Work, Energy & Power

01Work, Energy & Power

Work done

This section covers work done as energy transferred by a force acting through a displacement.

Energy transferred by a force

Work is done when a force transfers energy by moving an object through a displacement.

If a constant force acts parallel to the displacement:

W=FsW=Fs

where WW is work done in joules, FF is the force in newtons and ss is displacement in metres.

A newton metre is equivalent to a joule:

1N m=1J1\,\text{N m}=1\,\text{J}

When the force and displacement are not parallel, only the component of the force in the direction of displacement does work.

displacementFFcosµµ

If the force makes an angle θ\theta with the direction of motion:

W=FscosθW=Fs\cos\theta

The term FcosθF\cos\theta is the component of the force parallel to the displacement.

When θ=0\theta=0^\circ, cosθ=1\cos\theta=1, so the equation reduces to W=FsW=Fs.

Work done against a resistive force such as friction transfers energy away from the object's mechanical energy, commonly into thermal energy and sound.

Worked example: A force pulls an object through 6.0m6.0\,\text{m}. The component of the force parallel to the motion is 1.61×103N1.61\times10^3\,\text{N}.

The work done is:

W=FsW=Fs

W=(1.61×103)(6.0)=9.7×103JW=(1.61\times10^3)(6.0) =9.7\times10^3\,\text{J}

Exam Tip: Use the component of force parallel to the displacement. If the force is angled, resolve it before substituting into the work equation.

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