Rocket nozzles
Typical temperatures (T) and pressures (p) and
speeds (v) in a De Laval Nozzle. The large bell or cone shaped expansion nozzle
gives a rocket engine its characteristic shape.
In rockets the hot gas produced in the combustion
chamber is permitted to escape from the combustion chamber through an opening
(the "throat"), within a high expansion-ratio 'de Laval' nozzle.
Provided sufficient pressure is provided to the
nozzle (about 2.5-3x above ambient pressure) the nozzle chokes and a supersonic
jet is formed, dramatically accelerating the gas, converting most of the
thermal energy into kinetic energy.
The exhaust speeds vary, depending on the expansion
ratio the nozzle is designed to give, but exhaust speeds as high as ten times
the speed of sound of sea level air are not uncommon.
Rocket thrust is caused by pressures acting in the
combustion chamber and nozzle. From Newton's third law, equal and opposite
pressures act on the exhaust, and this accelerates it to high speeds.
About half of the rocket engine's thrust comes from
the unbalanced pressures inside the combustion chamber and the rest comes from
the pressures acting against the inside of the nozzle (see diagram). As the gas
expands (adiabatically) the pressure against the nozzle's walls forces the rocket
engine in one direction while accelerating the gas in the other.
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