We assume that the tank is almost empty, with its maximum internal volume, and that the small amount of liquid remaining is in vapor-liquid equilibrium at that temperature. We calculate the heat inflow and outflow from the tank, including solar radiation, radiant heat, and convective heat transfer due to wind, to the tank's roof and side walls. We then determine the rate of temperature rise in the gas phase inside the tank and calculate the release rate of the vent gas from the volume expansion rate of the gas phase.
Since the amount of radiant heat from the sun is determined by the latitude and longitude of the installation location, the date, and the sun's altitude at that time, it is possible to understand the changes in the hazardous area over time by determining the change in the gas emission rate over time.