Step 1: Define Total Energy - The total energy E of a simple harmonic oscillator is given by:
E = \(\frac{1}{2}KA^2\)
- Where K is the spring constant and A is the amplitude.
Step 2: Calculate Potential Energy U at Displacement \(\frac{A}{3}\) - When the displacement is \(\frac{A}{3}\):
U = \(\frac{1}{2}K \left(\frac{A}{3}\right)^2 = \frac{KA^2}{18} = \frac{E}{9}\)
Step 3: Calculate Kinetic Energy KE - Kinetic energy is the difference between total energy and potential energy:
KE = E - U = E - \(\frac{E}{9} = \frac{8E}{9}\)
Step 4: Calculate the Ratio of Total Energy to Kinetic Energy:
\(\frac{\text{Total Energy}}{\text{KE}} = \frac{E}{\frac{8E}{9}} = \frac{9}{8}\)
Step 5: Determine x - Since the ratio is \(\frac{x}{8}\), we have x = 9.
So, the correct answer is: x = 9
Step 1: Total energy in SHM.
\[ E = \frac{1}{2} k A^2 \] where \( A \) is the amplitude.
In SHM, potential energy at displacement \( y \) is: \[ U = \frac{1}{2} k y^2 \] Hence, kinetic energy: \[ K = E - U = \frac{1}{2}kA^2 - \frac{1}{2}ky^2 = \frac{1}{2}k(A^2 - y^2) \]
\[ K = \frac{1}{2}k\left(A^2 - \frac{A^2}{9}\right) \] \[ K = \frac{1}{2}kA^2\left(\frac{8}{9}\right) \]
\[ \frac{E}{K} = \frac{\frac{1}{2}kA^2}{\frac{1}{2}kA^2 \times \frac{8}{9}} = \frac{1}{\frac{8}{9}} = \frac{9}{8} \]
\[ \boxed{x = 9} \]
A particle is subjected to simple harmonic motions as: $ x_1 = \sqrt{7} \sin 5t \, \text{cm} $ $ x_2 = 2 \sqrt{7} \sin \left( 5t + \frac{\pi}{3} \right) \, \text{cm} $ where $ x $ is displacement and $ t $ is time in seconds. The maximum acceleration of the particle is $ x \times 10^{-2} \, \text{m/s}^2 $. The value of $ x $ is:
Two simple pendulums having lengths $l_{1}$ and $l_{2}$ with negligible string mass undergo angular displacements $\theta_{1}$ and $\theta_{2}$, from their mean positions, respectively. If the angular accelerations of both pendulums are same, then which expression is correct?
A bob of mass \(m\) is suspended at a point \(O\) by a light string of length \(l\) and left to perform vertical motion (circular) as shown in the figure. Initially, by applying horizontal velocity \(v_0\) at the point ‘A’, the string becomes slack when the bob reaches at the point ‘D’. The ratio of the kinetic energy of the bob at the points B and C is: 
Two light beams fall on a transparent material block at point 1 and 2 with angle \( \theta_1 \) and \( \theta_2 \), respectively, as shown in the figure. After refraction, the beams intersect at point 3 which is exactly on the interface at the other end of the block. Given: the distance between 1 and 2, \( d = \frac{4}{3} \) cm and \( \theta_1 = \theta_2 = \cos^{-1} \left( \frac{n_2}{2n_1} \right) \), where \( n_2 \) is the refractive index of the block and \( n_1 \) is the refractive index of the outside medium, then the thickness of the block is …….. cm.

Let \( y^2 = 12x \) be the parabola and \( S \) its focus. Let \( PQ \) be a focal chord of the parabola such that \( (SP)(SQ) = \frac{147}{4} \). Let \( C \) be the circle described by taking \( PQ \) as a diameter. If the equation of the circle \( C \) is: \[ 64x^2 + 64y^2 - \alpha x - 64\sqrt{3}y = \beta, \] then \( \beta - \alpha \) is equal to: