To find the correct relation between Young's modulus \(Y\), bulk modulus \(K\), and modulus of rigidity \(\eta\), we start by understanding the interrelations between these elastic constants. The following relationships are fundamental:
Our goal is to express \(K\) in terms of \(Y\) and \(\eta\). Begin by using the above relationships to express \(\nu\) and then substitute to obtain the desired formula.
First, express \(\nu\) from the second relationship:
\nu = \frac{Y}{2\eta} - 1Substitute \(\nu\) in the first relationship:
Y = 3K \left(1 - 2\left(\frac{Y}{2\eta} - 1\right)\right)Simplifying:
Y = 3K \left(1 - \frac{2Y}{2\eta} + 2\right)This leads to:
Y = 3K \left(\frac{9\eta - Y}{2\eta}\right)Simplifying we arrive at:
K = \frac{Y\eta}{9\eta - 3Y}This confirms the correct option is K = \frac{Y\eta}{9\eta - 3Y} \text{ N/m}^2.
Thus:
One end of a steel wire is fixed to the ceiling of an elevator moving up with an acceleration \( 2\,\text{m/s}^2 \) and a load of \( 10\,\text{kg} \) hangs from the other end. If the cross-section of the wire is \( 2\,\text{cm}^2 \), then the longitudinal strain in the wire is given. (Take \( g=10\,\text{m/s}^2 \) and \( Y=2.0\times10^{11}\,\text{N/m}^2 \)). 