The correct option is(A): \(\frac{1}{\sqrt{3}}\)
Potential of the given oscillator is \(V=\frac{1}{2} k(x-k)^{2}\)
Given: \(M=10 ;\, m=5,\, u=1 ;\, k=1\)
Initial momentum of the particle of mass \(m=m u=m \times 5=5\, m\)
Momentum of (oscillator + particle) after collision \(=(M+ m)\)
Velocity of oscillator after collision \(=v\)
So, momentum of system \(=(M+ m) v\)
From conservation of linear momentum, we have
\((M +m)=m u=5 \times 1=5\)
For second collision, oscillator and particle have momentum in opposite direction.
Net or total momentum is zero.
Likewise after \(4^{\text {th }}, 6^{\text {th }}, 8^{\text {th }}, 10^{\text {th }}, 12^{\text {th }}\) collision the momentum is zero.
After \(12^{\text {th }}\) collision, Mass of oscillator and 12 particles will be \((10+12 \times 5)=70\)
Now, from conservation of linear momentum, for \(13^{\text {th }}\) collision, we have
\(70 \times 0+5 \times 1=(70+5) v'\)
\(\Rightarrow v'=\frac{5}{75}\)
\(\Rightarrow \frac{1}{15}\)
Total mass after \(13^{\text {th }}\) collision \(=(10+13 \times 5)=75\)
Kinetic energy of system \(=\frac{1}{2} m v'^{2}\)
\(\Rightarrow K E=\frac{1}{2} \times 75 \times \frac{1}{15} \times \frac{1}{15}\)
\(\Rightarrow \frac{1}{2} k A^{2}=\frac{1}{2} \times \frac{75}{225}=\frac{1}{6}\)
\(\Rightarrow \frac{1}{2} \times 1 \times A^{2}=\frac{1}{6}\)
\(\Rightarrow A^{2}=\frac{1}{3}\)
\(\Rightarrow A=\frac{1}{\sqrt{3}}\)
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): 
Given below are two statements: one is labelled as Assertion (A) and the other is labelled as Reason (R).
Assertion (A): Time period of a simple pendulum is longer at the top of a mountain than that at the base of the mountain.
Reason (R): Time period of a simple pendulum decreases with increasing value of acceleration due to gravity and vice-versa. In the light of the above statements.
choose the most appropriate answer from the options given below:
In the experiment for measurement of viscosity \( \eta \) of a given liquid with a ball having radius \( R \), consider following statements:
A. Graph between terminal velocity \( V \) and \( R \) will be a parabola.
B. The terminal velocities of different diameter balls are constant for a given liquid.
C. Measurement of terminal velocity is dependent on the temperature.
D. This experiment can be utilized to assess the density of a given liquid.
E. If balls are dropped with some initial speed, the value of \( \eta \) will change.
Given below are two statements: one is labelled as Assertion \(A\) and the other as Reason \(R\):
Assertion \(A\): A sound wave has higher speed in solids than in gases.
Reason \(R\): Gases have higher value of Bulk modulus than solids.
A bead of mass \( m \) slides without friction on the wall of a vertical circular hoop of radius \( R \) as shown in figure. The bead moves under the combined action of gravity and a massless spring \( k \) attached to the bottom of the hoop. The equilibrium length of the spring is \( R \). If the bead is released from the top of the hoop with (negligible) zero initial speed, the velocity of the bead, when the length of spring becomes \( R \), would be (spring constant is \( k \), \( g \) is acceleration due to gravity): 
Oscillation is a process of repeating variations of any quantity or measure from its equilibrium value in time . Another definition of oscillation is a periodic variation of a matter between two values or about its central value.
The term vibration is used to describe the mechanical oscillations of an object. However, oscillations also occur in dynamic systems or more accurately in every field of science. Even our heartbeats also creates oscillations. Meanwhile, objects that move to and fro from its equilibrium position are known as oscillators.
Read More: Simple Harmonic Motion
The tides in the sea and the movement of a simple pendulum of the clock are some of the most common examples of oscillations. Some of examples of oscillations are vibrations caused by the guitar strings or the other instruments having strings are also and etc. The movements caused by oscillations are known as oscillating movements. For example, oscillating movements in a sine wave or a spring when it moves up and down.
The maximum distance covered while taking oscillations is known as the amplitude. The time taken to complete one cycle is known as the time period of the oscillation. The number of oscillating cycles completed in one second is referred to as the frequency which is the reciprocal of the time period.