Check of Modelica.Fluid.Examples.HeatExchanger.HeatExchangerSimulation
The model has the same number of unknowns and equations: 3731
Check of Modelica.Fluid.Examples.HeatExchanger.HeatExchangerSimulation successful.
| MSL410 experiment tolerance | MSL410 tightend tolerance | |
|---|---|---|
| Testrun ID | 20250225023730 | 20250224233152 |
| Simulator | Dymola | Dymola |
| Status | PASS | PASS |
| Run time | 7.75 | 8.23 |
| Workdir | D:/MSL_Nightly/Output/Testruns/Dymola/Modelica_org\Modelica.Fluid.Examples.HeatExchanger.HeatExchangerSimulation\WorkDir | D:/MSL_Nightly/Output/Testruns/Dymola/Modelica\Modelica.Fluid.Examples.HeatExchanger.HeatExchangerSimulation\WorkDir |
| MSL410 experiment tolerance | MSL410 tightend tolerance | |
|---|---|---|
| Status | PASS | PASS |
| Task runtime | 1.03 s | 1.03 s |
| Simulation time | 200.00 s | 200.00 s |
| Copy result file path | Copy result file path | |
| Open log | Open log | |
| Time Events | 2 | 2 |
| State Events | 0 | 0 |
| Jacobian evaluations | 64 | 64 |
| Integrator Steps | 160 | 218 |
| Total CPU time | 0.76 s | 0.76 s |
| CPU time Integration | 0.74 s | 0.74 s |
| CPU time Initialization | 0.02 s | 0.02 s |
check - Open log
Check of Modelica.Fluid.Examples.HeatExchanger.HeatExchangerSimulation
The model has the same number of unknowns and equations: 3731
Check of Modelica.Fluid.Examples.HeatExchanger.HeatExchangerSimulation successful.
check - Open log
Check of Modelica.Fluid.Examples.HeatExchanger.HeatExchangerSimulation
The model has the same number of unknowns and equations: 3731
Check of Modelica.Fluid.Examples.HeatExchanger.HeatExchangerSimulation successful.
translate - Open log
Translation of Modelica.Fluid.Examples.HeatExchanger.HeatExchangerSimulation
The DAE has 3731 scalar unknowns and 3731 scalar equations.
Statistics
Original Model
Number of components: 277
Variables: 2315
Constants: 56 (56 scalars)
Parameters: 345 (624 scalars)
Unknowns: 1914 (3735 scalars)
Differentiated variables: 180 scalars
Equations: 904
Nontrivial: 614
Translated Model
Constants: 1119 scalars
Free parameters: 45 scalars
Parameter depending: 292 scalars
Continuous time states: 100 scalars
Time-varying variables: 1125 scalars
Alias variables: 1834 scalars
Number of mixed real/discrete systems of equations: 0
Sizes of linear systems of equations: {2, 3, 2, 3, 2, 3, 2, 3, 2, 3, 2, 3, 2, 3, 2, 3, 2, 3, 2, 3, 2, 3, 2, 3, 2, 3, 2, 3, 2, 3, 2, 3, 2, 3, 2, 3, 2, 3, 2, 3, 2, 3, 2, 3, 2, 3, 2, 3, 2, 3, 2, 3, 2, 3, 2, 3, 2, 3, 2, 3, 2, 2, 3, 2, 2, 3, 3, 3, 2, 3, 2, 3, 2, 3, 2, 3, 2, 3, 2, 3}
Sizes after manipulation of the linear systems: {0, 2, 0, 2, 0, 2, 0, 2, 0, 2, 0, 2, 0, 2, 0, 2, 0, 2, 0, 2, 0, 2, 0, 2, 0, 2, 0, 2, 0, 2, 0, 2, 0, 2, 0, 2, 0, 2, 0, 2, 0, 2, 0, 2, 0, 2, 0, 2, 0, 2, 0, 2, 0, 2, 0, 2, 0, 2, 0, 2, 0, 0, 2, 0, 0, 2, 2, 2, 0, 2, 0, 2, 0, 2, 0, 2, 0, 2, 0, 2}
Sizes of nonlinear systems of equations: { }
Sizes after manipulation of the nonlinear systems: { }
Number of numerical Jacobians: 0
Initialization problem
Sizes of nonlinear systems of equations: {724}
Sizes after manipulation of the nonlinear systems: {160}
Sizes of simplified homotopy nonlinear systems of equations: {562}
Sizes after manipulation of the simplified homotopy nonlinear systems: {120}
Number of numerical Jacobians: 2
Settings
Advanced.StoreProtectedVariables = true
Sparse solvers enabled: false
Enabled for systems of equations: false
Number of systems sparse enough: 2.
System: size, density:
simplified homotopy initialization.nonlinear[1]: 120, 0.0316667
initialization.nonlinear[1]: 160, 0.0292188
Enable sparse solvers by setting Advanced.Translation.SparseActivate.
Selected continuous time states
Statically selected continuous time states
HEX.pipe_1.mediums[1].p
HEX.pipe_1.mediums[1].T
HEX.pipe_1.mediums[2].p
HEX.pipe_1.mediums[2].T
HEX.pipe_1.mediums[3].p
HEX.pipe_1.mediums[3].T
HEX.pipe_1.mediums[4].p
HEX.pipe_1.mediums[4].T
HEX.pipe_1.mediums[5].p
HEX.pipe_1.mediums[5].T
HEX.pipe_1.mediums[6].p
HEX.pipe_1.mediums[6].T
HEX.pipe_1.mediums[7].p
HEX.pipe_1.mediums[7].T
HEX.pipe_1.mediums[8].p
HEX.pipe_1.mediums[8].T
HEX.pipe_1.mediums[9].p
HEX.pipe_1.mediums[9].T
HEX.pipe_1.mediums[10].p
HEX.pipe_1.mediums[10].T
HEX.pipe_1.mediums[11].p
HEX.pipe_1.mediums[11].T
HEX.pipe_1.mediums[12].p
HEX.pipe_1.mediums[12].T
HEX.pipe_1.mediums[13].p
HEX.pipe_1.mediums[13].T
HEX.pipe_1.mediums[14].p
HEX.pipe_1.mediums[14].T
HEX.pipe_1.mediums[15].p
HEX.pipe_1.mediums[15].T
HEX.pipe_1.mediums[16].p
HEX.pipe_1.mediums[16].T
HEX.pipe_1.mediums[17].p
HEX.pipe_1.mediums[17].T
HEX.pipe_1.mediums[18].p
HEX.pipe_1.mediums[18].T
HEX.pipe_1.mediums[19].p
HEX.pipe_1.mediums[19].T
HEX.pipe_1.mediums[20].p
HEX.pipe_1.mediums[20].T
HEX.pipe_2.mediums[1].p
HEX.pipe_2.mediums[1].T
HEX.pipe_2.mediums[2].p
HEX.pipe_2.mediums[2].T
HEX.pipe_2.mediums[3].p
HEX.pipe_2.mediums[3].T
HEX.pipe_2.mediums[4].p
HEX.pipe_2.mediums[4].T
HEX.pipe_2.mediums[5].p
HEX.pipe_2.mediums[5].T
HEX.pipe_2.mediums[6].p
HEX.pipe_2.mediums[6].T
HEX.pipe_2.mediums[7].p
HEX.pipe_2.mediums[7].T
HEX.pipe_2.mediums[8].p
HEX.pipe_2.mediums[8].T
HEX.pipe_2.mediums[9].p
HEX.pipe_2.mediums[9].T
HEX.pipe_2.mediums[10].p
HEX.pipe_2.mediums[10].T
HEX.pipe_2.mediums[11].p
HEX.pipe_2.mediums[11].T
HEX.pipe_2.mediums[12].p
HEX.pipe_2.mediums[12].T
HEX.pipe_2.mediums[13].p
HEX.pipe_2.mediums[13].T
HEX.pipe_2.mediums[14].p
HEX.pipe_2.mediums[14].T
HEX.pipe_2.mediums[15].p
HEX.pipe_2.mediums[15].T
HEX.pipe_2.mediums[16].p
HEX.pipe_2.mediums[16].T
HEX.pipe_2.mediums[17].p
HEX.pipe_2.mediums[17].T
HEX.pipe_2.mediums[18].p
HEX.pipe_2.mediums[18].T
HEX.pipe_2.mediums[19].p
HEX.pipe_2.mediums[19].T
HEX.pipe_2.mediums[20].p
HEX.pipe_2.mediums[20].T
HEX.wall.T[1]
HEX.wall.T[2]
HEX.wall.T[3]
HEX.wall.T[4]
HEX.wall.T[5]
HEX.wall.T[6]
HEX.wall.T[7]
HEX.wall.T[8]
HEX.wall.T[9]
HEX.wall.T[10]
HEX.wall.T[11]
HEX.wall.T[12]
HEX.wall.T[13]
HEX.wall.T[14]
HEX.wall.T[15]
HEX.wall.T[16]
HEX.wall.T[17]
HEX.wall.T[18]
HEX.wall.T[19]
HEX.wall.T[20]
Finished
translate - Open log
Translation of Modelica.Fluid.Examples.HeatExchanger.HeatExchangerSimulation
The DAE has 3731 scalar unknowns and 3731 scalar equations.
Statistics
Original Model
Number of components: 277
Variables: 2315
Constants: 56 (56 scalars)
Parameters: 345 (624 scalars)
Unknowns: 1914 (3735 scalars)
Differentiated variables: 180 scalars
Equations: 904
Nontrivial: 614
Translated Model
Constants: 1119 scalars
Free parameters: 45 scalars
Parameter depending: 292 scalars
Continuous time states: 100 scalars
Time-varying variables: 1125 scalars
Alias variables: 1834 scalars
Number of mixed real/discrete systems of equations: 0
Sizes of linear systems of equations: {2, 3, 2, 3, 2, 3, 2, 3, 2, 3, 2, 3, 2, 3, 2, 3, 2, 3, 2, 3, 2, 3, 2, 3, 2, 3, 2, 3, 2, 3, 2, 3, 2, 3, 2, 3, 2, 3, 2, 3, 2, 3, 2, 3, 2, 3, 2, 3, 2, 3, 2, 3, 2, 3, 2, 3, 2, 3, 2, 3, 2, 2, 3, 2, 2, 3, 3, 3, 2, 3, 2, 3, 2, 3, 2, 3, 2, 3, 2, 3}
Sizes after manipulation of the linear systems: {0, 2, 0, 2, 0, 2, 0, 2, 0, 2, 0, 2, 0, 2, 0, 2, 0, 2, 0, 2, 0, 2, 0, 2, 0, 2, 0, 2, 0, 2, 0, 2, 0, 2, 0, 2, 0, 2, 0, 2, 0, 2, 0, 2, 0, 2, 0, 2, 0, 2, 0, 2, 0, 2, 0, 2, 0, 2, 0, 2, 0, 0, 2, 0, 0, 2, 2, 2, 0, 2, 0, 2, 0, 2, 0, 2, 0, 2, 0, 2}
Sizes of nonlinear systems of equations: { }
Sizes after manipulation of the nonlinear systems: { }
Number of numerical Jacobians: 0
Initialization problem
Sizes of nonlinear systems of equations: {724}
Sizes after manipulation of the nonlinear systems: {160}
Sizes of simplified homotopy nonlinear systems of equations: {562}
Sizes after manipulation of the simplified homotopy nonlinear systems: {120}
Number of numerical Jacobians: 2
Settings
Advanced.StoreProtectedVariables = true
Sparse solvers enabled: false
Enabled for systems of equations: false
Number of systems sparse enough: 2.
System: size, density:
simplified homotopy initialization.nonlinear[1]: 120, 0.0316667
initialization.nonlinear[1]: 160, 0.0292188
Enable sparse solvers by setting Advanced.Translation.SparseActivate.
Selected continuous time states
Statically selected continuous time states
HEX.pipe_1.mediums[1].p
HEX.pipe_1.mediums[1].T
HEX.pipe_1.mediums[2].p
HEX.pipe_1.mediums[2].T
HEX.pipe_1.mediums[3].p
HEX.pipe_1.mediums[3].T
HEX.pipe_1.mediums[4].p
HEX.pipe_1.mediums[4].T
HEX.pipe_1.mediums[5].p
HEX.pipe_1.mediums[5].T
HEX.pipe_1.mediums[6].p
HEX.pipe_1.mediums[6].T
HEX.pipe_1.mediums[7].p
HEX.pipe_1.mediums[7].T
HEX.pipe_1.mediums[8].p
HEX.pipe_1.mediums[8].T
HEX.pipe_1.mediums[9].p
HEX.pipe_1.mediums[9].T
HEX.pipe_1.mediums[10].p
HEX.pipe_1.mediums[10].T
HEX.pipe_1.mediums[11].p
HEX.pipe_1.mediums[11].T
HEX.pipe_1.mediums[12].p
HEX.pipe_1.mediums[12].T
HEX.pipe_1.mediums[13].p
HEX.pipe_1.mediums[13].T
HEX.pipe_1.mediums[14].p
HEX.pipe_1.mediums[14].T
HEX.pipe_1.mediums[15].p
HEX.pipe_1.mediums[15].T
HEX.pipe_1.mediums[16].p
HEX.pipe_1.mediums[16].T
HEX.pipe_1.mediums[17].p
HEX.pipe_1.mediums[17].T
HEX.pipe_1.mediums[18].p
HEX.pipe_1.mediums[18].T
HEX.pipe_1.mediums[19].p
HEX.pipe_1.mediums[19].T
HEX.pipe_1.mediums[20].p
HEX.pipe_1.mediums[20].T
HEX.pipe_2.mediums[1].p
HEX.pipe_2.mediums[1].T
HEX.pipe_2.mediums[2].p
HEX.pipe_2.mediums[2].T
HEX.pipe_2.mediums[3].p
HEX.pipe_2.mediums[3].T
HEX.pipe_2.mediums[4].p
HEX.pipe_2.mediums[4].T
HEX.pipe_2.mediums[5].p
HEX.pipe_2.mediums[5].T
HEX.pipe_2.mediums[6].p
HEX.pipe_2.mediums[6].T
HEX.pipe_2.mediums[7].p
HEX.pipe_2.mediums[7].T
HEX.pipe_2.mediums[8].p
HEX.pipe_2.mediums[8].T
HEX.pipe_2.mediums[9].p
HEX.pipe_2.mediums[9].T
HEX.pipe_2.mediums[10].p
HEX.pipe_2.mediums[10].T
HEX.pipe_2.mediums[11].p
HEX.pipe_2.mediums[11].T
HEX.pipe_2.mediums[12].p
HEX.pipe_2.mediums[12].T
HEX.pipe_2.mediums[13].p
HEX.pipe_2.mediums[13].T
HEX.pipe_2.mediums[14].p
HEX.pipe_2.mediums[14].T
HEX.pipe_2.mediums[15].p
HEX.pipe_2.mediums[15].T
HEX.pipe_2.mediums[16].p
HEX.pipe_2.mediums[16].T
HEX.pipe_2.mediums[17].p
HEX.pipe_2.mediums[17].T
HEX.pipe_2.mediums[18].p
HEX.pipe_2.mediums[18].T
HEX.pipe_2.mediums[19].p
HEX.pipe_2.mediums[19].T
HEX.pipe_2.mediums[20].p
HEX.pipe_2.mediums[20].T
HEX.wall.T[1]
HEX.wall.T[2]
HEX.wall.T[3]
HEX.wall.T[4]
HEX.wall.T[5]
HEX.wall.T[6]
HEX.wall.T[7]
HEX.wall.T[8]
HEX.wall.T[9]
HEX.wall.T[10]
HEX.wall.T[11]
HEX.wall.T[12]
HEX.wall.T[13]
HEX.wall.T[14]
HEX.wall.T[15]
HEX.wall.T[16]
HEX.wall.T[17]
HEX.wall.T[18]
HEX.wall.T[19]
HEX.wall.T[20]
Finished
translate - Continuous time states
- HEX.pipe_1.mediums[1].p
- HEX.pipe_1.mediums[1].T
- HEX.pipe_1.mediums[2].p
- HEX.pipe_1.mediums[2].T
- HEX.pipe_1.mediums[3].p
- HEX.pipe_1.mediums[3].T
- HEX.pipe_1.mediums[4].p
- HEX.pipe_1.mediums[4].T
- HEX.pipe_1.mediums[5].p
- HEX.pipe_1.mediums[5].T
- HEX.pipe_1.mediums[6].p
- HEX.pipe_1.mediums[6].T
- HEX.pipe_1.mediums[7].p
- HEX.pipe_1.mediums[7].T
- HEX.pipe_1.mediums[8].p
- HEX.pipe_1.mediums[8].T
- HEX.pipe_1.mediums[9].p
- HEX.pipe_1.mediums[9].T
- HEX.pipe_1.mediums[10].p
- HEX.pipe_1.mediums[10].T
- HEX.pipe_1.mediums[11].p
- HEX.pipe_1.mediums[11].T
- HEX.pipe_1.mediums[12].p
- HEX.pipe_1.mediums[12].T
- HEX.pipe_1.mediums[13].p
- HEX.pipe_1.mediums[13].T
- HEX.pipe_1.mediums[14].p
- HEX.pipe_1.mediums[14].T
- HEX.pipe_1.mediums[15].p
- HEX.pipe_1.mediums[15].T
- HEX.pipe_1.mediums[16].p
- HEX.pipe_1.mediums[16].T
- HEX.pipe_1.mediums[17].p
- HEX.pipe_1.mediums[17].T
- HEX.pipe_1.mediums[18].p
- HEX.pipe_1.mediums[18].T
- HEX.pipe_1.mediums[19].p
- HEX.pipe_1.mediums[19].T
- HEX.pipe_1.mediums[20].p
- HEX.pipe_1.mediums[20].T
- HEX.pipe_2.mediums[1].p
- HEX.pipe_2.mediums[1].T
- HEX.pipe_2.mediums[2].p
- HEX.pipe_2.mediums[2].T
- HEX.pipe_2.mediums[3].p
- HEX.pipe_2.mediums[3].T
- HEX.pipe_2.mediums[4].p
- HEX.pipe_2.mediums[4].T
- HEX.pipe_2.mediums[5].p
- HEX.pipe_2.mediums[5].T
- HEX.pipe_2.mediums[6].p
- HEX.pipe_2.mediums[6].T
- HEX.pipe_2.mediums[7].p
- HEX.pipe_2.mediums[7].T
- HEX.pipe_2.mediums[8].p
- HEX.pipe_2.mediums[8].T
- HEX.pipe_2.mediums[9].p
- HEX.pipe_2.mediums[9].T
- HEX.pipe_2.mediums[10].p
- HEX.pipe_2.mediums[10].T
- HEX.pipe_2.mediums[11].p
- HEX.pipe_2.mediums[11].T
- HEX.pipe_2.mediums[12].p
- HEX.pipe_2.mediums[12].T
- HEX.pipe_2.mediums[13].p
- HEX.pipe_2.mediums[13].T
- HEX.pipe_2.mediums[14].p
- HEX.pipe_2.mediums[14].T
- HEX.pipe_2.mediums[15].p
- HEX.pipe_2.mediums[15].T
- HEX.pipe_2.mediums[16].p
- HEX.pipe_2.mediums[16].T
- HEX.pipe_2.mediums[17].p
- HEX.pipe_2.mediums[17].T
- HEX.pipe_2.mediums[18].p
- HEX.pipe_2.mediums[18].T
- HEX.pipe_2.mediums[19].p
- HEX.pipe_2.mediums[19].T
- HEX.pipe_2.mediums[20].p
- HEX.pipe_2.mediums[20].T
- HEX.wall.T[1]
- HEX.wall.T[2]
- HEX.wall.T[3]
- HEX.wall.T[4]
- HEX.wall.T[5]
- HEX.wall.T[6]
- HEX.wall.T[7]
- HEX.wall.T[8]
- HEX.wall.T[9]
- HEX.wall.T[10]
- HEX.wall.T[11]
- HEX.wall.T[12]
- HEX.wall.T[13]
- HEX.wall.T[14]
- HEX.wall.T[15]
- HEX.wall.T[16]
- HEX.wall.T[17]
- HEX.wall.T[18]
- HEX.wall.T[19]
- HEX.wall.T[20]
translate - Continuous time states
- HEX.pipe_1.mediums[1].p
- HEX.pipe_1.mediums[1].T
- HEX.pipe_1.mediums[2].p
- HEX.pipe_1.mediums[2].T
- HEX.pipe_1.mediums[3].p
- HEX.pipe_1.mediums[3].T
- HEX.pipe_1.mediums[4].p
- HEX.pipe_1.mediums[4].T
- HEX.pipe_1.mediums[5].p
- HEX.pipe_1.mediums[5].T
- HEX.pipe_1.mediums[6].p
- HEX.pipe_1.mediums[6].T
- HEX.pipe_1.mediums[7].p
- HEX.pipe_1.mediums[7].T
- HEX.pipe_1.mediums[8].p
- HEX.pipe_1.mediums[8].T
- HEX.pipe_1.mediums[9].p
- HEX.pipe_1.mediums[9].T
- HEX.pipe_1.mediums[10].p
- HEX.pipe_1.mediums[10].T
- HEX.pipe_1.mediums[11].p
- HEX.pipe_1.mediums[11].T
- HEX.pipe_1.mediums[12].p
- HEX.pipe_1.mediums[12].T
- HEX.pipe_1.mediums[13].p
- HEX.pipe_1.mediums[13].T
- HEX.pipe_1.mediums[14].p
- HEX.pipe_1.mediums[14].T
- HEX.pipe_1.mediums[15].p
- HEX.pipe_1.mediums[15].T
- HEX.pipe_1.mediums[16].p
- HEX.pipe_1.mediums[16].T
- HEX.pipe_1.mediums[17].p
- HEX.pipe_1.mediums[17].T
- HEX.pipe_1.mediums[18].p
- HEX.pipe_1.mediums[18].T
- HEX.pipe_1.mediums[19].p
- HEX.pipe_1.mediums[19].T
- HEX.pipe_1.mediums[20].p
- HEX.pipe_1.mediums[20].T
- HEX.pipe_2.mediums[1].p
- HEX.pipe_2.mediums[1].T
- HEX.pipe_2.mediums[2].p
- HEX.pipe_2.mediums[2].T
- HEX.pipe_2.mediums[3].p
- HEX.pipe_2.mediums[3].T
- HEX.pipe_2.mediums[4].p
- HEX.pipe_2.mediums[4].T
- HEX.pipe_2.mediums[5].p
- HEX.pipe_2.mediums[5].T
- HEX.pipe_2.mediums[6].p
- HEX.pipe_2.mediums[6].T
- HEX.pipe_2.mediums[7].p
- HEX.pipe_2.mediums[7].T
- HEX.pipe_2.mediums[8].p
- HEX.pipe_2.mediums[8].T
- HEX.pipe_2.mediums[9].p
- HEX.pipe_2.mediums[9].T
- HEX.pipe_2.mediums[10].p
- HEX.pipe_2.mediums[10].T
- HEX.pipe_2.mediums[11].p
- HEX.pipe_2.mediums[11].T
- HEX.pipe_2.mediums[12].p
- HEX.pipe_2.mediums[12].T
- HEX.pipe_2.mediums[13].p
- HEX.pipe_2.mediums[13].T
- HEX.pipe_2.mediums[14].p
- HEX.pipe_2.mediums[14].T
- HEX.pipe_2.mediums[15].p
- HEX.pipe_2.mediums[15].T
- HEX.pipe_2.mediums[16].p
- HEX.pipe_2.mediums[16].T
- HEX.pipe_2.mediums[17].p
- HEX.pipe_2.mediums[17].T
- HEX.pipe_2.mediums[18].p
- HEX.pipe_2.mediums[18].T
- HEX.pipe_2.mediums[19].p
- HEX.pipe_2.mediums[19].T
- HEX.pipe_2.mediums[20].p
- HEX.pipe_2.mediums[20].T
- HEX.wall.T[1]
- HEX.wall.T[2]
- HEX.wall.T[3]
- HEX.wall.T[4]
- HEX.wall.T[5]
- HEX.wall.T[6]
- HEX.wall.T[7]
- HEX.wall.T[8]
- HEX.wall.T[9]
- HEX.wall.T[10]
- HEX.wall.T[11]
- HEX.wall.T[12]
- HEX.wall.T[13]
- HEX.wall.T[14]
- HEX.wall.T[15]
- HEX.wall.T[16]
- HEX.wall.T[17]
- HEX.wall.T[18]
- HEX.wall.T[19]
- HEX.wall.T[20]
translate - Largest NL equation system
translate - Largest NL equation system
simulate - Open log
Log-file of program ./dymosim
(generated: Tue Feb 25 03:04:16 2025)
dymosim started
... "Modelica.Fluid.Examples.HeatExchanger.HeatExchangerSimulation" simulating
... "dsin.txt" loading (dymosim input file)
... "result.mat" creating (simulation result file)
Integration started at T = 0 using integration method DASSL
(DAE multi-step solver (dassl/dasslrt of Petzold modified by Dassault Systemes))
Integration terminated successfully at T = 200
CPU-time for integration : 0.741 seconds
CPU-time for one grid interval : 0.148 milliseconds
CPU-time for initialization : 0.021 seconds
Number of result points : 5004
Number of grid points : 5001
Number of accepted steps : 160
Number of f-evaluations (dynamics) : 325
Number of crossing function evaluations : 5160
Number of Jacobian-evaluations : 64
Number of model time events : 2
Number of input time events : 0
Number of state events : 0
Number of step events : 0
Minimum integration stepsize : 4e-05
Maximum integration stepsize : 21
Maximum integration order : 5
Calling terminal section
... "dsfinal.txt" creating (final states)
SUCCESSFUL simulation of Modelica.Fluid.Examples.HeatExchanger.HeatExchangerSimulation
simulate - Open log
Log-file of program ./dymosim
(generated: Mon Feb 24 23:59:30 2025)
dymosim started
... "Modelica.Fluid.Examples.HeatExchanger.HeatExchangerSimulation" simulating
... "dsin.txt" loading (dymosim input file)
... "result.mat" creating (simulation result file)
Integration started at T = 0 using integration method DASSL
(DAE multi-step solver (dassl/dasslrt of Petzold modified by Dassault Systemes))
Integration terminated successfully at T = 200
CPU-time for integration : 0.738 seconds
CPU-time for one grid interval : 0.148 milliseconds
CPU-time for initialization : 0.021 seconds
Number of result points : 5004
Number of grid points : 5001
Number of accepted steps : 218
Number of f-evaluations (dynamics) : 446
Number of crossing function evaluations : 5218
Number of Jacobian-evaluations : 64
Number of model time events : 2
Number of input time events : 0
Number of state events : 0
Number of step events : 0
Minimum integration stepsize : 4e-05
Maximum integration stepsize : 21
Maximum integration order : 5
Calling terminal section
... "dsfinal.txt" creating (final states)
SUCCESSFUL simulation of Modelica.Fluid.Examples.HeatExchanger.HeatExchangerSimulation