Imagine you are looking at a closed container holding a mixture of two volatile liquids, A and B. The space above the liquid isn't empty; it's filled with the vapours of both A and B constantly evaporating and condensing. This dynamic equilibrium is governed by two beautiful laws of physical chemistry: Raoult's Law and Dalton's Law of Partial Pressures.
Analyzing the Liquid Phase
We are given the pure vapour pressures of the two liquids at 25∘C: pA∘=90 mm Hg and pB∘=15 mm Hg. We also know the composition of the liquid mixture. The mole fraction of A in the liquid phase is χA=0.6.
Since a mixture is made entirely of its components, the sum of all mole fractions must equal 1. Therefore, the mole fraction of B in the liquid phase is simply:
Applying Raoult's Law
Raoult's Law tells us that the partial vapour pressure of a component in an ideal solution is directly proportional to its mole fraction in the liquid phase. Let's calculate the partial pressures pA and pB exerted by the vapours of A and B respectively.
pA=χApA∘=0.6×90=54 mm Hg
pB=χBpB∘=0.4×15=6 mm Hg
The Total Vapour Pressure
Now, we look at the vapour phase as a whole. According to Dalton's Law of Partial Pressures, the total pressure pT exerted by a mixture of non-reacting gases is the sum of their individual partial pressures.
pT=pA+pB=54+6=60 mm Hg
Composition of the Vapour Phase
The question asks for the mole fraction of B in the vapour phase, which we will denote as YB. Dalton's Law also provides a direct relationship between the partial pressure of a gas, the total pressure, and its mole fraction in the gaseous mixture: pB=YBpT.
Rearranging this, we can find YB:
Final Calculation
The problem states that the mole fraction of B in the vapour phase is given in the format x×10−1. Let's convert our result into scientific notation to match this format.
By comparing 1×10−1 with x×10−1, it is crystal clear that the value of x is exactly 1.