1 For pumps and turbines, mechanical efficiency is expressed as A. Power input/Fower output B. Power output/Power input C Losses/Fower Output D. (Fower input + Losses)/Power Output 2. Combine power W, diameter d, pressure drop Ap, and average ve ocity V into a dimensionless group. A. W/dVag B. W/NAp C wavap D. W/Vdap 3. Select the dimension of viscosity using the -I system: B. FT/ A FTA CNs/m D. Ns/m 4. For an ideal incompressibie fluid flowing inside a pipe of varying diameters D, the velocity ratio, VNa is equal to A (D/D 8 (Da/D. C D/D. D. D/D.

Elements Of Electromagnetics
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Author:Sadiku, Matthew N. O.
Publisher:Sadiku, Matthew N. O.
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1. For pumps and turbines, mechanical efficiency is expressed as
A. Power input/Power output
B. Power output/Power input
C. Losses/Fower Output
D. (Power input + Losses)/Power Output
2. Combine power W, diameter d, pressure drop Ap, and average ve ocity V into a
dimensionless group.
A. W/d vAp B. W/Ap
C. Wa/Vap
D. W/Vdap
3. Select the dimension of viscosity using the F-L-T system:
B. FT/
A. FTA
C.N.s/m?
D. N.s/m
4. For an ideal incompressible fluid flowing inside a pipe of varying diameters D, the velocity
ratio, V/Vz is equal to
A. (D/D:J²
B (D2F/D:
C. D/D:
D. D/D:
Transcribed Image Text:1. For pumps and turbines, mechanical efficiency is expressed as A. Power input/Power output B. Power output/Power input C. Losses/Fower Output D. (Power input + Losses)/Power Output 2. Combine power W, diameter d, pressure drop Ap, and average ve ocity V into a dimensionless group. A. W/d vAp B. W/Ap C. Wa/Vap D. W/Vdap 3. Select the dimension of viscosity using the F-L-T system: B. FT/ A. FTA C.N.s/m? D. N.s/m 4. For an ideal incompressible fluid flowing inside a pipe of varying diameters D, the velocity ratio, V/Vz is equal to A. (D/D:J² B (D2F/D: C. D/D: D. D/D:
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