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Consider a ideal solution of component 1...

Consider a ideal solution of component 1 and component 2 component 1 being more volatile `x_(1)` and `x_(2)` represent the respective liquid phase compositions at equilibrium while `y_(1),y_(2)` denote the respective vapour phase compositions at equilibrium. `p_(1),p_(2)` are respective partial pressure in vapour phase at equilibrium which of the following is/are necessarly are?

A

`p_(1)gtp_(2)`

B

`y_(1)lty_(2)`

C

`y_(1)gtx_(1)`

D

`x_(2)gty_(2)`

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To solve the problem regarding the ideal solution of components 1 and 2, we need to analyze the relationships between their liquid and vapor phase compositions at equilibrium, as well as their partial pressures. Here’s a step-by-step solution: ### Step 1: Understand the Components We have two components in an ideal solution: - Component 1 (more volatile) - Component 2 Let: - \( x_1 \) = mole fraction of component 1 in the liquid phase - \( x_2 \) = mole fraction of component 2 in the liquid phase - \( y_1 \) = mole fraction of component 1 in the vapor phase - \( y_2 \) = mole fraction of component 2 in the vapor phase - \( P_1 \) = partial pressure of component 1 - \( P_2 \) = partial pressure of component 2 - \( P_{total} \) = total pressure of the system ### Step 2: Apply Raoult's Law According to Raoult's Law, the partial pressure of each component in the vapor phase is given by: - \( P_1 = P_{1}^{0} \cdot x_1 \) - \( P_2 = P_{2}^{0} \cdot x_2 \) Where \( P_{1}^{0} \) and \( P_{2}^{0} \) are the vapor pressures of the pure components 1 and 2, respectively. ### Step 3: Apply Dalton's Law of Partial Pressures According to Dalton's Law, the total pressure is the sum of the partial pressures: \[ P_{total} = P_1 + P_2 \] ### Step 4: Relate Vapor Phase Compositions to Partial Pressures From Dalton's Law, we can express the mole fractions in the vapor phase as: - \( y_1 = \frac{P_1}{P_{total}} \) - \( y_2 = \frac{P_2}{P_{total}} \) ### Step 5: Analyze the Volatility Since component 1 is more volatile, we know: \[ P_{1}^{0} > P_{2}^{0} \] This implies that \( P_1 \) will be greater than \( P_2 \) when the liquid phase compositions are considered. ### Step 6: Establish Relationships From the equations derived: 1. \( y_1 = \frac{P_{1}^{0} \cdot x_1}{P_{total}} \) 2. \( y_2 = \frac{P_{2}^{0} \cdot x_2}{P_{total}} \) Since \( P_{1}^{0} > P_{2}^{0} \) and given that \( P_{total} \) is a constant, we can conclude: - \( y_1 > x_1 \) (because \( P_{1}^{0} \) is greater) - \( y_2 < x_2 \) (because \( P_{2}^{0} \) is less) ### Step 7: Final Conclusions From the analysis: - \( y_1 > x_1 \) implies that the composition of component 1 in the vapor phase is greater than in the liquid phase. - \( y_2 < x_2 \) implies that the composition of component 2 in the vapor phase is less than in the liquid phase. ### Summary of Results - \( y_1 > x_1 \) - \( x_2 > y_2 \)

To solve the problem regarding the ideal solution of components 1 and 2, we need to analyze the relationships between their liquid and vapor phase compositions at equilibrium, as well as their partial pressures. Here’s a step-by-step solution: ### Step 1: Understand the Components We have two components in an ideal solution: - Component 1 (more volatile) - Component 2 Let: ...
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