Difference between revisions of "Description"
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= Description of the Benchmark = | = Description of the Benchmark = | ||
| − | This benchmark is composed of 4 major steps that should be performed carefully one after the other. | + | This benchmark is composed of '''4 major steps''' that should be performed carefully one after the other. |
| − | + | The objective of the following pages is to give a self-contained description of the benchmarks so that anyone can reproduce the [[results]] with its own high-fidelity code. | |
| − | * The [[Step | + | * The [[Step 1]] is a simple '''2D configuration''' with a single species at '''Reynolds number''' of 1,600. |
| − | * The [[Step | + | * The [[Step 2]] is the extension of the '''Step 1''' to '''3D'''. The Reynolds number is still 1,600. A transition to turbulence is expected to occur. |
| − | * The [[Step 4]] is a real flame configuration, very similar (but not identical) to Step 3 with reactions enabled. | + | * The [[Step 3]] builds on top of the '''Step 2''' by including '''multiple species''' with steep gradients of concentrations as well as an inhomogeneous temperature. This situation is clearly closer to a real flame but the '''chemical reactions must not be activated yet'''. |
| + | |||
| + | * The [[Step 4]] is a '''real flame configuration''', very similar (but not identical) to '''Step 3''' with '''reactions enabled'''. | ||
Latest revision as of 14:19, 25 August 2020
Description of the Benchmark
This benchmark is composed of 4 major steps that should be performed carefully one after the other.
The objective of the following pages is to give a self-contained description of the benchmarks so that anyone can reproduce the results with its own high-fidelity code.
- The Step 1 is a simple 2D configuration with a single species at Reynolds number of 1,600.
- The Step 2 is the extension of the Step 1 to 3D. The Reynolds number is still 1,600. A transition to turbulence is expected to occur.
- The Step 3 builds on top of the Step 2 by including multiple species with steep gradients of concentrations as well as an inhomogeneous temperature. This situation is clearly closer to a real flame but the chemical reactions must not be activated yet.
- The Step 4 is a real flame configuration, very similar (but not identical) to Step 3 with reactions enabled.
