Work

Also called Work done by a force

The energy transferred into or out of a system by a force acting over a distance. Only the component of the force parallel to the displacement counts, so work is a scalar measured in joules and can be positive, negative or zero.

Work is a transfer, not something an object carries around. The AP Physics 1 CED defines it as the amount of energy transferred into or out of a system by a force exerted on that system over a distance, and the equation sheet prints W=Fd=FdcosθW = F_{\parallel} d = F d \cos\theta.

The cosine carries the sign, with θ\theta measured between the force and the displacement.

  • At θ=0\theta = 0^\circ the transfer is fully positive, W=FdW = Fd.
  • At θ=90\theta = 90^\circ it is zero. A perpendicular force can change the direction of the motion without changing the kinetic energy, which is why the normal force on a level floor, the string tension on a conical pendulum and the inward force in circular motion all do no work whatsoever.
  • At θ=180\theta = 180^\circ it is negative, W=FdW = -Fd. Kinetic friction on a sliding block is the standard case, and the minus sign means energy is leaving.

Work is a scalar quantity that may be positive, negative or zero, measured in joules, where one joule is one newton meter. Negative work is not less work than none, it is energy travelling the other way.

For a force that varies, work is the area under a graph of the parallel component against displacement.

Adding up the signed works and setting the total equal to ΔK\Delta K is the work energy theorem, and that procedure is the job of the work energy theorem guide.

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