Height of a fluid in a small tube

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SUMMARY

The discussion focuses on calculating the height of fluid (h2) in a small tube connected to a larger tube using Bernoulli's equation and the continuity equation. The equations applied include Bernoulli's equation, which states that P1 + ρgh1 + 1/2*ρv1² = constant, and the continuity equation A1v1 = A2v2. The final derived formula for h2 is h2 = h1 - 3v²/(2g), indicating that as fluid velocity increases, the height h2 decreases, potentially reaching negative values, which suggests a vacuum condition.

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Ampere
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Homework Statement



An upper tube of cross sectional area A, atmospheric pressure, and height h1 is connected to a lower tube with cross sectional area A/2 (and height 0). A fluid of uniform density rho flows through the system, with velocity v measured in the upper tube. A small open tube branches up off the lower one, with a column of fluid of height h2 inside it. Find h2.

(See attached diagram.)

Homework Equations



Bernoulli's equation,

P1 + pgh1 +1/2*pv12 = constant

Continuity equation,

A1v1 = A2v2

The Attempt at a Solution



Applying Bernoulli's equation between the top of fluid of height h2 and the left endpoint of the system, I got:

(point 1 = left endpoint, point 2 = top of the column with height h2)

P1 = atmospheric
P2 = atmospheric
KE1 = 1/2*rho*v2
KE2 = 0
PE1 = rho*g*h1
PE2 = rho*g*h2

Therefore h2 = h1 + v2/(2g). Is this right? I would think that a faster moving fluid pushes h2 up even higher (with h2 = h1 when v=0).

The continuity equation tells us that the speed of the fluid inside the smaller tube is 2v. But does this even matter?
 

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Welcome to PF!

Hi Ampere! Welcome to PF! :smile:
Ampere said:
Applying Bernoulli's equation between the top of fluid of height h2 and the left endpoint of the system …

No, you can't do that … Bernoulli's equation only applies along a streamline

and the streamline doesn't go up that little tube, does it? :wink:
The continuity equation tells us that the speed of the fluid inside the smaller tube is 2v. But does this even matter?

Yes, because that is in the streamline!
 
Thanks. So in that case you can find the pressure right under the small tube (with height h2 - did this below). But what equation do I use to travel outside the streamline?

P1 = atmospheric
P2 = unknown
KE1 = 1/2*rho*v2
KE2 = 1/2*rho*(2v)2
PE1 = rho*g*h1
PE2 = 0

So P2 = Patm + rho*g*h1 - 3/2*rho*v2
 
Hi Ampere! :smile:
Ampere said:
Thanks. So in that case you can find the pressure right under the small tube (with height h2 - did this below). But what equation do I use to travel outside the streamline?

The fluid in the thin vertical tube is stationary, so just use pressure difference = ρgh :wink:

(technically, you can use any line in a stationary fluid as a streamline … but that doesn't mean you can then tag it onto a "real" streamline in a moving part of the fluid :wink:)
 
So I get

dP = rho*g*h2
P2 - Patm = rho*g*h2

and

h2 = h1 - 3v2/(2g)

So the faster the fluid flows, the lower the height h2 is? Is there actually a flow rate which would make h2 = 0, or even less than 0?
 
Ampere said:
So the faster the fluid flows, the lower the height h2 is?

Bernoulli's equation does mean that when the speed is faster the pressure is lower. :smile:
Is there actually a flow rate which would make h2 = 0, or even less than 0?

work it out! :wink:
 
I found that the speed at which h2=0 is √(2gh1/3).

So if h1 = 1m, then v = 2.556 m/s. What if I had v = 3 m/s, or even 6 m/s? What would be the physical meaning of a negative height?

For example, if we go with h1 = 1m and v = 6 m/s, we get h2 = -4.51m. Huh?
 
Ampere said:
What would be the physical meaning of a negative height?

It would mean you have a vacuum pump! :smile:
 
Ah so air would be sucked into the tube along with the fluid? Interesting!

Thanks, this makes sense now.
 

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