For a particle performing S.H.M. the equation $ \frac{d^2x}{dt^2} + \alpha x = 0 $. Then the time period of the motion will be:
2πα
\(\frac {2π}{\sqrt {α}}\)
\(\frac {2π}{α}\)
\(2π\sqrt {α}\)
In the given equation,
\(\frac {d^2x}{dt^2}\) + αx = 0,
we can see that the equation represents simple harmonic motion (S.H.M.)
The general form of the equation for S.H.M. is:
\(\frac {d^2x}{dt^2}\) + ω²x = 0,
where ω represents the angular frequency. Comparing this with the given equation, we can see that:
ω² = α.
The angular frequency (ω) of an oscillating system in S.H.M. is related to the time period (T) by the equation
ω = \(\frac {2π}{T}\)
Solving for T, we have:
T = \(\frac {2π}{ω}\)
T = \(\frac {2π}{\sqrt {α}}\)
Therefore, the correct answer is (B) \(\frac {2π}{\sqrt {α}}\), which represents the time period of the motion.
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):