- A$(2.0 \pm 0.3) \times 10^{11} \mathrm{~N} / \mathrm{m}^2$
- ✓$(2.0 \pm 0.2) \times 10^{11} \mathrm{~N} / \mathrm{m}^2$
- C$(2.0 \pm 0.1) \times 10^{11} \mathrm{~N} / \mathrm{m}^2$
- D$(2.0 \pm 0.05) \times 10^{11} \mathrm{~N} / \mathrm{m}^2$
Taking long both the sides
$\log Y =\log 4 Fl -\log \pi D ^2 e$
Now, partially differentiating,
$\frac{\Delta Y }{ Y }=-\left(\frac{2 \Delta D }{ D }+\frac{\Delta e }{ e }\right)$
$\frac{\Delta Y }{ Y }=-\left(\frac{2 \times 0.01}{0.4}+\frac{0.05}{0.8}\right)$
$\frac{\Delta Y }{ Y }=-0.1125$
$\text { Also, } Y =\frac{ Fl }{ Ae }=\frac{9.8 \times 2}{\pi(0.2)^2 \times 0.8}=194.96 \times 10^9 \approx 2 \times 10^{11}$
$\Delta Y =- Y \times\left(\frac{2 \Delta r }{ r }+\frac{\Delta e }{ e }\right)$
$\Delta Y =0.225 \times 10^{11}$
$Y =(2 \pm 0.2) \times 10^{11} Nm ^{-2}$
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(Assume stones do not rebound after hitting the ground and neglect air resistance, take $g = 10\ m/ s^2$)
(The figures are schematic and not drawn to scale)

$1.$ If the piston is pushed at a speed of $5 \ mms ^{-1}$, the air comes out of the nozzle with a speed of
$(A)$ $0.1 \ ms ^{-1}$ $(B)$ $1 \ ms ^{-1}$ $(C)$ $2 \ ms ^{-1}$ $(D)$ $8 \ ms ^{-1}$
$2.$ If the density of air is $\rho_{ a }$ and that of the liquid $\rho_{\ell}$, then for a given piston speed the rate (volume per unit time) at which the liquid is sprayed will be proportional to
$(A)$ $\sqrt{\frac{\rho_{ a }}{\rho_{\ell}}}$ $(B)$ $\sqrt{\rho_a \rho_{\ell}}$ $(C)$ $\sqrt{\frac{\rho_{\ell}}{\rho_{ a }}}$ $(D)$ $\rho_{\ell}$
Give the answer question $1$ and $2.$