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Interference and Doppler

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Presentation on theme: "Interference and Doppler"β€” Presentation transcript:

1 Interference and Doppler
Questions? Interference in Space Interference in Time (Beats) Doppler Shift Source moving Observer moving Both moving Examples

2 Interference in Space Occurs when 2 waves - of same frequency and wavelength - combine constructively or destructively because of different propagation paths. Two loudspeakers (stereo) animation Example 12-12 FM car radio AM car radio (cellphone) Noise-cancelling headphones Diffraction gratings

3 Interference in Space Animation
Two loudspeakers Two speaker animation Note: this is Java, not Flash

4 Example 12-13 πœ†= 𝑣 𝑓 = 343 π‘š 𝑠 1150 𝑠 Wavelength
πœ†= 𝑣 𝑓 = 343 π‘š 𝑠 𝑠 =0.298 π‘š For wavelength of 0.3 m, must be 0.15 m (half wavelength) further for destructive interference 4.15 m

5 Interference in Time Occurs when 2 waves - of slightly different frequency and wavelength - combine constructively or destructively with the variation in time. Produce β€œBeat” frequencies Instrument tuning Superheterodyne radio receiver Doppler weather radar

6 Interference in Time Derivation
Combine 2 waves with different frequencies 𝑦=π΄π‘π‘œπ‘  πœ” 1 𝑑 +π΄π‘π‘œπ‘  πœ” 2 𝑑 Use Trig identify to get 𝑦=2π΄π‘π‘œπ‘  πœ” 1 βˆ’ πœ” 𝑑 π΄π‘π‘œπ‘  πœ” 1 + πœ” 𝑑

7 Interference in Time Animation
Beats in time Animation (go to the last scene)

8 Example 12-3 Beat frequency is Guitar must be either 396 Hz or 404 Hz
βˆ†π‘“= 20 π‘£π‘–π‘π‘Ÿπ‘Žπ‘‘π‘–π‘œπ‘›π‘  5 π‘ π‘’π‘π‘œπ‘›π‘‘π‘  =4 𝐻𝑧 Guitar must be either 396 Hz or 404 Hz

9 Superheterodyne radio receiver
For FM, local oscillator always 10.7 MHz above desired station frequency Beat frequency of 10.7 MHz emerges. Can build very selective 10.7 MHz filters!

10 Doppler Shift (Source moving toward)
Wavelength compressed during wave creation Source moving toward observer compresses wavelength Ξ» β€² =Ξ»βˆ’ 𝑣 π‘ π‘œπ‘’π‘Ÿπ‘π‘’ 𝑇 But period T involves v and Ξ» in still air 𝑇= 1 𝑓 = 1 𝑣 π‘ π‘œπ‘’π‘›π‘‘ πœ† = Ξ» 𝑣 π‘ π‘œπ‘’π‘›π‘‘ Ξ» β€² =Ξ»βˆ’ 𝑣 π‘ π‘œπ‘’π‘Ÿπ‘π‘’ 𝑣 π‘ π‘œπ‘’π‘›π‘‘ Ξ» That shortened wave passing you ear sounds like 𝑓 β€² = 𝑣 π‘ π‘œπ‘’π‘›π‘‘ Ξ» β€² = 𝑣 π‘ π‘œπ‘’π‘›π‘‘ Ξ» 1βˆ’ 𝑣 π‘ π‘œπ‘’π‘Ÿπ‘π‘’ 𝑣 π‘ π‘œπ‘’π‘›π‘‘ 𝑓 β€² = 𝑓 1βˆ’ 𝑣 π‘ π‘œπ‘’π‘Ÿπ‘π‘’ 𝑣 π‘ π‘œπ‘’π‘›π‘‘ Moving away change β€œ-” to β€œ+”

11 Doppler shift Frequency and/or wavelength changed due to motion of source and/or listener Animation (moving source) (Play scene 1) s.html (Break the sound barrier!)

12 Doppler Shift (Observer moving toward)
Frequency increased as wave passes your ear Observer moving toward source increases frequency 𝑓 β€² = 𝑣 π‘ π‘œπ‘’π‘›π‘‘ + 𝑣 π‘œπ‘π‘ π‘’π‘Ÿπ‘£π‘’π‘Ÿ Ξ» 𝑓 β€² = 𝑓 𝑣 π‘ π‘œπ‘’π‘›π‘‘ + 𝑣 π‘œπ‘π‘ π‘’π‘Ÿπ‘£π‘’π‘Ÿ 𝑣 π‘ π‘œπ‘’π‘›π‘‘ 𝑓 β€² =𝑓 1+ 𝑣 π‘œπ‘π‘ π‘’π‘Ÿπ‘£π‘’π‘Ÿ 𝑣 π‘ π‘œπ‘’π‘›π‘‘ Summary 𝒇 β€² = 𝒇 πŸβˆ“ 𝒗 𝒔𝒐𝒖𝒓𝒄𝒆 𝒗 𝒔𝒐𝒖𝒏𝒅 𝑺𝒐𝒖𝒓𝒄𝒆 (βˆ’π’•π’π’˜π’‚π’“π’…, +π’‚π’˜π’‚π’š) 𝒇 β€² =𝒇 𝟏± 𝒗 𝒐𝒃𝒔𝒆𝒓𝒗𝒆𝒓 𝒗 𝒔𝒐𝒖𝒏𝒅 𝑢𝒃𝒔𝒆𝒓𝒗𝒆𝒓 (+π’•π’π’˜π’‚π’“π’…, βˆ’π’‚π’˜π’‚π’š)

13 Example 12-14 Toward Away Frequency shifts down as it passes you!
𝑓 β€² = 𝑓 1βˆ’ 𝑣 π‘ π‘œπ‘’π‘Ÿπ‘π‘’ 𝑣 π‘ π‘œπ‘’π‘›π‘‘ = 1600 𝐻𝑧 1βˆ’ 25 π‘š/𝑠 343 π‘š/𝑠 =1726 𝐻𝑧 Away 𝑓 β€² = 𝑓 1+ 𝑣 π‘ π‘œπ‘’π‘Ÿπ‘π‘’ 𝑣 π‘ π‘œπ‘’π‘›π‘‘ = 1600 𝐻𝑧 π‘š/𝑠 343 π‘š/𝑠 =1491 𝐻𝑧 Frequency shifts down as it passes you!

14 Example 12-15 Doppler shift 1 (listener moving toward sound)
𝑓 β€² = 1+ 𝑣 π‘œπ‘π‘  𝑣 𝑠𝑛𝑑 𝑓= π‘š/𝑠 343 π‘š/𝑠 𝐻𝑧 =5051 𝐻𝑧 Doppler shift 2 (listener re-emitting sound at shorter wavelength) 𝑓 β€²β€² = 𝑓′ 1βˆ’ 𝑣 π‘ π‘œπ‘’π‘Ÿπ‘π‘’ 𝑣 π‘ π‘œπ‘’π‘›π‘‘ = 5051 𝐻𝑧 1βˆ’ 3.5 π‘š/𝑠 343 π‘š/𝑠 =5103 𝐻𝑧

15 Problem 54 - Bat squeaking
Doppler shift 1 (bat creating squeak while flying toward wall) 𝑓 β€² = 𝑓 1βˆ’ 𝑣 π‘ π‘œπ‘’π‘Ÿπ‘π‘’ 𝑣 π‘ π‘œπ‘’π‘›π‘‘ = 30 π‘˜π»π‘§ 1βˆ’ 5 π‘š/𝑠 343 π‘š/𝑠 =30.44 π‘˜π»π‘§ Doppler shift 2 (bat listening to returning echo while flying toward wall) 𝑓 β€²β€² = 1+ 𝑣 π‘œπ‘π‘  𝑣 𝑠𝑛𝑑 𝑓′= 1+ 5 π‘š/𝑠 343 π‘š/𝑠 π‘˜π»π‘§ =30.88 π‘˜π»π‘§

16 Doppler Shift for Electromagnetic Waves
Doppler weather radar Red shift (Bell Labs – Cosmic background radiation)

17 Problem 55 - Tubas and Beats
Only one Doppler shift (tuba emitting sound while moving toward station) 𝑓 β€² = 𝑓 1βˆ’ 𝑣 π‘ π‘œπ‘’π‘Ÿπ‘π‘’ 𝑣 π‘ π‘œπ‘’π‘›π‘‘ = 75 𝐻𝑧 1βˆ’ 10 π‘š/𝑠 343 π‘š/𝑠 =77 𝐻𝑧 Beat frequency with tuba at station βˆ†π‘“=77 𝐻𝑧 βˆ’75 𝐻𝑧=2 𝐻𝑧

18 Problem 56 – Blood flow First Doppler shift (blood moving away from incoming sound) 𝑓 β€² = 1βˆ’ 𝑣 π‘œπ‘π‘  𝑣 𝑠𝑛𝑑 𝑓= 1βˆ’ 0.02 π‘š/𝑠 1540 π‘š/𝑠 3.5 𝑀𝐻𝑧 = 𝑀𝐻𝑧 Second Doppler shift (blood moving away while re-emitting reflected sound) 𝑓 β€²β€² = 𝑓′ 1+ 𝑣 π‘ π‘œπ‘’π‘Ÿπ‘π‘’ 𝑣 π‘ π‘œπ‘’π‘›π‘‘ = 𝑀𝐻𝑧 π‘š/𝑠 1540 π‘š/𝑠 = 𝑀𝐻𝑧 Beat frequency βˆ†π‘“= 𝑀𝐻𝑧 βˆ’ 𝑀𝐻𝑧= 𝑀𝐻𝑧=91 𝐻𝑧

19 Diagnose heart-valve problems with Ultrasound
Medical Applications Diagnose heart-valve problems with Ultrasound Measure blood velocity before and after valve using Doppler shift.* Get velocity difference very accurately using beat frequencies. Get pressure difference before and after valve using Bernoulli’s equation. 𝑃 β„Ž 𝜌 𝑣 β„Ž 2 = 𝑃 𝑙 𝜌 𝑣 𝑙 2 Get valve area from pressure difference. *Just like chapter 12, problem 56! High pressure Low pressure flow

20 End of Waves and Sound Next Thermodynamics


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