The same heat input can split into work and internal energy in several exact ways. Exact arithmetic here means exact results for the stated model inputs; measured inputs still carry uncertainty and significant-figure limits.

highlighted = computed this step

Most energy can stay internal

A 20 joule input can split into 4 joules of work and 16 joules of internal-energy change.

Qin=4 J+16 J=20 JQ_{\text{in}}=4\ \text{J}+16\ \text{J}=20\ \text{J}
First-law split scanEach row closes to the same heat input.4 Jwork one16 Jinternal one12 Jwork two8 Jinternal two16 Jwork three4 Jinternal threesplit

The middle split still closes

The middle row uses 12 joules of work and 8 joules stored internally.

Qin=12 J+8 J=20 JQ_{\text{in}}=12\ \text{J}+8\ \text{J}=20\ \text{J}

More work leaves less internal storage

The third row sends 16 joules to work and only 4 joules to internal energy. The total stays fixed.

WΔUQin4 J16 J20 J12 J8 J20 J16 J4 J20 J\begin{array}{c|c|c}W&\Delta U&Q_{\text{in}}\\4\ \text{J}&16\ \text{J}&20\ \text{J}\\12\ \text{J}&8\ \text{J}&20\ \text{J}\\16\ \text{J}&4\ \text{J}&20\ \text{J}\\\end{array}
First-law split scanThe split rows are shown on one energy scale.4 Jwork one16 Jinternal one12 Jwork two8 Jinternal two16 Jwork three4 Jinternal threesplit