Match List-I with List-II
|
List-I Term |
List-II Formula/expression |
|
(A) Raoult's law |
(I) \( \frac{P_1^0-P_1}{P_1^0}=x_2 \) |
|
(B) Henry's Law |
(II) \( P_{total} = P_1^0 + (P_2^0- P_1^0) x_2 \) |
|
(C) Dalton's Law of partial pressure |
(III) \( p = K_Hx \) |
|
(D) Relative lowering of vapor pressure |
(IV) \( P_2 = P_2^0 x_2 \) |
Choose the correct answer from the options given below:
Answer & explanation
Correct answer: option 1
The correct answer is Option (1) → (A)-(IV), (B)-(III), (C)-(II), (D)-(I)
All four expressions describe the vapour above a solution. Raoult’s law relates the partial vapour pressure of a component to its mole fraction in the solution; Dalton’s law adds the partial pressures; Henry’s law gives the solubility of a gas; and the relative lowering of vapour pressure follows from Raoult’s law for a solution of a non-volatile solute.
(A) Raoult's law — This matches (IV) \( P_2 = P_2^0 x_2 \). The partial vapour pressure of each volatile component is its pure vapour pressure multiplied by its mole fraction in the solution.
(B) Henry's Law — This matches (III) \( p = K_Hx \). The partial pressure of a gas over a solution is proportional to its mole fraction in the solution; \( K_H \) is the Henry’s law constant.
(C) Dalton's Law of partial pressure — This matches (II) \( P_{total} = P_1^0 + (P_2^0- P_1^0) x_2 \). The total pressure is the sum of the partial pressures; with Raoult’s law and \( x_1 = 1 - x_2 \):
\( \displaystyle p_{total} = p_1^0 x_1 + p_2^0 x_2 = p_1^0 (1 - x_2) + p_2^0 x_2 = p_1^0 + (p_2^0 - p_1^0)\,x_2 \)
(D) Relative lowering of vapor pressure — This matches (I) \( \frac{P_1^0-P_1}{P_1^0}=x_2 \). With a non-volatile solute, \( p_1 = p_1^0 x_1 = p_1^0 (1 - x_2) \), so the lowering divided by \( p_1^0 \) equals the mole fraction of the solute:
\( \displaystyle \frac{p_1^0 - p_1}{p_1^0} = x_2 \)
Shortcut: (A)-(IV) appears in Options (1) and (4), and (B)-(III) then leaves only Option (1).
Note: The same/similar question has been asked in different years by NTA as per the details given below:
| 2026 | 2025 | 2024 | 2023 | 2022 |
|---|---|---|---|---|
| 24-05 S2 | 02-06 S2 | – | – | – |