A simple pendulum of length l with a bob of mass M is suspended in a car. The car is moving on a circular track of radius R with a uniform speed v. If the pendulum makes small oscillations in a radial direction about its equilibrium position, what will be its time period?
The bob of the simple pendulum will experience acceleration due to gravity and the centripetal acceleration provided by the circular motion of the car.
Acceleration due to gravity = g
Centripetal acceleration =\( \frac{v^2}{R}\)
Where,
v is the uniform speed of the car
R is the radius of the track
Effective acceleration (aeff) is given as:
\(a_{eff}=\sqrt {g^2+(\frac{v^2}{R})^2}\)
Time period, \(T=T=2π\sqrt \frac{l}{a_{eff}}\)
Where, l is the length of the pendulum
∴ Time period, \(T = 2π\sqrt{\frac{l}{g^2+\frac{v^4}{R^2}}}\)
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):