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appendices:a20 [2021/12/07 09:46]
helene [3. Extrapolation method]
appendices:a20 [2022/09/30 09:49] (current)
helene [Appendix 20: Cycle jump procedure]
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 These 2 steps are then repeated until the calculation is completed. The number of cycles to be fully calculated $N_i$ and the number of "​jumped"​ cycles $N_j$ can vary during the simulation. One can also pick the results to be extrapolated during the jump. \\ These 2 steps are then repeated until the calculation is completed. The number of cycles to be fully calculated $N_i$ and the number of "​jumped"​ cycles $N_j$ can vary during the simulation. One can also pick the results to be extrapolated during the jump. \\
 \\ \\
-The cycle jump can be performed with Lagamine ​usign the Fortran EXTRAPOL program along with the attached Python script. \\+The cycle jump can be performed with Lagamine ​using the Fortran EXTRAPOL program along with the attached Python script. ​The code is available on the [[https://​gitlab.uliege.be/​UEE/​cycle-jump|GitLab]] ​\\
 ===== Structure of the data file ===== ===== Structure of the data file =====
 The cycle jump procedure can be used on any cyclic simulation. It is launched using the Python script and requires an additional info file. \\ The cycle jump procedure can be used on any cyclic simulation. It is launched using the Python script and requires an additional info file. \\
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 ^Line 4 (2 integers)^^ ^Line 4 (2 integers)^^
 |T| Period of the loading [s]| |T| Period of the loading [s]|
-|Tmax| Final/​Maximum value of the time step (this corresponds to ALAMBF in a classic simulation)|+|Tmax| Final/​Maximum value of the time (this corresponds to ALAMBF in a classic simulation)|
 ==== 2. Definition of $N_i$ and $N_j$ ==== ==== 2. Definition of $N_i$ and $N_j$ ====
  
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 ^Line 2^^ ^Line 2^^
 |IDENT| = 0 - $N_i$ and $N_j$ are kept constant over the whole simulation and defined at the next line \\ = 1 - $N_i$ and $N_j$ are predefined by blocks. This allows for instance to have low values of $N_j$ at the begining of the simulation and higher values later once the beaviour of the structure is stabilized.| |IDENT| = 0 - $N_i$ and $N_j$ are kept constant over the whole simulation and defined at the next line \\ = 1 - $N_i$ and $N_j$ are predefined by blocks. This allows for instance to have low values of $N_j$ at the begining of the simulation and higher values later once the beaviour of the structure is stabilized.|
-|:::| ≥ 10 - User-defined calculation of $N_j$ and $N_i$ defined according to the units (= 0 for constant $N_i$, = 1 for definition by block). The calculation of $N_j$ must be implemented by the user in the EXTRAPOL program.|+|:::| ≥ 10 - User-defined calculation of $N_j$. The calculation of $N_j$ must be implemented by the user in the EXTRAPOL program. \\ $N_i$ is defined according to the units (= 0 for constant $N_i$, = 1 for definition by block).|
  
 === If IDENT % 10 = 0 === === If IDENT % 10 = 0 ===
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 === If IDENT ≥ 10 === === If IDENT ≥ 10 ===
 +See specific definitions [[appendices:​a20:​ident|here]].
 ^Line 4 or 5 (1 integer)^^ ^Line 4 or 5 (1 integer)^^
 |NPAR|Number of parameters used for the user-defined computation of $N_j$\\ ≤ 50| |NPAR|Number of parameters used for the user-defined computation of $N_j$\\ ≤ 50|
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 ^Line 2 (integer) ^^ ^Line 2 (integer) ^^
 |METHO| = 0 - All nodal values, reactions, stresses, and state variables are extrapolated linearly during the jump.| |METHO| = 0 - All nodal values, reactions, stresses, and state variables are extrapolated linearly during the jump.|
-|:::| = XX1 (X can be 0 or 1) - The elements and state variables for which one wishes a linear extrapolation during the jump are defined by the user| +|:::| = XX1 (X can be 01, or 2) - The elements and state variables for which one wishes a linear extrapolation during the jump are defined by the user \\ = XX2 (X can be 0, 1, or 2) - The elements defined on the following lines will have their variables extrapolated through a user-defined method
-|:::| = X1X (X can be 0 or 1) - The nodal points and nodal values for which one wishes a linear extrapolation during the jump are defined by the user|+|:::| = X1X (X can be 0 or 1) - The nodal points and nodal values for which one wishes a linear extrapolation during the jump are defined by the user\\ = X2X (X can be 0, 1, or 2) - The nodes defined on the following lines will have their nodal values extrapolated through a user-defined method|
 |:::| = 1XX (X can be 0 or 1) = The reactions for which one wishes a linear extrapolation during the jump are defined by the user| |:::| = 1XX (X can be 0 or 1) = The reactions for which one wishes a linear extrapolation during the jump are defined by the user|
-|:::| ≥ 200 - User-defined method of extrapolation| +|:::| > 222 - User-defined method of extrapolation| 
-=== For 0 < METHO < 200 ===+=== For 0 < METHO < 222 ===
 __If units = 1 (XX1)__ __If units = 1 (XX1)__
 ^Line 1^^ ^Line 1^^
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 |IVAR(i)| First variable of the subgroup; the variable number corresponds to its position in [[appendices:​a22|SIGVA]]| |IVAR(i)| First variable of the subgroup; the variable number corresponds to its position in [[appendices:​a22|SIGVA]]|
 |IVAR(i+1)| Last element of the subgroup \\ = 0 if subgroup consists of 1 element| |IVAR(i+1)| Last element of the subgroup \\ = 0 if subgroup consists of 1 element|
 +__If units = 2 (XX2)__
 +^Line 1^^
 +|NGR| Number of groups of elements defined.|
 +The following lines are repeated NGR times:
 +^Line 1 (3 integers)^^
 +|NelGR| Number of subgroups of elements; a subgroup of elements can consist of 1 element or multiple consecutive elements. |
 +|NelTOT| Total number of elements in the group|
 +|Nmetho| Identification number of of the user-defined extrapolation method|
 +^Line 2 - repeated NelGR times (2 integers)^^
 +|IEL(i)| First element of the subgroup|
 +|IEL(i+1)| Last element of the subgroup \\ = 0 if subgroup consists of 1 element|
  
 __If tens = 1 (X1X)__ __If tens = 1 (X1X)__
appendices/a20.1638866809.txt.gz · Last modified: 2021/12/07 09:46 by helene