For a particle performing S.H.M. the equation \(\frac {d^2x}{dt^2}\)+αx=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.
A particle is executing simple harmonic motion with a time period of 3 s. At a position where the displacement of the particle is 60% of its amplitude, the ratio of the kinetic and potential energies of the particle is: