\(\sigma=\frac{3B-2G}{2G+6B}\)
\(\sigma=\frac{6B+2G}{3B-2G}\)
\(\sigma=\frac{9BG}{3B+G}\)
\(B=\frac{3\sigma-3G}{6\sigma+2G}\)
1. \( E = 2G(1 + \sigma) \) ……(1)
2. \( E = 3B(1 - 2\sigma) \) ……(2)
From (1) and (2), we equate \( E \):
\[
2G(1 + \sigma) = 3B(1 - 2\sigma)
\]
Expanding both sides: \[ 2G + 2G\sigma = 3B - 6B\sigma \] Collecting terms involving \( \sigma \) and constants: \[ 3B - 2G = \sigma(2G + 6B) \]
Divide through by \( (2G + 6B) \): \[ \sigma = \frac{3B - 2G}{2G + 6B} \]
The Poisson's ratio \( \sigma \) is:
\( \sigma = \frac{3B - 2G}{2G + 6B} \)
Thus, the correct answer is (A).
In a scattering experiment, a particle of mass $ 2m $ collides with another particle of mass $ m $, which is initially at rest. Assuming the collision to be perfectly elastic, the maximum angular deviation $ \theta $ of the heavier particle, as shown in the figure, in radians is: 

As shown below, bob A of a pendulum having a massless string of length \( R \) is released from 60° to the vertical. It hits another bob B of half the mass that is at rest on a frictionless table in the center. Assuming elastic collision, the magnitude of the velocity of bob A after the collision will be (take \( g \) as acceleration due to gravity):

In the given figure, the blocks $A$, $B$ and $C$ weigh $4\,\text{kg}$, $6\,\text{kg}$ and $8\,\text{kg}$ respectively. The coefficient of sliding friction between any two surfaces is $0.5$. The force $\vec{F}$ required to slide the block $C$ with constant speed is ___ N.
(Given: $g = 10\,\text{m s}^{-2}$) 
Two circular discs of radius \(10\) cm each are joined at their centres by a rod, as shown in the figure. The length of the rod is \(30\) cm and its mass is \(600\) g. The mass of each disc is also \(600\) g. If the applied torque between the two discs is \(43\times10^{-7}\) dyne·cm, then the angular acceleration of the system about the given axis \(AB\) is ________ rad s\(^{-2}\).

According to elastic collision, the kinetic energy of the system will remain constant which means there will be no change in the kinetic energy of the system before and after the collision. It also goes along with the conservation of momentum.
Examples of Elastic Collision
According to inelastic collision, the kinetic energy of the system is not conserved, unlike inelastic collision. The kinetic energy is lost as it gets debauched in other forms of energy like heat, sound, etc, or is absorbed by the body. But they go after the conservation of momentum, like an elastic collision.
Examples of Inelastic Collision
Read More: Elastic and Inelastic Collision