A force is said to do **work** if, when acting on a body, there is a displacement of the point of application in the direction of the force. For example, when a ball is held above the ground and then dropped, the work done on the ball as it falls is equal to the weight of the ball (a force) multiplied by the distance to the ground (a displacement).

The term *work* was introduced in 1826 by the French mathematician Gaspard-Gustave Coriolis as “weight *lifted* through a height”, which is based on the use of early steam engines to lift buckets of water out of flooded ore mines. The SI unit of work is the newton-metre or joule (J).

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Work and Work-energy theorem |

Forces and potential energy |

Conservation of energy |

Power |

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The work done by a constant force of magnitude *F* on a point that moves a displacement (not distance) *s* in the direction of the force is the product, W=F s

Work is closely related to energy. The law of conservation of energy states that the change in total internal energy of a system equals the added heat, minus the work performed by the system (the first law of thermodynamics).

**Power** is the rate of doing work. It is equivalent to an amount of energy consumed per unit time. In the SI system, the unit of **power** is the joule per second (J/s), known as the watt in honor of James Watt, the eighteenth-century developer of the steam engine.