TEMPERATURE

Subcase Information Entry Selects the temperature set to be used in either material property calculations or thermal loading.

Format

TEMPERATURE (type, SUBTYPE=subtype_option) = option

Examples

TEMPERATURE(LOAD)=15
TEMP(MATERIAL)=7
TEMPERATURE=7
TEMPERATURE(LOAD,HTIME=ALL)=8
TEMPERATURE(LOAD,TEMPT)=23

Definitions

Argument Options Description
type <INITIAL, MATERIAL, LOAD, BOTH>
INITIAL
The selected temperature set will be used to determine initial temperature distribution.
MATERIAL
The selected temperature set will be used to determine temperature-dependent material properties indicated on the MATTi Bulk Data Entries.
In addition, the SUBCASE ID of a thermal analysis SUBCASE can be specified. The calculated temperature field is then used to determine temperature-dependent material properties indicated on the MATTi Bulk Data Entries.
This is only allowed for linear analysis. For nonlinear analysis, TEMP(LOAD) will be used to update the temperature dependent material.
LOAD
The selected temperature set will be used to determine an equivalent static load.
For nonlinear analysis, this temperature set will also be used to update the temperature dependent material.
BOTH (Default)
Both MATERIAL and LOAD will use the same temperature set.
SUBTYPE <HTIME,TEMPT>
HTIME
Selects all the output time steps of a transient thermal subcase. This option is supported for linear and nonlinear static analysis.
TEMPT
Selects this option, where Grid-temperature is provided from either an external file or an internal transient thermal subcase. This option is only supported for nonlinear static subcases.
option <SID>

No default

SID
Set identification number of TEMP, TEMPD, or TEMPT Bulk Data Entries. This can also reference a Transient Heat Transfer subcase or a TSTRU Subcase Information Entry.
subtype_option <ALL, Blank>

No default

ALL
When SUBTYPE field is set to HTIME, then the subtype_option should be set to ALL.
Blank
When SUBTYPE field is set to TEMPT, then subtype_option should be Blank.

Comments

  1. The total load applied will be the sum of external (LOAD command), thermal (TEMP(LOAD/BOTH) command) and constrained displacement (SPC command) loads.
  2. In Linear static analysis, TEMP(BOTH), TEMP(LOAD), TEMP(MAT), and TEMP(INIT) can be used before the subcase level or inside the subcase. If used before the subcase level, it will apply to all subcases that do not have their own corresponding command. Additionally, only the last instance of TEMP(MAT) and TEMP(INIT) will be used to update the corresponding material or set the initial temperature for all subcases.
  3. In Nonlinear Static analysis TEMP(LOAD) and TEMP(INIT) can be used before the subcase level or inside the subcase. If used before the subcase level, it will apply to all subcases that do not have their corresponding command. Additionally, only the last instance of TEMP(INIT) will be used to the set the initial temperature or material properties (if TEMP(LOAD) is not present) for all subcases.
  4. Only one of TEMP(MAT) or TEMP(INIT) is allowed in any model. TEMP(MAT), TEMP(LOAD), and TEMP(BOTH) can point to a heat transfer subcase or TEMP/TEMPD. TEMP(INIT) cannot be used to reference a Heat Transfer Subcase.
  5. Static and thermal loads should have unique set identification numbers.
  6. In linear static analysis, temperature strains and material properties are calculated as: 2(1)
    ε T = A ( T ) ( T F i n a l T I n i t i a l )

    Material properties are also calculated based on their corresponding temperature-dependency (wherever applicable).

    Where,
    • A ( T F i n a l ) MathType@MTEF@5@5@+= feaagKart1ev2aqatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn hiov2DGi1BTfMBaeXatLxBI9gBaerbd9wDYLwzYbItLDharqqtubsr 4rNCHbGeaGqiVu0Je9sqqrpepC0xbbL8F4rqqrFfpeea0xe9Lq=Jc9 vqaqpepm0xbba9pwe9Q8fs0=yqaqpepae9pg0FirpepeKkFr0xfr=x fr=xb9adbaqaaeGaciGaaiaabeqaamaabaabaaGcbaGaamyqaiaacI cacaWGubWaaSbaaSqaaiaadAeacaWGPbGaamOBaiaadggacaWGSbaa beaakiaacMcaaaa@3DA8@ is the thermal expansion coefficient. The value of A ( T F i n a l ) MathType@MTEF@5@5@+= feaagKart1ev2aqatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn hiov2DGi1BTfMBaeXatLxBI9gBaerbd9wDYLwzYbItLDharqqtubsr 4rNCHbGeaGqiVu0Je9sqqrpepC0xbbL8F4rqqrFfpeea0xe9Lq=Jc9 vqaqpepm0xbba9pwe9Q8fs0=yqaqpepae9pg0FirpepeKkFr0xfr=x fr=xb9adbaqaaeGaciGaaiaabeqaamaabaabaaGcbaGaamyqaiaacI cacaWGubWaaSbaaSqaaiaadAeacaWGPbGaamOBaiaadggacaWGSbaa beaakiaacMcaaaa@3DA8@ and temperature-dependent material properties can be defined via the MATi or MATTi Bulk Data Entries depending on whether temperature-dependent material are used. Temperature-dependent material are used if TEMP(BOTH), TEMP(MAT), or TEMP(INIT) are specified in conjunction with MATTi entries. If more than one or all three of TEMP(BOTH/MAT/INIT) are specified, then OptiStruct picks one of them for material update based on the following priority.

      TEMP(BOTH/MAT) have precedence over TEMP(INIT). If both TEMP(BOTH) and TEMP(MAT) are present, then the last one is used for material update.

      If none of TEMP(BOTH/MAT/INIT) are specified, then the MATi material properties are used.

    • T F i n a l MathType@MTEF@5@5@+= feaagKart1ev2aqatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn hiov2DGi1BTfMBaeXatLxBI9gBaerbd9wDYLwzYbItLDharqqtubsr 4rNCHbGeaGqiVu0Je9sqqrpepC0xbbL8F4rqqrFfpeea0xe9Lq=Jc9 vqaqpepm0xbba9pwe9Q8fs0=yqaqpepae9pg0FirpepeKkFr0xfr=x fr=xb9adbaqaaeGaciGaaiaabeqaamaabaabaaGcbaGaamivamaaBa aaleaacaWGgbGaamyAaiaad6gacaWGHbGaamiBaaqabaaaaa@3B7F@ is the load temperature defined by TEMP(LOAD) or TEMP(BOTH). If both TEMP(BOTH) and TEMP(LOAD) are present, then OptiStruct picks the last one for the load temperature. TEMP(BOTH) and TEMP(LOAD) can be specified within the subcase in multiple subcases. In such situations, the load temperature can vary for each subcase depending on the entries specified within, and as mentioned previously, the last entry in each subcase will determine the load temperature for that particular subcase.
    • T I n i t i a l MathType@MTEF@5@5@+= feaagKart1ev2aqatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn hiov2DGi1BTfMBaeXatLxBI9gBaerbd9wDYLwzYbItLDharqqtubsr 4rNCHbGeaGqiVu0Je9sqqrpepC0xbbL8F4rqqrFfpeea0xe9Lq=Jc9 vqaqpepm0xbba9pwe9Q8fs0=yqaqpepae9pg0FirpepeKkFr0xfr=x fr=xb9adbaqaaeGaciGaaiaabeqaamaabaabaaGcbaGaamivamaaBa aaleaacaWGjbGaamOBaiaadMgacaWG0bGaamyAaiaadggacaWGSbaa beaaaaa@3D69@ is the initial temperature defined by TEMP(INIT) or TREF (TREF field on MATi). TEMP(INIT) has precedence over TREF. If TEMP(INIT) is not specified, then TREF is used for the initial temperature.
    • SYSSETTING, TLOADMAT can be used to activate TEMP(LOAD) for material update instead of TEMP(MAT/INIT). It can also be used to deactivate thermal loading in structural analysis.
  7. In nonlinear static analysis, temperature strains and material properties are calculated as: 3
    If PARAM, THMLSTN, 0 (Default)(2)
    ε T = A ( T F i n a l ) ( T F i n a l T I n i t i a l ) MathType@MTEF@5@5@+= feaagKart1ev2aaatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn hiov2DGi1BTfMBaeXatLxBI9gBaebbnrfifHhDYfgasaacH8srps0l bbf9q8WrFfeuY=Hhbbf9v8qqaqFr0xc9pk0xbba9q8WqFfea0=yr0R Yxir=Jbba9q8aq0=yq=He9q8qqQ8frFve9Fve9Ff0dmeaabaqaciGa caGaaeqabaqaaeaadaaakeaacqaH1oqzdaWgaaWcbaGaamivaaqaba GccqGH9aqpcaWGbbWaaeWaaeaacaWGubWaaSbaaSqaaiaadAeacaWG PbGaamOBaiaadggacaWGSbaabeaaaOGaayjkaiaawMcaamaabmaaba GaamivamaaBaaaleaacaWGgbGaamyAaiaad6gacaWGHbGaamiBaaqa baGccqGHsislcaWGubWaaSbaaSqaaiaadMeacaWGUbGaamyAaiaads hacaWGPbGaamyyaiaadYgaaeqaaaGccaGLOaGaayzkaaaaaa@4CDB@
    Or, if PARAM, THMLSTN, 1(3)
    ε T = A ( T F i n a l ) ( T F i n a l T R e f ) A ( T I n i t i a l ) ( T I n i t i a l T r e f ) MathType@MTEF@5@5@+= feaagKart1ev2aaatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn hiov2DGi1BTfMBaeXatLxBI9gBaebbnrfifHhDYfgasaacH8srps0l bbf9q8WrFfeuY=Hhbbf9v8qqaqFr0xc9pk0xbba9q8WqFfea0=yr0R Yxir=Jbba9q8aq0=yq=He9q8qqQ8frFve9Fve9Ff0dmeaabaqaciGa caGaaeqabaqaaeaadaaakeaacqaH1oqzdaWgaaWcbaGaamivaaqaba GccqGH9aqpcaWGbbWaaeWaaeaacaWGubWaaSbaaSqaaiaadAeacaWG PbGaamOBaiaadggacaWGSbaabeaaaOGaayjkaiaawMcaamaabmaaba GaamivamaaBaaaleaacaWGgbGaamyAaiaad6gacaWGHbGaamiBaaqa baGccqGHsislcaWGubWaaSbaaSqaaiaadkfacaWGLbGaamOzaaqaba aakiaawIcacaGLPaaacqGHsislcaWGbbWaaeWaaeaacaWGubWaaSba aSqaaiaadMeacaWGUbGaamyAaiaadshacaWGPbGaamyyaiaadYgaae qaaaGccaGLOaGaayzkaaWaaeWaaeaacaWGubWaaSbaaSqaaiaadMea caWGUbGaamyAaiaadshacaWGPbGaamyyaiaadYgaaeqaaOGaeyOeI0 IaamivamaaBaaaleaacaWGYbGaamyzaiaadAgaaeqaaaGccaGLOaGa ayzkaaaaaa@619F@

    Material properties are also calculated based on their corresponding temperature-dependency (wherever applicable).

    Where,
    • A ( T F i n a l ) MathType@MTEF@5@5@+= feaagKart1ev2aqatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn hiov2DGi1BTfMBaeXatLxBI9gBaerbd9wDYLwzYbItLDharqqtubsr 4rNCHbGeaGqiVu0Je9sqqrpepC0xbbL8F4rqqrFfpeea0xe9Lq=Jc9 vqaqpepm0xbba9pwe9Q8fs0=yqaqpepae9pg0FirpepeKkFr0xfr=x fr=xb9adbaqaaeGaciGaaiaabeqaamaabaabaaGcbaGaamyqaiaacI cacaWGubWaaSbaaSqaaiaadAeacaWGPbGaamOBaiaadggacaWGSbaa beaakiaacMcaaaa@3DA8@ is the thermal expansion coefficient. The value of A(T) and and temperature-dependent material properties can be defined via the MATi or MATTi Bulk Data Entries depending on whether temperature-dependent material are used. Temperature-dependent material is used if TEMP(LOAD) is specified in conjunction with MATTi entries. If TEMP(LOAD) is not specified, then TEMP(INIT) is used. If neither TEMP(LOAD) or TEMP(INIT) are specified then the MATi material properties are used.
    • T F i n a l MathType@MTEF@5@5@+= feaagKart1ev2aqatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn hiov2DGi1BTfMBaeXatLxBI9gBaerbd9wDYLwzYbItLDharqqtubsr 4rNCHbGeaGqiVu0Je9sqqrpepC0xbbL8F4rqqrFfpeea0xe9Lq=Jc9 vqaqpepm0xbba9pwe9Q8fs0=yqaqpepae9pg0FirpepeKkFr0xfr=x fr=xb9adbaqaaeGaciGaaiaabeqaamaabaabaaGcbaGaamivamaaBa aaleaacaWGgbGaamyAaiaad6gacaWGHbGaamiBaaqabaaaaa@3B7F@ is the load temperature defined by TEMP(LOAD). TEMP(LOAD) can be specified within the subcase in multiple subcases. In such situations, the load temperature can vary for each subcase depending on the entries specified within, and the last entry in each subcase will determine the load temperature for that particular subcase.
    • T I n i t i a l MathType@MTEF@5@5@+= feaagKart1ev2aqatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn hiov2DGi1BTfMBaeXatLxBI9gBaerbd9wDYLwzYbItLDharqqtubsr 4rNCHbGeaGqiVu0Je9sqqrpepC0xbbL8F4rqqrFfpeea0xe9Lq=Jc9 vqaqpepm0xbba9pwe9Q8fs0=yqaqpepae9pg0FirpepeKkFr0xfr=x fr=xb9adbaqaaeGaciGaaiaabeqaamaabaabaaGcbaGaamivamaaBa aaleaacaWGjbGaamOBaiaadMgacaWG0bGaamyAaiaadggacaWGSbaa beaaaaa@3D69@ is the initial temperature defined by TEMP(INIT), TREF (TREF field on MATi), or TEMPT entry. TEMP(INIT) has precedence over TREF and TEMPT entry. If TEMP(INIT) is not specified:
      • In a model with subcase continuation, the initial temperature is determined by the first subcase in the series. The determination follows the following rules.
        • For nonlinear static subcases with TEMP(LOAD,TEMPT), the temperature field corresponding to HTINI defined in the TEMPT entry is used as the initial temperature field.
        • If TEMPT format is not used, then TREF is used for the initial temperature.
      • Otherwise, TREF is used for the intial temperature.
    • TEMP(MAT), TEMP(BOTH) cannot be used in Nonlinear Static Analysis subcases. OptiStruct will error out, if they are specified inside Nonlinear Static Analysis subcases. If TEMP(MAT) or TEMP(BOTH) are specified outside Nonlinear Static Subcases (either globally or in subcases of other solution sequences), then TEMP(LOAD) should be defined inside the Nonlinear Static Subcases in the model.
  8. In versions prior to OptiStruct 8.0, thermal loads were selected in the Subcase Information section using the LOAD data selector. In version 8.0, the TEMPERATURE data selector was added to perform this function. It is possible to revert to the old behavior mode by setting the LOADTEMP option to SHAREID in the Configuration File.
  9. For Linear Static Subcase, TEMP(LOAD), TEMP(BOTH), or TEMP(MAT) can point to a heat transfer subcase or TSTRU ID. The temperature field from a steady-state heat transfer analysis or at the final time step of a transient heat transfer analysis will be used. When TEMP(LOAD) or TEMP(BOTH) points to a transient heat transfer subcase or TSTRU ID, TIME= ALL can be used to select temperature fields at all time steps for coupled thermal structural analysis. HTIME= ALL cannot be defined in TEMP(INIT) or TEMP(MAT) entry. For more information, refer to One Step Transient Thermal Stress Analysis.
  10. For Nonlinear Static Subcase, TEMP(LOAD) can point to heat transfer subcase. The temperature field from a steady-state heat transfer analysis will be used to update thermal loading and temperature-dependent material properties. If TEMP(LOAD) points to transient thermal subcase from Nonlinear Static Subcase, then HTIME= ALL can be used to select temperature fields at all time steps for coupled thermal structural analysis. HTIME=ALL cannot be defined in the TEMP(INIT) entry. For more information, refer to One Step Transient Thermal Stress Analysis.
  11. For Nonlinear One Step Transient Thermal Stress Analysis, a more flexible definition on thermal load can be used by the combination of TEMP(LOAD) and flag TEMPT. In this format, the thermal load can be read from either an external file (HFILE) or an internal transient thermal analysis (HSUB). In this case, grid temperature values at different time steps are predefined and mapped to the current nonlinear structural analysis. The mapping rule is defined in TEMPT card. The referenced TEMPT card ID is defined in SUBTYPE.
  12. In nonlinear analysis, the thermal expansion coefficient A ( T ) MathType@MTEF@5@5@+= feaagKart1ev2aqatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn hiov2DGi1BTfMBaeXatLxBI9gBaerbd9wDYLwzYbItLDharqqtubsr 4rNCHbGeaGqiVu0Je9sqqrpepC0xbbL8F4rqqrFfpeea0xe9Lq=Jc9 vqaqpepm0xbba9pwe9Q8fs0=yqaqpepae9pg0FirpepeKkFr0xfr=x fr=xb9adbaqaaeGaciGaaiaabeqaamaabaabaaGcbaGaamyqamaabm aabaGaamivaaGaayjkaiaawMcaaaaa@391F@ is a secant value. You can obtain its value from the instantaneous thermal expansion coefficient using:(4)
    A ( T ) = 1 ( T T i n i ) T i n i T α ( T ) d T MathType@MTEF@5@5@+= feaagKart1ev2aqatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn hiov2DGi1BTfMBaeXatLxBI9gBaerbd9wDYLwzYbItLDharqqtubsr 4rNCHbGeaGqiVu0Je9sqqrpepC0xbbL8F4rqqrFfpeea0xe9Lq=Jc9 vqaqpepm0xbba9pwe9Q8fs0=yqaqpepae9pg0FirpepeKkFr0xfr=x fr=xb9adbaqaaeGaciGaaiaabeqaamaabaabaaGcbaGaamyqamaabm aabaGaamivaaGaayjkaiaawMcaaiabg2da9maalaaabaGaaGymaaqa amaabmaabaGaamivaiabgkHiTiaadsfadaWgaaWcbaGaamyAaiaad6 gacaWGPbaabeaaaOGaayjkaiaawMcaaaaadaWdXbqaaiabeg7aHnaa bmaabaGaamivaaGaayjkaiaawMcaaiaadsgacaWGubaaleaacaWGub WaaSbaaWqaaiaadMgacaWGUbGaamyAaaqabaaaleaacaWGubaaniab gUIiYdaaaa@4F02@
    Where,
    T i n i MathType@MTEF@5@5@+= feaagKart1ev2aqatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn hiov2DGi1BTfMBaeXatLxBI9gBaerbd9wDYLwzYbItLDharqqtubsr 4rNCHbGeaGqiVu0Je9sqqrpepC0xbbL8F4rqqrFfpeea0xe9Lq=Jc9 vqaqpepm0xbba9pwe9Q8fs0=yqaqpepae9pg0FirpepeKkFr0xfr=x fr=xb9adbaqaaeGaciGaaiaabeqaamaabaabaaGcbaGaamivamaaBa aaleaacaWGPbGaamOBaiaadMgaaeqaaaaa@39CB@
    Initial temperature.
    α ( T ) MathType@MTEF@5@5@+= feaagKart1ev2aqatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn hiov2DGi1BTfMBaeXatLxBI9gBaerbd9wDYLwzYbItLDharqqtubsr 4rNCHbGeaGqiVu0Je9sqqrpepC0xbbL8F4rqqrFfpeea0xe9Lq=Jc9 vqaqpepm0xbba9pwe9Q8fs0=yqaqpepae9pg0FirpepeKkFr0xfr=x fr=xb9adbaqaaeGaciGaaiaabeqaamaabaabaaGcbaGaeqySde2aae WaaeaacaWGubaacaGLOaGaayzkaaaaaa@39F8@
    Instantaneous thermal expansion coefficient.
    A ( T ) MathType@MTEF@5@5@+= feaagKart1ev2aqatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn hiov2DGi1BTfMBaeXatLxBI9gBaerbd9wDYLwzYbItLDharqqtubsr 4rNCHbGeaGqiVu0Je9sqqrpepC0xbbL8F4rqqrFfpeea0xe9Lq=Jc9 vqaqpepm0xbba9pwe9Q8fs0=yqaqpepae9pg0FirpepeKkFr0xfr=x fr=xb9adbaqaaeGaciGaaiaabeqaamaabaabaaGcbaGaamyqamaabm aabaGaamivaaGaayjkaiaawMcaaaaa@391F@
    Secant thermal expansion coefficient at temperature T MathType@MTEF@5@5@+= feaagKart1ev2aaatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn hiov2DGi1BTfMBaeXatLxBI9gBaerbd9wDYLwzYbItLDharqqtubsr 4rNCHbGeaGqiVu0Je9sqqrpepC0xbbL8F4rqqrFfpeea0xe9Lq=Jc9 vqaqpepm0xbba9pwe9Q8fs0=yqaqpepae9pg0FirpepeKkFr0xfr=x fr=xb9adbaqaaeGaciGaaiaabeqaamaabaabaaGcbaGaamivaaaa@36CF@ . This is used by OptiStruct.
    When PARAM,THMLSTN,1 is specified, the secant thermal expansion coefficient can be obtained by:(5)
    A ( T ) = 1 ( T T r e f ) T i n i T α ( T ) d T + A ( T i n i ) T i n i T r e f T T r e f MathType@MTEF@5@5@+= feaagKart1ev2aqatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn hiov2DGi1BTfMBaeXatLxBI9gBaerbd9wDYLwzYbItLDharqqtubsr 4rNCHbGeaGqiVu0Je9sqqrpepC0xbbL8F4rqqrFfpeea0xe9Lq=Jc9 vqaqpepm0xbba9pwe9Q8fs0=yqaqpepae9pg0FirpepeKkFr0xfr=x fr=xb9adbaqaaeGaciGaaiaabeqaamaabaabaaGcbaGaamyqamaabm aabaGaamivaaGaayjkaiaawMcaaiabg2da9maalaaabaGaaGymaaqa amaabmaabaGaamivaiabgkHiTiaadsfadaWgaaWcbaGaamOCaiaadw gacaWGMbaabeaaaOGaayjkaiaawMcaaaaadaWdXbqaaiabeg7aHnaa bmaabaGaamivaaGaayjkaiaawMcaaiaadsgacaWGubaaleaacaWGub WaaSbaaWqaaiaadMgacaWGUbGaamyAaaqabaaaleaacaWGubaaniab gUIiYdGccqGHRaWkcaWGbbWaaeWaaeaacaWGubWaaSbaaSqaaiaadM gacaWGUbGaamyAaaqabaaakiaawIcacaGLPaaadaWcaaqaaiaadsfa daWgaaWcbaGaamyAaiaad6gacaWGPbaabeaakiabgkHiTiaadsfada WgaaWcbaGaamOCaiaadwgacaWGMbaabeaaaOqaaiaadsfacqGHsisl caWGubWaaSbaaSqaaiaadkhacaWGLbGaamOzaaqabaaaaaaa@6465@

    Where, T r e f MathType@MTEF@5@5@+= feaagKart1ev2aqatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn hiov2DGi1BTfMBaeXatLxBI9gBaerbd9wDYLwzYbItLDharqqtubsr 4rNCHbGeaGqiVu0Je9sqqrpepC0xbbL8F4rqqrFfpeea0xe9Lq=Jc9 vqaqpepm0xbba9pwe9Q8fs0=yqaqpepae9pg0FirpepeKkFr0xfr=x fr=xb9adbaqaaeGaciGaaiaabeqaamaabaabaaGcbaGaamivamaaBa aaleaacaWGYbGaamyzaiaadAgaaeqaaaaa@39C8@ is the reference temperature defined on the material entry.

    For the initial state, the secant thermal expansion coefficient, A( T ini )=α( T ini ) MathType@MTEF@5@5@+= feaagKart1ev2aqatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn hiov2DGi1BTfMBaeXatLxBI9gBaerbd9wDYLwzYbItLDharqqtubsr 4rNCHbGeaGqiVu0Je9sqqrpepC0xbbL8F4rqqrFfpeea0xe9Lq=Jc9 vqaqpepm0xbba9pwe9Q8fs0=yqaqpepae9pg0FirpepeKkFr0xfr=x fr=xb9adbaqaaeGaciGaaiaabeqaamaabaabaaGcbaGaamyqamaabm aabaGaamivamaaBaaaleaacaWGPbGaamOBaiaadMgaaeqaaaGccaGL OaGaayzkaaGaeyypa0JaeqySde2aaeWaaeaacaWGubWaaSbaaSqaai aadMgacaWGUbGaamyAaaqabaaakiaawIcacaGLPaaaaaa@4430@ .

  13. If an initial temperature (predefined outside of the subcases) is different from the temperature at the very beginning of a subcase and the resulting thermal expansion is nonzero, the thermal strain due to this temperature difference is counted.