diff options
author | jthorn <jthorn@f88db872-0e4f-0410-b76b-b9085cfa78c5> | 2003-07-10 16:08:45 +0000 |
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committer | jthorn <jthorn@f88db872-0e4f-0410-b76b-b9085cfa78c5> | 2003-07-10 16:08:45 +0000 |
commit | 4c225b249e899f8b5b2818fcb05e52a3d56f6933 (patch) | |
tree | 4b868957815f1ec82c43b1d06fefc2abfd147e80 /param.ccl | |
parent | 6c5417c54493595480e29131e3b1267b101fa4f4 (diff) |
add max_allowable_horizon_radius
parameter to (we think) fix a serious bug where if one horizon goes
off the edge of the grid, we fail to find any other horizons
git-svn-id: http://svn.einsteintoolkit.org/cactus/EinsteinAnalysis/AHFinderDirect/trunk@1130 f88db872-0e4f-0410-b76b-b9085cfa78c5
Diffstat (limited to 'param.ccl')
-rw-r--r-- | param.ccl | 16 |
1 files changed, 16 insertions, 0 deletions
@@ -676,6 +676,22 @@ real max_allowable_Delta_h_over_h \ } 0.1 # +# To avoid the Newton iteration diverging (or more accurately, to detect +# this divergence faster) if there is no horizon present or if the initial +# guess is bad, we also deem any horizon with a mean radius (measured around +# its local coordinate origin) larger than this to be "not found". The +# default is effectively "no limit"; you should (re)set this to the +# coordinate radius of a sphere with areal radius 4m or so, where m is +# the ADM mass of the slice. +# +real max_allowable_horizon_radius \ + "max mean-coordinate-radius allowed for any trial surface \ + before we give up and say we can't find this horizon" +{ +(0.0:* :: "any positive real number" +} 1.0e10 + +# # convergence tolerance for the Newton iteration # real Theta_norm_for_convergence \ |