Fluid in rotating tube with different initial levels

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SUMMARY

The discussion focuses on determining the constant C in the pressure equation for fluid in a rotating tube with differing initial fluid heights. The relevant equation is given as p(r,z) = -ρgz + (1/2)ρω²r² + C, where ρ is fluid density, g is gravitational acceleration, ω is angular velocity, and r is the radial coordinate. Participants emphasize that Bernoulli's principle cannot be applied in this scenario due to rotation, and the challenge lies in establishing the condition for C as a function of ω. The resolution of C is deemed essential for progressing with the problem.

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  • Understanding of fluid dynamics principles, specifically fluid rotation.
  • Familiarity with the pressure equation in rotating systems.
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Soren4
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Homework Statement


ddddddd.png


Homework Equations


Fluid in rotation

The Attempt at a Solution


This exercise is quite different from the classic one of fluidi in rotation. Before rotation starts the height in one branch is bigger than in the other, so I do not really know how to approach the problem.

My main difficulty is: how can I determine the constant ##C## in the following expression in this case?

$$p(r,z)=-\rho g z+\frac{1}{2} \rho \omega^2 r^2+C$$

(The frame of reference considered has the ##z## axis towards up and placed on axis of rotation, ##r## is the radial coordinate)

The fact is that I do not really know how to impose the condition for determinimg ##C## as a function of ##\omega## (which is what I want to determine). I think that, once ##C## is determined the rest of exercise is straightforward.

So how can I determine ##C##?
 
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Soren4 said:

Homework Statement


View attachment 103167

Homework Equations


Fluid in rotation

The Attempt at a Solution


This exercise is quite different from the classic one of fluidi in rotation. Before rotation starts the height in one branch is bigger than in the other, so I do not really know how to approach the problem.

My main difficulty is: how can I determine the constant ##C## in the following expression in this case?

$$p(r,z)=-\rho g z+\frac{1}{2} \rho \omega^2 r^2+C$$

(The frame of reference considered has the ##z## axis towards up and placed on axis of rotation, ##r## is the radial coordinate)

The fact is that I do not really know how to impose the condition for determinimg ##C## as a function of ##\omega## (which is what I want to determine). I think that, once ##C## is determined the rest of exercise is straightforward.

So how can I determine ##C##?
In condition a), what is the height of the fluid in the open section? What is the pressure at its top?
 
Soren4 said:
The fact is that I do not really know how to impose the condition for determinimg ##C## as a function of ##\omega## (which is what I want to determine). I think that, once ##C## is determined the rest of exercise is straightforward.
You can't use Bernoulli when the tube is rotated.
Instead:
What total centripetal force is needed to maintain the system in equilibrium when pA = 0.8e5 Pa?
How is this force going to be provided?
 

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