-17 02:26:48 +05:30
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2020-08-15 19:32:10 +05:30
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logical, dimension(:), allocatable :: myPlasticity
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2019-03-28 03:12:02 +05:30
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integer :: &
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2021-02-16 20:36:09 +05:30
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ph, &
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2021-03-05 01:46:36 +05:30
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Nmembers, &
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2020-07-02 00:52:05 +05:30
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sizeState, sizeDotState
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2020-03-16 17:44:44 +05:30
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real(pReal) :: &
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xi_0 !< initial critical stress
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2019-03-28 03:12:02 +05:30
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character(len=pStringLen) :: &
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extmsg = ''
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2022-10-25 21:39:36 +05:30
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type(tDict), pointer :: &
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2020-08-15 19:32:10 +05:30
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phases, &
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phase, &
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2020-11-03 03:16:46 +05:30
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mech, &
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2020-08-15 19:32:10 +05:30
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pl
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2020-02-14 11:47:30 +05:30
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2021-02-14 11:36:14 +05:30
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2020-08-15 19:32:10 +05:30
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myPlasticity = plastic_active('isotropic')
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2021-02-14 11:36:14 +05:30
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if(count(myPlasticity) == 0) return
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2020-07-02 00:52:05 +05:30
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2021-11-15 23:05:44 +05:30
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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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2021-02-13 17:37:35 +05:30
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2022-05-28 00:23:16 +05:30
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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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2020-09-14 00:30:34 +05:30
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2022-10-25 21:39:36 +05:30
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phases => config_material%get_dict('phase')
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2021-02-14 11:36:14 +05:30
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allocate(param(phases%length))
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allocate(state(phases%length))
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2021-02-16 20:36:09 +05:30
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do ph = 1, phases%length
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if(.not. myPlasticity(ph)) cycle
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2022-02-04 04:10:25 +05:30
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associate(prm => param(ph), stt => state(ph))
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2021-02-16 20:36:09 +05:30
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2022-10-25 21:39:36 +05:30
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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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2020-02-14 11:47:30 +05:30
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2020-09-14 00:30:34 +05:30
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#if defined (__GFORTRAN__)
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2021-03-11 22:30:07 +05:30
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prm%output = output_as1dString(pl)
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2020-08-15 19:32:10 +05:30
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#else
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2021-03-11 22:30:07 +05:30
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prm%output = pl%get_as1dString('output',defaultVal=emptyStringArray)
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2020-08-15 19:32:10 +05:30
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#endif
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2020-03-15 00:33:57 +05:30
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2020-08-15 19:32:10 +05:30
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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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2020-09-22 18:32:24 +05:30
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prm%h_0 = pl%get_asFloat('h_0')
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2021-06-22 02:52:51 +05:30
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prm%h = pl%get_asFloat('h', defaultVal=3.0_pReal) ! match for fcc random polycrystal
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2020-08-15 19:32:10 +05:30
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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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2020-02-14 11:47:30 +05:30
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2018-12-30 22:41:03 +05:30
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!--------------------------------------------------------------------------------------------------
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! sanity checks
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2020-03-16 17:44:44 +05:30
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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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2020-02-14 11:47:30 +05:30
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2016-01-09 01:15:20 +05:30
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!--------------------------------------------------------------------------------------------------
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! allocate state arrays
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2021-04-06 15:08:44 +05:30
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Nmembers = count(material_phaseID == ph)
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2021-07-04 12:21:53 +05:30
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sizeDotState = size(['xi'])
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2019-03-28 03:12:02 +05:30
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sizeState = sizeDotState
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2020-02-14 11:47:30 +05:30
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2021-03-05 01:46:36 +05:30
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call phase_allocateState(plasticState(ph),Nmembers,sizeState,sizeDotState,0)
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2022-02-04 04:10:25 +05:30
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deallocate(plasticState(ph)%dotState) ! ToDo: remove dotState completely
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2020-02-14 11:47:30 +05:30
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2016-01-22 06:38:36 +05:30
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!--------------------------------------------------------------------------------------------------
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2020-03-16 03:37:23 +05:30
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! state aliases and initialization
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2022-02-04 04:10:25 +05:30
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stt%xi => plasticState(ph)%state(1,:)
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stt%xi = xi_0
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2021-02-16 20:36:09 +05:30
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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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2019-03-28 03:12:02 +05:30
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end associate
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2020-02-14 11:47:30 +05:30
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2020-03-15 00:33:57 +05:30
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!--------------------------------------------------------------------------------------------------
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! exit if any parameter is out of range
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2022-05-27 03:54:40 +05:30
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if (extmsg /= '') call IO_error(211,ext_msg=trim(extmsg))
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2020-03-15 00:33:57 +05:30
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2021-11-15 23:05:44 +05:30
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end do
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2016-01-09 01:15:20 +05:30
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2020-08-15 19:32:10 +05:30
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end function plastic_isotropic_init
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2016-01-09 01:15:20 +05:30
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2018-06-01 13:54:42 +05:30
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2016-01-09 01:15:20 +05:30
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!--------------------------------------------------------------------------------------------------
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2020-02-14 11:47:30 +05:30
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!> @brief Calculate plastic velocity gradient and its tangent.
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2016-01-09 01:15:20 +05:30
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!--------------------------------------------------------------------------------------------------
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2021-04-25 11:36:52 +05:30
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module subroutine isotropic_LpAndItsTangent(Lp,dLp_dMp,Mp,ph,en)
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2020-02-14 11:47:30 +05:30
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2019-03-28 03:12:02 +05:30
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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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2020-02-14 11:47:30 +05:30
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2019-03-28 03:12:02 +05:30
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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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2021-01-27 03:11:41 +05:30
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ph, &
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2021-04-25 11:36:52 +05:30
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en
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2020-07-03 20:15:11 +05:30
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2019-03-28 03:12:02 +05:30
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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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2019-03-28 11:09:07 +05:30
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dot_gamma, & !< strainrate
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2019-03-28 03:12:02 +05:30
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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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2020-02-14 11:47:30 +05:30
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2021-07-23 03:39:51 +05:30
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2021-02-14 11:36:14 +05:30
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associate(prm => param(ph), stt => state(ph))
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2020-02-14 11:47:30 +05:30
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2021-07-23 03:39:51 +05:30
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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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2022-02-04 04:10:25 +05:30
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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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2021-07-23 03:39:51 +05:30
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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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2020-02-14 11:47:30 +05:30
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2019-03-28 03:12:02 +05:30
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end associate
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2019-01-06 04:11:13 +05:30
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2021-01-26 12:03:04 +05:30
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end subroutine isotropic_LpAndItsTangent
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2016-01-09 01:15:20 +05:30
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2018-12-30 18:31:05 +05:30
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2016-01-09 01:15:20 +05:30
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!--------------------------------------------------------------------------------------------------
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2020-02-14 11:47:30 +05:30
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!> @brief Calculate inelastic velocity gradient and its tangent.
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2016-01-09 01:15:20 +05:30
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!--------------------------------------------------------------------------------------------------
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2021-04-13 00:51:15 +05:30
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module subroutine plastic_isotropic_LiAndItsTangent(Li,dLi_dMi,Mi,ph,en)
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2020-02-14 11:47:30 +05:30
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2020-03-16 18:03:14 +05:30
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real(pReal), dimension(3,3), intent(out) :: &
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2019-03-28 03:12:02 +05:30
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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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2019-09-20 17:34:56 +05:30
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dLi_dMi !< derivative of Li with respect to Mandel stress
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2020-02-14 11:47:30 +05:30
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2020-03-16 18:03:14 +05:30
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real(pReal), dimension(3,3), intent(in) :: &
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2020-02-14 11:47:30 +05:30
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Mi !< Mandel stress
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2020-03-16 18:03:14 +05:30
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integer, intent(in) :: &
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2021-02-14 11:36:14 +05:30
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ph, &
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2021-04-13 00:51:15 +05:30
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en
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2020-07-03 20:15:11 +05:30
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2019-03-28 03:12:02 +05:30
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real(pReal) :: &
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2019-09-20 17:34:56 +05:30
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tr !< trace of spherical part of Mandel stress (= 3 x pressure)
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2019-03-28 03:12:02 +05:30
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integer :: &
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k, l, m, n
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2020-02-14 11:47:30 +05:30
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2021-07-23 03:39:51 +05:30
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2021-02-14 11:36:14 +05:30
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associate(prm => param(ph), stt => state(ph))
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2020-02-14 11:47:30 +05:30
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2021-07-23 03:39:51 +05:30
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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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2021-11-15 23:05:44 +05:30
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end if
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2020-02-14 11:47:30 +05:30
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2019-03-28 03:12:02 +05:30
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end associate
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2019-01-06 04:11:13 +05:30
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2018-05-25 04:01:32 +05:30
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end subroutine plastic_isotropic_LiAndItsTangent
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2016-01-09 01:15:20 +05:30
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!--------------------------------------------------------------------------------------------------
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2020-02-14 11:47:30 +05:30
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!> @brief Calculate the rate of change of microstructure.
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2016-01-09 01:15:20 +05:30
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!--------------------------------------------------------------------------------------------------
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2022-02-04 04:10:25 +05:30
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module function isotropic_dotState(Mp,ph,en) result(dotState)
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2020-02-14 11:47:30 +05:30
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2019-03-28 03:12:02 +05:30
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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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2021-01-27 03:11:41 +05:30
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ph, &
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2021-04-25 11:36:52 +05:30
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|
en
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2022-02-04 04:10:25 +05:30
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real(pReal), dimension(plasticState(ph)%sizeDotState) :: &
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dotState
|
2020-02-14 11:47:30 +05:30
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2019-03-28 03:12:02 +05:30
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real(pReal) :: &
|
2019-03-28 11:09:07 +05:30
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dot_gamma, & !< strainrate
|
2019-03-28 03:39:45 +05:30
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xi_inf_star, & !< saturation xi
|
2019-03-28 03:12:02 +05:30
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|
norm_Mp !< norm of the (deviatoric) Mandel stress
|
2020-02-14 11:47:30 +05:30
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|
2022-02-04 04:10:25 +05:30
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|
associate(prm => param(ph), stt => state(ph), dot_xi => dotState(1))
|
2020-02-14 11:47:30 +05:30
|
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|
2022-02-04 04:10:25 +05:30
|
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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))), &
|
|
|
|
|
prm%dilatation)
|
2020-02-14 11:47:30 +05:30
|
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|
2021-04-25 11:36:52 +05:30
|
|
|
|
dot_gamma = prm%dot_gamma_0 * (sqrt(1.5_pReal) * norm_Mp /(prm%M*stt%xi(en))) **prm%n
|
2020-02-14 11:47:30 +05:30
|
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|
|
|
2019-03-28 14:17:03 +05:30
|
|
|
|
if (dot_gamma > 1e-12_pReal) then
|
2019-03-28 03:39:45 +05:30
|
|
|
|
if (dEq0(prm%c_1)) then
|
|
|
|
|
xi_inf_star = prm%xi_inf
|
2019-03-28 03:12:02 +05:30
|
|
|
|
else
|
2019-03-28 03:39:45 +05:30
|
|
|
|
xi_inf_star = prm%xi_inf &
|
2019-04-04 11:22:36 +05:30
|
|
|
|
+ asinh( (dot_gamma / prm%c_1)**(1.0_pReal / prm%c_2))**(1.0_pReal / prm%c_3) &
|
2019-09-21 20:44:03 +05:30
|
|
|
|
/ prm%c_4 * (dot_gamma / prm%dot_gamma_0)**(1.0_pReal / prm%n)
|
2021-11-15 23:05:44 +05:30
|
|
|
|
end if
|
2022-02-04 04:10:25 +05:30
|
|
|
|
dot_xi = dot_gamma &
|
|
|
|
|
* ( prm%h_0 + prm%h_ln * log(dot_gamma) ) &
|
|
|
|
|
* sign(abs(1.0_pReal - stt%xi(en)/xi_inf_star)**prm%a *prm%h, 1.0_pReal-stt%xi(en)/xi_inf_star)
|
2019-03-28 03:12:02 +05:30
|
|
|
|
else
|
2022-02-04 04:10:25 +05:30
|
|
|
|
dot_xi = 0.0_pReal
|
2021-11-15 23:05:44 +05:30
|
|
|
|
end if
|
2020-02-14 11:47:30 +05:30
|
|
|
|
|
2019-03-28 03:12:02 +05:30
|
|
|
|
end associate
|
2016-01-09 01:15:20 +05:30
|
|
|
|
|
2022-02-04 04:10:25 +05:30
|
|
|
|
end function isotropic_dotState
|
2016-01-09 01:15:20 +05:30
|
|
|
|
|
2018-12-30 19:07:31 +05:30
|
|
|
|
|
2019-03-10 01:13:31 +05:30
|
|
|
|
!--------------------------------------------------------------------------------------------------
|
2020-02-14 11:47:30 +05:30
|
|
|
|
!> @brief Write results to HDF5 output file.
|
2019-03-10 01:13:31 +05:30
|
|
|
|
!--------------------------------------------------------------------------------------------------
|
2021-02-14 11:36:14 +05:30
|
|
|
|
module subroutine plastic_isotropic_results(ph,group)
|
2019-03-10 01:13:31 +05:30
|
|
|
|
|
2021-02-14 11:36:14 +05:30
|
|
|
|
integer, intent(in) :: ph
|
2019-04-04 11:22:36 +05:30
|
|
|
|
character(len=*), intent(in) :: group
|
2020-02-14 11:47:30 +05:30
|
|
|
|
|
2019-03-10 01:13:31 +05:30
|
|
|
|
integer :: o
|
|
|
|
|
|
2021-02-14 11:36:14 +05:30
|
|
|
|
associate(prm => param(ph), stt => state(ph))
|
2020-02-14 11:47:30 +05:30
|
|
|
|
outputsLoop: do o = 1,size(prm%output)
|
|
|
|
|
select case(trim(prm%output(o)))
|
2020-09-14 00:30:34 +05:30
|
|
|
|
case ('xi')
|
2021-06-01 20:35:13 +05:30
|
|
|
|
call results_writeDataset(stt%xi,group,trim(prm%output(o)), &
|
2020-08-15 19:32:10 +05:30
|
|
|
|
'resistance against plastic flow','Pa')
|
2019-03-10 01:13:31 +05:30
|
|
|
|
end select
|
2021-11-15 23:05:44 +05:30
|
|
|
|
end do outputsLoop
|
2019-03-10 01:13:31 +05:30
|
|
|
|
end associate
|
|
|
|
|
|
|
|
|
|
end subroutine plastic_isotropic_results
|
|
|
|
|
|
|
|
|
|
|
2021-01-26 05:41:32 +05:30
|
|
|
|
end submodule isotropic
|