User talk:Ferrandm - Revision history

Ferrandm: /* All_init.f90 */

2012-08-17T14:35:39Z

‎All_init.f90

Ferrandm: /* Meso-combustor case */

2012-07-27T14:02:18Z

‎Meso-combustor case

Ferrandm: /* Analysis of the call-graph profile */

2012-07-27T13:24:21Z

‎Analysis of the call-graph profile

Ferrandm: /* Analysis of the call-graph profile */

2012-07-27T13:24:09Z

‎Analysis of the call-graph profile

Ferrandm: /* Analysis of the call-graph profile */

2012-07-27T13:20:41Z

‎Analysis of the call-graph profile

Ferrandm: /* Analysis of the call-graph profile */

2012-07-27T13:10:40Z

‎Analysis of the call-graph profile

Ferrandm: /* Analysis of the call-graph profile */

2012-07-27T10:19:40Z

‎Analysis of the call-graph profile

Ferrandm: /* All_post.f90 */

2012-07-27T09:38:18Z

‎All_post.f90

Ferrandm: /* All_post.f90 */

2012-07-27T09:37:01Z

‎All_post.f90

Ferrandm: /* Meso-combustor case */

2012-07-26T10:07:25Z

‎Meso-combustor case

← Older revision		Revision as of 14:35, 17 August 2012
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	The routine interpolate1 is called in order to pass a scalar from the grid S to the grid of one momentum component. Thanks to this routine, speeds are expressed on V1, V2 and V3 grids.		The routine interpolate1 is called in order to pass a scalar from the grid S to the grid of one momentum component. Thanks to this routine, speeds are expressed on V1, V2 and V3 grids.
−

	== Meso-combustor case ==		== Meso-combustor case ==

@@ Line 612: / Line 612: @@
 * communs.f90 : coordinates of the fuel and air entries centers, this file contains variables common to several files.
 * all_init_propre.f90 : this file is used to start a calculation. Twall and Twall2 allow to create a fresh gas heart surrounded with a warm gas. A linear regression is used to describe temperature closed to the wall if <math>T \leq TT</math>. The fuel and air entries are defined (radius, speed of fluids, temperature, initial mass fractions).
-* all_init_restart.f90 :  this file is used to take back a calculation from a saving file. In this file, the fuel and air entries are not defined. If you want to run the case from a save file, you have to enter the value 0 for the variable I_fresh_run (cf fort.10) and to indicate the number of the save file chosen. If you want to run the case from a save file and to modify some properties (for instance, the wall temperature), you have to enter the value 2 for the variable I_fresh_run.
+* all_init_restart.f90 :  this file is used to take back a calculation from a saving file. If you want to run the case from a save file, you have to enter the value 0 for the variable I_fresh_run (cf fort.10) and to indicate the number of the save file chosen. If you want to run the case from a save file and to modify some properties (for instance, the wall temperature), you have to enter the value 2 for the variable I_fresh_run. In this file, the fuel and air entries are not defined. Be careful, two interpolations (one before and one after the indexes buckles) are realized instead of only one. It allows to keep the mass when you restart a calculation.
 * all_solver.f90 : this file is used to solve the case ( error treatment, continuity, convection and so on). A patch of viscosity must be added.
 * fort.11 : list of variables which are post-processed.

@@ Line 507: / Line 507: @@
 ** Self : it is the amount of time that was propagated directly from the child into the current function.
 ** Children : it is the amount of time that was propagated from the child's children to the current function.
-* Remark : if the function's parents are not determined, then the term "spontaneous" is used.
+Remark : if the function's parents are not determined, then the term "spontaneous" is used.
 The number of calls from a routine to another is also available.

@@ Line 507: / Line 507: @@
 ** Self : it is the amount of time that was propagated directly from the child into the current function.
 ** Children : it is the amount of time that was propagated from the child's children to the current function.
 The number of calls from a routine to another is also available.

@@ Line 501: / Line 501: @@
 ** Self : this information corresponds to the total amount of time spent in this function.
 ** Children : it represents the total amount of time propagated into this function by its children.
-* Function's parents (functions which call the current function):
+* Function's parents (functions which call the current function, above the current function):
 ** Self : it is the amount of time that was propagated from the current function into this parent.
 ** Children : it is the amount of time that was propagated from the current function's children into this parent.
 The number of calls from a routine to another is also available.

@@ Line 497: / Line 497: @@
 The routines are indexed in decreasing order by CPU time comsumption.
-This report details the percentage of the total time that was spent in a function and its children. The total of this percentages is not equal to 100 %. For instance the % run time for the main egals 100 % because it is a routine which takes a lot of time, but the routine solving the time stepping has a run time of 97.3%. This report gives also the amount of time that was propagated from the function into another, it depends of the different viewpoints. The number of calls from a routine to another is also available.
+This report details the percentage of the total time that was spent in a function and its children. The total of this percentages is not equal to 100 %. For instance the % run time for the main egals 100 % because it is a routine which takes a lot of time, but the routine solving the time stepping has a run time of 97.3%. This report gives also the amount of time that was propagated from the function into another, it depends of the different viewpoints (as explained when the comand gprof is run):
 Figure

@@ Line 633: / Line 633: @@
 ** Nfields calculation in function of the variables :
 <math>Nfields=\sum_1^{NIn}Ndim</math>, or <math>Nfields=\sum_1^{NIn}Nsc</math>, or <math>Nfields=\sum_1^{NIn}Nfields+1</math>
-** This subroutine defines variables which can be post-processed. Check up that variables correpond to what you want. The available variables are : Pres, Temp, Rho, Rho U, Rho E, Y, U, We, Mach, Mach T, Mach P, Vel, SL, Grad T, Grad Z, Grad Y1, Div U, Rot U, e, S, FP, Z, Q, C, Visc, Dilut, Q criteria, tak, c, Epsi.
+** This subroutine defines variables which can be post-processed. Check up that variables correpond to what you want. The available variables are : Pres, Temp, Rho, Rho U, Rho E, Y, U, We, Mach, Mach T, Mach P, Vel, SL, Grad T, Grad Z, Grad Y1, Div U, Rot U, e, S, FP, Z, C, Visc, Dilut, Q criteria, tak, c, Epsi.
 * Compute Fields :
 ** Calculation of curls, vectors, scalars.

@@ Line 606: / Line 606: @@
 == All_post.f90 ==
 * Parameters : variables definition (<math>\gamma</math>, <math>\gamma -1</math>, <math>P_{atm}</math>,  XNuF_MF, XNuO_MO, YF_O, YO_O).
-* Dimensions and allocations :
+* Dimensions and allocations.
-This subroutine defines variables which can be post-processed. Check up that variables correpond to what you want. The available variables are : Pres, Temp, Rho, Rho E, Y, U, We.
 * Init Grid Derivative :
 ** Average calculation :<math>Average = \sum \dfrac {moyenne(IP,N)}{compteur}</math> &nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;&nbsp;compteur = Xend - Xstart
@@ Line 634: / Line 633: @@
 ** Nfields calculation in function of the variables :
 <math>Nfields=\sum_1^{NIn}Ndim</math>, or <math>Nfields=\sum_1^{NIn}Nsc</math>, or <math>Nfields=\sum_1^{NIn}Nfields+1</math>
 * Compute Fields :
 ** Calculation of curls, vectors, scalars.