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If xA and xB are the respective mole fractions of A and B in an ideal solution of the two and TA, TB, T are the fusion temperatures of pure A, pure B and the ideal solution respectively, then

  • A.\(1-x_{B}=\)\(\exp[\frac{-\Delta H^{o}_{fus(B)}}{R}(\frac{1}{T}-\frac{1}{T_{B}})]\)
  • B.\(1-x_{B}=\)\(\exp[\frac{\Delta H^{o}_{fus(A)}}{R}(\frac{1}{T}-\frac{1}{T_{A}})]\)
  • C.\(1-x_{B}=\)\(\exp[\frac{\Delta H^{o}_{fus(B)}}{R}(\frac{1}{T}-\frac{1}{T_{B}})]\)
  • D.\(1-x_{B}=\)\(\exp[\frac{-\Delta H^{o}_{fus(A)}}{R}(\frac{1}{T}-\frac{1}{T_{A}})]\)

Answer: D

The correct relation is the one with A's enthalpy of fusion, A's melting point and a negative exponent: \(1-x_{B}=\)\(\exp[\frac{-\Delta H^{o}_{fus(A)}}{R}(\frac{1}{T}-\frac{1}{T_{A}})]\).

The solution freezes when its component A is in equilibrium with pure solid A, so the condition involves A's enthalpy of fusion and A's melting point. For an ideal solution:

\[ \begin{aligned} \ln x_{A} &= -\frac{\Delta H_{fus(A)}}{R}\left(\frac{1}{T} - \frac{1}{T_{A}}\right) \\ x_{A} &= 1 - x_{B} \end{aligned} \]

Exponentiating gives the last option. A check: T lies below TA, so 1/T - 1/TA is positive, the exponent is negative and xA is less than 1, as it must be.

The two options with B's enthalpy and TB describe solid B separating instead, and the option with a positive exponent would make xA greater than 1.

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