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 \( \frac{3}{2} \omega \).
In an oscillating spring mass system, a spring is connected to a box filled with sand. As the box oscillates, sand leaks slowly out of the box vertically so that the average frequency Γβ°(t) and average amplitude A(t) of the system change with time t. Which one of the following options schematically depicts these changes correctly? 
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): 
