A spring having with a spring constant 1200 N m–1 is mounted on a horizontal table as shown in Fig. 13.19. A mass of 3 kg is attached to the free end of the spring. The mass is then pulled sideways to a distance of 2.0 cm and released.
Determine (i) the frequency of oscillations, (ii) maximum acceleration of the mass, and (iii) the maximum speed of the mass
Spring constant, k = 1200 N m-1
Mass, m = 3 kg
Displacement, A = 2.0 cm = 0.02 cm
Frequency of oscillation v, is given by the relation:
\(v=\frac{1}{T}=\frac{1}{2\pi}\sqrt\frac{k}{m}\)
Where, T is the time period
\(∴v=\frac{1}{2x3.14}\sqrt\frac{1200}{3}=3.18\,m/s\)
Hence, the frequency of oscillations is 3.18 m/s
Maximum acceleration (a) is given by the relation:
a = ω2 A
Where,
ω = Angular frequency = \(\sqrt\frac{k}{m}\)
A = Maximum displacement
\(\therefore\,a=\frac{k}{m}A=\frac{1200×0.02}{3}=8\,ms^{-2}\)
Hence, the maximum acceleration of the mass is 8.0 m/s2
Maximum velocity, v max = Aω
\(=A\sqrt\frac{k}{m}=0.02x\sqrt\frac{1200}{3}=0.4 \,m/s.\)
Hence, the maximum velocity of the mass is 0.4 m/s.
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):