Open brittonsmith opened 6 years ago
Original comment by Britton Smith (Bitbucket: brittonsmith, GitHub: brittonsmith)
Fantastic! Looking forward to your pull request(s)!
Original comment by Yves Revaz (Bitbucket: revaz, GitHub: revaz)
Hi Britton, Thanks for your mail which precisely answers my questions.
Cheers, yves
Original comment by Britton Smith (Bitbucket: brittonsmith, GitHub: brittonsmith)
Hi Yves,
When you say that you would like to replace the ionizing/heating rates provided by the Cloudy tables with the radiative transfer variables, do you mean that you would like to completely remove the use of the Cloudy rates? I believe running Grackle with the Cloudy tables is the most popular use right now, so I don't think that should happen. However, if you just mean that you would like to add the option of providing H/He/He+ heating rates from the radiative transfer, then I think this would be a very nice addition.
As for renaming the variables in the C wrapper, I agree with this in principle, but such a change would break backward compatibility, which we would like very much to preserve. I think it would be fine to add RT_H*_heating_rate variables and allow for both the current use case as well as providing them individually.
For renaming the internal FORTRAN variables, this I think would be ok. We usually try not to do too much variable renaming as it can cause issues with merging in pull requests, but I think this would be fine as it would serve to clarify things for developers.
With regard to summing the RT and shielded rates, this should probably stay as is since running with radiative transfer is optional and I think not that widely used to begin with. When radiative transfer is not used, the kdissH2I
fields will be NULL pointers. If you have something different in mind, please correct me.
In conclusion, I definitely encourage you to issue a pull request for the first two of your proposed changes as long as we can preserve backward compatibility. You are also welcome to issue multiple PRs if you think it would be simpler. Finally, if you'd like to get more opinions on any proposed changes, I would suggest you write to the mailing list as more people will see it.
Thanks! Britton
Original comment by Yves Revaz (Bitbucket: revaz, GitHub: revaz)
Hi Britton,
Thanks for the very motivating answer. I went deeper into the code and have other suggestions still related to the rates linked to the radiative transfer. My motivation is that the ionizing/heating rates provided by the cloudy tables should be replaced by ionizing/heating rates provided by the radiative transver variables (at the execption that the rates provided by the cloudy tables cans be shielded by different methods). Implementing this "symetry" will be very very usefull to my opinion.
Thus, I suggest to rename the RT variables to be more consistent with the names addopted for the cloudy tables. This will strongly improve the code clarity:
variables in the C wrapper:
RT_HI_ionization_rate, (no modification) RT_HeI_ionization_rate, (no modification) RT_HeII_ionization_rate, (no modification) RT_H2_dissociation_rate, (no modification) RT_heating_rate, ->RT_HI_heating_rate ->RT_HeI_heating_rate ->RT_HeII_heating_rate
variables in the FORTRAN routines:
kphHI, ->RT_k24 kphHeI, ->RT_k26 kphHeII, ->RT_k25 kdissH2I, ->RT_k31 photogamma, ->RT_piHI ->RT_piHeI ->RT_piHeII
By the way, another improvement would be to sum RT_k24, RT_k26, RT_k25 directly with the shielded values : k24shield, k26shield, k25shield. This will remove a lots of
if (iradtrans .eq. 1)
slightly speeding the code, as it is done for
k31shield(i) = k31 + kdissH2I(i,j,k)
and also improve the code clarity.
I can certainly implemente those suggestions but as it implies quite a lots of changes, I would like again you opinions before investing time on that.
Cheers,
yves
Original comment by Britton Smith (Bitbucket: brittonsmith, GitHub: brittonsmith)
Hi Yves,
Like many things in grackle, this has been carried over from how things are done in Enzo. The modification you propose would be very welcome! I definitely encourage you to go ahead with it. Please, feel free to contact the users list or post to this issue if you have any questions. Thanks for taking this on!
Britton
Originally reported by Yves Revaz (Bitbucket: revaz, GitHub: revaz)
Hi all,
Currently, when using the heating rates from radiative transfer solutions, only the heating due to HI is included through the variable photogamma:
in cool1d_multi_g.F ! Photoheating from radiative transfer edot(i) = edot(i) + real(ipiht, DKIND) photogamma(i,j,k) / coolunit HI(i,j,k) /dom
However, when computing the radiative heating due to the UB background through the rates provided by the cloudy table, grackle also include the He heating:
in cool1d_multi_g.F ! Photoionization heating edot(i) = edot(i) + real(ipiht, DKIND)( & piHI HI (i,j,k) ! pi of HI & + piHeI HeI (i,j,k)0.25_DKIND ! pi of HeI & + piHeIIHeII(i,j,k)0.25_DKIND ! pi of HeII & )/dom
For the sake of consistency, in the radiative transfert mode, I suggest to let the possibility to provide piHI, piHeI and piHeII, replacing photogamma.
Doing so will still be compatible with the current version, if setting piHeI=0 and piHeII=0.
I think there is very few lines to change and if this is fine, I can certainly to the modifications.
yves