High-pressure compression of liquids

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Discussion Overview

The discussion revolves around generating high hydrostatic pressures in liquids, specifically exploring the mechanics of using a falling rod to create such pressures and the implications of pressure wave propagation in fluids. The scope includes theoretical considerations, fluid mechanics, and the application of Pascal's law in dynamic scenarios.

Discussion Character

  • Exploratory
  • Technical explanation
  • Debate/contested

Main Points Raised

  • One participant proposes using a 1-ton rod dropped from a height to generate a pressure of 400 kbar upon impact with a liquid, applying the impulse theorem to calculate the resulting pressure.
  • Another participant questions the validity of Pascal's law in the context of dynamic pressure waves, asserting that it applies only to static equilibrium and suggesting that the pressure wave will dissipate once it leaves the tube.
  • A different participant argues that pressure waves can propagate throughout a liquid and that Pascal's law could apply to these waves, provided the liquid remains at rest during the wave's propagation.
  • Concerns are raised about the elastic deformation of the tube and how it might affect the pressure pulse generated by the falling rod.
  • One participant suggests that the speed of the pressure wave could be approximated by the speed of sound in the liquid, which could help estimate how quickly the pressure wave reaches other areas of the container.
  • There is mention of using silicone oil as a pressure-transmitting liquid in high-pressure experiments, indicating a consideration of different fluids beyond water.

Areas of Agreement / Disagreement

Participants express differing views on the applicability of Pascal's law to dynamic pressure waves, with some agreeing that it only applies to static conditions while others argue for its relevance in dynamic scenarios. The discussion remains unresolved regarding the implications of pressure wave propagation and the effects of elastic deformation.

Contextual Notes

Participants highlight limitations in their reasoning, such as the assumptions about the impact time and the behavior of pressure waves in different fluid conditions. The discussion also touches on the complexities of modeling fluid mechanics under extreme conditions.

g_mogni
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Hello,

My memories of fluid mechanics are very rusty and therefore I was wondering if you could help me with this hypothetical problem. Let's say I want to generate very high hydrostatic pressures in a liquid (of order of 400 kbar). Would it be enough to do the following: take a rod weighting 1 ton and drop it through a narrow tube with cross sectional area of 2.5x10^-4 m2 from a height of 5m under free-fall, such that upon impact with the liquid at the bottom of the tube the velocity of the rod is 10 m/s. According to the impulse theorem, the force exerted by the falling rod on the liquid when its fall is suddenly stopped (e.g. by a crane) is F=m dV/dt, where m=1000 kg, dv is 10 m/s and dt is for example 1x10-3 s. After dividing the force by the cross-sectional area, the resulting pressure should be 4x10^10 Pa, or 400 kbar. Can you see anything wrong with this reasoning until here?

Also let's assume that I want to redistribute this 400 kbar pressure across a much larger area. Can I take advantage of Pascal's theorem and assume that the 400 kbar pressure generated inside the narrow tube will be redistributed equally across a larger area below the tube inlet?

Thanks you in advance...Gabriele
 
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I guess what makes my problem slightly more complicated is that the pressure wave that I generate in the liquid is dynamic and not static. In any case the pressure wave should still propagate everywhere across the liquid, right? You can assume that the liquid remains contained and gets compressed upon impact of the 1 ton load (i.e. the diameter of the load rod is exactly that of the tube)...

Gabriele
 
I have big problems with this. Pascal's law applies only to a fluid in static equilibrium. The compression wave you create in the tube will rapidly dissipate once it leaves the tube. I also have a problem with your 1 millisecond. What makes you think that is accurate? Also, once the piston bounces of the top of the fluid, all you will have left is a small confined pulse in the tube. What about elastic deformation of the tube itself? The expansion could be significant, and reduce the pressure pulse. If you really want to figure out what happens, you should consider modelling this system.

Chet
 
I agree that Pascal law requires static equilibrium. I need to think more carefully about a way to generate very high pressures in a liquid. Will keep you posted about any new ideas I will have!
 
Actually upon second thoughts I don't understand why Pascal's law shouldn't apply to a pressure wave just as well as to static pressure. Imagine launching a square wave pressure pulse into a liquid, which remains at rest: the wave front will first impact the liquid and by Pascal's law will propagate equally across the liquid bringing all the liquid to high pressure temporarily, and the same will happen to the final release wave at the end of the pressure pulse which brings the liquid back to ambient pressure. Hence the overall result should be the application of two consecutive pressures throughout the liquid! I think when they say that Pascal's law applies only to liquids in static equilibrium they mean the liquid has to remain at rest and not flow with constant velocity in a certain direction, which is the case in my example...G
 
g_mogni said:
Actually upon second thoughts I don't understand why Pascal's law shouldn't apply to a pressure wave just as well as to static pressure. Imagine launching a square wave pressure pulse into a liquid, which remains at rest: the wave front will first impact the liquid and by Pascal's law will propagate equally across the liquid bringing all the liquid to high pressure temporarily, and the same will happen to the final release wave at the end of the pressure pulse which brings the liquid back to ambient pressure. Hence the overall result should be the application of two consecutive pressures throughout the liquid! I think when they say that Pascal's law applies only to liquids in static equilibrium they mean the liquid has to remain at rest and not flow with constant velocity in a certain direction, which is the case in my example...G
If you can maintain the compression pulse long enough for the pressure wave to propagate throughout the region of interest, then that might be possible. But, outside your tube, there is a much larger mass of liquid to compress. I don't think the velocity of propagation in the larger mass will be the same as for a rectilinear wave, because the propagation will travel spherically (radially outward). The wave equation will be different for the spherical propagation.

Chet
 
As a quick approximation, you could assume the pressure wave propagates at the speed of sound in the liquid, so you could get a rough guess for how quickly the pressure wave would reach the other end of the container. If your impact time is substantially longer than the pressure wave propagation time, you might roughly be correct. Of course, calculating an impact time isn't an easy proposition either.
 
Thanks, do you know any software for modelling such simple fluid mechanics problems?G
 
  • #10
Well I don't necessarily have to use water... I can use a liquid like silicone oil which is commonly used as pressure-transmitting liquid in Diamond Anvil Cell experiments that routinely reach pressures of order 1 Mbar...G
 
  • #12
Yes non-hydrostatic pressure components are something I need to think about, but at least silicone oil remains liquid at high pressures...
 
  • #13
Input terminated
 

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