Determining Pipe Pressure of a system that discharges to air

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Discussion Overview

The discussion revolves around calculating the maximum water hammer pressure in a pipe system that discharges to air, specifically focusing on the application of the Bernoulli equation and the challenges in determining pipe velocity and pressure due to insufficient information about the reservoir's depth.

Discussion Character

  • Homework-related
  • Mathematical reasoning
  • Debate/contested

Main Points Raised

  • One participant expresses difficulty in determining water pipe velocity and pressure, noting the need for more details about the reservoir depth.
  • Another participant questions whether the velocity in the pipe should equal the velocity at the exit, suggesting that the volumetric flow rate should be constant and that the pressure at the reservoir should be atmospheric.
  • Some participants agree that the change in elevation from the bottom of the reservoir to the exit is given, but they highlight that this leads to an equation with two unknowns: velocity and pipe pressure.
  • There is a discussion about the cancellation of atmospheric pressures when applying the Bernoulli equation, but uncertainty remains regarding the elevation to the top of the reservoir.
  • One participant acknowledges a missed detail about needing to know the depth of the reservoir to proceed with calculations.

Areas of Agreement / Disagreement

Participants generally agree on the need for additional information regarding the reservoir depth to solve the problem, but there is no consensus on how to proceed with the calculations given the current information.

Contextual Notes

The discussion highlights limitations in the provided problem statement, particularly the lack of information about the total height of the reservoir, which affects the ability to determine both velocity and pressure accurately.

CivilSigma
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Homework Statement


A pipe 30 cm in diameter and 420 m long has a wall thickness of 1 cm. The pipe is commercial steel (ks = 0.045 mm) and carries water from a reservoir to an elevation 100 m below the bottom of the reservoir and discharges into the air. A rotary valve is installed at the downstream end. Minor losses include an entry (kL = 0.5) and rotary valve (kL = 10). Calculate the maximum water hammer pressure that can be expected on the valve if it closes in 0.5 sec. Also determine the total pressure the pipeline will be exposed to during the water hammer phenomenon. Assume: K = 2.2 x 109 N/m2, E = 1.9 x 1011 N/m2

Homework Equations


I am having trouble with determining the water pipe velocity and pipe pressure.
The Bernoulli:

$$ \frac{P_1}{2g} + \frac{v_1^2}{2g}+h_1 = \frac{P_2}{2g} + \frac{v_2^2}{2g}+h_2+ \frac{v^2}{2g}(\lambda \cdot L/D + \sum K_L) $$

The Attempt at a Solution


I am having a really hard with this problem. I think we need more details about the reservoir depth to solve the problem.

Applying the Bernoulli equation from the bottom of the reservoir to the exit of the pipe:

$$ \frac{P_{pipe}}{2g} + \frac{v_{pipe}^2}{2g}+h_1 = \frac{P_{exit}}{2g} + \frac{v_{exit}^2}{2g}+h_2+ \frac{v_{pipe}^2}{2g}(\lambda \cdot L/D + \sum K_L) $$

Exit pressure is atmospheric, and velocity in pipe and at exit are equal.

$$\frac{P_{pipe}}{2g} + \frac{v_{pipe}^2}{2g} = \frac{v_{exit}^2}{2g} - 100 + \frac{v_{pipe}^2}{2g}(\lambda \cdot 450/0.3 + 10.5) $$

So I get this equation with two unknowns velocity ( and lambda depends on v ...) and pipe pressure. Can some one please help - this is so frustrating to solve...
 
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Shouldn't the velocity in the pipe be the same as the velocity at the exit? Shouldn't the volumetic flow rate be constant? Shouldn't the pressure at the reservoir be atmospheric? Isn't this enough to determine the volumetric flow rate?
 
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Chestermiller said:
Shouldn't the velocity in the pipe be the same as the velocity at the exit? Shouldn't the volumetic flow rate be constant? Shouldn't the pressure at the reservoir be atmospheric? Isn't this enough to determine the volumetric flow rate?

Yes I agree with all that - however only the change in elevation of the bottom of the reservoir to the exit is given ( the 100 m) . So, when we apply the Bernoulli there we'll get 1 equation with 2 unknowns : velocity and pipe pressure. But i don't think it's enough to calculate both velocity and pressure
 
sakonpure6 said:
Yes I agree with all that - however only the change in elevation of the bottom of the reservoir to the exit is given ( the 100 m) . So, when we apply the Bernoulli there we'll get 1 equation with 2 unknowns : velocity and pipe pressure. But i don't think it's enough to calculate both velocity and pressure
If you apply the Bernoulli equation between the reservoir and the pipe exit, the atmospheric pressures cancel.
 
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Chestermiller said:
If you apply the Bernoulli equation between the reservoir and the pipe exit, the atmospheric pressures cancel.
Yes I agree, but we don't know what the elevation to the top of the reservoir is. From my understanding the 100 m elevation is from the bottom of the reservoir to the pipe exit, and at the bottom of the reservoir , pressure is not atmospheric
 
Ah. I missed that. It seems to me you need to know the depth of the reservoir.
 
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Chestermiller said:
Ah. I missed that. It seems to me you need to know the depth of the reservoir.

I guess so, I'm going to email my professor to see if there is a type some where in the question. Thank you for the confirmation Chestermiller!
 

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