The densities of a liquid at $0^{\circ} \mathrm{C}$ and $100^{\circ} \mathrm{C}$ are respectively 1.0127 and…

The densities of a liquid at $0^{\circ} \mathrm{C}$ and $100^{\circ} \mathrm{C}$ are respectively 1.0127 and 1 . A specific gravity bottle is filled with $300 \mathrm{~g}$ of the liquid at $0^{\circ} \mathrm{C}$ upto the brim and it is heated to $100^{\circ} \mathrm{C}$. Then, the mass of the liquid expelled in grams is: (Coefficient of linear expansion of glass $\left.=9 \times 10^{-6} /{ }^{\circ} \mathrm{C}\right)$
  1. $\frac{3}{10.1}$
  2. $\frac{3}{1.01}$
  3. $\frac{3.81}{1.0127}$
  4. $\frac{3.81}{0.0127}$

Solution

Density at $0^{\circ} \mathrm{C}, \rho_0=1.0127$ Density at $100^{\circ} \mathrm{C}, \rho_{100}=1$ Coefficient of real expansion of liquid, $\gamma_{\text {real }}=\frac{\rho_0-\rho_{100}}{\rho_{100} \times \Delta t}$ $=\frac{1.0127-1}{1 \times 100}=0.0127 \times 10^{-2}$ $=1.27 \times 10^{-4}$ $\gamma_{\text {real }}=\gamma_{\text {app }}+\gamma_g$ $\gamma_g=$ coefficient of volume expansion of glass $=3 \alpha$ $\therefore \quad 1.27 \times 10^{-4}=\gamma_{\mathrm{app}}+3 \alpha$ $1.27 \times 10^{-4}=\gamma_{\text {app }}+3 \times 9 \times 10^{-6}$ $\gamma_{\mathrm{app}}=1.27 \times 10^{-4}-27 \times 10^{-6}$ $=1.27 \times 10^{-4}-0.27 \times 10^{-4}$ $=1 \times 10^{-4}$ $\therefore \quad \gamma_{\text {app }}=\frac{\text { mass expelled }}{\text { remaining mass } \times \Delta t}$ $1 \times 10^{-4}=\frac{m_1-m_2}{m_2 \times 100}$ $\left(\frac{m_1}{m_2}-1\right)=1 \times 10^{-4} \times 100=10^{-2}$ $\frac{m_1}{m_2}=1+10^{-2}=1.01$ $m_2=\frac{m_1}{1.01}=\frac{300}{1.01}$ Mass expelled $=m_1-m_2$ $=300-\frac{300}{1.01}$ $=\frac{3}{1.01}$

Asked in: AP EAMCET 2003

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