A metal cylinder with a mass of 1.20 kg is attached to a spring and is able to oscillate horizontally with negligible friction. The cylinder is pulled to a distance of 0.200 mfrom its equilibrium position, held in place with a force of 17.0 N, and then released from rest. It then oscillates in simple harmonic motion. (The cylinder oscillates along the x-axis, where x = 0 is the equilibrium position.)
(a) What is the spring constant (in N/m)?
_____ N/m
(b) What is the frequency of the oscillations (in Hz)?
_____ Hz
(c) What is the maximum speed of the cylinder (in m/s)?
_____ m/s
(d) At what position(s) (in m) on the x-axis does the maximum speed occur?
x = ± ______ m
(e) What is the maximum acceleration of the cylinder? (Enter the magnitude in m/s2.)
______ m/s2
(f) At what position(s) (in m) on the x-axis does the maximum acceleration occur?
x = ± ______ m
(g) What is the total mechanical energy of the oscillating spring–cylinder system (in J)?
______ J
(h) What is the speed of the cylinder (in m/s) when its position is equal to one-third of the maximum displacement from equilibrium?
______ m/s
(i) What is the magnitude of the acceleration of the cylinder (in m/s2) when its position is equal to one-third of the maximum displacement from equilibrium?
_______ m/s2
a)
F = force applied to hold the cylinder in place = 17 N
x = stretch of the spring = 0.200 m
k = spring constant = ?
Using the equation for force of spring
F = k x
17 = (0.200) k
k = 85 N/m
b)
m = mass of the cylinder attached = 1.20 kg
frequency of oscillation is given as
f = (1/(2)) sqrt(k/m)
f = (1/(2(3.14))) sqrt(85/1.20)
f = 1.34 Hz
c)
vmax = maximum speed
A = amplitude = 0.200 m
angular frequency is given as
w = 2f = 2 (3.14) (1.34) = 8.42
maximum speed is given as
vmax = A w
vmax = (0.200) (8.42)
vmax = 1.7 m/s
d)
maximum speed occurs at the equilibrium position.
hence x = 0
e)
maximum acceleration is given as
amax = A w2
amax = (0.200) (8.42)2
amax = 14.2 m/s2
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