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Work and power

Work of a force (W = F·d·cos θ) and power (P = W/t or P = F·v), with the three regimes of cos θ named.

Parameters

0°: the force pushes along the motion. 90°: perpendicular. 180°: it opposes it.
Optional: leave empty for the work alone.

Result

Work

500 J

Calculation
W = F·d·cos θ = 50 N × 10 m × cos 0° = 500 J
Regime
motor work
Work
500 J
Power
25 W
Note

The force provides a motor work of 500 J.

Calculation, assumptions and sources

OverviewThe work of a force along a displacement: driving below 90°, zero at 90°, resistive and negative beyond.

The work of a force along a displacement: driving below 90°, zero at 90°, resistive and negative beyond. Power, in its two forms: W/t for work spread over time, F·v for steady-state traction. The regime is named with every result; resistive work gives a negative power.

Method & formulasW = F × d × cos θ
W = F × d × cos θP = W / tP = F × v (steady state)

Only the component of the force along the displacement does work, hence the cos θ. Power is the rate of work; in steady state, d = v·t gives P = F·v.

Work (J)
the energy the force gives to the motion (motor, positive) or takes from it (resistive, negative). One joule: one newton over one metre.
Power (W)
the rate of work; one watt is one joule per second, one metric horsepower 735.5 W.
Motor work
θ < 90°: the force accompanies the motion and feeds it energy.
Resistive work
θ > 90°: the force opposes the motion and drains its energy. Friction corresponds to 180°.
Validity domainW = F·d·cos θ assumes a constant force and a straight displacement; for a varying force (a spring) or a curved path, the work is the integral of F·dl.

W = F·d·cos θ assumes a constant force and a straight displacement; for a varying force (a spring) or a curved path, the work is the integral of F·dl. P = F·v is instantaneous; at constant speed, it equals W/t over the whole interval. Angles run from 0 to 180°.

Reading the resultThe work-energy theorem sums these works into the change of speed.

The work-energy theorem sums these works into the change of speed. No work is done by the centripetal force of a turn, the weight of a suitcase carried flat, or the normal reaction of the ground. At constant power, the available traction force drops with speed (P = F·v): 50 kW at 90 km/h give 2000 N.