\(\frac{1}{3}\)
\(\frac{1}{2}\)
\(\frac{2}{3}\)
\(\frac{1}{9}\)
\(\frac{4}{9}\)
Given:
Step 1: Express Energy in SHM
In SHM:
Step 2: Use Given Ratio
Given \( \frac{K}{U} = 3 \):
\[ \frac{\frac{1}{2}k(A^2 - x^2)}{\frac{1}{2}kx^2} = 3 \]
Simplify:
\[ \frac{A^2 - x^2}{x^2} = 3 \]
\[ A^2 - x^2 = 3x^2 \]
\[ A^2 = 4x^2 \]
\[ \frac{x^2}{A^2} = \frac{1}{4} \]
\[ \frac{x}{A} = \frac{1}{2} \]
Conclusion:
The ratio \( \frac{x}{A} \) is \( \frac{1}{2} \).
Answer: \(\boxed{B}\)
1. Potential Energy (U) and Kinetic Energy (K):
- The potential energy \(U\) at displacement \(x\) is given by:
\[ U = \frac{1}{2} k x^2 \]
- The total mechanical energy \(E\) in simple harmonic motion is:
\[ E = \frac{1}{2} k A^2 \]
- The kinetic energy \(K\) at displacement \(x\) is given by:
\[ K = E - U = \frac{1}{2} k A^2 - \frac{1}{2} k x^2 = \frac{1}{2} k (A^2 - x^2)\]
2. Given Ratio of Kinetic to Potential Energy:
\[ \frac{K}{U} = 3\]
Substitute the expressions for \(K\) and \(U\):
\[\frac{\frac{1}{2} k (A^2 - x^2)}{\frac{1}{2} k x^2} = 3 \]
3. Simplify the Equation:
\[ \frac{A^2 - x^2}{x^2} = 3\]
4. Solve for \(\frac{x}{A}\):
- Rearrange the equation:
\[A^2 - x^2 = 3x^2\]
- Combine like terms:
\[A^2 = 4x^2\]
- Divide both sides by \(A^2\):
\[1 = 4\left(\frac{x}{A}\right)^2 \]
- Take the square root of both sides:
\[ \frac{x}{A} = \pm \frac{1}{2}\]
Thus, the ratio \(\frac{x}{A}\) is \(\pm \frac{1}{2}\).
So, \(\frac{x}{A} = \frac{1}{2}\) or \(\frac{x}{A} = -\frac{1}{2}\).
So the correct Answer is Option B(2):\(\frac12\)
Step 1: Recall the expressions for kinetic and potential energy in simple harmonic motion.
In simple harmonic motion (SHM), the total energy \( E \) is conserved and is given by:
\[ E = K + U, \]
where:
We are given that the ratio of kinetic energy to potential energy is:
\[ \frac{K}{U} = 3. \]
Substitute the expressions for \( K \) and \( U \):
\[ \frac{\frac{1}{2} m \omega^2 (A^2 - x^2)}{\frac{1}{2} m \omega^2 x^2} = 3. \]
Simplify:
\[ \frac{A^2 - x^2}{x^2} = 3. \]
Rearrange:
\[ A^2 - x^2 = 3x^2. \]
Simplify further:
\[ A^2 = 4x^2. \]
Take the square root of both sides:
\[ \frac{x}{A} = \frac{1}{2}. \] ---
Final Answer: The value of \( \frac{x}{A} \) is \( \mathbf{\frac{1}{2}} \), which corresponds to option \( \mathbf{(B)} \).
As shown in the figures, a uniform rod $ OO' $ of length $ l $ is hinged at the point $ O $ and held in place vertically between two walls using two massless springs of the same spring constant. The springs are connected at the midpoint and at the top-end $ (O') $ of the rod, as shown in Fig. 1, and the rod is made to oscillate by a small angular displacement. The frequency of oscillation of the rod is $ f_1 $. On the other hand, if both the springs are connected at the midpoint of the rod, as shown in Fig. 2, and the rod is made to oscillate by a small angular displacement, then the frequency of oscillation is $ f_2 $. Ignoring gravity and assuming motion only in the plane of the diagram, the value of $\frac{f_1}{f_2}$ is:
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 ω(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 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): 
We can note there involves a continuous interchange of potential and kinetic energy in a simple harmonic motion. The system that performs simple harmonic motion is called the harmonic oscillator.
Case 1: When the potential energy is zero, and the kinetic energy is a maximum at the equilibrium point where maximum displacement takes place.
Case 2: When the potential energy is maximum, and the kinetic energy is zero, at a maximum displacement point from the equilibrium point.
Case 3: The motion of the oscillating body has different values of potential and kinetic energy at other points.