2. Benchmark 7 Refresher
• Uses the Method of Manufactured Solutions
(MMS) for the Allen-Cahn equation
• Three Primary Objectives
1. Provide an example to teach phase field practitioners
about MMS
2. Have users demonstrate that their code achieves the
expected order of accuracy
3. Provide a platform for comparing the performance of
different codes (or options within a code) at known
error levels
4. Three Parts
A: Non-computationally demanding test to calculate
spatial and temporal order of accuracy
B: More computationally demanding test to
examine computational performance; has a much
thinner interface than A
C: More computationally demanding test to
examine computational performance; has a much
thinner interface than A and faster interfacial
velocity than A/B
5. Results on PFHub
• 7a has 6 uploads (highest other than BM1)
• 7b has 1 upload (me)
• 7c has 0 uploads
6. Feedback and Action Items from Last
Meeting
1. The run times can be long, especially for Parts B and C
1. Eliminate Part C as redundant; Part B is already taxing
enough
2. Consider reducing the length of the simulation (more
later)
2. The temporal order of accuracy is hard to get,
because spatial error dominates
1. Choose a simulation with a small time step to get a
baseline spatial error, subtract that off to get the nominal
temporal error
3. Fix the SymPy code
4. Tweak the order of the introduction
5. Clarify that OOA is not needed for Part B
7. Does shortening the simulated time
hurt the OOA calculations?
The posted version goes until t = 8
Time Temporal OOA Spatial OOA
2 2.66 2.05
4 1.23 2.06
6 1.15 2.07
8 1.12 2.09
Upshot: Could reduce the simulated time by ½ without strongly
impacting the observed OOA
Is it worth invalidating the existing uploads to change this?
8. Other Thoughts
Fit the spatial and temporal error simultaneously
Assume the form:
I made a Jupyter notebook to calculate this fit, hard to pick up
the temporal OOA
Quantify the strength of the source term
Unclear how the length and time scales of the manufactured
solution compare to “real” phase field problems