When the two waves \( y_1 \) and \( y_2 \) are superposed, the resultant wave can be expressed as a combination of a carrier wave and a modulation wave. The carrier frequency is determined by the average of the angular frequencies, while the modulation frequency is determined by their difference.
\[ y_1 = A_0 \sin(kx - \omega t), \quad y_2 = A_0 \sin(\alpha kx - \beta \omega t) \]
The resultant wave is given by the superposition of \( y_1 \) and \( y_2 \):
\[ y_{\text{resultant}} = 2A_0 \cos\left(\frac{\beta \omega - \omega}{2} t\right) \sin\left(\frac{\beta \omega + \omega}{2} t\right) \]
For \( \alpha = \beta = 2 \), the carrier frequency becomes:
\[ \text{Carrier Frequency} = \frac{\omega + 2\omega}{2} = \frac{3}{2} \omega \]
Thus, the correct statement is that the carrier frequency of the resultant wave is \( \frac{3}{2} \omega \).
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 Hookeβs 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):