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Chemical Equilibrium question

2016 · Shift 2 · Q5
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  5. /2016 · Shift 2 · Q5

Chemical Equilibrium question

2016 · Shift 2 · Q5

JEE AdvancedChemistryChemical EquilibriumMCQ+3 / −1
Paragraph Thermal decomposition of gaseous X2X_2X2​ to gaseous X at 298 K takes place according to the following equations: X2X_2X2​ (g) ⇋\leftrightharpoons⇋ 2X (g) The standard reaction Gibbs energy, ΔrGo\Delta _rG^oΔr​Go, of this reaction is positive. At the start of the reaction, there is one mole of X2X_2X2​ and no X. As the reaction proceeds, the number of moles of X formed is given by β\betaβ. Thus, βequilibrium\beta _{equilibrium}βequilibrium​ is the number of moles of X formed at equilibrium. The reaction is carried out at a constant total pressure of 2 bar. Consider the gases to behave ideally. (Given R = 0.083 L bar K-1 mol-1) Question The INCORRECT statement among the following for this reaction, is
  1. A
    Decrease in the total pressure will result in formation of more moles of gaseous X
  2. B
    At the start of the reaction, dissociation of gaseous X2X_2X2​ takes place spontaneously
  3. C
    βequilibrium{{\beta _{equilibrium}}}βequilibrium​ = 0.7
  4. D
    Kc < 1
View written solutionFree

Correct answer: C

  1. Write the reaction and mole balance

The reaction is X2(g)⇌2X(g)X_2(g) \rightleftharpoons 2X(g)X2​(g)⇌2X(g)

Initially:

  • moles of X2=1X_2 = 1X2​=1
  • moles of X=0X = 0X=0

If β\betaβ moles of XXX are formed, then since 1 mole of X2X_2X2​ gives 2 moles of XXX, X2 consumed=β2X_2 \text{ consumed} = \frac{\beta}{2}X2​ consumed=2β​

So at any stage: nX2=1−β2,nX=βn_{X_2}=1-\frac{\beta}{2}, \qquad n_X=\betanX2​​=1−2β​,nX​=β

Total moles: ntot=1−β2+β=1+β2n_{\text{tot}}=1-\frac{\beta}{2}+\beta=1+\frac{\beta}{2}ntot​=1−2β​+β=1+2β​


  1. Reaction quotient at the start

For the reaction, Qp=(PX)2PX2Q_p=\frac{(P_X)^2}{P_{X_2}}Qp​=PX2​​(PX​)2​

Initially, no XXX is present, so PX=0  ⟹  Qp=0P_X=0 \implies Q_p=0PX​=0⟹Qp​=0

Given that ΔrG∘>0\Delta_r G^\circ >0Δr​G∘>0, we have ΔrG∘=−RTln⁡Kp\Delta_r G^\circ = -RT\ln K_pΔr​G∘=−RTlnKp​ Rightarrow Kp<1K_p<1Kp​<1

But initially, Qp=0<KpQ_p=0<K_pQp​=0<Kp​ so ΔrG=ΔrG∘+RTln⁡Qp<0\Delta_r G = \Delta_r G^\circ + RT\ln Q_p <0Δr​G=Δr​G∘+RTlnQp​<0 (in the limit, since ln⁡0→−∞\ln 0 \to -\inftyln0→−∞).

Hence, forward dissociation starts spontaneously. So Option B is correct.


  1. Effect of pressure

The reaction is X2(g)⇌2X(g)X_2(g) \rightleftharpoons 2X(g)X2​(g)⇌2X(g) Here, gaseous moles increase from 1 to 2.

By Le Chatelier’s principle, decreasing total pressure favors the side with more moles, i.e. the products. So more XXX is formed.

Hence, Option A is correct.


  1. Check whether Kc<1K_c<1Kc​<1

We know ΔrG∘>0\Delta_r G^\circ>0Δr​G∘>0, so Kp<1K_p<1Kp​<1

Now, Kp=Kc(RT)ΔnK_p=K_c(RT)^{\Delta n}Kp​=Kc​(RT)Δn Here, Δn=2−1=1\Delta n=2-1=1Δn=2−1=1 Therefore, Kp=Kc(RT)K_p=K_c(RT)Kp​=Kc​(RT) So, Kc=KpRTK_c=\frac{K_p}{RT}Kc​=RTKp​​

Given: R=0.083 L bar K−1mol−1,T=298 KR=0.083\ \text{L bar K}^{-1}\text{mol}^{-1}, \quad T=298\ \text{K}R=0.083 L bar K−1mol−1,T=298 K RT=0.083×298≈24.7RT=0.083\times 298\approx 24.7RT=0.083×298≈24.7

Thus, Kc=Kp24.7K_c=\frac{K_p}{24.7}Kc​=24.7Kp​​ Since Kp<1K_p<1Kp​<1, Kc<124.7<1K_c<\frac{1}{24.7}<1Kc​<24.71​<1 Hence, Option D is correct.


  1. Check Option C: βequilibrium=0.7\beta_{\text{equilibrium}}=0.7βequilibrium​=0.7

At equilibrium under total pressure P=2P=2P=2 bar:

Mole fractions are yX=β1+β/2,yX2=1−β/21+β/2y_X=\frac{\beta}{1+\beta/2}, \qquad y_{X_2}=\frac{1-\beta/2}{1+\beta/2}yX​=1+β/2β​,yX2​​=1+β/21−β/2​

So partial pressures are PX=2⋅β1+β/2,PX2=2⋅1−β/21+β/2P_X=2\cdot \frac{\beta}{1+\beta/2}, \qquad P_{X_2}=2\cdot \frac{1-\beta/2}{1+\beta/2}PX​=2⋅1+β/2β​,PX2​​=2⋅1+β/21−β/2​

Therefore, Kp=PX2PX2K_p=\frac{P_X^2}{P_{X_2}}Kp​=PX2​​PX2​​ Kp=(2β/(1+β/2))22(1−β/2)/(1+β/2)K_p=\frac{\left(2\beta/(1+\beta/2)\right)^2}{2(1-\beta/2)/(1+\beta/2)}Kp​=2(1−β/2)/(1+β/2)(2β/(1+β/2))2​ Kp=2β2(1+β/2)(1−β/2)K_p=\frac{2\beta^2}{(1+\beta/2)(1-\beta/2)}Kp​=(1+β/2)(1−β/2)2β2​ Kp=2β21−β2/4K_p=\frac{2\beta^2}{1-\beta^2/4}Kp​=1−β2/42β2​

Now test β=0.7\beta=0.7β=0.7: Kp=2(0.7)21−(0.7)2/4K_p=\frac{2(0.7)^2}{1-(0.7)^2/4}Kp​=1−(0.7)2/42(0.7)2​ =0.981−0.1225=\frac{0.98}{1-0.1225}=1−0.12250.98​ =0.980.8775≈1.12=\frac{0.98}{0.8775}\approx 1.12=0.87750.98​≈1.12

But from ΔrG∘>0\Delta_r G^\circ>0Δr​G∘>0, we know Kp<1K_p<1Kp​<1 So β=0.7\beta=0.7β=0.7 would imply Kp>1K_p>1Kp​>1, which is impossible.

Hence, Option C is incorrect.


  1. Final conclusion

The incorrect statement is: C\boxed{\text{C}}C​

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