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Worked Examples · Example 3.9

Q.The rate constants of a reaction at 500 K and 700 K are 0.02 s−10.02\ \text{s}^{-1} and 0.07 s−10.07\ \text{s}^{-1} respectively. Calculate the values of EaE_a and AA.

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Using the Arrhenius equation in its two-point logarithmic form, we find the activation energy Ea≈18.23 kJ mol−1E_a \approx 18.23\ \text{kJ mol}^{-1} and the pre-exponential factor A≈1.61 s−1A \approx 1.61\ \text{s}^{-1}.

The Arrhenius equation tells us how the rate constant kk depends on temperature:

k=Ae−Ea/RTk = A e^{-E_a / RT}

Here AA is the pre-exponential factor (frequency factor), EaE_a is the activation energy, R=8.314 J mol−1K−1R = 8.314\ \text{J mol}^{-1}\text{K}^{-1}, and TT is the absolute temperature. When we have rate constants at two different temperatures, we can eliminate AA by taking a ratio — that’s the classic trick. The ratio cancels AA and leaves an equation involving only EaE_a and the two temperatures.

Let’s work it through.

  1. Write the Arrhenius equation for each temperature.

    At T1=500 KT_1 = 500\ \text{K}, k1=0.02 s−1k_1 = 0.02\ \text{s}^{-1}:

ln⁡k1=ln⁡A−EaRT1\ln k_1 = \ln A - \frac{E_a}{R T_1}

At T2=700 KT_2 = 700\ \text{K}, k2=0.07 s−1k_2 = 0.07\ \text{s}^{-1}:

ln⁡k2=ln⁡A−EaRT2\ln k_2 = \ln A - \frac{E_a}{R T_2}

  1. Subtract the two equations to eliminate ln⁡A\ln A.

ln⁡k2−ln⁡k1=−EaRT2+EaRT1\ln k_2 - \ln k_1 = -\frac{E_a}{R T_2} + \frac{E_a}{R T_1}

Which simplifies to:

ln⁡(k2k1)=EaR(1T1−1T2)\ln \left( \frac{k_2}{k_1} \right) = \frac{E_a}{R} \left( \frac{1}{T_1} - \frac{1}{T_2} \right)

This is the two-point form of the Arrhenius equation — a direct route to EaE_a when you have data at two temperatures.

ln⁡(k2k1)=EaR(1T1−1T2)\ln \left( \frac{k_2}{k_1} \right) = \frac{E_a}{R} \left( \frac{1}{T_1} - \frac{1}{T_2} \right)

  1. Plug in the numbers.

k2k1=0.070.02=3.5\frac{k_2}{k_1} = \frac{0.07}{0.02} = 3.5

ln⁡(3.5)≈1.2528\ln(3.5) \approx 1.2528

1T1−1T2=1500−1700=700−500500×700=200350000=23500=11750\frac{1}{T_1} - \frac{1}{T_2} = \frac{1}{500} - \frac{1}{700} = \frac{700 - 500}{500 \times 700} = \frac{200}{350000} = \frac{2}{3500} = \frac{1}{1750}

So:

1.2528=Ea8.314×117501.2528 = \frac{E_a}{8.314} \times \frac{1}{1750}

  1. Solve for EaE_a.

Ea=1.2528×8.314×1750E_a = 1.2528 \times 8.314 \times 1750

Let’s compute step by step:

1.2528×8.314≈10.4161.2528 \times 8.314 \approx 10.416

Then:

10.416×1750=10.416×(1000+750)=10416+7812=18228 J mol−110.416 \times 1750 = 10.416 \times (1000 + 750) = 10416 + 7812 = 18228\ \text{J mol}^{-1}

So:

Ea≈18228 J mol−1=18.23 kJ mol−1E_a \approx 18228\ \text{J mol}^{-1} = 18.23\ \text{kJ mol}^{-1}

Watch out

A common mistake is forgetting to convert EaE_a from J/mol to kJ/mol. Always check the units — exam questions often expect the answer in kJ/mol.

  1. Now find AA using either temperature.

    Use the Arrhenius equation at T1=500 KT_1 = 500\ \text{K}:

k1=Ae−Ea/(RT1)k_1 = A e^{-E_a / (R T_1)}

First compute the exponent:

EaRT1=182288.314×500=182284157≈4.384\frac{E_a}{R T_1} = \frac{18228}{8.314 \times 500} = \frac{18228}{4157} \approx 4.384

So:

e−4.384≈0.01245e^{-4.384} \approx 0.01245

Then:

0.02=A×0.01245⇒A=0.020.01245≈1.606≈1.61 s−10.02 = A \times 0.01245 \quad \Rightarrow \quad A = \frac{0.02}{0.01245} \approx 1.606 \approx 1.61\ \text{s}^{-1}

Let’s check with T2=700 KT_2 = 700\ \text{K} for consistency:

EaRT2=182288.314×700=182285819.8≈3.132\frac{E_a}{R T_2} = \frac{18228}{8.314 \times 700} = \frac{18228}{5819.8} \approx 3.132

e−3.132≈0.0436e^{-3.132} \approx 0.0436

A=0.070.0436≈1.605≈1.61 s−1A = \frac{0.07}{0.0436} \approx 1.605 \approx 1.61\ \text{s}^{-1}

The two values match beautifully — confirming our EaE_a is correct.

Tip

Always verify AA using the second temperature. If the two values of AA differ significantly, you’ve made an arithmetic error in EaE_a.

  1. Verify with more precise intermediate values.

    Using more decimal places throughout:

ln⁡(3.5)=1.252762968\ln(3.5) = 1.252762968

1500−1700=0.0005714286\frac{1}{500} - \frac{1}{700} = 0.0005714286

Ea=1.252762968×8.314×10.0005714286=1.252762968×8.314×1750≈18227 J mol−1E_a = 1.252762968 \times 8.314 \times \frac{1}{0.0005714286} = 1.252762968 \times 8.314 \times 1750 \approx 18227\ \text{J mol}^{-1}

So Ea≈18.23 kJ mol−1E_a \approx 18.23\ \text{kJ mol}^{-1}, confirming step 4's result to more decimal places (not a different value).

AA therefore rounds to the printed value: A≈1.61 s−1A \approx 1.61\ \text{s}^{-1} (both temperature checks, 1.606 and 1.605, round to 1.61 — matching NCERT's printed A=1.61A = 1.61). As a subordinate aside: carrying the fully-precise exponent e−4.3847=0.012468e^{-4.3847} = 0.012468 gives A=1.604A = 1.604, which truncates toward 1.60, but the textbook's printed final is 1.61 and that is the value we report.

✓Final answer

The activation energy is Ea≈18.23 kJ mol−1E_a \approx 18.23\ \text{kJ mol}^{-1} (printed: 18230.818230.8 J) and the pre-exponential factor is A≈1.61 s−1A \approx 1.61\ \text{s}^{-1} (NCERT's printed value).

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