유체 역학 9 판 솔루션 - yuche yeoghag 9 pan sollusyeon

유체 역학 9 판 솔루션 - yuche yeoghag 9 pan sollusyeon

Problem 2.86[Difficulty: 3]

Given:Geometry of and flow rate through tapered nozzle

Find:At which point becomes turbulent

Solution:

Basic equationFor pipe flow (Section 2-6)ReρVD

μ

=2300=for transition to turbulence

Also flow rate Q is given byQπD2

4V=

We can combine these equations and eliminate V to obtain an expression for Re in terms of D and Q

Re ρVD

μ

=ρD

μ

4Q

πD2

=4Qρ

πμD

=Re 4Qρ

πμD

=

For a given flow rate Q, as the diameter is reduced the Reynolds number increases (due to the velocity increasing with A-1 or D-2).

Hence for turbulence (Re = 2300), solving for DD4Qρ

2300πμ

=

The nozzle is tapered:Din50mm=Dout

Din

5

=Dout22.4mm=

Carbon tetrachloride:μCT103Ns

m2

=(Fig A.2)For waterρ1000 kg

m3

=

SG1.595=(Table A.2)ρCTSGρ=ρCT1595kg

m3

=

For the given flow rateQ2

L

min

=

4QρCT

πμ

CT

Din

1354=LAMINAR

4QρCT

πμ

CT

Dout

3027=TURBULENT

For the diameter at which we reach turbulenceD

4QρCT

2300πμCT

=D29.4mm=

ButL250 mm=and linear ratios leads to the distance from Din at which D29.4 mm=

Lturb

L

DD

in

DoutDin

=

LturbL

DD

in

DoutDin

=Lturb186 mm=