Centrifugal Force and shape of water

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Discussion Overview

The discussion centers on the shape of the water surface in a rotating cylinder and whether it forms a parabola under the influence of centrifugal force. Participants explore the theoretical implications and mathematical derivations related to this phenomenon.

Discussion Character

  • Exploratory
  • Technical explanation
  • Mathematical reasoning

Main Points Raised

  • One participant inquires about the shape of the water in a spinning cylinder and whether it can be determined to be a parabola.
  • Another participant asserts that the surface of the rotating water will indeed assume a parabolic shape, suggesting that this can be derived from examining the forces acting on the water surface.
  • A participant proposes a specific equation for the parabolic shape, stating it as \(y = \frac{\omega^2}{2g} x^2\), and seeks confirmation of this derivation.
  • Another contributor mentions that the water surface acts as an equipotential surface in a corotating frame of reference.
  • One participant questions whether the turntable or the cylinder is being rotated, suggesting that water may spill out due to inertia in one scenario.
  • Further mathematical derivations are presented, with one participant attempting to reconcile kinetic and potential energy to arrive at the parabolic equation.
  • Another participant offers an alternative derivation using Newton's second law, emphasizing the forces acting on a mass element at the water surface.
  • One participant expresses confusion regarding the derivation presented by another, indicating a lack of understanding but later acknowledges clarity after further explanation.

Areas of Agreement / Disagreement

While some participants agree on the parabolic shape of the water surface and propose similar equations, there is no consensus on the derivations or the implications of the forces involved. Disagreements exist regarding the conditions under which water may spill out during rotation.

Contextual Notes

Participants' derivations depend on various assumptions about the forces acting on the water surface and the frame of reference used. Some calculations may rely on specific conditions that are not universally agreed upon.

amcavoy
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"Centrifugal" Force

Say you have a cylinder of radius r with πr2h liters of water in it. If you put it on some sort of turntable and spin it with an angular velocity ω, is there a way to tell what the shape of the water will be? I mean, if you look at the cross section will you be able to find out if it forms for example, a parabola?

This isn't a homework problem or anything, I'm just curious. Thanks for your help.
 
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Actually, the rotating water surface will assume the form of a parabola. The way to figure that out is to examine the forces on a element of the water surface. The net force is centripetal.
 
Doc Al said:
Actually, the rotating water surface will assume the form of a parabola. The way to figure that out is to examine the forces on a element of the water surface. The net force is centripetal.

Relative to some origin (let's say the vertex), is there a way to find the equation of that parabola or is the shape the most that can be determined?
 
According to my calculation, the equation (using the vertex as the origin) should be:
y = \frac{\omega^2}{2 g} x^2
 
Said another way,the surface of the water will be an equipotential surface in a corotating frame of reference.
 
Are you rotating just the turntable or the cylinder as well? In the former case I think some water will fall out due to its inertia of rest.Tell me if I am wrong,and also if water would fall out in the latter case too.
 
Doc Al said:
According to my calculation, the equation (using the vertex as the origin) should be:
y = \frac{\omega^2}{2 g} x^2

Is this shown by the following?:

E_k=E_p\implies v=\sqrt{2gh}

y=h;\quad x=r

\frac{ds}{dt}=v=x\frac{d\theta}{dt}=x\omega

\sqrt{2gy}=x\omega\implies y=\frac{{\omega}^2}{2g}x^2

This was the only way I could derive the equation you posted above, and I figured that the kinetic energy would be the same as the potential energy because if you look at a single molecule of water, it is doesn't experience any friction because it is rotating with every other molecule. Also, I just said that the distance from the center of the cylinder r was x (since the origin is the center) and the height above that center is y. Am I correct with what I posted above?

Thanks again.
 
I can't say I understand your derivation or reasoning, but maybe I'm just dense today.

Here's how I would derive it (from an inertial frame). Take an element of mass on the surface. The force due to the water/air pressure must be perpendicular to the surface. Call that force F. The only other force is the weight, mg. Applying Newton's 2nd law to vertical and horizontal components gives:
F \cos \theta = mg
F \sin \theta = m\omega^2 x
where \theta is the angle the tangent to the curve makes with the horizontal axis, thus:
\tan \theta = dy/dx = \frac{\omega^2}{g} x
y = \frac{\omega^2}{2g} x^2

Viewed from the rotating frame, the derivation is even simpler. Just realize that the surface of the fluid will be perpendicular to the direction of the apparent "gravity": the sum of real gravity plus the outward centrifugal force.
 
For an excellent practical application of this idea, check this out.
 
  • #10
Doc Al said:
I can't say I understand your derivation or reasoning, but maybe I'm just dense today.

Here's how I would derive it (from an inertial frame). Take an element of mass on the surface. The force due to the water/air pressure must be perpendicular to the surface. Call that force F. The only other force is the weight, mg. Applying Newton's 2nd law to vertical and horizontal components gives:
F \cos \theta = mg
F \sin \theta = m\omega^2 x
where \theta is the angle the tangent to the curve makes with the horizontal axis, thus:
\tan \theta = dy/dx = \frac{\omega^2}{g} x
y = \frac{\omega^2}{2g} x^2

Viewed from the rotating frame, the derivation is even simpler. Just realize that the surface of the fluid will be perpendicular to the direction of the apparent "gravity": the sum of real gravity plus the outward centrifugal force.

Ahh, ok that makes sense. I don't know what I was thinking when I derived it the other way :rolleyes:

Thanks for the help :smile:
 

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