Gas Flow into Vacuum Paradox ?

In summary: The pressure ratio and area ratio are optimum values for a given nozzle, but the basic gist is that the lower your pressure drop, the greater your area ratio must be -The laws of thermodynamics don't allow you to expand a gas all the way to a complete vacuum as that requires 100% usage of the fluid's energy -Starting with a small pressure at the nozzle exit allows for choked flow, but exhausts down to 0.0005 MPa to achieve sonic flow
  • #1
arhanbezbora
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Gas Flow into Vacuum Paradox ??

Hi,

I've just been reading up on 1-D isentropic, compressible flow through a nozzle (constant cross-sectional area) and have hit a bit of a conceptual road block which I was hoping someone would help resolve.

I'm interested in the mass flow rate of the gas through the pipe which should be proportional to the difference in pressures between the two ends of the nozzle. Thus if we hold the front pressure constant and reduce the back pressure (or do vice versa), then presumably the mass flow would increase (proportionally with respect to the difference in pressure) until the advent of choked flow whereupon the mass flow would attain a constant value and be independent of further reductions in the back pressure. The critical pressure at which this occurs can be easily obtained from the stagnation pressure via the specific heat ratio of the gas.

Now what if start our experiment with the back pressure set to 0 (a vacuum) and have a gas in the reservoir at a pressure P that is just a tiny bit greater than 0, say 0.001 Pa. Based on my understanding of the equations, it seems that the flow will be choked no matter what the front pressure is, as long as it is nonzero. This seems hard to believe; the pressure gradient is tiny but we still have choked flow ?? Is this true at all ?

Does anyone know any resources that will help to understand the compressible flow of a gas into a vacuum ?

Thank you very much.
 
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  • #2


This is an interesting question, but I think your paradox can be explained by a few small details.
First, choked flow is not the result of increasing flow rate, but rather the increase of the fluid velocity to the speed of sound, which is a direct result of the fact that the mass flow must be conserved. Likewise, the flow acceleration is governed by the continuity equation, which says that for a constant density fluid, the only method of acceleration is area decrease (for subsonic flows) or increase (for supersonic flows). The pressure ratio and area ratio of a nozzle are related and they have optimum values for a given nozzle, but the basic gist is that the lower your pressure drop, the greater your area ratio must be.
Additionally, the laws of thermodynamics don't allow you to expand a gas all the way to a complete vacuum as that requires 100% usage of the fluid's energy.
So if you start with 0.001 MPa, you would need to exhaust down to at most 0.0005 MPa at the nozzle exit to get sonic (and hence choked). That small expansion would take a huge area ration, and hence enormous nozzle to achieve, which is why rocket nozzles are all slightly underexpanded in the vacuum of space.
It's worth noting that the mathematics of isentropic flow also require the gas to have some small pressure at the exit, because to achieve absolute expansion, the area ratio from throat to exit goes to infinity.
I hope that helped.

-Max
 

Related to Gas Flow into Vacuum Paradox ?

1. What is the Gas Flow into Vacuum Paradox?

The Gas Flow into Vacuum Paradox, also known as the Knudsen Paradox, refers to the phenomenon where gas molecules appear to flow from a region of lower pressure to a region of higher pressure, which goes against the intuitive understanding of gas flow.

2. How does the Gas Flow into Vacuum Paradox occur?

The Gas Flow into Vacuum Paradox occurs due to the difference in molecular behavior between gases in the continuum regime (when the mean free path is smaller than the characteristic length of the system) and gases in the free molecular regime (when the mean free path is larger than the characteristic length of the system).

3. What is the role of mean free path in the Gas Flow into Vacuum Paradox?

The mean free path, which is the average distance a gas molecule travels between collisions, plays a crucial role in the Gas Flow into Vacuum Paradox. In the continuum regime, collisions between molecules dominate, resulting in a decrease in gas flow from high to low pressure. In the free molecular regime, collisions are rare, allowing gas molecules to travel longer distances and thus appear to flow from low to high pressure.

4. How does the Gas Flow into Vacuum Paradox impact real-world applications?

The Gas Flow into Vacuum Paradox has important implications in various technological applications, such as vacuum pumps, gas separation processes, and microfluidic devices. Understanding this phenomenon is crucial for optimizing the performance of these systems and improving their efficiency.

5. Can the Gas Flow into Vacuum Paradox be explained by classical physics?

No, the Gas Flow into Vacuum Paradox cannot be fully explained by classical physics. The phenomenon is better understood through the kinetic theory of gases, which takes into account the behavior of individual gas molecules. Quantum mechanics also plays a role in the explanation of this paradox.

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