In Exercise 13.9, let us take the position of mass when the spring is unstreched as x = 0, and the direction from left to right as the positive direction of x-axis. Give x as a function of time t for the oscillating mass if at the moment we start the stopwatch (t = 0), the mass is
(a) at the mean position,
(b) at the maximum stretched position, and
(c) at the maximum compressed position.
In what way do these functions for SHM differ from each other, in frequency, in amplitude or the initial phase?
x = 2sin 20t
x = 2cos 20t
x = –2cos 20t
The functions have the same frequency and amplitude, but different initial phases.
Distance travelled by the mass sideways, A = 2.0 cm
Force constant of the spring, k = 1200 N m–1
Mass, m = 3 kg
Angular frequency of oscillation:
\(w=\sqrt\frac{k}{m}\)
\(=\sqrt\frac{1200}{3}=\sqrt400=20\,rad\,s^{-1}\)
When the mass is at the mean position, initial phase is 0.
Displacement, x = Asin ωt
= 2sin 20t
At the maximum stretched position, the mass is toward the extreme right. Hence, the
initial phase is \(\frac{\pi}{2}.\)
Displacement, \(x= A \,sin(wt+\frac{\pi}{2})\)
\(=2 \,sin(20t+\frac{\pi}{2})\)
= 2cos 20t
At the maximum compressed position, the mass is toward the extreme left. Hence, the
initial phase is \(\frac{3\pi}{2}\)
Displacement, \(x= A \,sin(wt+\frac{\pi}{2})\)
\(=2\,sin(20t+\frac{3\pi}{2})=-2\,cos\,20t\)
The functions have the same frequency \((\frac{20}{2\pi}Hz)\) and amplitude (2 cm), but different initial phases (initial phases \((0,\frac{\pi}{2},\frac{3\pi}{2})\)
The center of a disk of radius $ r $ and mass $ m $ is attached to a spring of spring constant $ k $, inside a ring of radius $ R>r $ as shown in the figure. The other end of the spring is attached on the periphery of the ring. Both the ring and the disk are in the same vertical plane. The disk can only roll along the inside periphery of the ring, without slipping. The spring can only be stretched or compressed along the periphery of the ring, following Hooke’s law. In equilibrium, the disk is at the bottom of the ring. Assuming small displacement of the disc, the time period of oscillation of center of mass of the disk is written as $ T = \frac{2\pi}{\omega} $. The correct expression for $ \omega $ is ( $ g $ is the acceleration due to gravity):