Types of Fluid Flow Problems
Example 5- Determining the Head
Loss in a Water pipe
Water at 15°C ( ρ = 999 kg/m^3 and μ
= 1.138 × 〖10〗^(-3 )kg/m.s ) is flowing steadily in a 5-cm-diameter
horizontal pipe made of stainless steel at a rate of 6 L/s ( Fig. 8-32 ) .
Determine the pressure drop, the head loss, and the required pumping power
input for flow over a 60-m-long section of the pipe.
SOLUTION :
The flow rate through a specified
water pipe is given. The pressure drop, the head loss, and the pumping power
requirements are to be determined.
Assumptions :
1. The flow is steady and
incompressible.
2. The entrance effects are
negligible, and thus the flow is fully developed.
3. The pipe involves no components
such as bends, valves, and connectors.
4. The piping section involves no
work devices such as a pump or a turbine
Properties :
The density and dynamic
viscosity of water are given to be ρ = 999 kg/m^3 and μ = 1.138 × 〖10〗^(-3 )kg/m.s, respectively.
Analysis :
We recognize this as a problem of
the first type, since flow rate,pipe length, and pipe diameter are known. First
we calculate the average velocity and the Reynolds number to determine the flow
regime :
V = ὐ/A_C = ὐ/(〖πD〗^2/4) = 〖0.006 m〗^3/(〖π(0.05m)〗^2/4) = 3.06 m/s
Re = ρVD/μ = (〖999 kg/m〗^3 )(3.06 m/s)( 0.05m)/(1.138 ×〖10〗^(-3) kg/(m.s))=134,300
Re >4000 , the flow is turbulent,
The relative roughness of the pipe is estimated using table 8-2
ε/D = (0.002 mm)/(50 mm) = 0.000040
determine f from the
Colebrook equation on which the Moody chart is based :
1/√f = -2.0 log
((ε/D)/3.7+2.51/(Re√f)) → 1/√f = -2.0 log (0.000040/3.7 + 2.51/(134,300
√f))
f = 0.0172 , the pressure drop (
equivalent to pressure loss in this case), head loss, and the required power
input become
∆P= ∆P_(L )=f L/D 〖ρV〗^2/2=0.0172 60m/0.05m (( 999 kg/m^3 )(3.06 m/s^2
))/2((1 N)/(1 kg.m/s^2 ))
= 96,540 N/m^2 = 96.5 kPa
h_L= (∆P_L)/ρg = f L/D V^2/2g
= 0.0172 60m/0.05m (( 3.06 m/s^(2 ) ))/(2( 9.81 m/s^2 )) = 9.85 m
w_(pump= ὐ∆P)
= ( 0.006 m^3/s)(96,540 N/m2)((1 W)/(1 N.m/s)) = 579 W
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