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For a very small extent of dissociation ...

For a very small extent of dissociation of `PCl_(5)` into `PCl_(3)` and `Cl_(2)` is a gaseous phase reaction then degree of dissociation , x `:`

A

`x prop P`

B

`x prop (1)/(p)`

C

`x prop sqrtp`

D

`x prop sqrt((1)/(p))`

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The correct Answer is:
To solve the problem of finding the degree of dissociation (denoted as \( x \)) of \( PCl_5 \) into \( PCl_3 \) and \( Cl_2 \), we can follow these steps: ### Step 1: Write the Reaction The dissociation reaction of \( PCl_5 \) can be written as: \[ PCl_5(g) \rightleftharpoons PCl_3(g) + Cl_2(g) \] ### Step 2: Set Up Initial Conditions Assume we start with 1 mole of \( PCl_5 \) and no products at time \( t = 0 \): - Initial moles of \( PCl_5 = 1 \) - Initial moles of \( PCl_3 = 0 \) - Initial moles of \( Cl_2 = 0 \) ### Step 3: Define the Change in Moles Let \( x \) be the degree of dissociation of \( PCl_5 \). At equilibrium: - Moles of \( PCl_5 \) = \( 1 - x \) - Moles of \( PCl_3 \) = \( x \) - Moles of \( Cl_2 \) = \( x \) ### Step 4: Calculate Total Moles at Equilibrium The total number of moles at equilibrium is: \[ \text{Total moles} = (1 - x) + x + x = 1 + x \] ### Step 5: Calculate Mole Fractions Now, we can calculate the mole fractions of each component: - Mole fraction of \( PCl_5 \): \[ \chi_{PCl_5} = \frac{1 - x}{1 + x} \] - Mole fraction of \( PCl_3 \): \[ \chi_{PCl_3} = \frac{x}{1 + x} \] - Mole fraction of \( Cl_2 \): \[ \chi_{Cl_2} = \frac{x}{1 + x} \] ### Step 6: Calculate Partial Pressures Assuming the total pressure is \( P \): - Partial pressure of \( PCl_5 \): \[ P_{PCl_5} = \chi_{PCl_5} \cdot P = \frac{(1 - x)}{(1 + x)} \cdot P \] - Partial pressure of \( PCl_3 \): \[ P_{PCl_3} = \chi_{PCl_3} \cdot P = \frac{x}{(1 + x)} \cdot P \] - Partial pressure of \( Cl_2 \): \[ P_{Cl_2} = \chi_{Cl_2} \cdot P = \frac{x}{(1 + x)} \cdot P \] ### Step 7: Write the Expression for \( K_p \) The equilibrium constant \( K_p \) for the reaction is given by: \[ K_p = \frac{P_{PCl_3} \cdot P_{Cl_2}}{P_{PCl_5}} \] Substituting the partial pressures: \[ K_p = \frac{\left(\frac{x}{1 + x} \cdot P\right) \cdot \left(\frac{x}{1 + x} \cdot P\right)}{\frac{(1 - x)}{(1 + x)} \cdot P} \] This simplifies to: \[ K_p = \frac{x^2 P^2}{(1 - x)(1 + x)} \] ### Step 8: Approximation for Small \( x \) Since the extent of dissociation is very small, we can assume \( 1 - x \approx 1 \) and \( 1 + x \approx 1 \): \[ K_p \approx \frac{x^2 P^2}{1} \] Thus: \[ K_p = x^2 P^2 \] ### Step 9: Solve for \( x \) Rearranging gives: \[ x = \sqrt{\frac{K_p}{P}} \] ### Conclusion The degree of dissociation \( x \) is given by: \[ x = \sqrt{\frac{K_p}{P}} \]
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