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Physics · Ch 11 — Waves

Laws of Transverse Vibrations in Stretched Strings

11.8.5

Laws of Transverse Vibrations in Stretched Strings

Three separate experimental laws describe how the fundamental frequency of a stretched string responds to changing exactly one of its three controlling physical variables -- vibrating length, tension, and mass per unit length -- while the other two are held fixed; all three laws are, in fact, nothing more than the single sonometer formula f=(1/2l)T/μf=(1/2l)\sqrt{T/\mu} examined one variable at a time. The law of length states that, for a given wire under fixed tension TT and fixed mass per unit length μ\mu, frequency varies inversely with the vibrating length, f∝1/lf\propto1/l, so that l×f=Cl\times f=C for some constant CC -- doubling the vibrating length of a string, all else unchanged, halves its fundamental frequency. The law of tension states that, for a given vibrating length ll and mass per unit length μ\mu, frequency varies directly with the square root of the tension, f∝Tf\propto\sqrt{T}, so f=ATf=A\sqrt{T} for some constant AA -- tightening a string (increasing its tension) raises its pitch. The law of mass states that, for a given vibrating length ll and tension TT, frequency varies inversely with the square root of the mass per unit length, f∝1/μf\propto1/\sqrt{\mu}, so f=B/μf=B/\sqrt{\mu} for some constant BB -- a heavier (th …