p11_029.pdf
(
79 KB
)
Pobierz
Chapter 11 - 11.29
29. Since the belt does not slip, a point on the rim of wheel
C
has the same tangential acceleration as a
point on the rim of wheel
A
. This means that
α
A
r
A
=
α
C
r
C
,where
α
A
is the angular acceleration of
wheel
A
and
α
C
is the angular acceleration of wheel
C
.Thus,
α
C
=
r
A
r
C
(1
.
6rad
/
s
2
)=0
.
64 rad
/
s
2
.
Since the angular speed of wheel
C
is given by
ω
C
=
α
C
t
, the time for it to reach an angular speed of
ω
= 100 rev
/
min = 10
.
5rad
/
s starting from rest is
t
=
ω
C
10
.
5rad
/
s
0
.
64 rad
/
s
2
=16s
.
α
A
=
10 cm
25 cm
α
C
=
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p11_060.pdf
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p11_002.pdf
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p11_001.pdf
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p11_005.pdf
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p11_003.pdf
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Inne foldery tego chomika:
chap01
chap02
chap03
chap04
chap05
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