Calculate Gauge Pressure for Fire Hose Height of 25m w/ Bernoulli's Law

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    Bernoulli's Law
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Homework Help Overview

The problem involves calculating the gauge pressure required in a fire hose to achieve a water spray height of 25 meters, utilizing Bernoulli's equation as a framework for analysis.

Discussion Character

  • Exploratory, Conceptual clarification, Assumption checking

Approaches and Questions Raised

  • The original poster attempts to determine the necessary water velocity for the spray height using conservation of energy, leading to confusion regarding the implications of Bernoulli's law. Some participants question the assumption of negligible velocity inside the hose and its impact on conservation of mass.

Discussion Status

Participants are exploring different interpretations of the problem, particularly regarding the pressure inside the hose versus at the nozzle exit. Some guidance has been offered on selecting points for applying Bernoulli's equation, but no consensus has been reached on the assumptions being made.

Contextual Notes

There is an ongoing discussion about the assumptions related to flow velocity and pressure conditions within the hose, as well as the implications of these assumptions on the application of Bernoulli's equation.

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Homework Statement


What gauge pressure in the water mains is necessary if a fire hose is to spray water to a height of 25 m?


Homework Equations


Bernoulli's equation(?)


The Attempt at a Solution



I tried figuring out what water velocity was needed to make the water spray up 25 meters. The expression I got (using conservation of energy) was

<br /> v_0 = \sqrt{2 g h}<br />

But then I get confused and try to argue that, by Bernoulli's law,

<br /> P_G + \frac{1}{2} \rho v^2 + 0 = 0 + 0 + \rho g h<br />

and so the gauge pressure should be zero (using the expression above for the velocity). Thanks for any help.
 
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When the water exits the hose, the gauge pressure is, in fact, 0. The question is asking what's the pressure inside the hose. You're likely expected to assume that the flow rate is low enough that you can approximate the speed of the water inside the hose to be negligible.
 
How does water move through the hose if its velocity is negligible? Wouldn't this break conservation of mass (as the flow rate near the gauge would be different from that at the end of the hose)?

So if the gauge pressure is zero at the end of the hose, there is only atmospheric pressure: P(absolute) = P(gauge)+P(atmospheric)

Then

<br /> P_G + P_{atmos}+ \frac{1}{2}\rho v^2_g = P_{atmos} + \frac{1}{2} \rho v^2_{opening}<br />

But again, how can you claim the velocity at the gauge is zero (especially when the hose has been turned on for some time)? In order for water to flow, it has to move, right?
 
In this problem, please consider choosing the two points for applying the Bernoulli equation as (1) inside the hose (before the fluid enters the nozzle) and (2) at the top of the spray height z. Also please recognize, as Vela pointed out, that, inside the hose, the ρv2/2 term is implicitly assumed (in the problem statement) to be small compared to the gauge pressure PG.

Chet
 

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