Beats — Question 7

Section 17-7 · Physics pages 2764–2765

Question 7 Thermal drift turns a tuned pipe into a beat thermometer A fixed-length ideal pipe is tuned to a stable 440 Hz reference at T0 = 300 K. Its frequency obeys f(T) = 440 √ T/300. The pipe warms to 303 K; neglect dimensional expansion. L open open The pipe frequency drifts with gas temperature while the reference tone remains fixed. (a) Find the resulting beat frequency. (b) Derive the small-temperature-change relation between beat rate and temperature change. Use it to estimate the positive temperature change corresponding to 1.0 Hz beats.
Show solutionHide solution
Question 7 - Solution Thermal drift turns a tuned pipe into a beat thermometer L open open (a) Method and calculation Warming raises the pipe frequency, so fb = 440 (√ 303/300 −1 ) = 2.19453 Hz. The positive sign is known from the stated warming; the beat count alone would not supply it. (b) Interpretation and further calculation Linearizing near T0, f(T) ≃f0 ( 1 + ∆T 2T0 ) , fb ≃f0|∆T| 2T0 . For warming and fb = 1.0 Hz, ∆T ≃600/440 = 1.364 K. The exact result is 300[(441/440)2 −1] = 1.3652 K. Physical check The approximation requires |∆T| ≪T0. Gas composition changes or pipe-length changes would confound the thermal inference.

Question 7

Thermal drift turns a tuned pipe into a beat thermometer

A fixed-length ideal pipe is tuned to a stable 440Hz440\,\mathrm{Hz} reference at T0=300KT_0=300\,\mathrm K. Its frequency obeys f(T)=440T/300f(T)=440\sqrt{T/300}. The pipe warms to 303K303\,\mathrm K; neglect dimensional expansion.

Diagram shown in the original SVG worksheet.

  1. Find the resulting beat frequency.

  2. Derive the small-temperature-change relation between beat rate and temperature change. Use it to estimate the positive temperature change corresponding to 1.0Hz1.0\,\mathrm{Hz} beats.

Question 7 - Solution

Thermal drift turns a tuned pipe into a beat thermometer

Diagram shown in the original SVG worksheet.

(a) Method and calculation

Warming raises the pipe frequency, sofb=440(303/300−1)=2.19453Hz.f_b=440\left(\sqrt{303/300}-1\right)=2.19453\,\mathrm{Hz}.The positive sign is known from the stated warming; the beat count alone would not supply it.

(b) Interpretation and further calculation

Linearizing near T0T_0,f(T)≃f0(1+ΔT2T0),fb≃f0|ΔT|2T0.f(T)\simeq f_0\left(1+\frac{\Delta T}{2T_0}\right),\quad f_b\simeq\frac{f_0|\Delta T|}{2T_0}.For warming and fb=1.0Hzf_b=1.0\,\mathrm{Hz}, ΔT≃600/440=1.364K\Delta T\simeq600/440=1.364\,\mathrm K. The exact result is 300[(441/440)2−1]=1.3652K300[(441/440)^2-1]=1.3652\,\mathrm K.

Physical check

The approximation requires |ΔT|≪T0|\Delta T|\ll T_0. Gas composition changes or pipe-length changes would confound the thermal inference.