Given:
Initial pressure of the liquid \( P_i = 1 \, \text{atm} \)
Final pressure of the liquid \( P_f = 5 \, \text{atm} \)
The change in pressure (\( \Delta P \)) is:
\( \Delta P = P_f - P_i = 4 \, \text{atm} = 4 \times 10^5 \, \text{Pa} \)
The change in volume (\( \Delta V \)) is:
\( \Delta V = -0.8 \, \text{cm}^3 \)
The bulk modulus \( B \) is given as:
\( B = 2 \times 10^9 \, \text{Pa} \)
Now, using the formula for bulk modulus:
\( B = - \frac{\Delta P}{\frac{\Delta V}{V}} \)
We can calculate the volume \( V \):
\( V = -B \times \left( \frac{\Delta V}{\Delta P} \right) \)
Substituting the given values:
\( V = -2 \times 10^9 \times \left( \frac{-0.8 \times 10^{-6}}{4 \times 10^5} \right) \)
Thus, the volume \( V \) is:
\( V = 4 \times 10^{-3} \, \text{m}^3 = 4 \, \text{litre} \)
\( x \) is a peptide which is hydrolyzed to 2 amino acids \( y \) and \( z \). \( y \) when reacted with HNO\(_2\) gives lactic acid. \( z \) when heated gives a cyclic structure as below:

A steel wire of length 2 m and Young's modulus \( 2.0 \times 10^{11} \, \text{N/m}^2 \) is stretched by a force. If Poisson's ratio and transverse strain for the wire are \( 0.2 \) and \( 10^{-3} \) respectively, then the elastic potential energy density of the wire is \( \times 10^6\), in SI units .
Two slabs with square cross section of different materials $(1,2)$ with equal sides $(l)$ and thickness $\mathrm{d}_{1}$ and $\mathrm{d}_{2}$ such that $\mathrm{d}_{2}=2 \mathrm{~d}_{1}$ and $l>\mathrm{d}_{2}$. Considering lower edges of these slabs are fixed to the floor, we apply equal shearing force on the narrow faces. The angle of deformation is $\theta_{2}=2 \theta_{1}$. If the shear moduli of material 1 is $4 \times 10^{9} \mathrm{~N} / \mathrm{m}^{2}$, then shear moduli of material 2 is $\mathrm{x} \times 10^{9} \mathrm{~N} / \mathrm{m}^{2}$, where value of x is _______ .
Consider the sound wave travelling in ideal gases of $\mathrm{He}, \mathrm{CH}_{4}$, and $\mathrm{CO}_{2}$. All the gases have the same ratio $\frac{\mathrm{P}}{\rho}$, where P is the pressure and $\rho$ is the density. The ratio of the speed of sound through the gases $\mathrm{v}_{\mathrm{He}}: \mathrm{v}_{\mathrm{CH}_{4}}: \mathrm{v}_{\mathrm{CO}_{2}}$ is given by