Comments (6)
note also that the BS
integrator has only a single tolerance -- it takes the max of all the tolerances:
bs % atol(:) = 0.d0
bs % rtol(:) = max(rtol_spec, rtol_temp, rtol_enuc)
from microphysics.
the way to properly do this is to look at convergence of the results as we tighten the tolerances for each burner / integrator.
from microphysics.
there is some thought on this in the wdmerger II paper. It seems that 1.e-8 should be okay...
from microphysics.
I think that @abigailbishop largely has done this. We should add some plots to the user's guide
from microphysics.
I can do that.
from microphysics.
I think we've mostly addressed this now.
from microphysics.
Related Issues (20)
- support dense Jacobian in approx networks HOT 1
- have VODE jacobian caching consider how much rates have changed HOT 1
- JOSS paper
- running with test_sdc_vode_rhs gives an error saying integration failed in net
- CMake support HOT 5
- Enhancing the Helmholtz EOS
- create a eos_rh_t type HOT 1
- Rate tabulation inconsistencies in aprox19, aprox21, iso7 HOT 1
- Uninitialized variables in eos_t HOT 1
- create an nse_interp interface that doesn't compute X
- remove abort_on_failure HOT 1
- treat compiler warnings as errors HOT 3
- fix CMake build on Cray systems
- consider changing rhs() interface in integrator to pass y instead of integrator type HOT 2
- reintroduce the idea of multiple integrators
- switch Strang integration to work with (rho X, rho e) HOT 3
- burn_cell_primordial_chem should test if answer is correct
- what's the purpose of integrate_energy now? HOT 1
- for Strang scale_system are we doing the dedot/de term correctly
- for scale_system, the numerical Jacobian scaling is not correct
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from microphysics.