Thermodynamics · 03 / 06

Internal Energy & First Law

Track energy crossing a system boundary as heat or work, and use that transfer to account for the change in internal energy.

The learner question

When energy crosses a system boundary, how much stays inside?

Internal energy changes when energy enters or leaves. Heat transfer and mechanical work are two ways energy can cross the boundary. The first law is the accounting rule that keeps those transfers consistent.

Convention used here
ΔU=QWby\Delta U = Q - W_{by}

Positive Q enters the system. Positive W_by leaves the system as work done by the system. Equivalently, ΔU=Q+Won\Delta U=Q+W_{on}.

Boundary ledger

Push energy across the boundary and watch the ledger close.

internal energy increases
chosen system
ΔU = 80 Jinternal energy increases
Q: 80 J · heat in
Wby: 0 J · work out
heat Q
80 J
work by system
0 J
change in U
80 J
Heat into system Q80 J
Work done by system Wby0 J
Curated processes
Heat is one boundary transfer

Positive heat input increases the system's energy unless an equal or larger amount leaves as work.

Work can go either direction

Expansion often means the system does positive work on its surroundings. Compression means the surroundings do work on the system, so W_by is negative.

Internal energy is a state quantity

U belongs to the system state. Heat and work describe paths by which energy crossed the boundary during a process.

Sign convention must be stated

Some texts use work done on the system instead. Both conventions are valid when used consistently.

Adiabatic does not mean unchanged U

Q = 0 only says no heat crosses the boundary. Work alone can still raise or lower internal energy.

Transfer check

A gas is compressed adiabatically. Under our convention, which signs fit the process?

← Heat Transfer
Next: Phase Change · planned