How Does Nozzle Elevation Affect Water Flow and Pressure in a Hose System?

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Nozzle elevation significantly impacts water flow and pressure in a hose system. As the nozzle is elevated 1.3 meters, the speed of water exiting the nozzle can be determined using Bernoulli's principle and the continuity equation. The flow rate remains constant throughout the hose due to water's incompressibility, meaning the velocity decreases as elevation increases. The gauge pressure at ground level can be calculated by considering the potential energy change due to elevation. Understanding these principles is crucial for analyzing fluid dynamics in hose systems.
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Homework Statement



Frensley_Fluids_Bernoulli_001.gif


Consider a hose that carries water (density = 1000 kg/m3) leads to a nozzle that is elevated h = 1.3 meters above the ground. The nozzle has a diameter d, and the hose has a diameter D = 5d. Water flows through the hose with a speed vH = 0.6 m/s.

(a) What is the speed of the water as it leaves the nozzle?


(b) What is the gauge pressure of the water in the hose at ground level?

Homework Equations



P+pgh+(1/2)pV^2 = P+pgh+(1/2)pV^2
Area * V = Area * V

The Attempt at a Solution


I'm confused on the part where the hose is elevated upward, I know the velocity decreases, but I don't know by how much.
 
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Is water compressible or incompressible? What does that imply for the flow rate at any point along the (constant diameter) hose?
 
It is compressible, does that mean it stays the same throughout?
 
asheik234 said:
It is compressible, does that mean it stays the same throughout?

Are you guessing? If water is compressible, why can't we store a cubic meter of water in a one liter container? :smile:

For all practical purposes, water is NOT compressible. So for a filled, constant diameter pipe, the flow rate must be the same everywhere -- otherwise, wouldn't water "pile up" behind the slow regions and "thin out" in the speedy ones?
 
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