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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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