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 | |
Total Downloads | 75 |
Total Views | 164 |
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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FOLFNKHUHWRGRZQORDG 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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FOLFNKHUHWRGRZQORDG
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.
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ML . T2
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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
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L2 L4
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FOLFNKHUHWRGRZQORDG 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
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L2 L4
L T 2
1
ML2 T
3
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FOLFNKHUHWRGRZQORDG 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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FOLFNKHUHWRGRZQORDG 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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FOLFNKHUHWRGRZQORDG 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
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2
L ML2T
2
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FOLFNKHUHWRGRZQORDG 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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FOLFNKHUHWRGRZQORDG 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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FOLFNKHUHWRGRZQORDG 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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FOLFNKHUHWRGRZQORDG 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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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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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 constantis
is dimensionless. 8 Yes. This is a general homogeneous equation because it is valid in any consistent units system.
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FOLFNKHUHWRGRZQORDG 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
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