Maximizing Water Height in a Tank: Solving a Fluid Velocity Problem

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Discussion Overview

The discussion revolves around a fluid dynamics problem involving a tank of water with an open-ended pipe. Participants are attempting to determine the maximum height of water exiting the pipe as a function of the angle at which the pipe is positioned. The conversation includes theoretical considerations, mathematical reasoning, and the application of projectile motion principles.

Discussion Character

  • Technical explanation
  • Mathematical reasoning
  • Exploratory

Main Points Raised

  • One participant proposes that the velocity of water leaving the pipe can be expressed as sqrt(19.62(H-L sin theta)), considering the height of the water column above the exit point.
  • Another participant agrees with the expression for the vertical component of the velocity as [sqrt(19.62(H-L*sin theta))] * sin theta, but questions the inclusion of an additional term related to the height of the pipe.
  • There is a suggestion to calculate the maximum height by adding the vertical component of the water's velocity to the height of the pipe, L sin theta, although one participant cautions against adding velocity to distance.
  • A method involving the use of projectile motion equations is discussed, with one participant suggesting to use the formula d=(vf^2-vo^2)/2a to simplify the calculations.
  • Another participant mentions the possibility of substituting a time variable in the calculations, which is acknowledged as a valid approach.

Areas of Agreement / Disagreement

Participants express varying opinions on the correct approach to calculating the maximum height, with some agreeing on the use of certain equations while others raise questions about specific terms and their relevance. The discussion does not reach a consensus on a single method or formula.

Contextual Notes

Participants note the importance of correctly distinguishing between velocity and distance in their calculations. There are also references to unresolved assumptions regarding the time variable and the specific conditions under which the equations apply.

bossler
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Problem- I do not have a picture of the example so I will do my best to describe it.

Water is in a large tank of depth H. On the side of tank, on the very bottom, an open ended pipe of length L leaves the tank at angle theta. The question asks to determine the maximum height of the water (h) leaving the pipe as a function of angle theta.

I know that velocity = the square root of (2gH), so using SI units, my velocity at the very bottom of the tank would be the square root of 19.62H. However the exit to the pipe is higher than the bottom of the tank, so would my velocity leaving the pipe be sqrt (19.62(H-L sin theta))? If this is the case, would the velocity of water leaving the pipe be (sqrt(19.62(H-L sin theta))) sin theta + L sin theta?

I hope my description of the example is clear enough. Any suggestions/help is always appreciated.
Thanks
 
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bossler said:
Problem- I do not have a picture of the example so I will do my best to describe it.

Water is in a large tank of depth H. On the side of tank, on the very bottom, an open ended pipe of length L leaves the tank at angle theta. The question asks to determine the maximum height of the water (h) leaving the pipe as a function of angle theta.

I know that velocity = the square root of (2gH), so using SI units, my velocity at the very bottom of the tank would be the square root of 19.62H. However the exit to the pipe is higher than the bottom of the tank, so would my velocity leaving the pipe be sqrt (19.62(H-L sin theta))?

That seems to be correct to me for the velocity leaving the pipe at the angle theta.

If this is the case, would the velocity of water leaving the pipe be (sqrt(19.62(H-L sin theta))) sin theta + L sin theta?

I'm not sure I understand what you are asking in this part. If you mean the vertical component of the velocity leaving the pipe would be

[sqrt (19.62(H-L*sin theta))] * sin theta

I would agree.

I don't see where the extra term " + L sin theta " would come into play for the velocity, as that is a measure of the vertical height of the end of the pipe. It should be added to the vertical distance the water would travel after leaving the end of the pipe, not the velocity.
 
I understand what you are saying. I am trying to determine distance h (max height between stream of water and the ground). To do this would I add the vertical component of the water velocity ([sqrt (19.62(H-L*sin theta))] * sin theta) and the vertical component of the pipe L (L sin theta)? Am I missing something?
 
bossler said:
I understand what you are saying. I am trying to determine distance h (max height between stream of water and the ground). To do this would I add the vertical component of the water velocity ([sqrt (19.62(H-L*sin theta))] * sin theta) and the vertical component of the pipe L (L sin theta)? Am I missing something?

You cannot add a velocity to a distance. Use the velocity to determine the maximum vertical distance the water will travel, then add the height of the pipe.
 
So I will take my initial height, L sin theta, and add it to (([sqrt (19.62(H-L*sin theta))] * sin theta) T), and subtract acceleration due to gravity (-4.9T^2). This I hope will give me h.
 
bossler said:
So I will take my initial height, L sin theta, and add it to (([sqrt (19.62(H-L*sin theta))] * sin theta) T), and subtract acceleration due to gravity (-4.9T^2). This I hope will give me h.

I don't think you have a value for T. But you do have Vfinal (at least in terms of a vertical component), Vinitial, and acceleration due to gravity. You can calculate the maximum height from that information (refer to equations useful in projectile motion).
 
Would it work if I substituted in (vy - vyo)/g for t? If I did that it would be ((([sqrt (19.62(H-L*sin theta))] * sin theta) T) - 0)/9.81 ?
 
bossler said:
Would it work if I substituted in (vy - vyo)/g for t? If I did that it would be ((([sqrt (19.62(H-L*sin theta))] * sin theta) T) - 0)/9.81 ?

That will work fine. :cool:

I was actually thinking of avoiding the calculation of time altogether by using the formula vf2 = vi2 + 2ad, but either way will give you the same answer if you crunch the numbers properly.
 
Alright well I'm glad to see I'm making some progress. The equation you mentioned I had forgot about, and certainly makes things a bit simpler when not having to use time. If I used that equation I would set the formula up as d=(vf^2-vo^2)/2a ,with vf^2 being 0, and vo^ being ([sqrt (19.62(H-L*sin theta))] * sin theta)^2. Then divide by 2(9.81). Once that is done I would need to add my initial height L sin theta, to give me my total displacement h. Does this make sense?
 
  • #10
bossler said:
Alright well I'm glad to see I'm making some progress. The equation you mentioned I had forgot about, and certainly makes things a bit simpler when not having to use time. If I used that equation I would set the formula up as d=(vf^2-vo^2)/2a ,with vf^2 being 0, and vo^ being ([sqrt (19.62(H-L*sin theta))] * sin theta)^2. Then divide by 2(9.81). Once that is done I would need to add my initial height L sin theta, to give me my total displacement h. Does this make sense?

That makes sense to me. I think you're all set now.
 
  • #11
Thanks a lot for the help
 

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