The velocity of the exhaust gases at the nozzle exit for a liquid propellant rocket engine can be expressed using the continuity equation, which is based on the principle of conservation of mass.
The formula essentially states that the product of the cross-sectional area and velocity is constant between the nozzle inlet and exit for an incompressible flow (assuming no losses). As the cross-sectional area decreases, the velocity must increase to maintain mass flow continuity.
The continuity equation is given by:
where:
-  and  are the cross-sectional areas at the nozzle entrance and exit, respectively,
-  and  are the velocities at the nozzle entrance and exit, respectively.
which gives
where,
- A1Â is the Cross-sectional area at the throat of the nozzle in m2Â
- A2Â is the Cross-sectional area at the exit of the nozzle in m2
- V1Â is the Velocity of the exhaust gases at the throat in m/s
- V2Â is the Velocity of the exhaust gases at the nozzle exit in m/s