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1 change: 0 additions & 1 deletion examples/2D_kelvin_helmholtz/case.py
Original file line number Diff line number Diff line change
Expand Up @@ -2,7 +2,6 @@
import json
import math


eps = 1e-6
time_end = 1.0
time_save = time_end / 100.0
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1 change: 0 additions & 1 deletion examples/2D_richtmyer_meshkov/case.py
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Expand Up @@ -2,7 +2,6 @@
import json
import math


mu = 1.0e-4
lambd = 1.0
time_end = 15.0
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1 change: 0 additions & 1 deletion examples/2D_viscous_shock_tube/case.py
Original file line number Diff line number Diff line change
Expand Up @@ -2,7 +2,6 @@
import json
import math


mu = 1.0e-3
time_end = 1.0
time_save = time_end / 100.0
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1 change: 0 additions & 1 deletion examples/nD_perfect_reactor/analyze.py
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Expand Up @@ -6,7 +6,6 @@
import mfc.viz
from case import dt, Tend, SAVE_COUNT, sol


case = mfc.viz.Case(".", dt)

sns.set_theme(style=mfc.viz.generate_cpg_style())
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1 change: 0 additions & 1 deletion examples/nD_perfect_reactor/export.py
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Expand Up @@ -5,7 +5,6 @@
import mfc.viz
from case import dt, NS, Tend, SAVE_COUNT, sol


case = mfc.viz.Case(".", dt)

for name in tqdm(sol.species_names, desc="Loading Variables"):
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2 changes: 1 addition & 1 deletion src/simulation/m_ibm.fpp
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Expand Up @@ -1179,7 +1179,7 @@ contains
elseif (patch_ib(ib_marker)%geometry == 8) then ! sphere
patch_ib(ib_marker)%moment = 0.4*patch_ib(ib_marker)%mass*(patch_ib(ib_marker)%radius)**2
else ! we do not have an analytic moment of inertia calculation and need to approximate it directly
else ! we do not have an analytic moment of inertia calculation and need to approximate it directly via a sum
count = 0
moment = 0._wp
cell_volume = (x_cc(1) - x_cc(0))*(y_cc(1) - y_cc(0)) ! computed without grid stretching. Update in the loop to perform with stretching
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