&SPEC ID='POLYURETHANE', FORMULA='C25H42O6N2'/
&REAC FUEL='POLYURETHANE', SOOT_YIELD=0.131, HEAT_OF_COMBUSTION=23500. /
&VENT XB=1.80,2.20, 1.60,2.00, 0.60,0.60, COLOR='RED', SURF_ID='BURNER' /
&SURF ID='BURNER',HRRPUA=7791.625, RAMP_Q='HRR1', COLOR='RED', E_COEFFICIENT=0.03 /
&RAMP ID='HRR1', T=0.0, F=0.00 /
&RAMP ID='HRR1', T=25.0, F=0.00 /
&RAMP ID='HRR1', T=50.0, F=0.01 /
&RAMP ID='HRR1', T=75.0, F=0.01 /
&RAMP ID='HRR1', T=100.0, F=0.02 /
&RAMP ID='HRR1', T=125.0, F=0.02 /
&RAMP ID='HRR1', T=137.5, F=0.02 /
&RAMP ID='HRR1', T=150.0, F=0.03 /
&RAMP ID='HRR1', T=175.0, F=0.17 /
&RAMP ID='HRR1', T=200.0, F=0.51 /
&RAMP ID='HRR1', T=225.0, F=0.85 /
&RAMP ID='HRR1', T=250.0, F=1.00 /
&RAMP ID='HRR1', T=251.0, F=0.96 /
&RAMP ID='HRR1', T=275.0, F=0.64 /
&RAMP ID='HRR1', T=300.0, F=0.42 /
&RAMP ID='HRR1', T=325.0, F=0.28 /
&RAMP ID='HRR1', T=350.0, F=0.23 /
&RAMP ID='HRR1', T=375.0, F=0.19 /
&RAMP ID='HRR1', T=400.0, F=0.18 /
&SPEC ID='WATER VAPOR' /
&PART ID='WATER_DROPS'
SPEC_ID='WATER VAPOR'
DIAMETER=2000.
SAMPLING_FACTOR=1
QUANTITIES(1:2)='PARTICLE DIAMETER','PARTICLE VELOCITY' /
&PROP ID='ZSTP15'
SMOKEVIEW_ID='sprinkler_pendent'
PART_ID='WATER_DROPS'
PARTICLES_PER_SECOND=5000.
FLOW_RATE=50.6
ORIFICE_DIAMETER=0.0127
SPRAY_ANGLE=0.,105.
OFFSET=0.20 /
Based on a grid width of 10 cm, I calibrated the E coefficient to 0.03 with results of experiments with this setup. I then conducted a grid sensitivity study and found that even with a 1.25 cm grid there were still significant differences in the simulation results compared to a 2.5 cm grid. I then repeated the grid sensitivity study with an E coefficient of 2.0, believing that 0.03 might be too low a value. However, the results still showed significant deviations depending on the grid size.
Is there a specific grid size at which the submodel is validated to reduce the heat release rate through sprinklers, or is it necessary to use an even finer grid than 1.25 cm? or maybe it's because my HRRPUA keeps rising after sprinkler activation?
I also performed a sensitivity analysis of the other physical or numerical parameters.