How is the average exhaust gas velocity determined in complex nozzle designs?

AI Thread Summary
The discussion focuses on defining the nozzle exhaust plane in complex nozzle designs and understanding how to determine average exhaust gas velocity. It highlights that complex shapes enhance the mixing of hot and cold streams, which reduces noise and affects exhaust gas behavior. The conversation addresses the challenge of measuring average velocity in computational fluid dynamics (CFD) simulations, particularly in converging and diverging nozzles. Participants note that while velocity differences may be minimal in sound suppression applications, more pronounced nozzle designs could yield significant variations. Understanding these dynamics is crucial for accurate thrust calculations.
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I don't quite understand what exactly you're asking but physically, this kind of shapes enhances the mixing of the hot and cold streams with the freestream flow in order to reduce the noise. Better mixing leads to smaller length scales which means higher frequences hence faster decay.
 
Indeed, but with this shape of the nozzle some of the exhaust mass (gas) exits the engine while some of the gas is still traveling through it thus further accelerating (as the nozzle is further converging (or diverging in case of a supersonic nozzle)).

So how do we determine the average exhaust gas velocity (in order to calculate thrust)?
Or rather where (at which point down the length of the nozzle) can we “measure” it (in a cfd simulation)?
Of course when using such a nozzle for sound suppression the difference between velocities is minimal, but consider a more pronounced version of these nozzles.
 
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