How Does Water's Surface Shape Change in a Rotating Container?

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SUMMARY

The discussion focuses on calculating the depression of water's surface in a rotating cylindrical container. The container has a radius of 6.0 cm and is placed on a turntable rotating at 33.33 revolutions per minute, resulting in an angular velocity of 3.49 rad/s. The derived formula for the depression is characterized as w²R²/4g, leading to a calculated depression of 0.65 cm. Participants clarify the forces acting on the water surface, including gravity and centripetal force, and discuss the integration method to derive the surface shape.

PREREQUISITES
  • Understanding of angular velocity and its conversion (e.g., from revolutions per minute to rad/s).
  • Familiarity with the principles of centripetal force and gravitational force.
  • Knowledge of calculus, specifically integration techniques.
  • Basic concepts of fluid mechanics, particularly surface tension and hydrostatic pressure.
NEXT STEPS
  • Study the derivation of fluid surface shapes in rotating systems.
  • Learn about the effects of centripetal acceleration on fluid dynamics.
  • Explore the integration of differential equations in fluid mechanics.
  • Investigate the relationship between angular velocity and fluid pressure distribution.
USEFUL FOR

Physics students, fluid mechanics researchers, and engineers involved in rotational dynamics and fluid behavior analysis will benefit from this discussion.

mrojc
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Homework Statement

A cylindrical container of water with a radius of 6.0 cm is placed on a phonograph turntable so that its outer edge just touches the outer edge of the turntable. The radius of the turntable is 14.5 cm, and the turntable rotates at 33 and a 1/3 revolutions per minute. How much is the water depressed in the centre compared to the outer edge of its container?[/B]

Homework Equations

gz − 1/2 ω2 (x2 + y2 ) = constant[/B]

The Attempt at a Solution

I know that x2+y2 is equal to the radius squared. I think from my notes it's equal to the radius squared of the water in the container. So plugging this in, and omega I calculated to be 3.49 rad/s, I get a height of 0.0022 m. I'm not sure where to go from here though.[/B]
 
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The height is an answer to the problem, so what more do you want to do?
 
So you don't need to calculate another answer using the 14.5 cm?
 
It is not clear to me what center the problem is referring to, as the glass with water is not over the center of the turntable.
So probably the center of the glass with water.
 
How do you get an omega of 3.49 rev/s, when the problem says omega is 33.33 rev/min?

Omega in units of seconds is 0.56 rev/s.
 
mrojc said:
@DuckAmuck I converted it to rad/s
my bad, i read "rad" as "rev".
 
So I get a depression can be characterized as w^2 R^2 /4g, which results in 0.65 cm.
 
@DuckAmuck Might I ask how did you get that, if that's ok?
 
  • #10
mrojc said:
@DuckAmuck Might I ask how did you get that, if that's ok?
The depression is defined as original height of the liquid when it is not spinning, minus the central height when it is spinning?
 
  • #11
Why is it 4g though? Should it not be 2g?
 
  • #12
So there are two forces acting on the surface, gravity and centripetal force. The acceleration from gravity is g, the acceleration from centripetal force is a.
a is defined as a = rw^2.
The infinitesimal elements of the surface are dr (radial distance), dz (vertical distance).
The ratio between the forces and the elements are equal such that:
dz/dr = rw^2/g

Now integrate to get z(r). Then keep in mind the volume is still the same as when it was standing still to find the depression.
 
  • #13
mrojc said:
Why is it 4g though? Should it not be 2g?
It's possible I missed a factor of 2.
 
Last edited:

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