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AP® Physics 2: Algebra-Based · Unit 9 · Topic 9.4

The First Law of Thermodynamics: Revision Notes (Physics 2 9.4)

One-page recap of internal energy, the first law ΔU = Q + W with work done on the gas, PV diagram signs, the four special processes and cycles.

Short on time? This page is the recap. For explanations, Figure 1 and the worked examples, use the full study guide.

Recap

  • Internal energy U = kinetic energy of the particles + potential energy of their arrangement. An ideal gas has no internal potential energy.
  • For an ideal monatomic gas, U is the total kinetic energy of the atoms and depends only on T.
  • Energy crosses the boundary in two ways: heating (Q) and work (W). Both are transfers, not contents.
  • The first law is conservation of energy for a closed system. For an isolated system, total energy is constant.
  • On a PV diagram, area under the path = |W|; the direction of the path gives the sign.

Key relationships

Relationship Symbols and units Use it to
ΔU = Q + W all in J; Q > 0 into gas; W > 0 when work is done on the gas link heating, work and internal energy
W = −PΔV P in Pa, V in m³ find work on the gas at constant (or average) pressure
U = (3/2)nRT = (3/2)PV R = 8.31 J/(mol·K), T in K find U or ΔU for an ideal monatomic gas
ΔU_cycle = 0, Q_net = −W_net W_net
Process Condition First law becomes
Isochoric W = 0 ΔU = Q
Isobaric P constant Q = (5/2)nRΔT
Isothermal ΔU = 0 Q = −W
Adiabatic Q = 0 ΔU = W

Assumptions behind the numbers

  • The gas is ideal and monatomic unless the question says otherwise.
  • The system is closed: no gas leaks in or out.
  • Processes are slow enough that P and T are well defined at every point on the PV path.
  • Temperatures in U = (3/2)nRT are in kelvin.

Mistakes to avoid

  1. Wrong sign of W. An expanding gas has W < 0 in this course.
  2. Confusing isothermal and adiabatic. Isothermal: ΔU = 0. Adiabatic: Q = 0.
  3. Area always positive. Size from the area, sign from the direction.
  4. Calling heat a property. A gas has U, not “heat”.
  5. Using (5/2) for a constant-volume process. At constant V, Q = ΔU = (3/2)nRΔT.
  6. Forgetting ΔU = 0 around a cycle.

Quick self-check

  1. A gas is heated with 300 J and does 120 J of work on its surroundings. What is ΔU? (+180 J, because W = −120 J)
  2. A gas is compressed at a constant 2.0 × 10⁵ Pa from 5.0 × 10⁻³ m³ to 3.0 × 10⁻³ m³. What is the work done on it? (+400 J)
  3. In which process is all the work done on a gas stored as internal energy? (Adiabatic, Q = 0)

Next: practice questions.

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