-IBM Bow Shock (3D)
+Rayleigh-Taylor Instability (2D)
-Final Condition
-
+Final Condition and Linear Theory
+
-1D Multi-Component Reactive Shock Tube
-
References:
+1D Multi-Component Inert Shock Tube
+Reference:
P. J. Martínez Ferrer, R. Buttay, G. Lehnasch, and A. Mura, “A detailed verification procedure for compressible reactive multicomponent Navier–Stokes solvers”, Computers & Fluids, vol. 89, pp. 88–110, Jan. 2014. Accessed: Oct. 13, 2024. [Online]. Available: https://doi.org/10.1016/j.compfluid.2013.10.014
-
-H. Chen, C. Si, Y. Wu, H. Hu, and Y. Zhu, “Numerical investigation of the effect of equivalence ratio on the propagation characteristics and performance of rotating detonation engine”, Int. J. Hydrogen Energy, Mar. 2023. Accessed: Oct. 13, 2024. [Online]. Available: https://doi.org/10.1016/j.ijhydene.2023.03.190
-
Initial Condition
-
+
Results
-
+
-2D Riemann Test (2D)
-Reference:
-Chamarthi, A., & Hoffmann, N., & Nishikawa, H., & Frankel S. (2023). Implicit gradients based conservative numerical scheme for compressible flows. arXiv:2110.05461
-
+2D IBM CFL dt (2D)
-Density Initial and Final Conditions
-
+Result
+
Strong- & Weak-scaling
The Scaling case can exercise both weak- and strong-scaling. It adjusts itself depending on the number of requested ranks.
@@ -180,17 +174,6 @@
-e batch -p mypartition -N 8 -n 2 -w "01:00:00" -# "MFC Weak Scaling" \
--case-optimization -j 32 -- --scaling weak --memory 4
-Isentropic vortex problem (2D)
-
Reference:
-Coralic, V., & Colonius, T. (2014). Finite-volume Weno scheme for viscous compressible multicomponent flows. Journal of Computational Physics, 274, 95–121. https://doi.org/10.1016/j.jcp.2014.06.003
-
-
-Density
-
-
-Density Norms
-
-
Perfectly Stirred Reactor
Reference:
G. B. Skinner and G. H. Ringrose, “Ignition Delays of a Hydrogen—Oxygen—Argon Mixture at Relatively Low Temperatures”, J. Chem. Phys., vol. 42, no. 6, pp. 2190–2192, Mar. 1965. Accessed: Oct. 13, 2024. [Online]. Available: https://doi.org/10.1063/1.1696266.
@@ -201,69 +184,86 @@
+ Cantera: 5.130e-05 s
+ (Che)MFC: 5.130e-05 s
This figure shows the isosurface with zero q-criterion.
-
-P. D. Lax, Weak solutions of nonlinear hyperbolic equations and their numerical computation, Communications on pure and applied mathematics 7 (1) (1954) 159–193.
+V. A. Titarev, E. F. Toro, Finite-volume WENO schemes for three-dimensional conservation laws, Journal of Computational Physics 201 (1) (2004) 238–260.
-
-C. W. Shu, S. Osher, Efficient implementation of essentially non-oscillatory shock-capturing schemes, Journal of Computational Physics 77 (2) (1988) 439–471. doi:10.1016/0021-9991(88)90177-5.
+
+
+1D Multi-Component Reactive Shock Tube
+References:
+P. J. Martínez Ferrer, R. Buttay, G. Lehnasch, and A. Mura, “A detailed verification procedure for compressible reactive multicomponent Navier–Stokes solvers”, Computers & Fluids, vol. 89, pp. 88–110, Jan. 2014. Accessed: Oct. 13, 2024. [Online]. Available: https://doi.org/10.1016/j.compfluid.2013.10.014
+
+
+H. Chen, C. Si, Y. Wu, H. Hu, and Y. Zhu, “Numerical investigation of the effect of equivalence ratio on the propagation characteristics and performance of rotating detonation engine”, Int. J. Hydrogen Energy, Mar. 2023. Accessed: Oct. 13, 2024. [Online]. Available: https://doi.org/10.1016/j.ijhydene.2023.03.190
-
+
Initial Condition
-
+
+
+Results
+
+
+Lid-Driven Cavity Problem (2D)
+Reference:
+Bezgin, D. A., & Buhendwa A. B., & Adams N. A. (2022). JAX-FLUIDS: A fully-differentiable high-order computational fluid dynamics solver for compressible two-phase flows. arXiv:2203.13760
+
+
+Ghia, U., & Ghia, K. N., & Shin, C. T. (1982). High-re solutions for incompressible flow using the Navier-Stokes equations and a multigrid method. Journal of Computational Physics, 48, 387-411
+
+Video: https://youtube.com/shorts/JEP28scZrBM?feature=share
+
+Final Condition
+
+
+Centerline Velocities
+
+
+Isentropic vortex problem (2D)
+Reference:
+Coralic, V., & Colonius, T. (2014). Finite-volume Weno scheme for viscous compressible multicomponent flows. Journal of Computational Physics, 274, 95–121. https://doi.org/10.1016/j.jcp.2014.06.003
+
+
+Density
+
+
+Density Norms
+
+
+2D Riemann Test (2D)
+Reference:
+Chamarthi, A., & Hoffmann, N., & Nishikawa, H., & Frankel S. (2023). Implicit gradients based conservative numerical scheme for compressible flows. arXiv:2110.05461
+
-Result
-
+Density Initial and Final Conditions
+
2D Triple Point (2D)
Reference:
@@ -273,46 +273,46 @@
Numerical Schlieren at Final Time
-Rayleigh-Taylor Instability (2D)
+Shu-Osher problem (1D)
+Reference:
+C. W. Shu, S. Osher, Efficient implementation of essentially non-oscillatory shock-capturing schemes, Journal of Computational Physics 77 (2) (1988) 439–471. doi:10.1016/0021-9991(88)90177-5.
+
-Final Condition and Linear Theory
-
-
-2D IBM CFL dt (2D)
-
+Initial Condition
+
+
Result
-
-
-Lid-Driven Cavity Problem (2D)
+
+
+Taylor-Green Vortex (3D)
Reference:
-Bezgin, D. A., & Buhendwa A. B., & Adams N. A. (2022). JAX-FLUIDS: A fully-differentiable high-order computational fluid dynamics solver for compressible two-phase flows. arXiv:2203.13760
-
-
-Ghia, U., & Ghia, K. N., & Shin, C. T. (1982). High-re solutions for incompressible flow using the Navier-Stokes equations and a multigrid method. Journal of Computational Physics, 48, 387-411
+Hillewaert, K. (2013). TestCase C3.5 - DNS of the transition of the Taylor-Green vortex, Re=1600 - Introduction and result summary. 2nd International Workshop on high-order methods for CFD.
-Video: https://youtube.com/shorts/JEP28scZrBM?feature=share
-
+
Final Condition
-
-
-Centerline Velocities
-
-
-Rayleigh-Taylor Instability (3D)
-
-Final Condition and Linear Theory
-
-
-1D Multi-Component Inert Shock Tube
+This figure shows the isosurface with zero q-criterion.
+
+
+Lax shock tube problem (1D)
Reference:
-P. J. Martínez Ferrer, R. Buttay, G. Lehnasch, and A. Mura, “A detailed verification procedure for compressible reactive multicomponent Navier–Stokes solvers”, Computers & Fluids, vol. 89, pp. 88–110, Jan. 2014. Accessed: Oct. 13, 2024. [Online]. Available: https://doi.org/10.1016/j.compfluid.2013.10.014
+P. D. Lax, Weak solutions of nonlinear hyperbolic equations and their numerical computation, Communications on pure and applied mathematics 7 (1) (1954) 159–193.
-
+
Initial Condition
-
+
+
+Result
+
+
+Gas Jet (2D)
+
+Final Condition
+
+
+Rayleigh-Taylor Instability (3D)
-Results
-
+Final Condition and Linear Theory
+
diff --git a/documentation/navtreedata.js b/documentation/navtreedata.js
index ecd61f00a..3acade095 100644
--- a/documentation/navtreedata.js
+++ b/documentation/navtreedata.js
@@ -73,70 +73,70 @@ var NAVTREE =
] ]
] ],
[ "Example Cases", "md_examples.html", [
- [ "IBM Bow Shock (3D)", "md_examples.html#autotoc_md38", [
- [ "Final Condition", "md_examples.html#autotoc_md39", null ]
+ [ "Rayleigh-Taylor Instability (2D)", "md_examples.html#autotoc_md38", [
+ [ "Final Condition and Linear Theory", "md_examples.html#autotoc_md39", null ]
] ],
- [ "1D Multi-Component Reactive Shock Tube", "md_examples.html#autotoc_md40", [
+ [ "1D Multi-Component Inert Shock Tube", "md_examples.html#autotoc_md40", [
[ "Initial Condition", "md_examples.html#autotoc_md41", null ],
[ "Results", "md_examples.html#autotoc_md42", null ]
] ],
- [ "2D Riemann Test (2D)", "md_examples.html#autotoc_md43", [
- [ "Density Initial and Final Conditions", "md_examples.html#autotoc_md44", null ]
+ [ "2D IBM CFL dt (2D)", "md_examples.html#autotoc_md43", [
+ [ "Result", "md_examples.html#autotoc_md44", null ]
] ],
[ "Strong- & Weak-scaling", "md_examples.html#autotoc_md45", [
[ "Weak Scaling", "md_examples.html#autotoc_md46", null ],
[ "Strong Scaling", "md_examples.html#autotoc_md47", null ],
[ "Example", "md_examples.html#autotoc_md48", null ]
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- [ "Density", "md_examples.html#autotoc_md50", null ],
- [ "Density Norms", "md_examples.html#autotoc_md51", null ]
+ [ "Perfectly Stirred Reactor", "md_examples.html#autotoc_md49", null ],
+ [ "IBM Bow Shock (3D)", "md_examples.html#autotoc_md50", [
+ [ "Final Condition", "md_examples.html#autotoc_md51", null ]
] ],
- [ "Perfectly Stirred Reactor", "md_examples.html#autotoc_md52", null ],
- [ "Titarev-Toro problem (1D)", "md_examples.html#autotoc_md53", [
- [ "Initial Condition", "md_examples.html#autotoc_md54", null ],
- [ "Result", "md_examples.html#autotoc_md55", null ]
+ [ "2D Hardcodied IC Example", "md_examples.html#autotoc_md52", [
+ [ "Initial Condition and Result", "md_examples.html#autotoc_md53", null ]
] ],
- [ "Gas Jet (2D)", "md_examples.html#autotoc_md56", [
- [ "Final Condition", "md_examples.html#autotoc_md57", null ]
+ [ "Shock Droplet (2D)", "md_examples.html#autotoc_md54", [
+ [ "Initial Condition", "md_examples.html#autotoc_md55", null ],
+ [ "Result", "md_examples.html#autotoc_md56", null ]
] ],
- [ "Taylor-Green Vortex (3D)", "md_examples.html#autotoc_md58", [
- [ "Final Condition", "md_examples.html#autotoc_md59", null ]
+ [ "Titarev-Toro problem (1D)", "md_examples.html#autotoc_md57", [
+ [ "Initial Condition", "md_examples.html#autotoc_md58", null ],
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] ],
- [ "2D Hardcodied IC Example", "md_examples.html#autotoc_md60", [
- [ "Initial Condition and Result", "md_examples.html#autotoc_md61", null ]
+ [ "1D Multi-Component Reactive Shock Tube", "md_examples.html#autotoc_md60", [
+ [ "Initial Condition", "md_examples.html#autotoc_md61", null ],
+ [ "Results", "md_examples.html#autotoc_md62", null ]
] ],
- [ "Shock Droplet (2D)", "md_examples.html#autotoc_md62", [
- [ "Initial Condition", "md_examples.html#autotoc_md63", null ],
- [ "Result", "md_examples.html#autotoc_md64", null ]
+ [ "Lid-Driven Cavity Problem (2D)", "md_examples.html#autotoc_md63", [
+ [ "Final Condition", "md_examples.html#autotoc_md64", null ],
+ [ "Centerline Velocities", "md_examples.html#autotoc_md65", null ]
] ],
- [ "Lax shock tube problem (1D)", "md_examples.html#autotoc_md65", [
- [ "Initial Condition", "md_examples.html#autotoc_md66", null ],
- [ "Result", "md_examples.html#autotoc_md67", null ]
+ [ "Isentropic vortex problem (2D)", "md_examples.html#autotoc_md66", [
+ [ "Density", "md_examples.html#autotoc_md67", null ],
+ [ "Density Norms", "md_examples.html#autotoc_md68", null ]
] ],
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- [ "Initial Condition", "md_examples.html#autotoc_md69", null ],
- [ "Result", "md_examples.html#autotoc_md70", null ]
+ [ "2D Riemann Test (2D)", "md_examples.html#autotoc_md69", [
+ [ "Density Initial and Final Conditions", "md_examples.html#autotoc_md70", null ]
] ],
[ "2D Triple Point (2D)", "md_examples.html#autotoc_md71", [
[ "Numerical Schlieren at Final Time", "md_examples.html#autotoc_md72", null ]
] ],
- [ "Rayleigh-Taylor Instability (2D)", "md_examples.html#autotoc_md73", [
- [ "Final Condition and Linear Theory", "md_examples.html#autotoc_md74", null ]
+ [ "Shu-Osher problem (1D)", "md_examples.html#autotoc_md73", [
+ [ "Initial Condition", "md_examples.html#autotoc_md74", null ],
+ [ "Result", "md_examples.html#autotoc_md75", null ]
] ],
- [ "2D IBM CFL dt (2D)", "md_examples.html#autotoc_md75", [
- [ "Result", "md_examples.html#autotoc_md76", null ]
+ [ "Taylor-Green Vortex (3D)", "md_examples.html#autotoc_md76", [
+ [ "Final Condition", "md_examples.html#autotoc_md77", null ]
] ],
- [ "Lid-Driven Cavity Problem (2D)", "md_examples.html#autotoc_md77", [
- [ "Final Condition", "md_examples.html#autotoc_md78", null ],
- [ "Centerline Velocities", "md_examples.html#autotoc_md79", null ]
+ [ "Lax shock tube problem (1D)", "md_examples.html#autotoc_md78", [
+ [ "Initial Condition", "md_examples.html#autotoc_md79", null ],
+ [ "Result", "md_examples.html#autotoc_md80", null ]
] ],
- [ "Rayleigh-Taylor Instability (3D)", "md_examples.html#autotoc_md80", [
- [ "Final Condition and Linear Theory", "md_examples.html#autotoc_md81", null ]
+ [ "Gas Jet (2D)", "md_examples.html#autotoc_md81", [
+ [ "Final Condition", "md_examples.html#autotoc_md82", null ]
] ],
- [ "1D Multi-Component Inert Shock Tube", "md_examples.html#autotoc_md82", [
- [ "Initial Condition", "md_examples.html#autotoc_md83", null ],
- [ "Results", "md_examples.html#autotoc_md84", null ]
+ [ "Rayleigh-Taylor Instability (3D)", "md_examples.html#autotoc_md83", [
+ [ "Final Condition and Linear Theory", "md_examples.html#autotoc_md84", null ]
] ]
] ],
[ "Performance", "md_expectedPerformance.html", [
diff --git a/documentation/navtreeindex0.js b/documentation/navtreeindex0.js
index 207f2fa1b..95ba3115c 100644
--- a/documentation/navtreeindex0.js
+++ b/documentation/navtreeindex0.js
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diff --git a/documentation/search/all_0.js b/documentation/search/all_0.js
index 5052bff5a..8d57f869b 100644
--- a/documentation/search/all_0.js
+++ b/documentation/search/all_0.js
@@ -11,7 +11,7 @@ var searchData=
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['16m_20grid_20points_9',['16M Grid Points',['../md_expectedPerformance.html#autotoc_md93',1,'']]],
['1_3a_20setting_20up_20your_20environment_10',['Step 1: Setting up your Environment',['../md_visualization.html#autotoc_md124',1,'']]],
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- ['1d_20multi_20component_20inert_20shock_20tube_12',['1D Multi-Component Inert Shock Tube',['../md_examples.html#autotoc_md82',1,'']]],
- ['1d_20multi_20component_20reactive_20shock_20tube_13',['1D Multi-Component Reactive Shock Tube',['../md_examples.html#autotoc_md40',1,'']]]
+ ['1d_11',['1D',['../md_examples.html#autotoc_md78',1,'Lax shock tube problem (1D)'],['../md_examples.html#autotoc_md73',1,'Shu-Osher problem (1D)'],['../md_examples.html#autotoc_md57',1,'Titarev-Toro problem (1D)']]],
+ ['1d_20multi_20component_20inert_20shock_20tube_12',['1D Multi-Component Inert Shock Tube',['../md_examples.html#autotoc_md40',1,'']]],
+ ['1d_20multi_20component_20reactive_20shock_20tube_13',['1D Multi-Component Reactive Shock Tube',['../md_examples.html#autotoc_md60',1,'']]]
];
diff --git a/documentation/search/all_1.js b/documentation/search/all_1.js
index 32234a124..1c9c299e6 100644
--- a/documentation/search/all_1.js
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['2_3a_20customizing_20the_20script_2',['Step 2: Customizing the script',['../md_visualization.html#autotoc_md125',1,'']]],
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diff --git a/documentation/search/all_10.js b/documentation/search/all_10.js
index ff4c57404..3df8323e3 100644
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index 1b8964370..9b22dd11d 100644
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index a97c5996b..491cfa7d6 100644
--- a/documentation/search/all_12.js
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index 21b4af79f..da8d5e47c 100644
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index 8011dcc8a..ca0886a53 100644
--- a/documentation/search/all_14.js
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index 2d533c446..60aef8fed 100644
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index b51b085e8..4bc55f4c6 100644
--- a/documentation/search/all_16.js
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index ff6b91e3a..67ed30711 100644
--- a/documentation/search/all_17.js
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index b244390ff..8ca21544d 100644
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index 54f82a8d4..1d78d707a 100644
--- a/documentation/search/all_19.js
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index aa8bdd98e..a3c365e6d 100644
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index fd6e0cfa0..acec87dcd 100644
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index 0277ecac5..92f152d15 100644
--- a/documentation/search/all_2.js
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index 955f839c0..4ec6bdf2c 100644
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index a6c9f2f90..dd2a2a7e8 100644
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index 5238271cc..bcca9202d 100644
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index 4c9eee02f..3fbbefad8 100644
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index c2b5c6f56..b44559817 100644
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index ee42c1e66..f58b8c8e5 100644
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