For rotodynamic fluid machines of a given shape, and handling an incompressible fluid, the relevant variables involved are D (the rotor diameter), Q (the volume flow rate through the machine), N (the rotational speed of the machine), gH (the difference of head across the machine, i.e., energy per unit mass), p (the density of fluid), µ (the dynamic viscosity of the fluid) and P (the power transferred between fluid and rotor). Show with the helpof Buckingham's n theorem that the relationship between the variables can be expressed by a functional form of the pertinent dimensionless parameters as O (Q/N D², gH/N² D², p N D²1µ, P/p N³ D°) = 0 %3D

Elements Of Electromagnetics
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ISBN:9780190698614
Author:Sadiku, Matthew N. O.
Publisher:Sadiku, Matthew N. O.
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6.4 For rotodynamic fluid machines of a given shape, and handling an
incompressible fluid, the relevant variables involved are D (the rotor diameter),
Q (the volume flow rate through the machine), N (the rotational speed of the
machine), gH (the difference of head across the machine, i.e., energy per
mass), p (the density of fluid), µ (the dynamic viscosity of the fluid) and P (the
power transferred between fluid and rotor). Show with the helpof Buckingham's
n theorem that the relationship between the variables can be expressed by a
functional form of the pertinent dimensionless parameters as
unit
O (Q/N D², gH/N² D°, pN D²jµ, P/p N³ D°) = 0
Transcribed Image Text:6.4 For rotodynamic fluid machines of a given shape, and handling an incompressible fluid, the relevant variables involved are D (the rotor diameter), Q (the volume flow rate through the machine), N (the rotational speed of the machine), gH (the difference of head across the machine, i.e., energy per mass), p (the density of fluid), µ (the dynamic viscosity of the fluid) and P (the power transferred between fluid and rotor). Show with the helpof Buckingham's n theorem that the relationship between the variables can be expressed by a functional form of the pertinent dimensionless parameters as unit O (Q/N D², gH/N² D°, pN D²jµ, P/p N³ D°) = 0
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