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Commit b3552c39 authored by Philippe Marchner's avatar Philippe Marchner
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Update README.md

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## Problem description
These routines solve a convected Helmholtz propagation problem with a Dirac right-hand-side, in either a circular or square domain.
These routines solve a convected Helmholtz propagation problem with a Dirac right-hand-side, either in a circular or square domain.
Different ABCs are tested on the output boundary, and are compared to the analytical solution.
## Installation and usage
......@@ -20,10 +20,10 @@ Simply run
```
with `[PARAM]`:
* `-geometry [x]` where `[x]` is the domain geometry (0: disk, 1: square)
* `-k [x]` is the freefield wavenumber, $k>0$
* `-R [x]` where `[x]` is the disk radius or square size, $R>0$
* `-k [x]` is the freefield wavenumber, $`k>0`$
* `-R [x]` where `[x]` is the disk radius or square size, $`R>0`$
* `-xs [x]` and `-ys [x]` specify the point source location
* `-M [x]` is the mean flow Mach number, $0<M<1$
* `-M [x]` is the mean flow Mach number, $`0<M<1`$
* `-theta [x]` is the mean flow angle orientation, $\theta \in [0, 2\pi]$
* `-abcName [x]` is the ABC type. The available choices are `ABC-0`, `ABC-2`, `Pade` and `pml`
* `-padeOrder [x]` and `-angle [x]` specify respectively the number of auxiliary function and branch rotation angle for the `Pade` abc.
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