1 QUESTION 1 Consider a desired pump operating condition which adds 35 psi at a flowrate of 500 gpm to water (p= 62 11m/ft²³) Ignore any changes in Kinetic or potential energy and Tassume isothermal flow G.e. internal energy is constant, this is the normal assumption we make when analyzing fluid flows in piping systems). Apply the energy balance only across the pump with full energy Balance and simlifying to solve for the pump, Starting head symbolically. Then begin careful of units, Solve for pump head in feet. GIVEN: 35psi 500 gpm p=62 1bm/3 XA. 10.5 A B. 100.8 ft C. 50.1 ft D. 80.7A 35 500 62 (32.2) + 2(32.2) 35 + 500 F

Elements Of Electromagnetics
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QUESTION 1
Consider a desired pump operating condition which adds 35 psi at a flowrate
of 500 gpm to water (p= 62 11m/ft²³) Ignore any changes in Kinetic or
potential energy and Tassume isothermal flow C.e. internal energy is constant,
this is the normal assumption we make when analyzing fluid flows
in piping systems). Apply the energy balance only across the pump
with full energy
Balance and simlifying to solve for the pump,
Starting
head symbolically. Then begin careful of units, Solve for pump head in feet.
GIVEN: 35psi
500 gpm
p=62 1bm/3
XA. 10.5 A
B. 100.8 ft
C.
50.1 ft
D. 80.7f
35
500
62 (32.2) + 2(32.2)
35 +
500
Transcribed Image Text:1 QUESTION 1 Consider a desired pump operating condition which adds 35 psi at a flowrate of 500 gpm to water (p= 62 11m/ft²³) Ignore any changes in Kinetic or potential energy and Tassume isothermal flow C.e. internal energy is constant, this is the normal assumption we make when analyzing fluid flows in piping systems). Apply the energy balance only across the pump with full energy Balance and simlifying to solve for the pump, Starting head symbolically. Then begin careful of units, Solve for pump head in feet. GIVEN: 35psi 500 gpm p=62 1bm/3 XA. 10.5 A B. 100.8 ft C. 50.1 ft D. 80.7f 35 500 62 (32.2) + 2(32.2) 35 + 500
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