P16_017.PDF
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)
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Chapter 16 - 16.17
17. The maximum force that can be exerted by the surface must be less than
µ
s
N
or else the block will not
follow the surface in its motion. Here,
µ
s
is the coecient of static friction and
N
is the normal force
exerted by the surface on the block. Since the block does not accelerate vertically, we know that
N
=
mg
,
where
m
is the mass of the block. If the block follows the table and moves in simple harmonic motion,
the magnitude of the maximum force exerted on it is given by
F
=
ma
m
=
mω
2
x
m
=
m
(2
πf
)
2
x
m
,where
a
m
is the magnitude of the maximum acceleration,
ω
is the angular frequency, and
f
is the frequency.
The relationship
ω
=2
πf
was used to obtain the last form. We substitute
F
=
m
(2
πf
)
2
x
m
and
N
=
mg
into
F<µ
s
N
to obtain
m
(2
πf
)
2
x
m
<µ
s
mg
. The largest amplitude for which the block does not slip is
x
m
=
(2
πf
)
2
=
(0
.
50)(9
.
8m
/
s
2
)
=0
.
031m
.
(2
π
×
2
.
0Hz)
2
A larger amplitude requires a larger force at the end points of the motion. The surface cannot supply
the larger force and the block slips.
µ
s
g
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