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Physics · Ch 3 — Laws of Motion

Lami's Theorem

3.4

Lami's Theorem

Statement. If three coplanar, concurrent forces F⃗1,F⃗2,F⃗3\vec F_1,\vec F_2,\vec F_3 keep a point in equilibrium, then the magnitude of each force is proportional to the sine of the angle between the other two, with the same constant of proportionality for all three:

F1sin⁡α=F2sin⁡β=F3sin⁡γ.\frac{F_1}{\sin\alpha}=\frac{F_2}{\sin\beta}=\frac{F_3}{\sin\gamma}.

Here α\alpha is the angle between F⃗2\vec F_2 and F⃗3\vec F_3 (i.e. the angle "opposite" F⃗1\vec F_1), and similarly for β\beta and γ\gamma.

Worked application (the swing/chain problem). A baby on a swing hangs at rest from two identical chains. Three forces act at the point where the chains meet the seat: gravity mgmg (down) and the two chain tensions TT (each at some angle θ\theta to the vertical). Applying Lami's theorem (or, equivalently, resolving vertically) gives

T=mg2cos⁡θ.T=\frac{mg}{2\cos\theta}.

When θ=0°\theta=0° (chains exactly vertical), this correctly reduces to T=mg/2T=mg/2 — each chain simply supports half the weight. …