The way I would remedy the situation is: - look at the Mathematica source file for thorn ML_ADMQuantities - remove the declaration of the external ML_BSSN variables - peek at thorn ML_BSSN to find how these are defined in terms of the ADM variables, and insert this definition where needed, e.g. calculating det g from g_ij instead of from W
For someone familiar with Kranc that should be straightforward, and not more difficult than creating a second version that attaches itself to ML_CCZ4. -erik On Wed, Apr 4, 2018 at 8:53 AM, Erik Schnetter <schnet...@cct.lsu.edu> wrote: > As written, thorn ML_ADMQuantities requires another thorn with the > name ML_BSSN to be present. > > -erik > > On Wed, Apr 4, 2018 at 7:52 AM, Wolfgang Kastaun <phy...@fangwolg.de> wrote: >> >> >> On 04/04/2018 01:14 AM, Roland Haas wrote: >>> Hello Wolfgang, >>> >>>> @Roland: In the interface.ccl of ML_ADMConstraints I only see the ADM >>>> constraints, no expressions for ADM energy and angular momentum. Or did >>>> you mean something else? >>> I meant ML_ADMConstraint but did not check its interface.ccl. If they >>> are not there then I have no better suggestion than Erik. Are the >>> changes from BSSN to ccZ4 or Z4c more than just "replace K with K+X"? >>> >> >> As far as I remember, the BSSN variables are also present in the CCZ4 >> system, with differences only in the case of constraint violating states. >> >>> Yours, >>> Roland >>> > > > > -- > Erik Schnetter <schnet...@cct.lsu.edu> > http://www.perimeterinstitute.ca/personal/eschnetter/ -- Erik Schnetter <schnet...@cct.lsu.edu> http://www.perimeterinstitute.ca/personal/eschnetter/ _______________________________________________ Users mailing list Users@einsteintoolkit.org http://lists.einsteintoolkit.org/mailman/listinfo/users
