The Energy Landscape
Imagine you are standing at the foot of a massive mountain, representing the energy barrier of a chemical reaction.
To get to the other side, you must climb to the peak. This climb is the activation energy.
For our reaction, A2+B2⇌2AB, the forward climb is Ea(f)=180 kJ mol−1.
If you were to make the return journey from the products back to the reactants, the climb would be even steeper: Ea(b)=200 kJ mol−1.
The Master Equation for Enthalpy
Now, what exactly is the enthalpy change (ΔH) of this reaction?
Enthalpy change is simply the difference in altitude between your starting point and your final destination.
Mathematically, it is the difference between the forward and backward activation energies:
Let's calculate this for our uncatalyzed reaction.
Substituting the values, we get:
The negative sign is crucial here. It tells us that the final destination is lower than the starting point, meaning the reaction is exothermic and releases energy.
Enter the Catalyst
Next, we introduce a catalyst into the system.
Think of a catalyst as a secret tunnel through the mountain. It provides an alternative pathway with a much lower peak.
In our problem, the catalyst lowers the activation energy barrier by 100 kJ mol−1.
Because the peak itself is lowered, the climb is reduced equally for both the forward and reverse journeys!
The new forward activation energy becomes:
Ea(f)′=180−100=80 kJ mol−1
And the new reverse activation energy becomes:
Ea(b)′=200−100=100 kJ mol−1
The Grand Conclusion
Let's find the new enthalpy change using our catalyzed pathway.
Notice something beautiful? The enthalpy change remains exactly the same!
This highlights a fundamental law of nature: a catalyst only affects the kinetics (speed) of a reaction, never its thermodynamics (initial and final states).
Since the question asks for the magnitude of the enthalpy change, our final answer is 20 kJ mol−1.