Energy Scale and the Nature of Boiling
General Chemistry I – Week 1
First-Class Question
When water boils at 100 °C (1 atm), why are the O–H covalent bonds not broken? Answer this question using energy arguments.
1. Start from Kinetic Theory
From last semester, we learned that the average translational kinetic energy of a molecule is:
E ≈ (3/2) kT
At the boiling point of water:
T = 373 K
Boltzmann constant:
k = 1.38 × 10−23 J/K
Therefore:
kT ≈ 5.1 × 10−21 J ≈ 0.032 eV
3kT ≈ 1.5 × 10−20 J per molecule ≈ 0.1 eV
2. Convert to Energy per Mole
Multiply by Avogadro's number (6.02 × 1023):
3kT ≈ 9 kJ/mol (order of magnitude)
3. Compare Energy Scales
Covalent O–H bond energy:
≈ 460 kJ/mol ≈ 4.8 eV
Hydrogen bond (intermolecular):
≈ 10–25 kJ/mol ~0.1–0.25 eV
4. What Does This Tell Us?
The average thermal energy at 373 K:
- Is far smaller than covalent bond energy.
- Is comparable to intermolecular interaction energies.
Therefore:
- Molecules do not break apart.
- Hydrogen bonds between molecules can be overcome.
- Molecules separate → phase transition occurs.
5. The Deeper Point
Boiling is not about breaking molecules. It is about overcoming intermolecular potential energy.
Chemistry often depends on comparing energy scales.
If the available thermal energy is:
- Much smaller than bond energy → no chemical reaction.
- Comparable to intermolecular forces → phase change possible.
6. A Question for This Semester
Why does boiling occur sharply at 100 °C (1 atm)?
In this semester, we will learn that at the boiling point:
ΔG = 0
Liquid and vapor phases have equal chemical potential (molar Gibbs energy).
Today we just compared energy scales. In this semester we will minimize Gibbs free energy.
Chemistry begins when we learn to think in energy scales.
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