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doc:user:elements:volumes:iso_hypo_materials

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doc:user:elements:volumes:iso_hypo_materials [2026/06/12 14:30] – [TmElastHypoMaterial] papeleuxdoc:user:elements:volumes:iso_hypo_materials [2026/06/12 14:43] (current) – [TmContinuousDamageEvpIsoHHypoMaterial] papeleux
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 | Thermal expansion                             |  ''THERM_EXPANSION''  |  ''TO/TM''  | | Thermal expansion                             |  ''THERM_EXPANSION''  |  ''TO/TM''  |
 | Conductivity                                  |    ''CONDUCTIVITY''   |  ''TO/TM''  | | Conductivity                                  |    ''CONDUCTIVITY''   |  ''TO/TM''  |
-| Heat capacity                                 |    ''HEAT_CAPACITY''  |  ''TO/TM''  | +| Heat Capacity                                 |    ''HEAT_CAPACITY''  |  ''TO/TM''  | 
-| Heat capacity type \\   ENTHALPY_CONSISTENT (default) necessary for high variation of HEAT_CAPACITY (phase change) \\    POINT_WISE for slow variation of HAT_CAPACITY | ''HEAT_CAPACITY_TYPE'' |  -  |+| Heat Capacity Type : \\ - ENTHALPY_CONSISTENT (default) necessary \\ for high variation of the Heat capacity (phase change) \\ - POINT_WISE for slow variation of Heat Capacity | ''HEAT_CAPACITY_TYPE'' |  -  |
 | Dissipated thermoelastic power fraction       |     ''DISSIP_TE''     |      -      | | Dissipated thermoelastic power fraction       |     ''DISSIP_TE''     |      -      |
 | Dissipated (visco)plastic power fraction (Taylor-Quinney factor)  |     ''DISSIP_TQ''     |      -      | | Dissipated (visco)plastic power fraction (Taylor-Quinney factor)  |     ''DISSIP_TQ''     |      -      |
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 :!: Thermomechanical calculation method : :!: Thermomechanical calculation method :
   * When the thermal expansion changes, an average value is computed over the time step is estimated to model this thermal expansion properly.   * When the thermal expansion changes, an average value is computed over the time step is estimated to model this thermal expansion properly.
-  * If the heat capacity changes, an average value is computed to estimate properly the energy balance. An equivalent heat capacity can be used to take into account the latent heat (= heat capacity + latent heat).+  * Heat Capacity Type allows to manage varying Heat Capacity :  
 +    * POINT_WISE : compute the Heat Capacity at T1 (soft variation of Heat Capacity only) 
 +    * ENTHALPY_CONSISTENT (default) : an average value is computed to estimate properly the energy balance. An equivalent heat capacity can be used to take into account the latent heat (= heat capacity + latent heat). Needed for fast variation of HeatCapacity (ex: solid phase changes).
  
 ---- ----
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 | Conductivity                                                                 |    ''CONDUCTIVITY''   |  ''TO/TM''  | | Conductivity                                                                 |    ''CONDUCTIVITY''   |  ''TO/TM''  |
 | Heat capacity                                                         |   ''HEAT_CAPACITY''   |  ''TO/TM''  | | Heat capacity                                                         |   ''HEAT_CAPACITY''   |  ''TO/TM''  |
 +| Heat capacity type : \\ - ENTHALPY_CONSISTENT (default) necessary \\ for high variation of the Heat capacity (phase change) \\ - POINT_WISE for slow variation of Heat Capacity       | ''HEAT_CAPACITY_TYPE'' |  -  |
 | Dissipated thermoelastic power fraction                               |     ''DISSIP_TE''     |      -      | | Dissipated thermoelastic power fraction                               |     ''DISSIP_TE''     |      -      |
 | Dissipated (visco)plastic power fraction (Taylor-Quinney factor)  |     ''DISSIP_TQ''     |      -      | | Dissipated (visco)plastic power fraction (Taylor-Quinney factor)  |     ''DISSIP_TQ''     |      -      |
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 :!: Thermomechanical calculation method : :!: Thermomechanical calculation method :
   * When the thermal expansion changes, an average value is computed over the time step is estimated to model this thermal expansion properly.   * When the thermal expansion changes, an average value is computed over the time step is estimated to model this thermal expansion properly.
-  * If the heat capacity changes, an average value is computed to estimate properly the energy balance. An equivalent heat capacity can be used to take into account the latent heat (= heat capacity + latent heat).+  * Heat Capacity Type allows to manage varying Heat Capacity :  
 +    * POINT_WISE : compute the Heat Capacity at T1 (soft variation of Heat Capacity only) 
 +    * ENTHALPY_CONSISTENT (default) : an average value is computed to estimate properly the energy balance. An equivalent heat capacity can be used to take into account the latent heat (= heat capacity + latent heat). Needed for fast variation of HeatCapacity (ex: solid phase changes).
  
 ---- ----
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 | Conductivity                                         |    ''CONDUCTIVITY''   |  ''TO/TM''  | | Conductivity                                         |    ''CONDUCTIVITY''   |  ''TO/TM''  |
 | Heat Capacity                                 |   ''HEAT_CAPACITY''   |  ''TO/TM''  | | Heat Capacity                                 |   ''HEAT_CAPACITY''   |  ''TO/TM''  |
 +| Heat Capacity Type : \\ - ENTHALPY_CONSISTENT (default) necessary \\ for high variation of the Heat capacity (phase change) \\ - POINT_WISE for slow variation of Heat Capacity | ''HEAT_CAPACITY_TYPE'' |  -  |
 | Dissipated thermoelastic power fraction                               |     ''DISSIP_TE''     |      -      | | Dissipated thermoelastic power fraction                               |     ''DISSIP_TE''     |      -      |
 | Dissipated (visco)plastic power fraction (Taylor-Quinney factor)  |     ''DISSIP_TQ''     |      -      | | Dissipated (visco)plastic power fraction (Taylor-Quinney factor)  |     ''DISSIP_TQ''     |      -      |
Line 468: Line 474:
 :!: Thermomechanical calculation method : :!: Thermomechanical calculation method :
   * When the thermal expansion changes, an average value is computed over the time step is estimated to model this thermal expansion properly.   * When the thermal expansion changes, an average value is computed over the time step is estimated to model this thermal expansion properly.
-  * If the heat capacity changes, an average value is computed to estimate properly the energy balance. An equivalent heat capacity can be used to take into account the latent heat (= heat capacity + latent heat).+  * Heat Capacity Type allows to manage varying Heat Capacity :  
 +    * POINT_WISE : compute the Heat Capacity at T1 (soft variation of Heat Capacity only) 
 +    * ENTHALPY_CONSISTENT (default) : an average value is computed to estimate properly the energy balance. An equivalent heat capacity can be used to take into account the latent heat (= heat capacity + latent heat). Needed for fast variation of HeatCapacity (ex: solid phase changes).
  
 ---- ----
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 | Conductivity                                                      |    ''CONDUCTIVITY''   |  ''TO/TM''  | | Conductivity                                                      |    ''CONDUCTIVITY''   |  ''TO/TM''  |
 | Heat Capacity                                             |   ''HEAT_CAPACITY''   |  ''TO/TM''  | | Heat Capacity                                             |   ''HEAT_CAPACITY''   |  ''TO/TM''  |
 +| Heat Capacity Type \\ - ENTHALPY_CONSISTENT (default) necessary \\ for high variation of the Heat capacity (phase change) \\ - POINT_WISE for slow variation of Heat Capacity | ''HEAT_CAPACITY_TYPE'' |  -  |
 | Dissipated thermoelastic power fraction                               |     ''DISSIP_TE''     |      -      | | Dissipated thermoelastic power fraction                               |     ''DISSIP_TE''     |      -      |
 | Dissipated (visco)plastic power fraction (Taylor-Quinney factor)  |     ''DISSIP_TQ''     |      -      | | Dissipated (visco)plastic power fraction (Taylor-Quinney factor)  |     ''DISSIP_TQ''     |      -      |
  
                                                                                                    
doc/user/elements/volumes/iso_hypo_materials.1781267444.txt.gz · Last modified: by papeleux
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