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PROBLEM 19.161 (Continued)
osition 2 2
2
2
0
2
C
Cm
T
Vmgh
mg
=
=
=
PROBLEM 19.162
The block shown is depressed 1.2 in. from its equilibrium position and released.
Knowing that after 10 cycles the maximum displacement of the block is 0.5 in.,
determine (a) the damping factor c/c, (b) the value of the coefficient of viscous damping.
(Hint: See Problems 19.129 and 19.130.)
SOLUTION
From Problems 19.130 and 19.129:
2
1ln
c
c
c
n
x
π
⎛⎞
⎛⎞ =
c
PROBLEM 19.162 (Continued)
k
PRO
An 0.8
consta
accord
the ma
ecom
LEM 19.1
lb ball is con
t
5lb/ft.k=
ng to the rel
ximum allo
slack.
3
ected to a pa
Knowing t
tion
m
δ
=
able circular
ddle by mean
at the pad
sin ,
f
t
ω
whe
frequency
of an elastic
le is move
e
8 in.,
m
δ
=
f
if the cor
cord AB of
vertically
determine
is not to
1
e
1
PROBLEM 19.163 (Continued)
f
f
PROBLEM 19.164
A 3-kg slender rod AB is bolted to a 5-kg uniform disk. A dashpot of
damping coefficient 9N s/mc
⋅ is attached to the disk as shown.
Determine (a) the differential equation of motion for small oscillations,
(b) the damping factor /.
c
cc
SOLUTION
disk
22
AB d AB AB
Wx Fr I I m
θθ θ
−−= ++
⎜⎟
⎝⎠
PROBLEM 19.164 (Continued)
l
cc
c
SO
Sm
LUTION
ll angles:
sin ,
θ
PROBLE
A 4-lb unif
and is conn
equation of
rod will for
0.9 in. dow
os 1
θ
≈
19.165
rm rod is sup
cted to a das
motion for s
with the ho
and released
ported by a p
pot at B. Det
all oscillatio
izontal 5 s aft
n at O and a
rmine (a) the
ns, (b) the a
er end B has
spring at A,
differential
gle that the
een pushed
L
−
α
=
−
PROBLEM 19.165 (Continued)
44
==
0.07246 0.3375 1.25 0
θθθ
+=
(b) Substituting t
e
into the above differential equation,
00
0
(0) 0 2.329 sin 3.439 cos
3.439
tan 2.329
0.9755 rad
0.05 0.06039 rad
sin (0.9755)
θφ θφ
φ
φ
θ
==− +
=
=
==
PROBLEM 19.165 (Continued)
t
−
S
LUTION
PROBL
A 400-kg
a dashpot
Knowing
at a dista
800 rpm
foundatio
M 19.166
motor suppo
of constant
hat the unbal
ce of 100 m
(a) the amp
, (b) the amp
ted by four s
6500 N sc
⋅
nce of the ro
from the ax
litude of th
itude of the
rings, each o
/m
is constr
tor is equival
is of rotation
fluctuating
ertical motio
f constant 15
ined to mo
nt to a 23-g
determine f
force transm
of the motor
kN/m, and
e vertically.
ass located
r a speed of
itted to the
7
PROBLEM 19.166 (Continued)
m
PROBLEM 19.167
The compressor shown has a mass of 250 kg and operates at 2000 rpm. At this operating condition the force
transmitted to the ground is excessively high and is found to be 2
mr
where mr is the unbalance and
ω
f is the
forcing frequency. To fix this problem, it is proposed to isolate the compressor by mounting it on a square
concrete block separated from the rest of the floor as shown. The density of concrete is 2400 kg/m3 and the
spring constant for the soil is found to be 80 × 106 N/m. The geometry of the compressor leads to choosing a
block that is 1.5 m by 1.5 m. Determine the depth h that will reduce the force transmitted to the ground by 75%.
SOLUTION
PROBLEM 19.167 (Continued)
2
S
LUTION
PROBLE
A small bal
a tightly str
on a horiz
displaceme
cord and re
cord to re
equation of
period of vi
M 19.168
of mass m a
tched elastic
ntal plane.
t in a direc
leased. Assu
ain constant,
motion of t
ration.
tached at the
cord of lengt
he ball is gi
ion perpendi
ing the tens
(a) write th
e ball, (b) d
midpoint of
l can slide
en a small
ular to the
on T in the
differential
termine the
PROBLEM 19.169
A certain vibrometer used to measure vibration amplitudes consists
essentially of a box containing a slender rod to which a mass m is attached;
the natural frequency of the mass-rod system is known to be 5 Hz. When
the box is rigidly attached to the casing of a motor rotating at 600 rpm, the
mass is observed to vibrate with an amplitude of 0.06 m. relative to the box.
Determine the amplitude of the vertical motion of the motor.
SOLUTION
44
m
S
LUTION
PROBLE
If either a
acceleration
the string is
location of t
difficulty c
and B are pl
and the dist
then adjuste
Show that t
that g
=
4
π
2
19.170
simple or a
of gravity g,
not truly we
e mass cent
n be eliminat
aced so that t
nce l is me
d so that the
e period
τ
o
/
τ
2
.
compound
difficulties a
ightless, whil
r is difficult t
ed by using
ey are obvio
sured with g
eriod of osc
tained is eq
endulum is
e encountere
e in the case
establish. I
reversible, o
sly not at th
eat precision
llation
τ
is th
al to that of
sed to dete
d. In the cas
of the comp
the case of a
r Kater, pend
same distanc
The positio
e same when
true simple
mine experi
of the simpl
und pendulu
compound p
lum. Two k
e from the m
of a counte
either knife
pendulum of
entally the
pendulum,
, the exact
ndulum, the
ife edges A
ss center G,
weight D is
dge is used.
length l and
d
r
v
p
p
PROBLEM 19.170 (Continued)
2