Fluid mechanics: Flow and velocity of a fluid

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Discussion Overview

The discussion revolves around fluid mechanics, specifically the flow and velocity of water in a cylindrical tank with a small hole at the bottom. Participants explore how to determine the speed of water both exiting the hole and rising within the tank, considering factors such as height, time, and fluid dynamics principles.

Discussion Character

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

Main Points Raised

  • The original poster (OP) proposes a method to calculate the speed of water using Bernoulli's equation and questions how to analyze the system during the filling process.
  • One participant suggests considering the viscosity of the fluid and the dimensions of the hole to solve for back pressure.
  • Another participant recommends performing a transient mass balance on the volume of liquid in the tank, leading to a differential equation for the system.
  • The OP questions the correctness of their calculations, seeking validation from others.
  • A participant challenges the OP's approach, indicating the need to reference the Navier-Stokes equations for incompressible fluids or orifice flow equations.
  • Another participant notes that if the pressure head is significantly higher than the frictional pressure drop, it can be neglected, providing a mass balance equation for the tank.
  • The OP seeks clarification on the flow equation presented, expressing confusion about the continuity equation's application in this context.
  • A participant explains that the equation discussed is indeed a form of the continuity equation on a macroscopic scale, emphasizing that the downward velocity of the fluid does not vary with depth at any instant.

Areas of Agreement / Disagreement

Participants express various viewpoints on the approach to solving the problem, with no consensus reached on the best method or the correctness of specific calculations. Multiple competing views remain regarding the application of fluid dynamics principles.

Contextual Notes

Some assumptions regarding fluid properties, such as incompressibility and neglecting frictional losses, are discussed but not universally accepted. The discussion includes unresolved mathematical steps and varying interpretations of the continuity equation.

Who May Find This Useful

This discussion may be of interest to students and professionals in fluid mechanics, engineering, and physics, particularly those exploring transient flow systems and mass balance equations.

Pepealej
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I've rencently been thinking about several systems related to fluid mechanics, and I've asked myself the following question:

If I have a cylidrical tank with a small hole in the bottom (the surface area of the hole is small in comparison with that from the tank) and I'm filling the tank with water at a constant flow, how can I determine the speed of the water both coming from the whole and rising up the tank: (A) with respect to the height of the water in the tank, (B) with respect to time.

(This is not homework, although it sounds like so)

I know how to determine the maximum height of a system like this one with a specific flow Q. If the surface area of the cylinder is A and that from the hole is S, we have:

Av_A=Q=Sv_S thus v_S=\frac{Q}{S}
And, using Bernouilli's equation:
P_{at}+\rho g h=p_{at}+ \frac{1}{2}\rho v_S^2
h=\frac{v_S^2}{2g}
But that is considering the end point. Where the system is 'at rest' (there's the same amount of fluid in the tank and we can treat it like a pipe), but I don't know how to study the intermediate steps.

Thanks for your help :)
 
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You need to consider the viscosity of the fluid and the diameter and length of the hole, then solve for the back pressure equaling the static fluid pressure at the depth of the hole.
 
You need to do a transient mass balance on the volume of liquid in the tank. If V is the volume of liquid in the tank, then V = hA. The time rate of change of V is equal to the flow rate in minus the flow rate out. Write a differential equation for this.
 
By the way, the calculaitons I did are correct?
 
Not quite right. You need to take a look at the Navier-Stokes equations for incompressible fluids. Or you can just look up the equations for flow thru an orifice.
 
If the pressure head in the tank is much higher than the frictional pressure drop for flow through the oriface, the latter can be neglected (which is what, at the OPs level of experience, the problem statement intended). The mass balance on the tank is
A\frac{dh}{dt}=Q-Sv_s
with v_s=\sqrt{2gh}

So, A\frac{dh}{dt}=Q-S\sqrt{2gh}

Just solve this differential equation subject to some initial height h0.
 
Chestermiller said:
A\frac{dh}{dt}=Q-S\sqrt{2gh}

Why is the flow through the hole given by:? Q-S\sqrt{2gh} I understand it is the flow that comes in minus the flow that goes out. But when I think of it with the continuity equation, the flow is supposed to be constant.

When does the continuity equation apply?
 
This actually is the continuity equation (mass balance equation) on the macroscopic scale (input minus output = accumulation). On the microscopic scale, if the fluid is incompressible, the divergence of the velocity vector is still equal to zero everywhere in this situation. You know this because, at any instant of time, the downward velocity of the fluid in the tank is not varying with depth.

Chet
 

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