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At a sudden contraction in a pipe the diameter changes from D_1 to D_2. The pressure drop.
Delta p, which develops across the contraction is a function of D_1 and D_2. as well as the
velocity, V, in the larger pipe, and the fluid density, and viscosity, mu. Use Du K and n as
repeating variables to determine a suitable set of dimensionless parameters. Why would it be
incorrect to include the velocity in the smaller pipe as an additional variable?
Solution
Let DP= F(D1,d2,v,RHO,MU)
units dims pressure F/L^2
L
V =L/t
D = L
rho = FL^-4T^2
Mu= F L^-2T
First dimensionless group using D1 V mu are recurring variables
Pi1 = DelP * D1^a V^b MU^c
since this is non dim, obtains Pi1 = DELP *D1/(V*MU)
Similarly for P2: new entering variable D2, obtain D2/D1
Similarly Pi3, using rho as entering variable,
Pi3 = Rho*D1*V/Mu

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At a sudden contraction in a pipe the diameter changes from D_1 to D_.pdf

  • 1. At a sudden contraction in a pipe the diameter changes from D_1 to D_2. The pressure drop. Delta p, which develops across the contraction is a function of D_1 and D_2. as well as the velocity, V, in the larger pipe, and the fluid density, and viscosity, mu. Use Du K and n as repeating variables to determine a suitable set of dimensionless parameters. Why would it be incorrect to include the velocity in the smaller pipe as an additional variable? Solution Let DP= F(D1,d2,v,RHO,MU) units dims pressure F/L^2 L V =L/t D = L rho = FL^-4T^2 Mu= F L^-2T First dimensionless group using D1 V mu are recurring variables Pi1 = DelP * D1^a V^b MU^c since this is non dim, obtains Pi1 = DELP *D1/(V*MU) Similarly for P2: new entering variable D2, obtain D2/D1 Similarly Pi3, using rho as entering variable, Pi3 = Rho*D1*V/Mu