Thermodynamics (Copy)
A2 Level Physics – Section 16: Thermodynamics (Detailed Notes)
16.1 Internal Energy
1. Definition of Internal Energy
- Internal energy (U): The total energy associated with the random motion and interactions of the molecules in a system.
- It is a state function: depends only on the state (e.g. temperature, pressure, volume), not on how the system got there.
Internal energy = Kinetic energy (EK) + Potential energy (EP)
- EK: due to random molecular motion (translation, rotation, vibration)
- EP: due to intermolecular forces (negligible in ideal gases)
2. Temperature and Internal Energy
- Temperature is directly related to the average kinetic energy of molecules.
- When temperature increases, internal energy increases, mainly due to a rise in molecular kinetic energy.
- For ideal gases:
- Internal energy depends only on temperature
- No intermolecular forces → EP ≈ 0
16.2 First Law of Thermodynamics
1. Work Done at Constant Pressure
- When a gas expands or is compressed at constant pressure, the work done (W) is:
W = p·ΔV
- W = work done (J)
- p = pressure (Pa)
- ΔV = change in volume (m³)
Important Sign Conventions:
- W > 0: work done by the gas (expands)
- W < 0: work done on the gas (compressed)
2. First Law of Thermodynamics
∆U = q + W
Where:
- ∆U = change in internal energy (J)
- q = heat added to the system (J)
- W = work done on the system (J)
Alternate signs used in some texts:
- ∆U = q – W (if W = work done by system)
Interpretation:
- Adding heat (q > 0) → increases internal energy
- Doing work on gas (W > 0) → increases internal energy
- Doing work by gas (W < 0) → decreases internal energy
- For ideal gases, internal energy depends only on temperature, so ∆U ∝ ∆T
Summary:
- Heating → increases kinetic energy of molecules
- Compression → increases potential interactions (in real gases) and kinetic energy
- Expansion without heat → decreases internal energy (gas cools)
