Max Height Attained by Water Stream in P9.81 Tank

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Homework Help Overview

The discussion revolves around a physics problem involving a water tank with a valve, where participants are tasked with determining the maximum height attained by a water stream when the valve is opened. The problem involves concepts from fluid dynamics, specifically Bernoulli's equation, and projectile motion.

Discussion Character

  • Exploratory, Conceptual clarification, Mathematical reasoning, Assumption checking

Approaches and Questions Raised

  • Participants discuss the application of Bernoulli's equation and the implications of pressure at different points in the system. There are attempts to clarify the initial and final heights in relation to the water stream's trajectory. Questions arise regarding the interpretation of pressure conditions and the components of velocity affecting the height calculation.

Discussion Status

The discussion is active, with participants exploring various interpretations of the problem. Some have offered insights into the relationship between pressure and height, while others have expressed confusion about the initial conditions and the correct application of equations. A participant claims to have solved the problem independently, suggesting that some clarity has been achieved, though not all participants are in agreement on the method.

Contextual Notes

There is mention of assumptions regarding gauge pressure and the reference points for measuring height. The problem constraints include specific values for height and angles, which are critical for the calculations but are not fully resolved in the discussion.

parwana
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Homework Statement


Figure P9.81 shows a water tank with a valve at the bottom. If this valve is opened, what is the maximum height attained by the water stream coming out of the right side of the tank? Assume that h = 8.0 m, L = 1.50 m, and = 30° and that the cross-sectional area at A is very large compared with that at B.
p9_81.gif



Homework Equations


Bernouli's equation
P1 + 1/2(density)(v1)^2 + density(g)(y)= P2 + 1/2(density)(v2)^2 + density(g)(y)

The Attempt at a Solution



0+0+density(g)(y)= 0+1/2(density)(v2)^2 + density(g)(Lsin30)

I tried solving for v2


I am stuck now at this step

used that v2 as v initial to find y by

vfinal^2= vinitial^2-2g(y final-y initial)

I am not sure but would v initial be the v2 I found? And is v final 0? Also what is y final and what is y initial?

HELP
 
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Why do you think P1 and P2 are zero?. The water is being launched at an angle. Only the vertical component enters into the height calculation.
 
so the vertical component, which is Lsin30, is that the initial height? I am confused, I tried this again and again but I can't egt it right. And the gauge pressure is 0 since the air is touching the water, air's pressure is 1 atm
 
parwana said:
so the vertical component, which is Lsin30, is that the initial height? I am confused, I tried this again and again but I can't egt it right. And the gauge pressure is 0 since the air is touching the water, air's pressure is 1 atm

I assume they want the maximum height measured from the same place as the 8m height, but maybe they want it measured from where it leaves the spout. The second is easier, but the first can be obtained by just adding Lsinθ. You are OK on the pressure. I was misinterpreting. The height changes from 8m to Lsinθ to the height relative to the end of the spout. Using that (as I think you have done) you can solve for v at the exit of the spout. The vertical component of that velocity is v*sinθ. You can compute the height relative to the end of the spout by finding the point where the vertical velocity is zero. You can either do that by computing the time it takes to reach that point and plugging that into the y(t) equation, or you can use the equation that relates the change in the velocity squared to acceration and distance.
 
Last edited:
Hey, I solved it myself and get 1.8125 metres (I presume you already know the answer and need the method). Your method is flawed.

The Bernoulli equation tells us that the mechanical energy per unit mass, let's call it E is:

E = gz + v2/2 + (p-p0)/rho.

E = gravitational potential energy + kinetic energy + pressure energy.

When you open the valve you just say that the mechanical energy at A is the same as that at B. Because the pressure energy is the same at these points they cancel from both sides. Furthermore, because the cross-sectional at A is much larger than that at B you can ignore the kinetic energy at A. You end up with a fairly simple equation that you have to solve for velocity. Once you've got that velocity you need to find how high it gets which will involve a little projectile mechanics, if I could do it I'm sure you can.
 
thank u so much guys, I understand the method better now
 

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