$\mathrm{B}=-\frac{\mathrm{dpV}}{\Delta \mathrm{V}}$
Here $\mathrm{p}=$ Pressure (stress)
$-\frac{\Delta \mathrm{V}}{\mathrm{V}}=\text { Volume strain }$
But liquid is incompressible, so
${\Delta \mathrm{V}=0} $
Hence, ${\mathrm{B}=-\frac{\mathrm{pV}}{0}=\infty}$
or $\mathrm{B}=\infty$ (infinity)

| List-$I$ | List-$II$ |
| $(A)$ A force thatrestores anelastic body of unit area to its original state | $(I)$ Bulkmodulus |
| $(B)$ Two equal andopposite forcesparallel toopposite faces | $(II)$Young'smodulus |
| $(C)$Forcesperpendiculareverywhere tothe surface perunit areasameeverywhere | $(III)$ Stress |
| $(D)$Two equal andopposite forceperpendicular toopposite faces | $(IV)$ Shearmodulus |
Choose the correct answer from the options given below:
| $(i)$ Suspension fibre of galvanometer | $(a)$ Linear |
| $(ii)$ Bending of beam | $(b)$ Shear |
| $(iii)$ cutting piece of paper | $(c)$ Bulk |
| $(iv)$ mechanical waves in fluid | $(d)$ Shear |
(Take density of sea water $=10^3 \mathrm{kgm}^{-3}$, Bulk modulus of rubber $=9 \times 10^8 \mathrm{Nm}^{-2}$, and $\mathrm{g}=10 \mathrm{~ms}^{-2}$ )