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Question

a hollow metallic tube closed at one end produces resonance with a tuning fork of frequency n at temperature T0. The temperature of the tube is increased by dT. If the coefficient of thermal expansion of the tube metal is α, the beat frequency will be

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Solution

velocity of sound (v)=VRTM
vT
let v=βT..........(1)
let LB the length of rod at 0oC
L=L(1+αT){L= at TC
{L0=L(1+αT0)v0=βT0
now, for resonance
kλ04=L0
f0=k4v0L0
n=k4βT0L(1+αT0).......(iii)
L1=L0(1+αdT),α1=βT0+dt
{L1=L(1+αT0)(1(αdT)}
f1=k4v1L1=k4(βT0+dtL(1+αT0)(1+αdt))
f1=kβT04L(1+αT0)(1+dtT0(1αdT))
using binomial approximation
f1=n(1+12dTT0αdT)......(iii)
beat frequency(iii)(ii)=n(12dTT0αdT)

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