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Merge pull request #475 from fbraennstroem/master
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UoWuppertal - adding temperature plots
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@rmcdermo
rmcdermo authored Nov 30, 2023
2 parents 7256734 + 9a00fd5 commit 899c4e6
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5 changes: 3 additions & 2 deletions .github/workflows/Extinction.yml
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Expand Up @@ -127,9 +127,10 @@ jobs:
run: |
echo $GITHUB_WORKSPACE
cd $GITHUB_WORKSPACE/Extinction/FM_Burner/Computational_Results/2023/UWuppertal
python FM_Burner_plot_cmp.py
python FM_Burner_plot_cmp_Temperature.py
python FM_Burner_plot_cmp_RadiantPower.py
python FM_Burner_plot_cmp_RadiativeFraction_Chi.py
python FM_Burner_plot_cmp_Transient.py
python FM_Burner_plot_cmp_WallRadiation.py
# Step 2: push the plots to the releases page
- name: Push UWuppertal Results to release
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83 changes: 0 additions & 83 deletions Extinction/FM_Burner/Computational_Results/2023/UWuppertal/FM_Burner_cmp_config.csv
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96 changes: 96 additions & 0 deletions ...ion/FM_Burner/Computational_Results/2023/UWuppertal/FM_Burner_cmp_config_RadiantPower.csv
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29 changes: 29 additions & 0 deletions ...rner/Computational_Results/2023/UWuppertal/FM_Burner_cmp_config_RadiativeFraction_Chi.csv
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Exp_Filename ,Exp_Header_Row,Exp_Data_Row,Exp_x_Col_Name ,Exp_y_Col_Name ,Exp_Data_Label,Exp_Marker_Style,Exp_Line_Style,Exp_Line_Width,Cmp_Filename ,Cmp_Header_Row,Cmp_Data_Row,Cmp_x_Col_Name ,Cmp_y_Col_Name ,Cmp_Data_Label,Cmp_Line_Style,Plot_Title ,Plot_x_Label ,Plot_y_Label ,Plot_x_Min,Plot_x_Max,Plot_y_Min,Plot_y_Max,Plot_Flip_Axis,Plot_Legend_Location,Plot_Filename
Radiation_global/Radiant_fraction2.csv ,1,2,Time ,20p9 percent ,Exp , ,- ,2,v1_FM_15cm_Burner_C2H4_20p9_5mm_chir.csv,1,2,Time ,Chi_r ,v1 ,- ,Radiant Fraction; 21 % O$_2$ ,Time (s) ,Radiant Fraction ,0,200,0.2,0.4, ,lower right ,Chi_v1_v2_v3_v4_t0_200.pdf
Radiation_global/Radiant_fraction2.csv ,1,2,Time ,20p9 percent ,Exp , ,- ,2,v2_FM_15cm_Burner_C2H4_20p9_5mm_chir.csv,1,2,Time ,Chi_r ,v2 ,-- ,Radiant Fraction; 21 % O$_2$ ,Time (s) ,Radiant Fraction ,0,200,0.2,0.4, ,lower right ,Chi_v1_v2_v3_v4_t0_200.pdf
Radiation_global/Radiant_fraction2.csv ,1,2,Time ,20p9 percent ,Exp , ,- ,2,v3_FM_15cm_Burner_C2H4_20p9_5mm_chir.csv,1,2,Time ,Chi_r ,v3 ,-. ,Radiant Fraction; 21 % O$_2$ ,Time (s) ,Radiant Fraction ,0,200,0.2,0.4, ,lower right ,Chi_v1_v2_v3_v4_t0_200.pdf
Radiation_global/Radiant_fraction2.csv ,1,2,Time ,20p9 percent ,Exp , ,- ,2,v4_FM_15cm_Burner_C2H4_20p9_5mm_chir.csv,1,2,Time ,Chi_r ,v4 ,: ,Radiant Fraction; 21 % O$_2$ ,Time (s) ,Radiant Fraction ,0,200,0.2,0.4, ,lower right ,Chi_v1_v2_v3_v4_t0_200.pdf

Radiation_global/Radiant_fraction2.csv ,1,2,Time ,20p9 percent ,Exp , ,- ,2,v1_FM_15cm_Burner_C2H4_20p9_5mm_chir.csv,1,2,Time ,Chi_r ,v1 ,- ,Radiant Fraction; 21 % O$_2$ ,Time (s) ,Radiant Fraction ,10,200,0.2,0.4, ,lower right ,Chi_v1_v2_v3_v4_t10_200.pdf
Radiation_global/Radiant_fraction2.csv ,1,2,Time ,20p9 percent ,Exp , ,- ,2,v2_FM_15cm_Burner_C2H4_20p9_5mm_chir.csv,1,2,Time ,Chi_r ,v2 ,-- ,Radiant Fraction; 21 % O$_2$ ,Time (s) ,Radiant Fraction ,10,200,0.2,0.4, ,lower right ,Chi_v1_v2_v3_v4_t10_200.pdf
Radiation_global/Radiant_fraction2.csv ,1,2,Time ,20p9 percent ,Exp , ,- ,2,v3_FM_15cm_Burner_C2H4_20p9_5mm_chir.csv,1,2,Time ,Chi_r ,v3 ,-. ,Radiant Fraction; 21 % O$_2$ ,Time (s) ,Radiant Fraction ,10,200,0.2,0.4, ,lower right ,Chi_v1_v2_v3_v4_t10_200.pdf
Radiation_global/Radiant_fraction2.csv ,1,2,Time ,20p9 percent ,Exp , ,- ,2,v4_FM_15cm_Burner_C2H4_20p9_5mm_chir.csv,1,2,Time ,Chi_r ,v4 ,: ,Radiant Fraction; 21 % O$_2$ ,Time (s) ,Radiant Fraction ,10,200,0.2,0.4, ,lower right ,Chi_v1_v2_v3_v4_t10_200.pdf

Radiation_global/Radiant_fraction2.csv ,1,2,Time ,20p9 percent ,Exp , ,- ,2,v1_FM_15cm_Burner_C2H4_20p9_5mm_chir.csv,1,2,Time ,Chi_r ,v1 ,- ,Radiant Fraction; 21 % O$_2$ ,Time (s) ,Radiant Fraction ,10,20,0.2,0.4, ,lower right ,Chi_v1_v2_v3_v4_t10_20.pdf
Radiation_global/Radiant_fraction2.csv ,1,2,Time ,20p9 percent ,Exp , ,- ,2,v2_FM_15cm_Burner_C2H4_20p9_5mm_chir.csv,1,2,Time ,Chi_r ,v2 ,-- ,Radiant Fraction; 21 % O$_2$ ,Time (s) ,Radiant Fraction ,10,20,0.2,0.4, ,lower right ,Chi_v1_v2_v3_v4_t10_20.pdf
Radiation_global/Radiant_fraction2.csv ,1,2,Time ,20p9 percent ,Exp , ,- ,2,v3_FM_15cm_Burner_C2H4_20p9_5mm_chir.csv,1,2,Time ,Chi_r ,v3 ,-. ,Radiant Fraction; 21 % O$_2$ ,Time (s) ,Radiant Fraction ,10,20,0.2,0.4, ,lower right ,Chi_v1_v2_v3_v4_t10_20.pdf
Radiation_global/Radiant_fraction2.csv ,1,2,Time ,20p9 percent ,Exp , ,- ,2,v4_FM_15cm_Burner_C2H4_20p9_5mm_chir.csv,1,2,Time ,Chi_r ,v4 ,: ,Radiant Fraction; 21 % O$_2$ ,Time (s) ,Radiant Fraction ,10,20,0.2,0.4, ,lower right ,Chi_v1_v2_v3_v4_t10_20.pdf


Radiation_global/Radiant_fraction2.csv ,1,2,Time ,20p9 percent ,Exp , ,- ,2,v4_FM_15cm_Burner_C2H4_20p9_5mm_chir.csv,1,2,Time ,Chi_r ,v4 ,- ,Radiant Fraction; 21 % O$_2$ ,Time (s) ,Radiant Fraction ,0,200,0.2,0.4, ,lower right ,Chi_v4_v7_v10_t0_200.pdf
Radiation_global/Radiant_fraction2.csv ,1,2,Time ,20p9 percent ,Exp , ,- ,2,v10_FM_15cm_Burner_C2H4_20p9_5mm_chir.csv,1,2,Time ,Chi_r ,v10 ,-- ,Radiant Fraction; 21 % O$_2$ ,Time (s) ,Radiant Fraction ,0,200,0.2,0.4, ,lower right ,Chi_v4_v7_v10_t0_200.pdf
Radiation_global/Radiant_fraction2.csv ,1,2,Time ,20p9 percent ,Exp , ,- ,2,v7_FM_15cm_Burner_C2H4_20p9_5mm_chir.csv,1,2,Time ,Chi_r ,v7 ,-. ,Radiant Fraction; 21 % O$_2$ ,Time (s) ,Radiant Fraction ,0,200,0.2,0.4, ,lower right ,Chi_v4_v7_v10_t0_200.pdf

Radiation_global/Radiant_fraction2.csv ,1,2,Time ,20p9 percent ,Exp , ,- ,2,v4_FM_15cm_Burner_C2H4_20p9_5mm_chir.csv,1,2,Time ,Chi_r ,v4 ,- ,Radiant Fraction; 21 % O$_2$ ,Time (s) ,Radiant Fraction ,10,20,0.2,0.4, ,lower right ,Chi_v4_v7_v10_t10_20.pdf
Radiation_global/Radiant_fraction2.csv ,1,2,Time ,20p9 percent ,Exp , ,- ,2,v10_FM_15cm_Burner_C2H4_20p9_5mm_chir.csv,1,2,Time ,Chi_r ,v10 ,-- ,Radiant Fraction; 21 % O$_2$ ,Time (s) ,Radiant Fraction ,10,20,0.2,0.4, ,lower right ,Chi_v4_v7_v10_t10_20.pdf
Radiation_global/Radiant_fraction2.csv ,1,2,Time ,20p9 percent ,Exp , ,- ,2,v7_FM_15cm_Burner_C2H4_20p9_5mm_chir.csv,1,2,Time ,Chi_r ,v7 ,-. ,Radiant Fraction; 21 % O$_2$ ,Time (s) ,Radiant Fraction ,10,20,0.2,0.4, ,lower right ,Chi_v4_v7_v10_t10_20.pdf

Radiation_global/Radiant_fraction2.csv ,1,2,Time ,20p9 percent ,Exp , ,- ,2,v4_FM_15cm_Burner_C2H4_20p9_5mm_chir.csv,1,2,Time ,Chi_r ,v4 ,- ,Radiant Fraction; 21 % O$_2$ ,Time (s) ,Radiant Fraction ,10,20,0.2,0.4, ,lower right ,Chi_v4_v7_v10_v14_t10_20.pdf
Radiation_global/Radiant_fraction2.csv ,1,2,Time ,20p9 percent ,Exp , ,- ,2,v10_FM_15cm_Burner_C2H4_20p9_5mm_chir.csv,1,2,Time ,Chi_r ,v10 ,-- ,Radiant Fraction; 21 % O$_2$ ,Time (s) ,Radiant Fraction ,10,20,0.2,0.4, ,lower right ,Chi_v4_v7_v10_v14_t10_20.pdf
Radiation_global/Radiant_fraction2.csv ,1,2,Time ,20p9 percent ,Exp , ,- ,2,v7_FM_15cm_Burner_C2H4_20p9_5mm_chir.csv,1,2,Time ,Chi_r ,v7 ,-. ,Radiant Fraction; 21 % O$_2$ ,Time (s) ,Radiant Fraction ,10,20,0.2,0.4, ,lower right ,Chi_v4_v7_v10_v14_t10_20.pdf
Radiation_global/Radiant_fraction2.csv ,1,2,Time ,20p9 percent ,Exp , ,- ,2,v14_FM_15cm_Burner_C2H4_20p9_5mm_chir.csv,1,2,Time ,Chi_r ,v14 ,-. ,Radiant Fraction; 21 % O$_2$ ,Time (s) ,Radiant Fraction ,10,20,0.2,0.4, ,lower right ,Chi_v4_v7_v10_v14_t10_20.pdf
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