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Problems · Problem 5.12

Q.Calculate ΔrG⊖\Delta_r G^\ominus for the conversion of oxygen to ozone, 32O2(g)→O3(g)\tfrac{3}{2} O_2(g) \rightarrow O_3(g) at 298 K, if KpK_p for this conversion is 2.47×10−292.47 \times 10^{-29}.

Rajasthan RbseTextbookSubjective· 2mImportance★★★★★est
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✓ Free question

The standard Gibbs free energy change is found directly from the equilibrium constant using ΔrG⊖=−RTln⁡Kp\Delta_r G^\ominus = -RT \ln K_p. Substituting R=8.314 J mol−1K−1R = 8.314\ \text{J mol}^{-1}\text{K}^{-1}, T=298 KT = 298\ \text{K}, and Kp=2.47×10−29K_p = 2.47 \times 10^{-29} gives ΔrG⊖=+163 kJ mol−1\Delta_r G^\ominus = +163\ \text{kJ mol}^{-1}.

The relationship between the standard Gibbs free energy change and the equilibrium constant is one of the most powerful in chemical thermodynamics. It connects a measurable, macroscopic quantity (KpK_p) directly to the spontaneity and energy of a reaction under standard conditions.

The key equation is:

ΔrG⊖=−RTln⁡Kp\Delta_r G^\ominus = -RT \ln K_p

Here, RR is the universal gas constant (8.314 J mol−1K−18.314\ \text{J mol}^{-1}\text{K}^{-1}), TT is the absolute temperature in Kelvin, and KpK_p is the equilibrium constant expressed in terms of partial pressures.

Why does this work? At equilibrium, the Gibbs free energy of the system is at a minimum, and the reaction quotient QQ equals KK. The standard free energy change tells you how far the reaction is from equilibrium under standard conditions. A very small KpK_p (like 10−2910^{-29}) means the equilibrium lies heavily toward reactants — so the forward reaction is highly non-spontaneous, and ΔrG⊖\Delta_r G^\ominus should be large and positive.

Let’s apply this step by step.

  1. Identify the given values.

    Temperature: T=298 KT = 298\ \text{K}

    Equilibrium constant: Kp=2.47×10−29K_p = 2.47 \times 10^{-29}

    Gas constant: R=8.314 J mol−1K−1R = 8.314\ \text{J mol}^{-1}\text{K}^{-1} (always use this value unless told otherwise)

  2. Plug into the formula.

ΔrG⊖=−(8.314 J mol−1K−1)(298 K)ln⁡(2.47×10−29)\Delta_r G^\ominus = - (8.314\ \text{J mol}^{-1}\text{K}^{-1}) (298\ \text{K}) \ln(2.47 \times 10^{-29})

  1. Compute the natural logarithm. First, break it into parts:

ln⁡(2.47×10−29)=ln⁡(2.47)+ln⁡(10−29)\ln(2.47 \times 10^{-29}) = \ln(2.47) + \ln(10^{-29})

ln⁡(2.47)≈0.9042\ln(2.47) \approx 0.9042 (since e0.904≈2.47e^{0.904} \approx 2.47)

ln⁡(10−29)=−29ln⁡(10)≈−29×2.3026=−66.7754\ln(10^{-29}) = -29 \ln(10) \approx -29 \times 2.3026 = -66.7754

Adding:

ln⁡(2.47×10−29)≈0.9042−66.7754=−65.8712\ln(2.47 \times 10^{-29}) \approx 0.9042 - 66.7754 = -65.8712

Tip

A quick check: ln⁡(10−29)\ln(10^{-29}) dominates, so the result is roughly −66.8-66.8. The small positive correction from ln⁡(2.47)\ln(2.47) barely changes it. This tells you the answer will be large and positive.

  1. Multiply through. First, RT=8.314×298=2477.572 J mol−1RT = 8.314 \times 298 = 2477.572\ \text{J mol}^{-1} (about 2.478 kJ mol−12.478\ \text{kJ mol}^{-1}). Then:

ΔrG⊖=−(2477.572)×(−65.8712)\Delta_r G^\ominus = - (2477.572) \times (-65.8712)

The two negatives cancel:

ΔrG⊖=2477.572×65.8712 J mol−1\Delta_r G^\ominus = 2477.572 \times 65.8712 \ \text{J mol}^{-1}

Compute:

2477.572×65.8712≈163,200 J mol−12477.572 \times 65.8712 \approx 163,200\ \text{J mol}^{-1}

  1. Convert to kilojoules per mole (standard practice for such magnitudes):

ΔrG⊖≈163.2 kJ mol−1\Delta_r G^\ominus \approx 163.2\ \text{kJ mol}^{-1}

Rounding to three significant figures (matching KpK_p's three significant figures):

ΔrG⊖=163 kJ mol−1\Delta_r G^\ominus = 163\ \text{kJ mol}^{-1}

Watch out

A common mistake is forgetting the negative sign in −RTln⁡Kp-RT \ln K_p. Since ln⁡Kp\ln K_p is negative for Kp<1K_p < 1, the product −RTln⁡Kp-RT \ln K_p becomes positive. If you get a negative answer here, check your sign handling.

✓Final answer

The standard Gibbs free energy change is +163 kJ mol−1\boxed{+163\ \text{kJ mol}^{-1}}.

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