Grade 12 Physics · Work at an angle
What a force actually buys
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What a force actually buys

Grade 11 asked what forces DO to motion. Grade 12 asks what they COST. The currency is work, and its unit is the joule: 1 J=1 Nm1\ \mathrm{J} = 1\ \mathrm{N \cdot m}, one newton pushing through one metre. Read aloud: W equals F d cos theta. Letter by letter — WW is the work in joules, FF is the constant force in newtons, dd is the displacement in metres, and θ\theta (Greek theta) is the angle between the force and the direction of travel. Whichever one the question leaves blank is what you solve for.

House rule for this chapter, stated once: W is work. Weight gets written Fg=mgF_g = mg, the way SPH4U writes it, because two different WW's in one chapter is a wound nobody needs.

The cosine is the whole idea. Only the part of the force lying ALONG the path does work. Pull straight along and cos0=1\cos 0^\circ = 1 — full price. Pull at 6060^\circ and cos60=0.5\cos 60^\circ = 0.5 — half of your force is going sideways and buys nothing. Push at 9090^\circ and cos90=0\cos 90^\circ = 0: carry a heavy bag across a level room and, in physics' strict accounting, you do zero work on it. Your shoulder disagrees; the ledger does not. And when the force points BACKWARD along the path, cos180=1\cos 180^\circ = -1 — friction's signature move, and the reason work can be negative.