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laws:evp-nh [2019/03/19 16:41]
chantal [Real parameters]
laws:evp-nh [2020/08/25 15:46] (current)
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 Project: continuous casting research for ARBED (RW2748)\\ Project: continuous casting research for ARBED (RW2748)\\
 ==== The model ==== ==== The model ====
-Coupled dynamic recrystallisation-thermo mechanical analysis of elasto visco plastic solids undergoing large strains.\\+Coupled dynamic recrystallisation-thermo-mechanical analysis of elasto-visco-plastic solids undergoing large strains.\\
 JAUMANN stress rate is used\\ JAUMANN stress rate is used\\
 __IANA= 2, 3, 5:__\\ __IANA= 2, 3, 5:__\\
-See report RW2748 (1, 8, 17, 24) and intermediate report of April 1998 \\+See intermediate ​report RW2748 (1, 8, 17, 24) and intermediate report of April 1998 \\
 For details on equations used in analytical compliance matrix computation,​ see appendix D of April 1998\\ For details on equations used in analytical compliance matrix computation,​ see appendix D of April 1998\\
 __IANA= 4:__\\ __IANA= 4:__\\
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 Lagamine: NHIC2E.F (IANA= 2, 3 or 5) or NHIC3D.F (IANA= 4) Lagamine: NHIC2E.F (IANA= 2, 3 or 5) or NHIC3D.F (IANA= 4)
 ==== Subroutines ==== ==== Subroutines ====
-In the following table, fill in the file (*.F) and the names of the subroutines used by the law. Generic subroutines such as ‘ANNULD’ (putting a vector to zero) or ‘MST_SOLVE’ (computing the solution to a system of linear equations) do not need to be listed here.+
 ^File^Subroutine^Description^ ^File^Subroutine^Description^
-|XXX.F| XXX|Main subroutine of the law |+|CALMAT.F | CALMAT|Computes material data at temperature T | 
 +|NHIMAT.F |CALSIGY | | 
 +|:::​|MATMSGS2|Used for analytical compliance matrix| 
 +|:::​|MATMSGL2|Used for analytical compliance matrix| 
 +|:::​|MATMSGS|Used for analytical compliance matrix (3D case)| 
 +|:::​|MATMSGL|Used for analytical compliance matrix (3D case)| 
 +|:::​|EIGVECT| Computes eigen vectors| 
 +|:::​|CMATINV| Inverse complex matrix| 
 +|:::​|VGMOYEN |Computes ​the constant velocities gradient matrix | 
 +|CALPNH.F| CALPNH|Computes $K_0, P_1, P_2, P_3, P_4$ at temperature T | 
 +|RECRYDYN.F|RECRYDYN |Dynamic recrystallization computation ​| 
 ===== Availability ===== ===== Availability =====
 |Plane stress state| NO | |Plane stress state| NO |
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 ^ If ICHP2 = 2: 1 Line repeated NTEMP2 times (6G10) \\ Note: parameters introduced by increasing temperature order^^ ^ If ICHP2 = 2: 1 Line repeated NTEMP2 times (6G10) \\ Note: parameters introduced by increasing temperature order^^
 |T| Temperature| |T| Temperature|
-|$K_0$| See X for formula+|$K_0$| See further
-|$P_1$| ​A ADAPTER+|$P_1$| ​See "​Information about EVP-NH"​
-|$P_2$| ​see 4.4 for more information|+|$P_2$| |
 |$P_3$| | |$P_3$| |
 |$P_4$| | |$P_4$| |
  
 ^ If ICHP2 ≠ 2: 2 Lines  (5G10/4G10) (**__only if nodes temperature in Kelvin !!!__**) ^^ ^ If ICHP2 ≠ 2: 2 Lines  (5G10/4G10) (**__only if nodes temperature in Kelvin !!!__**) ^^
-|$AK_0$| ​See X for formula+|$AK_0$| | 
-|$C_1$| ​A ADAPTER+|$C_1$| ​See further
-|$C_2$| ​see 4.4 for more information|+|$C_2$| ​See "​Information about EVP-NH"​|
 |$C_3$| | |$C_3$| |
 |$C_4$| | |$C_4$| |
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 $\bar{\sigma}= A. K_0. \bar{\varepsilon}^{P_4}. exp(-P_1.\bar{\varepsilon}). P_2. \sqrt{3}. (\sqrt{3}. \bar{\dot{\varepsilon}})^{P_3}$ with $P_1 \geq 0$ \\ $\bar{\sigma}= A. K_0. \bar{\varepsilon}^{P_4}. exp(-P_1.\bar{\varepsilon}). P_2. \sqrt{3}. (\sqrt{3}. \bar{\dot{\varepsilon}})^{P_3}$ with $P_1 \geq 0$ \\
 The parameters $K_0, P_1, P_2, P_3, P_4$ can be given at several temperatures (ICHP2 = 2) \\ The parameters $K_0, P_1, P_2, P_3, P_4$ can be given at several temperatures (ICHP2 = 2) \\
-Otherwise:  (ICHP2 ≠ 2) \\+Otherwise, if ICHP2 ≠ 2: (see the law in section: "​integer parameters"​) \\
 $P_1= (\frac{T}{C_1})^{C_2} + C_3$ \\ $P_1= (\frac{T}{C_1})^{C_2} + C_3$ \\
 $P_2= f(C_4, C_5, C_6, T)$ \\ $P_2= f(C_4, C_5, C_6, T)$ \\
laws/evp-nh.1553010103.txt.gz · Last modified: 2020/08/25 15:35 (external edit)