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For an ideal solution, if a graph is plo...

For an ideal solution, if a graph is plotted between `(1)/(P_(T))` and `y_(A)` (mole fraction of A in vapour phase) where `p_(A)^(0)gtp_(B)^(0)` then

A

intercept of the graph `=(1)/(p_(B)^(0))`

B

slope of the graph `=((1)/(p_(A)^(0))+(1)/(p_(B)^(0)))`

C

slope of the graph `((1)/(p_(B)^(0))-(1)/(p_(B)^(0)))`

D

the graph is linear

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To solve the problem, we need to analyze the relationship between the total pressure \( P_T \) and the mole fraction of component A in the vapor phase \( y_A \) for an ideal solution. We will derive the equation and identify the characteristics of the graph plotted between \( \frac{1}{P_T} \) and \( y_A \). ### Step 1: Understand the relationship for an ideal solution For an ideal solution, the total vapor pressure \( P_T \) is given by Raoult's Law: \[ P_T = P_A^0 \cdot x_A + P_B^0 \cdot x_B \] where: - \( P_A^0 \) and \( P_B^0 \) are the vapor pressures of pure components A and B, respectively. - \( x_A \) and \( x_B \) are the mole fractions of components A and B in the liquid phase. ### Step 2: Express \( x_A \) in terms of \( y_A \) Since \( x_A + x_B = 1 \), we can express \( x_B \) as: \[ x_B = 1 - x_A \] Now, substituting \( x_B \) in the equation for \( P_T \): \[ P_T = P_A^0 \cdot x_A + P_B^0 \cdot (1 - x_A) = P_A^0 \cdot x_A + P_B^0 - P_B^0 \cdot x_A \] This simplifies to: \[ P_T = (P_A^0 - P_B^0) \cdot x_A + P_B^0 \] ### Step 3: Relate \( y_A \) and \( P_T \) The mole fraction of A in the vapor phase \( y_A \) is given by: \[ y_A = \frac{P_A}{P_T} \] where \( P_A = P_A^0 \cdot x_A \) (from Raoult's Law). ### Step 4: Substitute \( P_A \) in terms of \( y_A \) From the expression for \( P_T \), we can express \( P_A \): \[ P_A = P_A^0 \cdot x_A \] Substituting this into the equation for \( y_A \): \[ y_A = \frac{P_A^0 \cdot x_A}{P_T} \] ### Step 5: Rearranging the equation Now, we can express \( \frac{1}{P_T} \): \[ \frac{1}{P_T} = \frac{1}{P_A^0 \cdot x_A + P_B^0 \cdot (1 - x_A)} \] This leads to the equation: \[ \frac{1}{P_T} = \frac{1}{P_B^0} + \frac{1}{P_A^0 - P_B^0} \cdot y_A \] This is a linear equation of the form \( y = mx + c \), where: - \( y = \frac{1}{P_T} \) - \( x = y_A \) - The slope \( m = \frac{1}{P_A^0 - P_B^0} \) - The intercept \( c = \frac{1}{P_B^0} \) ### Step 6: Analyze the graph From the derived equation, we can conclude: 1. The intercept of the graph is \( \frac{1}{P_B^0} \). 2. The slope of the graph is \( \frac{1}{P_A^0 - P_B^0} \). 3. The graph is linear. ### Conclusion Based on the analysis: - The first option (intercept is \( \frac{1}{P_B^0} \)) is correct. - The second option (slope is \( \frac{1}{P_A^0 + P_B^0} \)) is incorrect. - The third option (slope is \( \frac{1}{P_A^0 - P_B^0} \)) is correct. - The fourth option (the graph is linear) is correct. Thus, the correct options are 1, 3, and 4.

To solve the problem, we need to analyze the relationship between the total pressure \( P_T \) and the mole fraction of component A in the vapor phase \( y_A \) for an ideal solution. We will derive the equation and identify the characteristics of the graph plotted between \( \frac{1}{P_T} \) and \( y_A \). ### Step 1: Understand the relationship for an ideal solution For an ideal solution, the total vapor pressure \( P_T \) is given by Raoult's Law: \[ P_T = P_A^0 \cdot x_A + P_B^0 \cdot x_B \] where: ...
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