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SOLUTIONS MANUAL TO ACCOMPANY
INTRODUCTION TO FLIGHT
8th
Edition
By
John D. Anderson, Jr.
Chapter 2
2.1 

2.2 Mean
kinetic energy of each atom 

One kg-mole,
which has a mass of 4 kg, has 6.02 × 1026 atoms. Hence 1 kg has
atoms.


2.3 


2.4 

Since the
volume of the room is the same, we can simply compare densities between the two
problems.


2.5 First, calculate the density from the
known mass and volume, 

In
consistent units,
Also, T = 70 F = 70 + 460 = 530 R.

Hence,


or 

2.6 


Differentiating
with respect to time,

or, 

or,
(1)

At
the instant there is 1000 lbm of air in the tank, the density is


Also, in
consistent units, is given that
T = 50 + 460 = 510 R
and that

From the given
pumping rate, and the fact that the volume of the tank is 900 ft3,
we also have


Thus, from
equation (1) above,

2.7 In consistent units,

Thus,

2.8 

2.9




Magnitude of
the resultant aerodynamic force =

2.10 

Minimum
velocity occurs when sin q = 0,
i.e., when q = 0° and 180°.
Vmin = 0 at q
= 0° and 180°, i.e., at its most forward and rearward points.
Maximum
velocity occurs when sin q = 1,
i.e., when q = 90°. Hence,

i.e., the
entire rim of the sphere in a plane perpendicular to the freestream direction.
2.11 The
mass of air displaced is

The weight of
this air is

This is the
lifting force on the balloon due to the outside air. However, the helium inside
the balloon has weight, acting in the downward direction. The weight of the
helium is less than that of air by the ratio of the molecular weights

Hence, the
maximum weight that can be lifted by the balloon is
0.168 - 0.0233 = 0.145 lb.
2.12 Let
p3, r3,
and T3 denote the conditions
at the beginning of combustion, and p4,
r4, and T4 denote conditions at the end of combustion. Since the
volume is constant, and the mass of the gas is constant, then p4 = r3 = 11.3 kg/m3. Thus, from the equation of state,

or,

2.13 The area of the piston face, where the
diameter is 9 cm = 0.09 m, is

(a) The pressure of the gas mixture at the
beginning of combustion is

The
force on the piston is

Since
4.45 N = l lbf,

(b) 

The
force on the piston is


2.14 Let p3
and T3
denote conditions at the inlet to the combustor, and T4 denote the temperature at
the exit. Note: 

(a) 

(b) 

2.15 1
mile = 5280 ft, and 1 hour = 3600 sec.
So:

A very useful
conversion to remember is that

also, 1 ft = 0.3048 m

Thus 

2.16 


2.17 On the front face

On the back
face

The net force
on the plate is

From Appendix C,

So,

This force acts in
the same direction as the flow (i.e., it is aerodynamic drag.)
2.18 

In SI units:

In terms of
kilogram force,

2.19 


2.20 

2.21 From Fig. 2.16,
length of
fuselage = 33 ft, 4.125 inches = 33.34 ft

wing span = 40 ft, 11.726 inches = 40.98 ft

2.22 (a) From App. C 1 ft. = 0.3048 m.
Thus,
354,200
ft = (354,000)(0.3048) = 107,960 m =
107.96 km
(b) From Example 2.6: 60 mph = 26.82 m/sec
Thus,

2.23

From
Newton’s 2nd Law


2.24

2.25 From Appendix
C, one pound of force equals 4.448 N. Thus, the thrust of the Rolls-Royce Trent
engine in pounds is

2.26
(a) 

(b) 

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