(III) We usually neglect the mass of a spring if it is small compared to the truss attached to it. But in some applications, the mass of the spring must be taken into account. Consider a spring of unstretched length l and mass M S uniformly distributed along the length of the spring. A mass m is attached to the end of the spring. One end of the spring is fixed and the mass m is allowed to vibrate horizontally without friction (Fig. 7–30). Each point on the spring moves with a velocity proportional to the distance from that point to the fixed end. For example, if the mass on the end moves with speed ϑ 0 , the midpoint of the spring moves with speed ϑ 0 / 2 Show that the kinetic energy of the mass plus spring when the mass is moving with velocity ϑ is K = 1 2 M ϑ 2 where M = m 1 3 M S is the “effective mass” of the system. [ Hint : Let D be the total length of the stretched spring. Then the velocity of a mass d m of a spring of length d x located at x is ϑ ( x ) − ϑ 0 ( x / D ) . Note also d m = d x ( M S / D ) .] FIGURE 7-30 Problem 68.
(III) We usually neglect the mass of a spring if it is small compared to the truss attached to it. But in some applications, the mass of the spring must be taken into account. Consider a spring of unstretched length l and mass M S uniformly distributed along the length of the spring. A mass m is attached to the end of the spring. One end of the spring is fixed and the mass m is allowed to vibrate horizontally without friction (Fig. 7–30). Each point on the spring moves with a velocity proportional to the distance from that point to the fixed end. For example, if the mass on the end moves with speed ϑ 0 , the midpoint of the spring moves with speed ϑ 0 / 2 Show that the kinetic energy of the mass plus spring when the mass is moving with velocity ϑ is K = 1 2 M ϑ 2 where M = m 1 3 M S is the “effective mass” of the system. [ Hint : Let D be the total length of the stretched spring. Then the velocity of a mass d m of a spring of length d x located at x is ϑ ( x ) − ϑ 0 ( x / D ) . Note also d m = d x ( M S / D ) .] FIGURE 7-30 Problem 68.
(III) We usually neglect the mass of a spring if it is small compared to the truss attached to it. But in some applications, the mass of the spring must be taken into account. Consider a spring of unstretched length
l
and mass
M
S
uniformly distributed along the length of the spring. A mass
m
is attached to the end of the spring. One end of the spring is fixed and the mass m is allowed to vibrate horizontally without friction (Fig. 7–30). Each point on the spring moves with a velocity proportional to the distance from that point to the fixed end. For example, if the mass on the end moves with speed
ϑ
0
, the midpoint of the spring moves with speed
ϑ
0
/
2
Show that the kinetic energy of the mass plus spring when the mass is moving with velocity
ϑ
is
K
=
1
2
M
ϑ
2
where
M
=
m
1
3
M
S
is the “effective mass” of the system. [Hint: Let D be the total length of the stretched spring. Then the velocity of a mass
d
m
of a spring of length
d
x
located at
x
is
ϑ
(
x
)
−
ϑ
0
(
x
/
D
)
. Note also
d
m
=
d
x
(
M
S
/
D
)
.]
(C) Increase its length to 2L
(d)increase its length to 4L
9) A simple pendulum of length L is set to oscillate in simple harmonic motion. When its potential
energy is one-half its total mechanical energy, U = E/2, then which of the following is true about its
velocity:
(a) v = tvmax /2
(b) v = tvmay (4
Problem 2 ( ). A very light spring with spring constant 200 N/m hangs vertically
the ceiling with equilbrium length Lo = 6 cm. When a 300 g mass is attached to the end
spring, the mass-spring system extends to a new equilibrium length.
Lo
y = 0
(a)
What is the length L of the spring when the mass-spring system is in equilibrium?
If the mass is released from rest with the spring at its original equilibrium length
(b)
6 cm, find the velocity of the mass when the spring has stretched to the length L you found in (a).
000000
2) (a)The springs of a mountain bike are compressed vertically by 5 mm when a cyclist of
mass 60 kg sits on it. When the cyclist rides the bike over a bump on a track, the frame of the
bike and the cyclist oscillate up and down. Using the formula F = - ks, calculate the value of
k, the constant for the springs of the bike. (b)The total mass of the frame of the bike and the
cyclist is 80 kg. Calculate the period of oscillation of the cyclist. (c)Calculate the number of
oscillations of the cyclist per second.
Chapter 7 Solutions
Physics for Scientists and Engineers with Modern Physics
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