The Battle Against Oxidation
Imagine you are heating a piece of copper to a scorching 1250 K. At such high temperatures, copper is highly susceptible to oxidation. To protect it, we flush the system with nitrogen gas (N2). However, there's a catch—the nitrogen gas isn't perfectly pure; it contains 1 mole % of water vapor (H2O).
This tiny amount of water vapor is enough to act as an oxidizing agent, threatening to tarnish our pristine copper surface according to the following reaction:
2Cu(s)+H2O(g)→Cu2O(s)+H2(g)
Our mission is to find the minimum partial pressure of hydrogen gas (pH2) that we must maintain in the system to completely halt this oxidation process.
Hess's Law to the Rescue
To understand the thermodynamics of our target reaction, we first need its standard Gibbs free energy change (ΔG∘). The problem provides us with the thermodynamic data for two related reactions at 1250 K:
1. The formation of copper oxide:
2Cu(s)+21O2(g)→Cu2O(s)ΔG1∘=−78,000 J mol−1
2. The formation of water vapor:
H2(g)+21O2(g)→H2O(g)ΔG2∘=−1,78,000 J mol−1
We can use Hess's Law to construct our target reaction. By reversing the second reaction (which changes the sign of its ΔG∘) and adding it to the first reaction, the oxygen molecules cancel out perfectly!
ΔGnet∘=ΔG1∘−ΔG2∘
ΔGnet∘=−78,000−(−1,78,000)=+100,000 J mol−1
A positive standard free energy tells us that under standard conditions, the oxidation is not spontaneous. But we are not under standard conditions!
The Equilibrium Condition
The actual spontaneity of the reaction depends on the reaction quotient, Q, through the isotherm equation:
For the oxidation of copper to be prevented, the forward reaction must not be spontaneous. This requires ΔG≥0. To find the minimum required partial pressure of hydrogen, we look at the boundary condition where the system is exactly at equilibrium, meaning ΔG=0.
Let's define our reaction quotient, Q. Since solids (Cu and Cu2O) have an activity of 1, they do not appear in the expression. Q is simply the ratio of the partial pressures of the gaseous product and reactant:
We are given that the total pressure is 1 bar, and water vapor constitutes 1 mole % of the gas mixture. Therefore, the partial pressure of water vapor is:
pH2O=0.01×1 bar=0.01 bar
The Final Calculation
Now, we substitute all our known values into the isotherm equation. Remember to use the value of R=8 J K−1mol−1 as given in the problem, and ensure all energy units are in Joules.
0=100,000+(8)(1250)ln(0.01pH2)
Let's simplify the arithmetic. Multiplying 8 by 1250 gives exactly 10,000.
0=100,000+10,000ln(0.01pH2)
Dividing the entire equation by 10,000 makes it much cleaner:
Using the properties of logarithms, we can expand the right side:
We need to evaluate ln(0.01). We can rewrite 0.01 as 10−2:
ln(0.01)=ln(10−2)=−2ln(10)
The problem kindly provides ln(10)=2.3. Substituting this in:
Finally, we plug this back into our main equation to solve for ln(pH2):
−10=ln(pH2)−(−4.6)
−10=ln(pH2)+4.6
ln(pH2)=−10−4.6=−14.6
And there we have it! The natural logarithm of the minimum hydrogen partial pressure required to prevent the tarnishing of copper is -14.6.