Supersonic Flow in Diverging Nozzle

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SUMMARY

The discussion centers on the behavior of fluid dynamics in diverging nozzles, particularly regarding supersonic flow. It is established that as fluid velocity exceeds the speed of sound, an increase in cross-sectional area leads to an increase in velocity due to a pressure differential, as described by the equation (P1-P2)=(rho/2(V2^2-V1^2)). The principles of compressible flow dictate that density changes allow for different behavior compared to incompressible flow. The design of nozzles must account for Mach number and energy balances to facilitate efficient flow, particularly in applications involving internal combustion engines (ICE).

PREREQUISITES
  • Understanding of fluid dynamics principles, particularly compressible flow
  • Familiarity with the concept of Mach number and its implications
  • Knowledge of thermodynamics, specifically energy and mass balances
  • Experience with nozzle design and its impact on flow characteristics
NEXT STEPS
  • Study the principles of compressible flow in detail, focusing on the behavior of fluids at varying Mach numbers
  • Learn about the design and function of De Laval nozzles and their applications in supersonic flow
  • Investigate the effects of temperature variations on fluid dynamics in internal combustion engines
  • Explore the concept of choked flow and its implications for mass flow rates in nozzles
USEFUL FOR

This discussion is beneficial for mechanical engineers, fluid dynamics researchers, and anyone involved in the design and analysis of nozzles and supersonic flow systems.

NickPorter
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Clearly, at low speeds the velocity of a fluid increases when the area through which it is traveling decreases. I am curious as to why a fluid traveling faster than the speed of sound increases its velocity when its area is increased. Thank you
 
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Im not 100% sure why, however the reason it works going from big to small is because of the pressure differential. (P1-P2)=(rho/2(V2^2-V1^2)), as you can see the density times velocity needs to equal the pressure difference. so at a higher speed the pressure differential going from small to large may be larger thus needing a larger V2 to keep the ratio equal to the pressure differential. My best guess!
 
At low speeds the fluid is treated as incompressible, so when the nozzle contracts, the only way for the molecules to get out of the way of one another and conserve mass is by speeding up.

In a compressible flow, that same fluid can change in density, meaning it isn't required to follow the same rules as incompressible flows.

I may be wrong here, as I haven't ever really considered this question aside from what the equations say, but when the area increases, the density decreases and the temperature drops. This is a net loss of energy that is balanced by the resulting increase in kinetic energy.
 
From my fuzzy recollection of intermediate thermodynamics (and looking it up):

\frac{dA}{A}=-\frac{dV}{V}(1-M^{2})

So in the design of a nozzle's cross-sectional area using mass and energy balances, the rate of change in area of the nozzle at any point is related to the area, velocity, change in velocity, and Mach number.

Putting it another way, compressed fluids going through a converging nozzle can only pass through the nozzle at up to Mach 1 (speed of sound in the fluid). This limitation is due to back pressure and "choked flow," meaning the maximum mass flow rate through an orifice is limited to Mach 1 through that orifice. To increase velocity after a throat (minimum area) requires a diverging (supersonic) nozzle which allows the fluid's pressure to drop, reducing back pressure and accelerating the flow. This is of course not taking into account things like normal shockwaves and the like...

http://en.wikipedia.org/wiki/De_laval_nozzle
 
Not to intrude, but I have a question for Mech. Engineer. How sensative are these to different levels of temperature of the working fluid? In my case, an ICE.
 

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