Overview
This lesson brings the thermal physics and gas models together. You describe internal energy,
calculate work done during volume changes at constant pressure, and use the first law of
thermodynamics to track energy transfers into or out of a gas system.
What You Need to Know
- Internal energy is the sum of the random molecular kinetic and potential energies in a system.
- A temperature rise means the internal energy of an object increases.
- At constant pressure, gas work is W = p delta V.
- Work done by the gas and work done on the gas have opposite signs, so define the system clearly.
- The first law is delta U = q + W, where q is heating of the system and W is work done on the
system.
How to Work Through It
- Identify the system and decide whether energy is entering or leaving by heating.
- Decide whether the gas is expanding or being compressed.
- Calculate any constant-pressure work using W = p delta V.
- Substitute signs carefully into delta U = q + W and interpret the result.
Check Your Understanding
- What happens to internal energy when temperature increases?
- If a gas expands at constant pressure, is work done by the gas or on the gas?
- What does a negative value of delta U tell you about the system?
Common Mistakes
- Treating q, W, and delta U as always positive quantities.
- Mixing up work done by the gas with work done on the gas.
- Forgetting that W = p delta V only applies for constant pressure in this course context.
- Describing internal energy as only kinetic energy and leaving out molecular potential energy.
Next Steps
- Practise sign conventions until each term has a clear physical meaning.
- Use the revision lesson to connect temperature, ideal gases, kinetic theory, and thermodynamics.