Commit Graph

10 Commits

Author SHA1 Message Date
Martin Diehl 3bb5a5e7b5 line too long in DAMASK_spectral_solverPolarisation.f90, reordered curl calculation for clearer look, fixed test for Marc 2013 2013-08-08 18:10:58 +00:00
Martin Diehl 7f3c24e1f1 fixed some buggy last minute changes in the last commit 2013-08-08 09:13:29 +00:00
Martin Diehl ac92b90e0b fixed al and pol solver, now checking for div(p) = curl(f) = 0 2013-08-07 17:20:05 +00:00
Martin Diehl 5b80ef3a4c fixed wrong error calculation in Polarisation and AL solvers, and strictened tolerances for tests 2013-08-02 13:55:44 +00:00
Martin Diehl 74791a6686 corrected invalid error for mismatch_p 2013-08-02 11:48:24 +00:00
Martin Diehl 2dc985f558 set tolerances to useful values and renamed them.
allowed "keyword = value" in numerics.config (simply removing "=" from line)
2013-07-31 15:03:38 +00:00
Martin Diehl b5a11f9d31 fixed bug in AL, weakened correction slightly 2013-07-30 21:04:41 +00:00
Martin Diehl 81531097f1 changes on convergence tolerances of AL and Polarisation, switched back to immediate correction of stress bc but only when last two average stresses are close to each other (cosine decay) 2013-07-30 15:32:55 +00:00
Pratheek Shanthraj 03d8f14a98 introduced dynamics for high strain rate simulations. so far only works for materials with homogeneous density. the density is read in as an optional argument in the load file using the keyword 'den' or 'density'. if density > 0 then inertial terms are added to the stress equilibrium. an implicit euler time discretisation is used to calculate the inertial terms.
dynamic problems are length scale dependent so make sure the geometry size is meaningful (1 m^3 or N m^3 for example is too big for a RVE!).

not specifying a density (density = 0) will perform a quasi static simulation as before.
2013-07-26 16:25:37 +00:00
Martin Diehl 216063fe36 added Polarisation scheme as solver 2013-07-24 13:06:16 +00:00