Fluid Mechanics Question - Pipes and Pumps

In summary, the task is to design a system to deliver 1 m^3/s of water from reservoir A at elevation 300m to reservoir B at 500m, with a distance of 1000km between them. The elevation between the two reservoirs can be approximated as parabolic, with a maximum elevation of 660m reached 600km from A. Negative pressures should not exceed 70% of atmospheric pressure to prevent cavitation. A steel pipe with a roughness of 0.5cm and diameter of 1.1m, and a pressure rating of 150m head, is available. The pumps can deliver 1m^3/s at 100m head. Calculations are being done
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eyraincg
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Fluid Mechanics Question -- Pipes and Pumps

Homework Statement



Design a system to deliver [itex]1 m^{3}/s[/itex] of water from reservoir A at elevation 300m to reservoir B at 500m. The distance from A to B is 1000km (1000,000m) and the elevation between the two reservoirs can be approximated as parabolic with a maximum elevation of 660m reached 600km from A.

Negative pressures shouldn’t be allowed to exceed about 70% of atmospheric pressure, use this figure to prevent cavitation.

The steel pipe with a roughness of e=0.5cm and diameter of 1.1m and a pressure rating of 150m head is available. The pumps can deliver [itex]1m^3/s[/itex] at 100m head.

*Since the horizontal distance is significantly greater than the vertical distance. I approximated the parabola with straight lines from A to the maximum point of 600,000m from A and elevation 660m and then from that point to B.
I am then doing calculations separately for the 2 parts

*I am trying to calculate amount of pumps that would make this system work and prevent cavitation

*Any help would be appreciated, thanks!

Homework Equations



Extended bernoulli’s equation:
[itex]\frac{V_{1}^{2}}{2g}[/itex] + [itex]\frac{p_{1}}{\gamma}[/itex] + [itex]Z_{1}[/itex] + [itex]h_{p}[/itex] = [itex]\frac{V_{2}^{2}}{2g}[/itex] + [itex]\frac{p_{2}}{\gamma}[/itex] + [itex]Z_{2}[/itex] + [itex]h_{L}[/itex]
V: Velocity
P: Pressure
[itex]\gamma[/itex]: Specific Weight
Z: Height/ Altitude
[itex]h_{p}[/itex]: Pump Head
[itex]h_{L}[/itex]: Head Loss

Head Loss:
[itex]
h_{L} = f \frac{L}{D} \frac{V^{2}}{2g}
[/itex]
f: friction factor
L: Pipe Length
D: Pipe Diameter

Volumetric flow rate to Velocity:

V = Q/A

Q: Volumetric Flow Rate[itex] (m^{3}/s)[/itex]
A: Area
V = Velocity



The Attempt at a Solution



For part 1 [0km to 600km] only:
D = 1.1m
A = 0.95 m^{2}
Q = 1[itex]m^{3}/s[/itex]
V = [itex]\frac{Q}{A}[/itex] = 1.053 m/s

f = 0.0171 (from moody diagram)
R[itex]_{e}[/itex] = 1157490

P[itex]_{minimum}[/itex] (absolute) = 101315Pa*0.7 = 70927.5Pa
P[itex]_{minimum}[/itex] (gage) = P_{min,absolute} – P_{atmospheric} = -30397.5Pa

H[itex]_{p}[/itex] = 100m
L ~= 600km = 600,000m
Using Bernoulli’s formula solve for maximum Length before cavitation:

[itex]\frac{V_{1}^{2}}{2g}[/itex] + [itex]\frac{p_{1}}{\gamma}[/itex] + Z[itex]_{1}[/itex] + h[itex]_{p}[/itex] = [itex]\frac{V_{2}^{2}}{2g}[/itex] + [itex]\frac{p_{2}}{\gamma}[/itex] + Z[itex]_{2}[/itex] + [itex]h_{L}[/itex]

P[itex]_{1}[/itex] = 0
P[itex]_{2}[/itex] = -30397.5
V[itex]_{1}[/itex] = V[itex]_{2}[/itex]
Z[itex]_{1}[/itex] = 300m
Z[itex]_{2}[/itex] = 660m
[itex]\gamma[/itex] = 9800

Sub in Head Loss:

[itex]\frac{V_{1}^{2}}{2g}[/itex] + [itex]\frac{p_{1}}{\gamma}[/itex] + Z[itex]_{1}[/itex] + h[itex]_{p}[/itex] = [itex]\frac{V_{2}^{2}}{2g}[/itex] + [itex]\frac{p_{2}}{\gamma}[/itex] + Z[itex]_{2}[/itex] + [itex]f*\frac{L}{D}*\frac{V^{2}}{2g}
[/itex]
Rearrange:

L = [itex](\frac{V_{1}^{2}}{2g}[/itex] + [itex]\frac{p_{1}}{\gamma}[/itex] + Z[itex]_{1}[/itex] – Z[itex]_{2}[/itex] + h[itex]_{p}[/itex] - [itex]\frac{V_{2}^{2}}{2g}[/itex] - [itex]\frac{p_{2}}{\gamma}[/itex] ) [itex]*\frac{2D*g}{fV^{2}}[/itex]
Cancelling terms:

L = (Z[itex]_{1}[/itex] – Z[itex]_{2}[/itex] +h[itex]_{p}[/itex] - [itex]\frac{p_{2}}{\gamma}[/itex]) [itex]*\frac{2D*g}{fV^{2}}[/itex]

L = (300m – 660m + 100m +3.0986) *1144.77
L = -293076m

I don’t understand why this is the answer, what am I doing wrong?
 
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  • #2
I have also tried doing this using the Darcy-Weisbach equation but I cannot get an answer that makes sense.
 

Related to Fluid Mechanics Question - Pipes and Pumps

What is fluid mechanics?

Fluid mechanics is the study of how fluids (liquids and gases) behave when they are in motion or at rest.

How do pipes and pumps work?

Pipes and pumps work together to transport fluids from one location to another. The pump creates pressure and pushes the fluid through the pipes, while the pipes provide a pathway for the fluid to flow.

What factors affect the flow of fluids through pipes?

The flow of fluids through pipes is affected by various factors such as the fluid's viscosity, density, velocity, and the diameter and length of the pipe. Other factors include the roughness of the pipe's inner surface and the presence of obstructions or bends in the pipe.

What is the difference between laminar and turbulent flow?

Laminar flow is a smooth, orderly flow of fluid in which the fluid particles move in parallel layers. In contrast, turbulent flow is characterized by chaotic, irregular motion of fluid particles, with eddies and swirls forming throughout the flow.

What are some common applications of fluid mechanics in everyday life?

Fluid mechanics has many practical applications in our daily lives, such as in plumbing systems, hydraulic systems in cars and airplanes, pumps and compressors in industrial processes, and even in everyday activities like swimming and drinking from a straw.

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