Hi Chris,
Thanks for sharing this example of a case where the 1D solver struggles.
I spent a bit of time looking at what's happening, and found a few things that may be of interest. The failure mode here comes from cases where the solver hits the limit on number of time steps taken without being able to solve the steady-state problem. It seems like it ends up in a place where only relatively small timesteps can be taken (in the 1e-5 to 1e-4 s range), and you don't get the usual pattern of acceleration where the solver is able to start taking much larger time steps as a prelude to success at solving the steady-state problem.
I tried using a timestep callback to collect the solution after each successive timestep, and found that what seems to be happening is that within the timestepping period, the solution starts to become very sharp at some location within the grid, for example with the temperature changing by 2000 K between successive grid points. This led me to think that it might be beneficial to try regridding within the time stepping process, instead of only regridding after a successful steady-state solve. There doesn't seem to be a great way to do this right now, but I set something up by catching the exception raised when timestepping fails, where I then regrid the flame and use that as the initial condition for a new call to the solver. With this approach, I was able to get solutions up to 15 MPa, higher than the ~7 MPa cases that seemed to be the limit with your approach of incrementally increasing the pressure, though it's certainly far from perfect. I've attached my script for reference.
Regards,
Ray