jet engine thrust
Thrust is created by accelerating the air mass that has passed through it. For this purpose, kinetic energy must be supplied to the air. If the pressure loss caused by the thrust nozzle can be neglected, the nozzle is called adapted.
According to the law of conservation of momentum, the following applies to the net thrust of an engine:

with
: Thrust (Force)
: mass flow rate of ejected air
: mass flow rate of the aspirated air
: velocity of the ejected air (velocity)
: velocity of the aspirated air
Since the gas expands due to the combustion of the fuel and the associated increase in temperature, and the increased volume must escape through the narrowed cross-section of the nozzle, the velocity c of the airflow increases (for more details see: jet engine). In propeller machines, the airflow acceleration is achieved by a driven propeller.
Since the engine nacelle generates a drag D (the drag of the aircraft can be neglected), this must be subtracted from the net thrust. This means that two aircraft can have different thrust even though they are equipped with the same engines (e.g. A350 and Boeing 787). The following therefore applies

However, since air gets thinner the higher you fly, the mass flow also decreases with increasing altitude. So one defines an engine thrust at ISA-conditions and then says

where the air density (ρ - rho) can be estimated, for example, by the barometric altitude formula.
rocket thrust
When propelling a rocket, the speed is especially important when the fuel is exhausted.
For the shear momentum, (according to the momentum theorem
):

F: Propulsive force
Δt: Burning time of the engine
Δm: Mass loss of the rocket due to the loss of the burnt fuel.
vs: outflow velocity
Note: This is one of the rare cases in elementary mechanics where mass is not a constant. In this case, it is also easy to express the power of the rocket engine as
! The effective exhaust velocity is also called the (mass) specific impulse of the rocket engine.
If the propulsion
(not always given, see e.g. thrust curve for solid rockets), it follows for the terminal velocity
with
and consideration of the rocket empty mass
and the propellant mass
:
{ "basic rocket equation".)
The terminal velocity increases with the ejection velocity (typical value is 4500 m/s) and the ratio of initial to terminal mass (typically 30:1 to 100:1). Corrections for drag must be considered analogous to the jet engine case.
An important use case for rocket engines is to overcome the acceleration due to gravity. To do this, the rocket must reach escape velocity
(e for escape) reach.
In a launch vehicle, for example, the final mass is approximately identical to the payload, only the latter reaches the target altitude (with the payload fairing):
Ariane 5G: launch mass ≈750 t, payload ≈20 t LEO, 7 t GTO, launch thrust ≈12,000 kN, maximum thrust ≈14,400 kN.