An equation of a simple harmonic progressive wave is given by y = A sin (100πt-3x).The distance between two particles having a phase difference of \(\frac {π}{3}\) in metre is
\(\frac {π}{3}\)
\(\frac {π}{18}\)
\(\frac {π}{9}\)
\(\frac {π}{6}\)
The general equation for a wave is y = A sin(kx - ωt)
Comparing this equation to the given equation, we have:
k = 3
ω = 100π
In this case, we are given a phase difference of \(\frac {π}{3}\). The general equation for the phase difference in terms of the wave number and wavelength is:
Δϕ = k.Δx
To find the distance between two particles with a phase difference of \(\frac {π}{3}\), we need to find Δx such that:
k.Δx = \(\frac {π}{3}\)
Substituting the value of k = 3, we have:
3.Δx = \(\frac {π}{3}\)
To isolate Δx, we divide both sides by 3:
Δx = \(\frac {π}{9}\)
Therefore, the distance between two particles with a phase difference of \(\frac {π}{3}\) is \(\frac {π}{9}\) meters.
So, the correct option is (C) \(\frac {π}{9}\).
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):