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Chemical Equilibrium question

2022 · 24 Jun · Shift 1 · Q4
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  5. /2022 · 24 Jun · Shift 1 · Q4

Chemical Equilibrium question

2022 · 24 Jun · Shift 1 · Q4

JEE MainChemistryChemical EquilibriumMCQ+4 / −1
For a reaction at equilibrium A(g) ⇌\rightleftharpoons⇌ B(g) +12{1 \over 2}21​ C(g) the relation between dissociation constant (K), degree of dissociation (α\alphaα) and equilibrium pressure (p) is given by :
  1. A
    K=α12p32(1+32α)12(1−α)K = {{{\alpha ^{{1 \over 2}}}{p^{{3 \over 2}}}} \over {{{\left( {1 + {3 \over 2}\alpha } \right)}^{{1 \over 2}}}(1 - \alpha )}}K=(1+23​α)21​(1−α)α21​p23​​
  2. B
    K=α32p12(2+α)12(1−α)K = {{{\alpha ^{{3 \over 2}}}{p^{{1 \over 2}}}} \over {{{\left( {2 + \alpha } \right)}^{{1 \over 2}}}(1 - \alpha )}}K=(2+α)21​(1−α)α23​p21​​
  3. C
    K=(α p)32(1+32α)12(1−α)K = {{{{(\alpha \,p)}^{{3 \over 2}}}} \over {{{\left( {1 + {3 \over 2}\alpha } \right)}^{{1 \over 2}}}(1 - \alpha )}}K=(1+23​α)21​(1−α)(αp)23​​
  4. D
    K=(α p)32(1+α)(1−α)12K = {{{{(\alpha \,p)}^{{3 \over 2}}}} \over {{{\left( {1 + \alpha } \right)}}{{(1 - \alpha )}^{{1 \over 2}}}}}K=(1+α)(1−α)21​(αp)23​​
View written solutionFree

Correct answer: B

  1. Assume initial moles

Let initially we have 111 mole of AAA.

For the reaction A(g)⇌B(g)+12C(g)A(g) \rightleftharpoons B(g) + \frac12 C(g)A(g)⇌B(g)+21​C(g) if degree of dissociation is α\alphaα, then at equilibrium:

  • moles of A=1−αA = 1-\alphaA=1−α
  • moles of B=αB = \alphaB=α
  • moles of C=α2C = \frac{\alpha}{2}C=2α​
  1. Total moles at equilibrium

ntotal=(1−α)+α+α2=1+α2n_{\text{total}}=(1-\alpha)+\alpha+\frac{\alpha}{2}=1+\frac{\alpha}{2}ntotal​=(1−α)+α+2α​=1+2α​

  1. Partial pressures

If total pressure at equilibrium is ppp, then pA=1−α1+α/2pp_A=\frac{1-\alpha}{1+\alpha/2}ppA​=1+α/21−α​p pB=α1+α/2pp_B=\frac{\alpha}{1+\alpha/2}ppB​=1+α/2α​p pC=α/21+α/2pp_C=\frac{\alpha/2}{1+\alpha/2}ppC​=1+α/2α/2​p

  1. Write equilibrium constant in terms of partial pressures

For the reaction, K=pB (pC)1/2pAK=\frac{p_B\,(p_C)^{1/2}}{p_A}K=pA​pB​(pC​)1/2​

Substitute the partial pressures: K=(αp1+α/2)((α/2)p1+α/2)1/2((1−α)p1+α/2)K=\frac{\left(\frac{\alpha p}{1+\alpha/2}\right)\left(\frac{(\alpha/2)p}{1+\alpha/2}\right)^{1/2}}{\left(\frac{(1-\alpha)p}{1+\alpha/2}\right)}K=(1+α/2(1−α)p​)(1+α/2αp​)(1+α/2(α/2)p​)1/2​

  1. Simplify

First cancel the common factor: K=α1−α((α/2)p1+α/2)1/2K=\frac{\alpha}{1-\alpha}\left(\frac{(\alpha/2)p}{1+\alpha/2}\right)^{1/2}K=1−αα​(1+α/2(α/2)p​)1/2

So, K=α1−α⋅(αp/2)1/2(1+α/2)1/2K=\frac{\alpha}{1-\alpha}\cdot \frac{(\alpha p/2)^{1/2}}{(1+\alpha/2)^{1/2}}K=1−αα​⋅(1+α/2)1/2(αp/2)1/2​

K=α3/2p1/2(1−α) [2(1+α/2)]1/2K=\frac{\alpha^{3/2}p^{1/2}}{(1-\alpha)\,[2(1+\alpha/2)]^{1/2}}K=(1−α)[2(1+α/2)]1/2α3/2p1/2​

Now, 2(1+α2)=2+α2\left(1+\frac\alpha2\right)=2+\alpha2(1+2α​)=2+α

Hence, K=α3/2p1/2(1−α)(2+α)1/2K=\frac{\alpha^{3/2}p^{1/2}}{(1-\alpha)(2+\alpha)^{1/2}}K=(1−α)(2+α)1/2α3/2p1/2​

or K=α3/2p1/22+α (1−α)K=\frac{\alpha^{3/2}p^{1/2}}{\sqrt{2+\alpha}\,(1-\alpha)}K=2+α​(1−α)α3/2p1/2​

  1. Match with options

This matches Option B: K=α3/2p1/2(2+α)1/2(1−α)K = \frac{\alpha^{3/2}p^{1/2}}{(2+\alpha)^{1/2}(1-\alpha)}K=(2+α)1/2(1−α)α3/2p1/2​

  1. Comparison with stored answer

Stored correct answer: B

Our derived answer: B

So they agree.

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