Fluid dynamics: Initial velocity of milk outflow from carton

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Homework Help Overview

The discussion revolves around determining the initial velocity of milk outflow from a carton with a hole punched 10cm below the top. The problem is situated within the context of fluid dynamics, specifically exploring concepts related to pressure, energy conservation, and flow dynamics.

Discussion Character

  • Exploratory, Conceptual clarification, Mathematical reasoning, Assumption checking

Approaches and Questions Raised

  • Participants discuss the application of Bernoulli's equation and Torricelli's Law, questioning the assumptions made regarding pressure at the hole and the effects of fluid density. There are attempts to derive the initial velocity using energy conservation principles, while some participants express confusion about the initial conditions of fluid flow and the implications of compressibility.

Discussion Status

The discussion is active with various interpretations being explored. Some participants have provided insights into the derivation of relevant equations and the conditions under which they apply. There is no explicit consensus yet, but several lines of reasoning are being examined, particularly regarding the initial conditions of fluid flow and the assumptions about pressure.

Contextual Notes

Participants note that the problem may be tricky, particularly in relation to the immediate flow conditions after the hole is created. There are discussions about the assumptions of steady flow and the effects of elevation on pressure, as well as the implications of fluid compressibility on the initial velocity of outflow.

vetgirl1990
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Homework Statement


A hole is punched in a full milk carton, 10cm below the top. What's the initial velocity of outflow?

Homework Equations


P2 = P1 + ρgh
Conservation of energy of fluids: P2 + 1/2ρv22 + ρgy2 = P1 + 1/2ρv12 + ρgy1

The Attempt at a Solution


Set the top of the carton as P1, and the point 10cm below the surface as P2.
Assume that milk has the same density as water: 1000kg/m3

P1 = atmospheric pressure = 101325Pa
P2 = 101325 + 1000(9.8)(0.1) = 102305Pa

P2 + 1/2ρv22 + ρgh2 = P1 + 1/2ρv12 + ρgy1
The milk doesn't have kinetic energy at the top of the carton, so K=1/2ρv22 =0
At 10cm below the surface, y=0 (although this is still elevated above the ground, we're trying to find the change in energy between the top of the carton and hole punched in it); therefore U = ρgy1 = 0

P2 + ρgh2 = P1 + 1/2ρv12
102305 + 1000(9.8)(0.1) = 101325 + 1/2(1000)v12
103285 - 101325 = 500v12
V1 = 1.98m/s Is my method correct? The actual answer is V=1.4m/s, but perhaps it's because I assumed that the density of milk is the same as water...
 
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I think you'll find that for the fluid stream coming out of the hole the pressure is atmospheric pressure. That's the environment it is in as soon as it passes through the wall of the carton, and that's where you want to determine its speed. So the pressure terms should cancel, and you're left with the energy change due to the change in elevation.

Essentially this is the derivation of Torricelli's Law. I think a web search on that will be helpful :smile:
 
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vetgirl1990 said:

Homework Statement


A hole is punched in a full milk carton, 10cm below the top. What's the initial velocity of outflow?

Homework Equations


P2 = P1 + ρgh
Conservation of energy of fluids: P2 + 1/2ρv22 + ρgy2 = P1 + 1/2ρv12 + ρgy1

The Attempt at a Solution


Set the top of the carton as P1, and the point 10cm below the surface as P2.
Assume that milk has the same density as water: 1000kg/m3

P1 = atmospheric pressure = 101325Pa
P2 = 101325 + 1000(9.8)(0.1) = 102305Pa

P2 + 1/2ρv22 + ρgh2 = P1 + 1/2ρv12 + ρgy1
The milk doesn't have kinetic energy at the top of the carton, so K=1/2ρv22 =0
At 10cm below the surface, y=0 (although this is still elevated above the ground, we're trying to find the change in energy between the top of the carton and hole punched in it); therefore U = ρgy1 = 0

P2 + ρgh2 = P1 + 1/2ρv12
102305 + 1000(9.8)(0.1) = 101325 + 1/2(1000)v12
103285 - 101325 = 500v12
V1 = 1.98m/sIs my method correct? The actual answer is V=1.4m/s, but perhaps it's because I assumed that the density of milk is the same as water...
The density of milk is not your problem here.

Review the derivation of Torricelli's Law from the Bernoulli equation:

https://en.wikipedia.org/wiki/Torricelli's_law
 
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gneill said:
I think you'll find that for the fluid stream coming out of the hole the pressure is atmospheric pressure. That's the environment it is in as soon as it passes through the wall of the carton, and that's where you want to determine its speed. So the pressure terms should cancel, and you're left with the energy change due to the change in elevation.

Essentially this is the derivation of Torricelli's Law. I think a web search on that will be helpful :smile:

Extremely useful, thank you so much!

My logic (although wrong) was that the pressure at the hole would be affected by the volume of milk above it, which would have a direct effect on speed of the milk leaving the carton.
I suppose using P2 = P1 + ρgh then, would only be applicable [if for some reason], they were asking what the pressure was at the bottom of the carton vs. the top, in a closed container with no holes.
 
vetgirl1990 said:
Extremely useful, thank you so much!

My logic (although wrong) was that the pressure at the hole would be affected by the volume of milk above it, which would have a direct effect on speed of the milk leaving the carton.
I suppose using P2 = P1 + ρgh then, would only be applicable [if for some reason], they were asking what the pressure was at the bottom of the carton vs. the top, in a closed container with no holes.
Yes. That's why it's called the hydrostatic equation.
 
vetgirl1990 said:
What's the initial velocity of outflow?
This is rather a tricky question, too tricky for the question setter, it seems.
Torricelli's Law does not apply to the flow immediately after creating the hole. It applies only once a steady flow has been established.
The difference is observable. If you pull a plug out near the bottom of a barrel you will see the flow strengthen for the first second, or thereabouts.
The immediate flow can be estimated by considering rate of change of momentum. The water inside the tank, near the hole, is going from a standing start. If it exits at speed v through a hole area A, the mass flow rate is ##\rho A v##, the rate of gain of momentum is ##\rho A v^2##, which therefore equals the force ##\rho h g A##. This gives ##v=\sqrt{gh}##.
To get the ##\sqrt{2gh}## answer, it would be better to state that after some seconds the water is 10cm above the hole, and ask what the velocity is then.
 
haruspex said:
This is rather a tricky question, too tricky for the question setter, it seems.
Torricelli's Law does not apply to the flow immediately after creating the hole. It applies only once a steady flow has been established.
The difference is observable. If you pull a plug out near the bottom of a barrel you will see the flow strengthen for the first second, or thereabouts.
The immediate flow can be estimated by considering rate of change of momentum. The water inside the tank, near the hole, is going from a standing start. If it exits at speed v through a hole area A, the mass flow rate is ##\rho A v##, the rate of gain of momentum is ##\rho A v^2##, which therefore equals the force ##\rho h g A##. This gives ##v=\sqrt{gh}##.
To get the ##\sqrt{2gh}## answer, it would be better to state that after some seconds the water is 10cm above the hole, and ask what the velocity is then.
Hi haruspex,

I'm a little confused. :confused: Shouldn't the velocity be zero when you first pull the plug since there have been no impulsive forces applied? I mean, doesn't it take time for the fluid to accelerate?
 
Chestermiller said:
Hi haruspex,

I'm a little confused. :confused: Shouldn't the velocity be zero when you first pull the plug since there have been no impulsive forces applied? I mean, doesn't it take time for the fluid to accelerate?
Yes, but consider the first 'plug' of water to emerge. It will accelerate from nothing as it emerges, but by the time it is clear of the hole and falling freely it will have reached roughly the velocity calculated from force. An experiment is in order.
 
haruspex said:
Yes, but consider the first 'plug' of water to emerge. It will accelerate from nothing as it emerges, but by the time it is clear of the hole and falling freely it will have reached roughly the velocity calculated from force. An experiment is in order.
In my judgement, only if the compressibility of the water were taken into account could this happen. Otherwise, to satisfy continuity, any initial velocity of any part of the water would mean that all the water would have to be moving initially. If compressibility were included, then an infinitecimal amount of water could start emerging at finite velocity without all the water it being affected.
 
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Chestermiller said:
In my judgement, only if the compressibility of the water were taken into account could this happen. Otherwise, to satisfy continuity, any initial velocity of any part of the water would mean that all the water would have to be moving initially. If compressibility were included, then an infinitecimal amount of water could start emerging at finite velocity without all the water it being affected.
No, I think you miss the point of my last post.
I agree that if you were to watch the emergence of the stream from the hole in the first microseconds then it would accelerate from a negligible velocity. But the front of that continues to be accelerated by the pressure of the water behind. Yes, a pedantic reading of "initial velocity" could justify an answer of 0. But a reasonable interpretation of the initial velocity of outflow would be the horizontal speed that the first 'plug' of water reaches.
My argument is that even if we abjure pedantry and allow an interpretation that makes the question interesting, the given answer is still wrong.
 

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