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T C said:As per this page on choked flow, in a convergent nozzle when the speed at the throat reached its limit i.e. sonic speed, no further increase in speed occurs despite increase in input pressure but the number of particles at the throat increase. In short, as the speed can't increase, to keep the mass flow rate constant, the number of particles at the throat increase. Increase in number of particles at the throat means increase in density and that means increase in pressure.
russ_watters said:That's correct.
No, it's not correct. When the nozzle becomes choked, the speed can absolutely still change, e.g. if the temperature changes. What becomes fixed is the Mach number. It also means that, no matter what you do to the back pressure, the mass flow rate remains constant because the conditions at the throat have not changed, and mass has to be conserved. That said, if you change the reservoir conditions, you can still change the mass flow rate through the throat or the velocity, but the Mach number is still fixed at 1.
russ_watters said:That - again - is why a typical blower won't work for this application.
As long as the blower can create sufficient pressure on its downstream edges, there is no reason a blower couldn't work in principle. That said, the requirements of CD nozzles will rapidly outpace a blower's ability to keep up.
T C said:In case of a convergent nozzle, there is no way to measure the speed of the fluid after the throat.
Wait, what? Why do you say this? You can measure speed in any flow if you have the right instrument (subject to the usual constraints of experimental uncertainty).
T C said:But in case of c/d nozzle or De Laval nozzle, the speed can be measured and it has been found that the speed increases after the flow exits the throat. How that can happen? In my opinion, the increase in pressure at the throat is released and that is converted into more speed at the divergent section.
What I want to say is that the same phenomenon can occur when we use a blower.
This isn't really a matter of opinion. In a subsonic flow, a decrease in area results in a flow acceleration and its complementary pressure decrease (after all, you need a pressure gradient to provide the force for the acceleration). For a supersonic flow, the situation is reversed, and an increase in area results in the same effect (faster flow, lower pressure). In other words, throughout the entire length of a de Laval nozzle, the pressure monotonically decreases and the speed and Mach number each monotonically increase provided that the pressure ratio is large enough to fully start the nozzle.
It makes no difference whether the pressure was provided by a blower or an air storage system. As long as the pressure can be maintained at the desired mass flow rate, then the nozzle runs as designed.