In a cold gas propulsion system, the propellant is stored in gaseous form, and there is typically no combustion involved. The cold gas is expelled through a rocket nozzle to generate thrust. The design of the throat in a cold gas rocket nozzle is critical for controlling the flow and optimizing the exhaust velocity.
The relationship between the cross-sectional areas and velocities at the throat and exit of a rocket nozzle can be described by the rocket equation:
where:
-  and  are the cross-sectional areas at the nozzle Throat and exit, respectively,
-  and  are the velocities at the nozzle Throat and exit, respectively.
which gives
where,
In this equation:
- Â is the cross-sectional area of the nozzle at the throat,
- Â is the velocity of the exhaust gases at the throat,
- Â is the cross-sectional area of the nozzle at the exit,
- Â is the velocity of the exhaust gases at the nozzle exit.