Connect 1 Semester Access Card For Fluid Mechanics Fundamentals And Applications
Connect 1 Semester Access Card For Fluid Mechanics Fundamentals And Applications
3rd Edition
ISBN: 9780077670245
Author: CENGEL
Publisher: McGraw-Hill Education
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Chapter 14, Problem 43P

A water pump is used to pump water from one large reservoir to another large reservoir that is at a higher elevation. The free surfaces of both reservoirs are exposed to atmospheric pressure, as sketched in Fig. P 14-39. The dimensions and minor loss coefficients are provided in the figure. The pump' s performance is approximated by the expression H a v a i l a b l e = H 0 a V ˙ 2 , where shutoff head H 0 = 24.4 m of water column, coefficient a = 0.0678 m / ( L p m ) 2 available pump head H a v a i l a b l e is in units of meters of water column, and capacity is in units of liters per minute (Lpm). Estimate the capacity delivered by the pump. .

   z 2 z 1 = 7.85 m (elevation difference)

   D = 2.03 c m (Pipe diameter)

   K L , e n t r a n c e = 0.50 (Pipe entrance)

   K L , v a l u e = 17.5 (value)

   K L , e l b o w = 0.92 (each elbow-there are 5)

   K L , e x i t = 1.05 (pipe exit)

   L = 176.5 m (total pipe length)

   ε = 0.25 m m (pipe roughless)

Chapter 14, Problem 43P, A water pump is used to pump water from one large reservoir to another large reservoir that is at a

Expert Solution & Answer
Check Mark
To determine

The volume capacity delivered by the pump.

Answer to Problem 43P

The volume capacity delivered by the pump is 11.576Lpm.

Explanation of Solution

Given information:

The diameter of pipe is 2.03cm, elevation difference is 7.85m, total length of pipe is 176.5m, shutoff head is 24.4m, coefficient ais 0.0678m/Lpm2, pipe roughness is 0.25mm, coefficient of entrance loss is 0.5, coefficient of valve loss is 17.5, coefficient of elbow loss is 0.92and coefficient of exit loss is 1.05.

Write the expression for head required.

  Hrequired=P2P1ρg+V22V122g+(z2z1)+hL   ....(I)

Here, pressure at exit is P2, pressure at inlet is P1, velocity at exit is V2, velocity inlet is V1, elevation difference is z2z1, head loss is hL.

Write the expression for coefficient of total minor head loss.

  K=K1+K2+K3+K4  ....(II)

Here, coefficient of entrance loss is K1, coefficient ofvalve loss is K2, coefficient of elbow loss is K3, coefficient of exit loss is K4.

Write the expression for head loss.

  hL=(fLD+K)V22g   ....(III)

Here, length of pipe is L, diameter of pipe is D, coefficient of friction loss is f, velocity of flow is Vand acceleration due to gravity is g.

Write the expression for Havailable.

  Havailable=H0aV˙2  ....(IV)

Here, shutoff head is H0, coefficient is aand volume flow rate is V˙.

Write the expression for Reynolds number.

  Re=ρVDμ.  ....(V)

Here, density of water is ρand dynamic viscosity is μ.

Write the expression for Colebrook equation.

  1f=2.0log(ε/D3.7+2.51Ref)  ....(VI)

Here, coefficient of friction is fand pipe roughness factor is ε.

Write the expression for volume flow rate.

  V˙=π4D2V   ....(VII)

Calculation:

Substitute 0.5for K1, 17.5for K2, 5×0.92for K3, 1.05for K4in Equation (II).

  K=0.5+17.5+(5×0.92)+1.05=0.5+17.5+4.6+1.05=23.65

Substitute 23.65for K, 176.5mfor L, 2.03cmfor Dand 9.81m/s2for gin Equation (III).

  hL=(f×176.5m2.03cm+23.65)V22×9.81m/s2=(f×176.5m2.03cm× 1m 100cm+23.65)V22×9.81m/s2=(f×176.5m0.0203m+23.65)V22×9.81m/s2=(8694.58f+23.65)V219.62m/s2

Substitute 0for P1, 0for P2, 0for V1, 0for V2, 9.81m/s2for g, 7.85mfor z2z1, (8694.58f+23.65)V219.62for hLin Equation (I).

  Hrequired=00ρg+002g+(7.85m)+(8694.58f+23.65)V219.62m/s2=(7.85m)+(8694.58f+23.65)V219.62m/s2

Substitute 2.03cmfor Din Equation (VII).

  V˙=π4(2.03cm)2V=π4(2.03cm× 1m 100cm)2V=π4(0.0203m)2V=3.2365×104m2×V

Refer Table-A-3 "Properties of saturated water" at 20°Cto obtain density of water as 998kg/m3and dynamic viscosity as 1.002×103kg/ms

Substitute 3.2365×104m2×Vfor V˙, 24.4mfor H0, 0.0678m/Lpm2for aand (7.85m)+(8694.58f+23.65)V219.62for Havailablein Equation (IV).

  [( 7.85m)+( 8694.58f+23.65) V2 19.62m/s2 =24.4m0.0678m/ Lpm 2( 3.2365× 10 4m2×V)2][( 8694.58f+23.65) V2 19.62m/s2 =16.55m( 0.0678m/ Lpm2 ×3.6× 10 8 s2 / m5 1m/ Lpm2 )( 3.2365× 10 4m2×V)2][( 8694.58f+23.65) V2 19.62m/s2 =16.55m( 244080000s2/m5 )( 3.2365× 10 4m2×V)2](443.148s2/mf+1.205s2/m)V2=16.55m25.56s2/m×V2

  f=0.03734m2/s2V20.06041

Substitute 998kg/m3for ρ, 2.03cmfor Dand 1.002×103kg/msfor μin Equation (V).

  Re=998kg/m3×2.03cm×V1.002×103kg/ms=998kg/m3×2.03cm×1m100cm×V1.002×103kg/ms=20218.96s/m×V

Substitute 0.25mmfor ε, 2.03cmfor D, 20218.96s/m×Vfor Reand 0.03734m2/s2V20.06041for fin Equation (VI).

  [1 0.03734 m2 / s2 V 20.06041 =2.0log( 0.25mm/ 2.03cm 3.7 + 2.51 20218.96s/m×V 0.03734 m2 / s2 V 20.06041 )][1 0.03734 m2 / s2 V 20.06041 =2.0log( 0.25mm/ 2.03cm× 10mm 1cm 3.7 + 2.51 20218.96s/m×V 0.03734 m2 / s2 V 20.06041 )][1 0.03734 m2 / s2 V 20.06041 =2.0log( 0.00332432 + 2.51 20218.96s/m×V 0.03734 m2 / s2 V 20.06041 )]  ....(VIII)

Here, apply hit and trial method to calculate the velocity of flow.

Trial-(1)

Substitute 1m/sfor Vin Equation (VIII).

  [1 0.03734 m2 / s2 (1m/s) 20.06041 =2.0log( 0.00332432 + 2.51 20218.96s/m×1m/s 0.03734 m2 / s2 ( 1m/s ) 20.06041 )]10.02307=2.0log(0.00332432+ 2.51 20218.96 0.020307)

Since the value on both sides are not equal, so assumption of V=1m/sis not correct.

Trial-(2)

Substitute 0.596126m/sfor Vin Equation (VIII).

  [1 0.03734 m2 / s2 (0.596126m/s) 20.06041 =2.0log( 0.00332432 + 2.51 20218.96s/m×0.596126m/s 0.03734 m2 / s2 0.596126m/s0.06041 )]10.105074=2.0log(0.00332432+ 2.51 20218.96 0.105074)3.0849=3.084969

Here, the values on both sides are equal, so assumption is correct and velocity of flow is 0.596126m/s

Substitute 0.596126m/sfor Vin Equation (VII).

  V˙=3.2365×104m2×0.596126m/s=1.92939×104m3/s×60000Lpm1m3/s=11.576Lpm

Conclusion:

The volume capacity delivered by the pump is 11.576Lpm.

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Chapter 14 Solutions

Connect 1 Semester Access Card For Fluid Mechanics Fundamentals And Applications

Ch. 14 - Prob. 11CPCh. 14 - Prob. 12CPCh. 14 - There are three main categories of dynamic pumps....Ch. 14 - Consider flow through a water pump. For each...Ch. 14 - Prob. 15CPCh. 14 - Prob. 16CPCh. 14 - Prob. 17CPCh. 14 - Prob. 18CPCh. 14 - Prob. 19CPCh. 14 - Prob. 20PCh. 14 - Prob. 21PCh. 14 - Prob. 22PCh. 14 - Consider the flow system sketched in Fig....Ch. 14 - Prob. 24PCh. 14 - Repeat Prob. 14-25, but with a rough pipe-pipe...Ch. 14 - The performance data for a centrifugal water pump...Ch. 14 - Suppose the pump of Probs. 14-29 and 14-30 is used...Ch. 14 - The performance data for a centrifugal water pump...Ch. 14 - Prob. 32PCh. 14 - Prob. 34PCh. 14 - The performance data of a water pump follow the...Ch. 14 - For the application at hand, the how rate of Prob....Ch. 14 - A water pump is used to pump water from one large...Ch. 14 - For the pump and piping system of Prob. 14-35E,...Ch. 14 - A water pump is used to pump water from one large...Ch. 14 - Calculate the volume flow rate between the...Ch. 14 - Comparing the resu1t of Probs. 14—43 and 14—47,the...Ch. 14 - Repeat Prob. 14—43, but neglect all minor losses....Ch. 14 - A local ventilation system (a hood and duct...Ch. 14 - The performance data for a centrifugal water pump...Ch. 14 - Transform each column of the pump performance data...Ch. 14 - A local ventilation system (a hood and duct...Ch. 14 - For the duct system and fan of Prob. 14—55E,...Ch. 14 - Repeat Prob. 14—55E. Ignoring all minor losses....Ch. 14 - 14-51 A local ventilation system (a hood and duct...Ch. 14 - The two-lobe rotary pump of Fig. P14-63E moves...Ch. 14 - Prob. 64EPCh. 14 - Prob. 65PCh. 14 - Prob. 66PCh. 14 - A centrifugal pump rotates at n=750rpm . Water...Ch. 14 - Prob. 68PCh. 14 - Suppose the pump of Prob. I 4—67 has some reverse...Ch. 14 - Prob. 70PCh. 14 - Prob. 71PCh. 14 - Prob. 72PCh. 14 - Prob. 73CPCh. 14 - Name and briefly describe the differences between...Ch. 14 - Discuss the meaning of reverse swirl in reaction...Ch. 14 - Prob. 76CPCh. 14 - Prob. 77PCh. 14 - Prob. 78PCh. 14 - Prob. 79PCh. 14 - Prob. 80PCh. 14 - Prob. 81PCh. 14 - Wind (=1.204kg/m3) blows through a HAWT wind...Ch. 14 - Prob. 83PCh. 14 - Prob. 85PCh. 14 - Prob. 86EPCh. 14 - Prob. 88PCh. 14 - Prob. 89PCh. 14 - Prob. 90EPCh. 14 - The average wind speed at a proposed HAWT wind...Ch. 14 - Prob. 92CPCh. 14 - Prob. 93CPCh. 14 - Discuss which dimensionless pump performance...Ch. 14 - Prob. 95PCh. 14 - Prob. 96PCh. 14 - Prob. 97PCh. 14 - Prob. 98PCh. 14 - Prob. 99PCh. 14 - Prob. 100PCh. 14 - Prob. 101PCh. 14 - Prob. 102PCh. 14 - Prob. 103PCh. 14 - Prob. 104PCh. 14 - Prob. 105PCh. 14 - Prob. 106PCh. 14 - Prob. 107PCh. 14 - Prob. 108PCh. 14 - Prob. 109PCh. 14 - Prob. 110PCh. 14 - Prob. 111PCh. 14 - Prob. 112PCh. 14 - Prob. 114PCh. 14 - Prob. 115PCh. 14 - Prove that the model turbine (Prob. 14—114) and...Ch. 14 - In Prob. 14—116, we scaled up the model turbine...Ch. 14 - Prob. 118PCh. 14 - Prob. 119PCh. 14 - Prob. 120PCh. 14 - For two dynamically similar pumps, manipulate the...Ch. 14 - Prob. 122PCh. 14 - Prob. 123PCh. 14 - Prob. 124PCh. 14 - Calculate and compare the turbine specific speed...Ch. 14 - Which turbomachine is designed to deliver a very...Ch. 14 - Prob. 127PCh. 14 - Prob. 128PCh. 14 - Prob. 129PCh. 14 - Prob. 130PCh. 14 - Prob. 131PCh. 14 - Prob. 132PCh. 14 - Prob. 133PCh. 14 - Prob. 134PCh. 14 - Prob. 135PCh. 14 - Prob. 136PCh. 14 - Prob. 137PCh. 14 - The snail-shaped casing of centrifugal pumps is...Ch. 14 - Prob. 139PCh. 14 - Prob. 140PCh. 14 - Prob. 141PCh. 14 - Prob. 142PCh. 14 - Prob. 143PCh. 14 - Prob. 144PCh. 14 - Prob. 145PCh. 14 - Prob. 146PCh. 14 - Prob. 147PCh. 14 - Prob. 148PCh. 14 - Prob. 149PCh. 14 - Prob. 150PCh. 14 - Prob. 151PCh. 14 - Prob. 152P
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