Water in a tank being driven up and down

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Discussion Overview

The discussion revolves around the dynamics of water in a tank that is being driven up and down, specifically examining the relationship between the tank's motion and the pressure field within the water. Participants explore the implications of ignoring gravity, the effects of acceleration on pressure, and the modeling of these phenomena in computational fluid dynamics (CFD).

Discussion Character

  • Exploratory
  • Technical explanation
  • Mathematical reasoning
  • Experimental/applied

Main Points Raised

  • Some participants propose that moving the tank up and down can be modeled as a time-varying pressure field, while others question the validity of this assumption without gravity.
  • There is a discussion about the relationship between the height of the tank and the pressure field, with some arguing that using the same variable names in different contexts leads to confusion.
  • Participants explore the idea of replacing gravitational effects with an equivalent acceleration due to the tank's motion, suggesting that the pressure can be modeled with a time-dependent gravitational term.
  • One participant suggests that a body force proportional to the tank's motion could be used in CFD analysis to simulate the effects of the tank moving up and down.
  • There is a proposal to use the linearized Bernoulli equation to relate pressure and velocity potential in the context of the tank's motion.
  • Some participants discuss the implications of frequency changes on the system, suggesting that a frequency sweep could be modeled as a time-varying height function.

Areas of Agreement / Disagreement

Participants express differing views on the role of gravity in the analysis, with some advocating for its inclusion while others explore the implications of ignoring it. The discussion remains unresolved regarding the best approach to model the dynamics of the water in the tank under the described conditions.

Contextual Notes

Participants note that the assumptions made about gravity and acceleration may affect the validity of the models discussed. There are also concerns about the accuracy of the physical representation when using variable names interchangeably in different equations.

  • #31
So the liquid is not displacing up and down like a rigid body?
 
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  • #32
Chestermiller said:
So the liquid is not displacing up and down like a rigid body?
The tank that holds the liquid is a rigid body. The liquid inside is not. Think the approximation was initially done here.
 
  • #33
joshmccraney said:
Funny you say this, because we're actually sending a rocket up to the ISS this September (so perhaps not on earth). And we go up and down because the experiments are controlled this way (I don't do the experiments, just the math mentioned above). The theory suggests looking at oscillations normal to the equilibrium configuration (zero-g, so perfect curvature arc). Vibrating up and down isn't perfect, but the experiments agree very well with theory.
Should be interesting, these experiments. But with zero g you don't even have an equilibrium liquid surface.
I take it no XL heavy beam as described in the link is going up; what is the scale of the experiment ?

Anything else you forgot to mention ? Any preliminary practical tests in zero g planes or at NASA 0 g ?
 
  • #34
joshmccraney said:
The liquid pressure waves, specifically capillary pressure. There's an analogy that can be drawn from the linearized Navier-Stokes equations to a damped harmonic oscillator. The eigenvalues of this equation are the fundamental frequencies of the liquid, call the first ##\Omega_1##. When we turn the shaker table (think elevator) on at a particular frequency (##h=A\cos (\Omega t)##) we get minimal response (can't see the drop of water do anything). However, as we sweep through a range of frequencies, once ##\Omega=\Omega_1## we see a large disturbance in the shape of the predicted mode. As the frequency sweep exceeds ##\Omega_1##, the disturbances die down again (until ##\Omega_2##).
What happens if you set the frequency directly to ##\Omega=\Omega_1## ? Is the "sweep" somehow relevant here?

And what do you mean by "drop of water". I thought it's a tank with water. Is the tank filled completely and closed, or does the water have have a free surface?
 
  • #35
BvU said:
Should be interesting, these experiments. But with zero g you don't even have an equilibrium liquid surface.
The equilibrium in zero g is a circular arc (in 2D). So taking normal disturbances from that.

BvU said:
I take it no XL heavy beam as described in the link is going up; what is the scale of the experiment ?
Yea, definitely not a heavy beam. The scale is several cm footprint drops, so pretty big.

BvU said:
Anything else you forgot to mention ? Any preliminary practical tests in zero g planes or at NASA 0 g ?
I don't think so. Again, I pretty much just do the math, but some modeling enters and I like to double check with you all on here.

Should say we have done lots of terrestrial work below the capillary length scale. Have also worked with a university using their drop tower. But no aircraft tests (those would be fun I think though)!

A.T. said:
What happens if you set the frequency directly to ##\Omega=\Omega_1## ? Is the "sweep" somehow relevant here?
Yea, my first thought was to do this. But numerics and experiments don't always agree with theory, so while we should see resonance, perhaps not. Even a 5% error could cause lots of confusion without a sweep.

A.T. said:
And what do you mean by "drop of water". I thought it's a tank with water. Is the tank filled completely and closed, or does the water have have a free surface?
Sorry, I mixing and matching terms here (mainly because I was only interested in the shaker table up and down).

Some of our tests do drops of water on the shaker table. Something I'm looking at is liquid in channels (tanks), which are on shaker tables. And yea, they have a free surface (not closed).
 

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