Internal Energy
The internal energy of a system is the sum of the random kinetic and potential energies of its molecules. It depends only on the state of the system (its temperature, volume, phase), not on how it got there. A rise in temperature means more random kinetic energy. During a change of state the potential energy changes while the temperature stays constant. For an ideal gas there are no intermolecular forces, so internal energy is all kinetic: .
Learning objectives
- Define internal energy in terms of molecular kinetic and potential energies.
- Explain that internal energy is a function of state.
- Relate temperature rise to increased random kinetic energy.
- Explain why an ideal gas's internal energy depends only on temperature.
A ball is thrown fast across a room. Its molecules are all moving quickly. Has its internal energy increased?
Core idea
Heat ice at 0 °C and it melts without warming. The energy is going somewhere: into the potential energy of molecules pulling apart. Internal energy has two parts, and only one shows up on a thermometer.
= sum of random KE + PE of molecules. Ideal gas: no intermolecular forces, so (monatomic).
1. Two parts
- Kinetic: set by temperature.
- Potential: set by separation; changes during melting and boiling.
- Per molecule (kinetic theory).
- No PE: no intermolecular forces.
2.0 mol from 300 K to 400 K at constant volume.
- Goal
- ; heat supplied.
- Strategy
- .
- Formula.
- Fixed volume: no work.
Summary
- = random KE + PE.
- Ideal gas: .
- Internal energy
- Total random molecular KE + PE.
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