JEE Challenger
More from Equilibrium

Thermodynamic and Equilibrium Analysis of Gaseous Dissociation Reaction

Comprehension Passage

Thermal decomposition of gaseous X2X_2 into gaseous XX at 298 K298\text{ K} proceeds via the reaction: X2(g)⇌2X(g)X_2(g) \rightleftharpoons 2X(g) The standard reaction Gibbs free energy, ΔrG∘\Delta_r G^\circ, for this system is positive. Initially, 1 mole1\text{ mole} of X2X_2 is present without any XX. As decomposition progresses, the number of moles of XX produced is denoted by β\beta. Hence, βequilibrium\beta_{\text{equilibrium}} represents the moles of XX present at equilibrium. The process occurs under a constant total pressure of 2 bar2\text{ bar}. Assume ideal gas behavior. (Given: R=0.083 L bar K−1 mol−1R = 0.083\text{ L bar K}^{-1}\text{ mol}^{-1})

Which of the following statements is INCORRECT regarding this reaction?

Options

A

A decrease in the total pressure will lead to the formation of a greater quantity of gaseous XX

B

At the beginning of the reaction, the dissociation of gaseous X2X_2 occurs spontaneously

C

βequilibrium=0.7\beta_{\text{equilibrium}} = 0.7

Correct
D

Kc<1K_c < 1

Step-by-Step Solution

To determine which statement is INCORRECT, we analyze the given thermodynamic and chemical equilibrium properties of the reaction:

X2(g)⇌2X(g)X_2(g) \rightleftharpoons 2X(g)

1. Equilibrium Constant Expression (KpK_p)

Let the initial moles of X2X_2 be 1 mol1\text{ mol} and XX be 0 mol0\text{ mol}. At equilibrium, the moles of XX produced is βequilibrium\beta_{\text{equilibrium}}.

  • Moles of X2X_2 at equilibrium = 1−βequilibrium21 - \frac{\beta_{\text{equilibrium}}}{2}
  • Moles of XX at equilibrium = βequilibrium\beta_{\text{equilibrium}}
  • Total moles at equilibrium = (1−βequilibrium2)+βequilibrium=1+βequilibrium2=2+βequilibrium2\left(1 - \frac{\beta_{\text{equilibrium}}}{2}\right) + \beta_{\text{equilibrium}} = 1 + \frac{\beta_{\text{equilibrium}}}{2} = \frac{2 + \beta_{\text{equilibrium}}}{2}

Given the total pressure P=2 barP = 2\text{ bar}, the partial pressures are: PX2=(1−βequilibrium/21+βequilibrium/2)P=(2−βequilibrium2+βequilibrium)(2 bar)P_{X_2} = \left(\frac{1 - \beta_{\text{equilibrium}}/2}{1 + \beta_{\text{equilibrium}}/2}\right) P = \left(\frac{2 - \beta_{\text{equilibrium}}}{2 + \beta_{\text{equilibrium}}}\right) (2\text{ bar})

PX=(βequilibrium1+βequilibrium/2)P=(2βequilibrium2+βequilibrium)(2 bar)P_X = \left(\frac{\beta_{\text{equilibrium}}}{1 + \beta_{\text{equilibrium}}/2}\right) P = \left(\frac{2\beta_{\text{equilibrium}}}{2 + \beta_{\text{equilibrium}}}\right) (2\text{ bar})

The equilibrium constant KpK_p is: Kp=(PX)2PX2=[4βequilibrium2+βequilibrium]22(2−βequilibrium)2+βequilibrium=8βequilibrium24−βequilibrium2K_p = \frac{(P_X)^2}{P_{X_2}} = \frac{\left[\frac{4\beta_{\text{equilibrium}}}{2 + \beta_{\text{equilibrium}}}\right]^2}{\frac{2(2 - \beta_{\text{equilibrium}})}{2 + \beta_{\text{equilibrium}}}} = \frac{8\beta_{\text{equilibrium}}^2}{4 - \beta_{\text{equilibrium}}^2}


2. Evaluation of Options

  • Statement (A): For the given reaction, Δng=2−1=+1>0\Delta n_g = 2 - 1 = +1 > 0. According to Le Chatelier's Principle, a decrease in total pressure causes the equilibrium to shift towards the side with a greater number of gas moles (the forward direction). This leads to the formation of a greater quantity of gaseous XX. Thus, Statement (A) is CORRECT.

  • Statement (B): At the beginning of the reaction, no XX is present (PX=0P_X = 0), which implies Qp=0Q_p = 0. The reaction Gibbs free energy is given by: ΔrG=ΔrG∘+RTln⁡Qp\Delta_r G = \Delta_r G^\circ + RT \ln Q_p As Qp→0Q_p \to 0, ln⁡Qp→−∞\ln Q_p \to -\infty, causing ΔrG→−∞\Delta_r G \to -\infty. Since ΔrG<0\Delta_r G < 0, the reaction occurs spontaneously in the forward direction initially. Thus, Statement (B) is CORRECT.

  • Statement (C): We are given that ΔrG∘>0\Delta_r G^\circ > 0. From thermodynamics: ΔrG∘=−RTln⁡Kp∘>0  ⟹  ln⁡Kp∘<0  ⟹  Kp<1\Delta_r G^\circ = -RT \ln K_p^\circ > 0 \implies \ln K_p^\circ < 0 \implies K_p < 1 Substituting the expression for KpK_p: 8βequilibrium24−βequilibrium2<1\frac{8\beta_{\text{equilibrium}}^2}{4 - \beta_{\text{equilibrium}}^2} < 1 8βequilibrium2<4−βequilibrium28\beta_{\text{equilibrium}}^2 < 4 - \beta_{\text{equilibrium}}^2 9βequilibrium2<4  ⟹  βequilibrium<23≈0.679\beta_{\text{equilibrium}}^2 < 4 \implies \beta_{\text{equilibrium}} < \frac{2}{3} \approx 0.67 Since βequilibrium\beta_{\text{equilibrium}} must be strictly less than 0.670.67, it cannot equal 0.70.7. Thus, Statement (C) is INCORRECT.

  • Statement (D): The relationship between KpK_p and KcK_c is: Kp=Kc(RT)ΔngK_p = K_c (RT)^{\Delta n_g} Since Δng=1\Delta n_g = 1, R=0.083 L bar K−1 mol−1R = 0.083\text{ L bar K}^{-1}\text{ mol}^{-1}, and T=298 KT = 298\text{ K}: RT=0.083×298=24.734 L bar mol−1RT = 0.083 \times 298 = 24.734\text{ L bar mol}^{-1} Kc=KpRT=Kp24.734K_c = \frac{K_p}{RT} = \frac{K_p}{24.734} Since Kp<1K_p < 1, we get: Kc<124.734<1K_c < \frac{1}{24.734} < 1 Thus, Statement (D) is CORRECT.


Conclusion

The incorrect statement is C.