Feature #1292: mdrun features to deprecate for 5.0
shell code issues (broken with DD+grid; broken with Verlet scheme)
Removing particle decomposition requires that the regression test perl script stops always triggering -pd when simple grid searching is being used. Currently, the complex/sw test uses the shell-model polarization code, with simple, thus -pd (and vsites and "flexible" constraints). This would have to change to grid+DD when we remove PD.
Using installs of either master or release-4-6 HEAD with
gmxtest.pl complex -only sw\\b
by changing the grompp.mdp and/or gmxtest.pl files, I observed:
-pd and simple passes the test with 1-8 tMPI ranks
-pd and grid passes the test with 1-8 tMPI ranks
-dd and simple passes the test with 1 rank, and gives the expected fatal error with DD+simple unsupported (perl script hack required to remove the hard-coded -pd flag)
-dd and grid passes the test with 1 rank, and fails with all higher numbers
The fails are pretty subtle:
comparing energy file reference_s.edr and ener.edr There are 31 terms in the energy files There are 5 terms to compare in the energy files Angle step 19: 71.2642, step 19: 71.1485 Angle step 20: 70.2909, step 20: 70.1638 Files read successfully
So, if there's a problem, then I think it is already present in the code and release-4-6 should get a fatal error for shells + DD and ranks > 1. It could have the same cause as the problem that was swept under the carpet in #993 (the forces may not be very reproducible in single precision), but when I tested release-4-6 in double precision I got the same error with DD, grid, and -ntmpi > 1.
To see if OpenMP was useful as parallelism, I tried to test the shell code with the Verlet scheme (using verlet-buffer-drift=-1 because the test case has a box that's only just large enough for the unmodified rlist), and it segfaulted with both grid and simple, even with just 1 rank and 1 thread. So I believe that needs a fix or a fatal error, also.
The above poses a problem for the proposed removal of PD - the existence of what might be an historical bug reduces the support in 5.0 for shells from "MPI with group scheme and PD" to "serial with group scheme." We have a few open bugs for / suspicions of the shell code (#879, #993, #713). I suggest we proceed with removing PD, and require the complex/sw test to run with 1 rank, unless/until someone wants to find out what the real problem is. Hopefully, with the interest in polarizable models expressed in #1292 that will be sooner rather than later!
Issue fatal errors rather than use broken shell code
Fix sw test case
The former version had trouble reproducing the serial results in some
cases in parallel. This change replaces the input conf.gro file with
the confout.gro file from the former version of the test run in
Reference mode, because that starting configuration seems more
stable. The former input .gro file had velocities for particles named
DW, but it is not known whether this is related to the problem.
Also switched it to use ns-type=grid in line with future changes in
Reinstate shell code with DD
Further work on the complex/sw test case in the 5.0 regressiontests
branch reveals that the initial conditions may have been the reason
for the problems observed with DD and more than one node, rather than
Made shells work with the Verlet scheme
The issue was that atoms iso charge group should be put in the box.
Additionally water_pol only worked within a charge group, now fixed.
Note that with shells working across charge groups, which is always
the case with the Verlet scheme, no shell prediction is done.
We should implement prediction, since it improves performance.
#1 Updated by Justin Lemkul over 4 years ago
Thanks for pointing this out, Mark. I'm currently working through the code to see which parts I can reuse and which functions I will have to write on my own for our implementation of the Drude model. I remain hopeful that Drude will be fairly straightforward and should play nicely with parallelism, DD, etc because the Drudes are not really special - they're just low-mass particles in our force field. There are some bells and whistles with bonded interactions, temperature, and Thole screening, but those should be fairly simple to add in. Nothing I'm planning to do should be inherently dependent upon PD, unless I am reusing some aspect of the shell code that needs it. If that's the case, I'm sure I'll come across it and will probably just rewrite whatever that function happens to be.
#3 Updated by Mark Abraham over 4 years ago
Roland observed at https://gerrit.gromacs.org/#/c/2703/:
Of course DD isn't suppose to give the exact same results for different number of domains. But it is odd that for just complex/sw the difference between 1 domain and 2 is larger than our margin. Also the results for 2,3,4,5 domains are all very similar. On the other hand if one takes the results after 20 steps (confout.gro) generated with either 1 or 2 domains as starting configuration (conf.gro), and regenerates the reference values, then the tests pass. So it might just be that the starting configuration is particular sensitive to the rounding error of DD.
#8 Updated by Berk Hess about 4 years ago
- Status changed from New to Fix uploaded
- Target version set to 4.6.6
The uploaded a fix, which was relatively simple.
But without charge groups there is not shell prediction. This means that for the test we need reasonable initial shell coordinates, which can done by e.g. running one step of md and using confout.gro.
Also not using prediction deteriorates performance, I filed a feature issue #1522 for this.