\(\sigma=\frac{3B-2G}{2G+6B}\)
\(\sigma=\frac{6B+2G}{3B-2G}\)
\(\sigma=\frac{9BG}{3B+G}\)
\(B=\frac{3\sigma-3G}{6\sigma+2G}\)
To find the correct relation between Poisson's ratio \(\sigma\), Bulk modulus \(B\), and modulus of rigidity \(G\), we will determine the expressions and relationships between these mechanical properties.
The relationships between different elastic constants in material science are key to solving this problem. Let's start by understanding the basics:
For isotropic materials, the relationships between these moduli and Poisson's ratio are given by:
By eliminating \(E\), we can relate \(B\), \(G\), and \(\sigma\):
| Given: | \(E = 2G(1+\sigma)\) |
| \(E = 3B(1-2\sigma)\) |
Setting the equations equal gives:
\(2G(1+\sigma) = 3B(1-2\sigma)\)
Expanding both sides and solving for \(\sigma\):
\(2G + 2G\sigma = 3B - 6B\sigma\)
\(2G\sigma + 6B\sigma = 3B - 2G\)
\(\sigma(2G + 6B) = 3B - 2G\)
\(\sigma = \frac{3B - 2G}{2G + 6B}\)
Therefore, the correct relation is:
The correct option showing the correct relation is:
\(\sigma=\frac{3B-2G}{2G+6B}\)
Hence, the answer is correct.
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):

