Work

Physics

In physics, work is done when a force moves an object through a distance in the direction of the force (W = Fd), measured in joules.

Formula

W = Fd
Visualization

Definition

In science, work happens when a push or pull makes something move; if you push and nothing moves, no work is done, no matter how tired you get. Work is done when a force causes displacement in the direction of the force, $W = Fd$, with $F$ in newtons and $d$ in meters, measured in joules ($1\ \text{J} = 1\ \text{N}\cdot\text{m}$); work transfers energy, so doing work on an object increases its energy by that amount, and a force perpendicular to the motion does no work. In general, work is the scalar product $W = \vec{F}\cdot\vec{d} = Fd\cos\theta$, where $\theta$ is the angle between force and displacement, and for a variable force $W = \int \vec{F}\cdot d\vec{r}$, the area under a force-versus-position graph. The work-energy theorem states $W_{\text{net}} = \Delta K$. Work can be negative when a force opposes motion, as with friction, and the work done by a conservative force equals $-\Delta U$.

Example

Lifting a backpack onto your shoulder is work, because you applied a force and the backpack moved up; holding it still on your shoulder is not work, even though it feels hard. A student pushing a desk with $40\ \text{N}$ across $3\ \text{m}$ of floor does $W = 40 \times 3 = 120\ \text{J}$, and lifting a $5\ \text{kg}$ box $2\ \text{m}$ requires $W = mgh = 5 \times 9.8 \times 2 = 98\ \text{J}$. With an angled force, a $20\ \text{kg}$ sled pulled $10\ \text{m}$ by a $50\ \text{N}$ rope at $30^\circ$ above horizontal while friction exerts $15\ \text{N}$ receives rope work of $50 \times 10 \times \cos 30^\circ \approx 433\ \text{J}$ and friction work of $-150\ \text{J}$. Net work is about $283\ \text{J}$, so the sled gains $283\ \text{J}$ of kinetic energy.

Key Insight

Work needs motion in the same direction as the force. Carrying a box across a room does no work on the box, because the upward force from your arms is sideways to the motion. Simple machines do not reduce work either: a ramp lets you use less force, but over a longer distance, so the product $Fd$ comes out the same. Centripetal force is the extreme case, doing zero work because it is always perpendicular to velocity. That is why a satellite in circular orbit keeps a constant speed forever without any energy input.