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, \(T = 2π\sqrt{\frac{l}{g^2+\frac{v^4}{R^2}}}\)
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
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?