Can I apply Bernoulli's equation to rigid body rotation?

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Discussion Overview

The discussion revolves around the application of Bernoulli's equation to a rotating fluid system, specifically a can of water being spun about its central axis. Participants explore the behavior of the fluid, the nature of streamlines, and the implications of viscosity and pressure gradients in this context.

Discussion Character

  • Exploratory
  • Technical explanation
  • Debate/contested
  • Mathematical reasoning

Main Points Raised

  • One participant proposes using Bernoulli's equation along a specific path in the rotating fluid system, assuming steady state and constant density.
  • Another participant confirms that the streamlines in the rotating fluid are circular and that the analysis is being conducted normal to these streamlines.
  • Some participants express the view that the inner fluid rotates faster than the outer fluid, raising concerns about the validity of Bernoulli's equation due to the presence of curved streamlines and pressure gradients.
  • There is a suggestion that viscosity may not be significant once the system reaches steady state, although it is acknowledged that different parts of the fluid may move at different speeds.
  • A later reply questions the application of Bernoulli's equation, suggesting that a force balance in the radial direction may be necessary to establish a relationship between pressure gradient and fluid speed.
  • One participant references prior discussions about lift and streamlines, indicating confusion about the implications of curvature on pressure and flow rates.
  • Another participant suggests analyzing the system using equations of motion in cylindrical coordinates or through a force balance approach.

Areas of Agreement / Disagreement

Participants do not reach consensus on the applicability of Bernoulli's equation in this scenario. There are competing views regarding the behavior of the fluid, the role of viscosity, and the nature of streamlines.

Contextual Notes

Participants note limitations related to the assumptions of steady state, the effects of viscosity, and the implications of curved streamlines on pressure gradients. The discussion highlights the complexity of fluid dynamics in rotating systems.

RAP1234
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1. The problem statement, all variables and given/know

Say I have a can of water, and I am rotating it about its central axis at a constant angular rate. The water in the tank should make a 3D almost parabolic curve as it touches the the walls of the tank. Can I use Bernoulli's equation along y=0, r =0 ( starting from the minima of my parabola) to the radius (r=R) to solve a problem involving this system? Is P = (1/2) + rho*v^2 = const valid?


Homework Equations



P = (1/2) + rho*v^2 = const

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rig_roth.gif


The Attempt at a Solution



I would think P = (1/2) + rho*v^2 = const may be valid because

if the fluid is rotating with the tank as a rigid body, assuming we are looking at it after it has been spun up and is rotating with constant angular rate, then it is at steady state?

The density of the fluid I am assuming is constant.

I am assuming viscosity is negligible

Are the streamlines just circles and I'm going normal to them?

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Yes, the streamlines are circles, and you're going normal to them.

Chet
 
I had the impression that the inner fluid has a faster rate of rotation than the outer fluid. Also streamlines aren't really streamlines if they are curved. Curvature requires a pressure gradient perpendicular to the direction of flow, and Bernoulli doesn't deal with that. Viscosity is going to have an effect, since different parts of the fluid are moving at different speeds.
 
rcgldr said:
I had the impression that the inner fluid has a faster rate of rotation than the outer fluid.
Once the system reaches steady state, the fluid will be rotating like a rigid body, and the angular velocity will be constant throughout the fluid. Of course the circumferential velocity will be equal to the angular velocity times the radial location.
Also streamlines aren't really streamlines if they are curved.
What could possibly have made you think this? It simply is not correct.
Viscosity is going to have an effect, since different parts of the fluid are moving at different speeds.
Viscosity won't be a factor once the system reaches steady state and the fluid is rotating like a rigid body.

Chet
 
rcgldr said:
I had the impression that the inner fluid has a faster rate of rotation than the outer fluid.
Chestermiller said:
Once the system reaches steady state, the fluid will be rotating like a rigid body
OK, don't recall where I read about this before that gave me the false impression.

rcgldr said:
Also streamlines aren't really streamlines if they are curved. Curvature requires a pressure gradient perpendicular to the direction of flow, and Bernoulli doesn't deal with that.

Chestermiller said:
What could possibly have made you think this? It simply is not correct.
I thought this was mentioned in one or more prior threads about wings and lift. Maybe it was in reference to how lift calculations are based on streamline velocities just outside the boundary layer of a wing and the fact that the streamlines had to be broken up into small componennts along the wing chord to deal with the effects of curvature. I think the issue was that the flow past a cross section of a streamline was supposed to be constant, but if the streamline is curved, the pressure is lower and the flow rate faster on the inner part of the streamline.

Back to the spinning bucket with water. Assuming the angular velocity is constant, then the lowest pressure and lowest speed occurs near the center of the bucket, which would violate Bernoulli, so some other method would need to be used to find a mathematical relationship between the pressure gradient and the speed of the water.
 
Last edited:
rcgldr said:
OK, don't recall where I read about this before that gave me the false impression.
You were probably reading about flow between concentric rotating cylinders.
Back to the spinning bucket with water. Assuming the angular velocity is constant, then the lowest pressure and lowest speed occurs near the center of the bucket, which would violate Bernoulli, so some other method would need to be used to find a mathematical relationship between the pressure gradient and the speed of the water.
A force balance in the radial direction would do the trick.

Rap1234: Have you learned about the Equations of Motion in cylindrical coordinates yet? If not, this can still be analyzed by doing a force balance on an element between r and r + dr, and θ and θ+dθ.

Chet
 

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