$\text{The fractional compression } \left( \frac{\Delta V}{V} \right) \text{ of water at the depth of } 2.5 \, \text{km below the sea level is } \_\_\_\_\_\_\_\_\_\_ \%. \text{ Given, the Bulk modulus of water } = 2 \times 10^9 \, \text{N m}^{-2}, \text{ density of water } = 10^3 \, \text{kg m}^{-3}, \text{ acceleration due to gravity } g = 10 \, \text{m s}^{-2}.$
To find the fractional compression of water at a depth of 2.5 km below sea level, we use the formula for fractional compression given by:
\(\frac{\Delta V}{V} = \frac{P}{K}\)
Where \(P\) is the pressure applied and \(K\) is the bulk modulus of the water.
The pressure \(P\) at a depth \(h\) is given by:
\(P = \rho \cdot g \cdot h\)
Given:
Substitute these values into the pressure formula:
\(P = 10^3 \cdot 10 \cdot 2500 = 2.5 \times 10^7 \, \text{N m}^{-2}\)
Now, substitute \(P\) and \(K\) into the fractional compression formula:
\(\frac{\Delta V}{V} = \frac{2.5 \times 10^7}{2 \times 10^9} = 0.0125\)
To express this as a percentage, multiply by 100:
\(0.0125 \times 100 = 1.25\%\)
Thus, the fractional compression of water at the given depth is 1.25%.

A flexible chain of mass $m$ is hanging as shown. Find tension at the lowest point. 
Let the lines $L_1 : \vec r = \hat i + 2\hat j + 3\hat k + \lambda(2\hat i + 3\hat j + 4\hat k)$, $\lambda \in \mathbb{R}$ and $L_2 : \vec r = (4\hat i + \hat j) + \mu(5\hat i + + 2\hat j + \hat k)$, $\mu \in \mathbb{R}$ intersect at the point $R$. Let $P$ and $Q$ be the points lying on lines $L_1$ and $L_2$, respectively, such that $|PR|=\sqrt{29}$ and $|PQ|=\sqrt{\frac{47}{3}}$. If the point $P$ lies in the first octant, then $27(QR)^2$ is equal to}