Irradiance and mode are scanned through a pressure ceiling. Exact arithmetic here means exact results for the stated model inputs; measured inputs still carry uncertainty and significant-figure limits.

highlighted = computed this step

Radiation pressure is scanned against a pressure ceiling

The training speed is fixed at 6 m/s and the mode is absorber. The source irradiance 3 watts per square meter gives pressure 1 over 2 Pa which is below the 1 Pa ceiling.

p=mI/c=13/6=12 Pap=mI/c=1\cdot3/6=\frac{1}{2}\ \text{Pa}
Pressure boundary rowMode and irradiance set the pressure row.power=12 WbeamArea=4 m^2irradiance=3 W/m^2irradianceSource=boundspeed=6 m/smode=absorberpressure=1/2 Padirection=normal

Radiation pressure is scanned against a pressure ceiling

The training speed is fixed at 6 m/s and the mode is absorber. The source irradiance 6 watts per square meter gives pressure 1 Pa which is at the 1 Pa ceiling.

p=mI/c=16/6=1 Pap=mI/c=1\cdot6/6=1\ \text{Pa}
Pressure boundary rowMode and irradiance set the pressure row.power=24 WbeamArea=4 m^2irradiance=6 W/m^2irradianceSource=boundspeed=6 m/smode=absorberpressure=1 Padirection=normal

Radiation pressure is scanned against a pressure ceiling

The training speed is fixed at 6 m/s and the mode is mirror. The source irradiance 6 watts per square meter gives pressure 2 Pa which is above the 1 Pa ceiling.

p=mI/c=26/6=2 Pap=mI/c=2\cdot6/6=2\ \text{Pa}
Pressure boundary rowMode and irradiance set the pressure row.power=24 WbeamArea=4 m^2irradiance=6 W/m^2irradianceSource=boundspeed=6 m/smode=mirrorpressure=2 Padirection=normal