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Chapter 16 - 16.27
27. We wish to find the effective spring constant for the combination of springs shown in Fig. 16–31. We do
this by finding the magnitude
F
of the force exerted on the mass when the total elongation of the springs
is ∆
x
.Then
k
eff
=
F/
∆
x
. Suppose the left-hand spring is elongated by ∆
x
and the right-hand spring is
elongated by ∆
x
r
. The left-hand spring exerts a force of magnitude
k
∆
x
on the right-hand spring and
the right-hand spring exerts a force of magnitude
k
∆
x
r
on the left-hand spring. By Newton’s third law
these must be equal, so ∆
x
=∆
x
r
. The two elongations must be the same and the total elongation is
twice the elongation of either spring: ∆
x
=2∆
x
. The left-hand spring exerts a force on the block and
its magnitude is
F
=
k
∆
x
.Thus
k
eff
=
k
∆
x
/
2∆
x
r
=
k/
2. The block behaves as if it were subject to
the force of a
single
spring, with spring constant
k/
2. To find the frequency of its motion replace
k
eff
in
k
2
m
.
f
=
1
2
π
f
=(1
/
2
π
)
k
eff
/m
with
k/
2toobtain
Plik z chomika:
kf.mtsw
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P16_096.PDF
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P16_006.PDF
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P16_013.PDF
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P16_009.PDF
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P16_002.PDF
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