The figure shows a system of two equal masses \( m \) and three massless horizontal springs with spring constants \( k_1 \), \( k_2 \), and \( k_1 \). Ignore gravity. The masses can move only in the horizontal direction, and there is no dissipation. If \( m = 1 \), \( k_1 = 2 \), and \( k_2 = 3 \) (all in appropriate units), the frequencies of the normal modes of the system in the same system of units are:
We will calculate the frequencies of the normal modes for a system of two equal masses connected by three springs with spring constants \( k_1 \), \( k_2 \), and \( k_1 \).
Let the displacements of the two masses be denoted by \( x_1 \) and \( x_2 \). The forces acting on the masses using Hooke's law are:
For mass 1:
\( m \ddot{x}_1 = -k_1 x_1 - k_2(x_1 - x_2) \)
For mass 2:
\( m \ddot{x}_2 = -k_1 x_2 - k_2(x_2 - x_1) \)
Assume solutions of the form \( x_1 = A_1 e^{i\omega t} \), \( x_2 = A_2 e^{i\omega t} \). Substituting, we get:
\[ m\omega^2 \begin{pmatrix} A_1 \\ A_2 \end{pmatrix} = \begin{pmatrix} k_1 + k_2 & -k_2 \\ -k_2 & k_1 + k_2 \end{pmatrix} \begin{pmatrix} A_1 \\ A_2 \end{pmatrix} \]
We now solve the determinant equation:
\[ \text{det} \begin{pmatrix} k_1 + k_2 - m\omega^2 & -k_2 \\ -k_2 & k_1 + k_2 - m\omega^2 \end{pmatrix} = 0 \]
Using determinant properties, this simplifies to:
\[ (k_1 + k_2 - m\omega^2)^2 - k_2^2 = 0 \]
Solving this quadratic gives:
\[ \omega^2 = \frac{(k_1 + k_2 \pm k_2)}{m} \Rightarrow \omega_1^2 = \frac{k_1}{m}, \quad \omega_2^2 = \frac{k_1 + 2k_2}{m} \]
Given \( k_1 = 2 \), \( k_2 = 3 \), and \( m = 1 \):
\[ \omega_1 = \sqrt{\frac{2}{1}} = \sqrt{2}, \quad \omega_2 = \sqrt{\frac{2 + 2 \times 3}{1}} = \sqrt{8} \]
Final Answer: The correct frequencies are \( \omega_1 = \sqrt{2}, \omega_2 = \sqrt{8} \).
Therefore, the correct option is (A).
The figure shows an opamp circuit with a 5.1 V Zener diode in the feedback loop. The opamp runs from \( \pm 15 \, {V} \) supplies. If a \( +1 \, {V} \) signal is applied at the input, the output voltage (rounded off to one decimal place) is:
A wheel of mass \( 4M \) and radius \( R \) is made of a thin uniform distribution of mass \( 3M \) at the rim and a point mass \( M \) at the center. The spokes of the wheel are massless. The center of mass of the wheel is connected to a horizontal massless rod of length \( 2R \), with one end fixed at \( O \), as shown in the figure. The wheel rolls without slipping on horizontal ground with angular speed \( \Omega \). If \( \vec{L} \) is the total angular momentum of the wheel about \( O \), then the magnitude \( \left| \frac{d\vec{L}}{dt} \right| = N(MR^2 \Omega^2) \). The value of \( N \) (in integer) is: