p08_009.pdf
(
79 KB
)
Pobierz
Chapter 8 - 8.9
9. (a) If
K
i
is the kinetic energy of the flake at the edge of the bowl,
K
f
is its kinetic energy at the
bottom,
U
i
is the gravitational potential energy of the flake-Earth system with the flake at the top,
and
U
f
is the gravitational potential energy with it at the bottom, then
K
f
+
U
f
=
K
i
+
U
i
.Taking
the potential energy to be zero at the bottom of the bowl, then the potential energy at the top is
U
i
=
mgr
where
r
=0
.
220 m is the radius of the bowl and
m
is the mass of the flake.
K
i
=0 since
the flake starts from rest. Since the problem asks for the speed at the bottom, we write
2
mv
2
for
K
f
. Energy conservation leads to
2
mv
2
=
⇒
v
=
2
gr
=
2(9
.
8)(0
.
220) =2
.
08 m
/
s
.
(b) We note that the expression for the speed (
v
=
√
2
gr
) does not contain the mass of the flake. The
speed would be the same, 2
.
08m
/
s, regardless of the mass of the flake.
(c) The final kinetic energy is given by
K
f
=
K
i
+
U
i
−
mgr
=
1
U
f
.Since
K
i
is greater than before,
K
f
is
greater. This means the final speed of the flake is greater.
Plik z chomika:
kf.mtsw
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p08_004.pdf
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p08_005.pdf
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p08_003.pdf
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p08_002.pdf
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Inne foldery tego chomika:
chap01
chap02
chap03
chap04
chap05
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