To solve this problem, we need to understand the behavior of ideal solutions and the concepts of Raoult's law regarding vapour pressure in a solution.
To determine the relationship between the mole fractions of components A and B in both the liquid and vapor phases, we can use Raoult's Law for ideal solutions:
Raoult's Law: For a two-component system, the partial vapor pressure of each component is given by:
\( P_{A} = P_{A}^0 \times x_A \)
\( P_{B} = P_{B}^0 \times x_B \)
where \( P_{A}^0 \) and \( P_{B}^0 \) are the vapor pressures of the pure components A and B, respectively.
Total Vapor Pressure: The total vapor pressure of the solution is:
\( P_{total} = P_{A} + P_{B} = P_{A}^0 \times x_A + P_{B}^0 \times x_B \)
Mole Fraction in Vapor Phase: The mole fractions in the vapor phase can be calculated using Dalton's Law:
\( y_A = \frac{P_{A}}{P_{total}} = \frac{P_{A}^0 \times x_A}{P_{total}} \)
\( y_B = \frac{P_{B}}{P_{total}} = \frac{P_{B}^0 \times x_B}{P_{total}} \)
Comparison: We need to compare \( \frac{x_A}{x_B} \) with \( \frac{y_A}{y_B} \).
Given that \( P_{A}^0 = 350 \) mm Hg and \( P_{B}^0 = 750 \) mm Hg, and knowing that \( P_{B}^0 > P_{A}^0 \), it follows that component B is more volatile than component A. Therefore, in the vapor phase, the mole fraction of B will be greater as compared to A, leading to:
\( \frac{x_A}{x_B} > \frac{y_A}{y_B} \)
Thus, the correct answer is:
\( \frac{x_A}{x_B}>\frac{y_A}{y_B} \)
A substance 'X' (1.5 g) dissolved in 150 g of a solvent 'Y' (molar mass = 300 g mol$^{-1}$) led to an elevation of the boiling point by 0.5 K. The relative lowering in the vapour pressure of the solvent 'Y' is $____________ \(\times 10^{-2}\). (nearest integer)
[Given : $K_{b}$ of the solvent = 5.0 K kg mol$^{-1}$]
Assume the solution to be dilute and no association or dissociation of X takes place in solution.
Inductance of a coil with \(10^4\) turns is \(10\,\text{mH}\) and it is connected to a DC source of \(10\,\text{V}\) with internal resistance \(10\,\Omega\). The energy density in the inductor when the current reaches \( \left(\frac{1}{e}\right) \) of its maximum value is \[ \alpha \pi \times \frac{1}{e^2}\ \text{J m}^{-3}. \] The value of \( \alpha \) is _________.
\[ (\mu_0 = 4\pi \times 10^{-7}\ \text{TmA}^{-1}) \]
A small block of mass \(m\) slides down from the top of a frictionless inclined surface, while the inclined plane is moving towards left with constant acceleration \(a_0\). The angle between the inclined plane and ground is \(\theta\) and its base length is \(L\). Assuming that initially the small block is at the top of the inclined plane, the time it takes to reach the lowest point of the inclined plane is _______. 