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The concept of work involves force and displacement; meanwhile, the work-energy theorem relates the net work done on a body to the difference in its kinetic energy, calculated between two points on its trajectory. While none of these quantities or relations involves time explicitly, we know that the time available to accomplish work is often just as important as the amount of work itself. For example, sprinters in a race may have achieved the same velocity at the finish, therefore, accomplishing the same amount of work, but the winner of the race did it in the least amount of time.

We can express the relationship between work done and the time taken to do it by introducing the concept of power. Since work can vary as a function of time, we first define average power as the work done during a time interval, divided by the interval. Work and energy are measured in units of joules, so power is measured in joules per second, which has the SI name watts, W: 1 J/s = 1 W. Another common unit for expressing the power capability of everyday devices is horsepower: 1 hp = 746 W.

This text is adapted from Openstax, University Physics Volume 1, Section 7.4: Power.

Tags
PowerWorkEnergyForceDisplacementWork energy TheoremKinetic EnergyTimeAverage PowerWattsHorsepower

From Chapter 7:

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