all chapter Munson , Young and Okiishi’s Fundamentals of Fluid Mechanics 8th edition solution manual PDF

Title all chapter Munson , Young and Okiishi’s Fundamentals of Fluid Mechanics 8th edition solution manual
Author farsh sardar
Course Fluid Mechanics
Institution University of Auckland
Pages 14
File Size 301.6 KB
File Type PDF
Total Downloads 75
Total Views 164

Summary

Authors: Philip M. Gerhart , Andrew L. Gerhart , John I. Hochstein
Published: Wiley 2016
Edition: 8th
Pages: 1855
Type: pdf
Size: 55MB
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FOLFNKHUHWRGRZQORDG Problem 1.1 The force, F , of the wind blowing against a building is given by F CD V 2A 2, where V is the wind speed, the density of the air, A the cross-sectional area of the building, and CD is a constant termed the drag coefficient. Determine the dimensions of the drag coefficient.

Solution 1.1 F

CD V 2

A 2

or

CD

2F V 2A

, where

F  MLT 2 ,  ML 3 , V  LT 1, A  L2 Thus, MLT CD 

ML 3

LT

2 1 2

M 0 L0T 0 L2

Hence, CD is dimensionless.

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FOLFNKHUHWRGRZQORDG

Problem 1.2

The Mach number is a dimensionless ratio of the velocity of an object in a fluid to the speed of sound in the fluid. For an airplane flying at velocity V in air at absolute temperature T , the Mach number M a is, Ma

V , kRT

where k is a dimensionless constant and R is the specific gas constant for air. Show that M a is dimensionless.

Solution 1.2

We denote the dimension of temperature by

and use Newton’s second law to get F

Then L T

Ma 1

FL M

L T ML T2 F

L2 T2

or

Ma

1.

@solutionmanual1

ML . T2

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FOLFNKHUHWRGRZQORDG

Problem 1.3

Verify the dimensions, in both the FLT and the M LT systems, of the following quantities, which appear in Table B.1 Physical Properties of Water (BG/EE Units). (a) Volume, (b) acceleration, (c) mass, (d) moment of inertia (area), and (e) work.

Solution 1.3 a) volume  L3 b) acceleration

time rate of change of velocity 

LT T

1

LT

2

c) mass  M

or with F  MLT

2

mass  FL 1T 2 d) m oment of inertia area e) work

second moment of area  L2

force distance  FL

or with F  MLT work  ML2 T

2

2

@solutionmanual1

L2  L4

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FOLFNKHUHWRGRZQORDG Problem 1.4

Verify the dimensions, in both the FLT and the M LT systems, of the following quantities, which appear in Table B.1 Physical Properties of Water (BG/EE Units). (a) Angular velocity, (b) energy, (c) moment of inertia (area), (d) power, and (e) pressure.

Solution 1.4 angular displacement T 1 time b) energy ~ capacity of body to do work single work force distance ➔ energy  FL

a) angular velocity

o r with F  MLT

2

➔ energy  MLT

c) moment of inertia area d) p ower e) pressure

2

2

2

L  ML T

second moment of area  L2

rate of doing work 

FL  FLT T

force F   FL 2  MLT area L2

2

1

 MLT

2

L 2  ML 1T

@solutionmanual1

L2  L4

L T 2

1

 ML2 T

3

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FOLFNKHUHWRGRZQORDG Problem 1.5

Verify the dimensions, in both the FLT system and the MLT system, of the following quantities, which appear in Table B.1 Physical Properties of Water (BG/EE Units). (a) Frequency, (b) stress, (c) strain, (d) torque, and (e) work. Solution 1.5 cycles T 1 time force F  2  FL b) stress = area L

a) frequency =

2

S ince F  MLT 2 , stress 

MLT 2

2

 ML 1T

2

L change in length L c) strain =   L0 dimensionless length L d) torque = force distance  FL  MLT 2 L  ML2 T

e) work = force distance  FL  MLT

2

L  ML2 T

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2

2

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FOLFNKHUHWRGRZQORDG Problem 1.6

If u is velocity, x is length, and t is time, what are the dimensions (in the M LT system) of (a) u / t, (b) 2 u / x t, and (c) ( u / t )dx ?

Solution 1.6

a)

u LT  t T

1

 LT

2

b)

c)

2

u LT 1  T x t ( L)( T)

LT u x t T

2

1

(L)  L2T

2

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FOLFNKHUHWRGRZQORDG Problem 1.7

Verify the dimensions, in both the FLT system and the MLT system, of the following quantities, which appear in Table B.1 Physical Properties of Water (BG/EE Units). (a) Acceleration, (b) stress, (c) moment of a force, (d) volume, and (e) work. Solution 1.7

velocity L  2  LT time T F force b) stress  2  FL 2 area L S ince F  MLT 2,

a) acceleration

MLT

2

2

 ML 1T 2 L2 c) m oment of a force force distance  FL  MLT stress 

2

d) v olume (length)3  L3 e) work

force distance  FL  MLT

2

L  ML2T

@solutionmanual1

2

L  ML2T

2

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FOLFNKHUHWRGRZQORDG Problem 1.8

If p is pressure, V is velocity, and is fluid density, what are the dimensions (in the MLT system) of (a) p / , (b) pV , and (c) p / V 2?

Solution 1.8

a)

p



FL 2 ML

MLT 2 L 2

3

b) pV  ML 1T c)

ML 2

ML 1T

3

ML 1

LT

p ML 1T 2  V2 ML 3 LT 1

2

ML

3

2

3

 L2T

2

 M 2L 3T

3

 M 0 L0T 0 dimensionless

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FOLFNKHUHWRGRZQORDG Problem 1.9

If P is force and x is length, what are the dimensions (in the FLT system) of (a) d P / dx , (b) d 3P / dx 3 , and (c) P dx ?

Solution 1.9 dP F   FL 1 a) dx L

b) c)

d3 P F  3  FL 3 dx3 L Pdx  FL

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FOLFNKHUHWRGRZQORDG Problem 1.10

If V is velocity, is length, and is a fluid property (the kinematic viscosity) having dimensions of L2 T 1 , which of the following combinations are dimensionless: (a) V (b) V , (c) V 2 , and (d) V ?

Solution 1.10

a) V

b)

V

LT 

d)

LT 1

LT 

2

2

1

LT

0

0

dimensionless

1

 L4T

L LT

1

2

c) V 2  LT V

1

 LT

L

L T

1

2

L2T

4

3

2

not dimensionless

not dimensionless

1

L LT

1

L

2

not dimensionless

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,

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FOLFNKHUHWRGRZQORDG Problem 1.11

The momentum flux is given by the product mV , where m is mass flow rate and V is velocity. If mass flow rate is given in units of mass per unit time, show that the momentum flux can be expressed in units of force.

Solution 1.11

M T

mV

where

1 gc

L T

M

L F T2 T2 M L

F

FT  2 comes from Newton’s Second Law. ML 

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FOLFNKHUHWRGRZQORDG

Problem 1.12

An equation for the frictional pressure loss p (inches H2O) in a circular duct of inside diameter d in. and length L ft for air flowing with velocity V ft/min is

p 0.027

L

V Vo

d1.22

1.82

,

where V0 is a reference velocity equal to 1000 ft/min. Find the units of the “constant” 0 .027.

Solution 1.12

Solving for the constant gives pL

0.027 L

V Vo

1.22

D

1.82

.

The units give

0.027

in. H 2O ft in.1.22

0.027

ft min ft min

1.82

in. H2O in.1.22 ft

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FOLFNKHUHWRGRZQORDG

Problem 1.13

The volume rate of flow, Q , through a pipe containing a slowly moving liquid is given by the equation R4 p Q 8 where R is the pipe radius, p the pressure drop along the pipe, is a fluid property called viscosity FL 2 T , and is the length of pipe. What are the dimensions of the constant Would you classify this equation as a general homogeneous equation? Explain.

Solution 1.13 3

LT L3T

1

1

L4 



8

8

FL

FL 2 T L3 T

2

L

1

The constantis

is dimensionless. 8 Yes. This is a general homogeneous equation because it is valid in any consistent units system.

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/8?

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FOLFNKHUHWRGRZQORDG Problem 1.14

Show that each term in the following equation has units of lb/ft3 . Consider u as velocity, y as length, x as length, p as pressure, and as absolute viscosity. 0

2

p x

u . y2

Solution 1.14

lb ft2 ft

p x

p x

or

lb , ft3

and 2

u

lb sec

2

2

y

ft

ft sec ft

2

2

or

u

lb

2

ft3

y

@solutionmanual1

....


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