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e(ho0n3
Apr1-07, 06:21 PM
Problem. Show that if the tension in a streched string is change by a small amount \Delta F_T, the frequency of the fundamental is changed by a small amount \Delta f = 1/2 (\Delta F_T / F_T) f.

Let T be the intial tension and h the change in tension. The velocity of a transverse wave on the string is v = \sqrt{T/\mu}. The initial frequency is

f = \frac{v}{\lambda} = \frac{\sqrt{T}}{\lambda \sqrt{\mu}}

The new frequency f' is

f' = \frac{v'}{\lambda} = \frac{\sqrt{T + h}}{\lambda \sqrt{\mu}}

The difference is:

f' - f = \frac{1}{\lambda \sqrt{\mu}} \, (\sqrt{T + h} - \sqrt{T})

That looks nothing like what I'm trying to show. Now, if I multiply the RHS by \sqrt{T} / \sqrt{T}, I get

f' - f = \frac{\sqrt{T + h} - \sqrt{T}}{\sqrt{T}} \, f

and if I do it again, I get

f' - f = \frac{\sqrt{T(T + h)} - T}{T} \, f

which is as close as I could get to what needs to be shown.

Doc Al
Apr1-07, 08:10 PM
\sqrt{T + h} = \sqrt{T}(1 + h/T)^{1/2}

Hint: Approximate that expression by taking a binomial expansion to first order in h/T. (Note that h/T << 1)

e(ho0n3
Apr2-07, 10:34 AM
Hint: Approximate that expression by taking a binomial expansion to first order in h/T. (Note that h/T << 1)

Great hint! I never considered it. The approximation is given below:

\sqrt{T(T + h)} = T + 1/2 \, h

and so

f' - f = \frac{T + 1/2 \, h - T}{T} \, f = \frac{h}{2T} \, f

Thanks.