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Chapter 3: Sound Wave

Chapter 3: Sound Wave. The Doppler Effect. Objectives : The student will be able to Define the Doppler Effect. Understand some applications on sound. Doppler Effect.

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Chapter 3: Sound Wave

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  1. Chapter 3: Sound Wave The Doppler Effect FCI

  2. Objectives: The student will be able to • Define the Doppler Effect. • Understand some applications on sound FCI

  3. Doppler Effect A tone is not always heard at the same frequency at which it is emitted. When a train sounds its horn as it passes by, the pitch of the horn changes from high to low. Any time there is relative motion between the source of a sound and the receiver of it, there is a difference between the actual frequency and the observed frequency. This is called the Doppler effect. Click to hear effect: FCI

  4. The Doppler effect applied to electomagnetic waves helps meteorologists to predict weather, allows astronomers to estimate distances to remote galaxies, and aids police officers catch you speeding. The Doppler effect applied to ultrasound is used by doctors to measure the speed of blood in blood vessels, just like a cop’s radar gun. The faster the blood cell are moving toward the doc, the greater the reflected frequency. FCI

  5. ) ( v  vL fL=fS v  vS fL = frequency as heard by a listener fS = frequency produced by the source v = speed of sound in the medium vL = speed of the listener vS = speed of the source Doppler Equation This equation takes into account the speed of the source of the sound, as well as the listener’s speed, relative to the air (or whatever the medium happens to be). The only tricky part is the signs. First decide whether the motion will make the observed frequency higher or lower. (If the source is moving toward the listener, this will increase fL, but if the listener is moving away from the source, this will decrease fL.) Then choose the plus or minus as appropriate. A plus sign in the numerator will make fL bigger, but a plus in the denominator will make fL smaller. Examples are on the next slide. FCI

  6. ) ( v  vL fL=fS v  vS Doppler Set-ups The horn is producing a pure 1000 Hz tone. Let’s find the frequency as heard by the listener in various motion scenarios. The speed of sound in air at 20 C is 343 m/s. ) ( 343 fL=1000 343 -10 = 1030 Hz still 10 m/s ) ( 343 + 10 fL=1000 343 = 1029 Hz still 10 m/s Note that these situation are not exactly symmetric. Also, in real life a horn does not produce a single tone. More examples on the next slide. FCI

  7. ) ( v  vL fL=fS v  vS Doppler Set-ups (cont.) The horn is still producing a pure 1000 Hz tone. This time both the source and the listener are moving with respect to the air. ) ( 343 - 3 fL=1000 343 -10 = 1021 Hz 10 m/s 3 m/s ) ( 343 + 3 fL=1000 343 - 10 = 1039 Hz 10 m/s 3 m/s Note the when they’re moving toward each other, the highest frequency possible for the given speeds is heard. Continued . . . FCI

  8. ) ( v  vL fL=fS v  vS Doppler Set-ups (cont.) The horn is still producing a pure 1000 Hz tone. Here are the final two motion scenarios. ) ( 343 - 3 fL=1000 343 + 10 = 963 Hz 10 m/s 3 m/s ) ( 343 + 3 fL=1000 343 + 10 = 980 Hz 10 m/s 3 m/s Note the when they’re moving toward each other, the highest frequency possible for the given speeds is heard. Continued . . . FCI

  9. ( ) v  vL ( ) 343 + vL fL=fS 750=650 v  vS 343 - 21 vL= 28.5 m/s Doppler Problem Mr. Magoo & Betty Boop are heading toward each other. Mr. Magoo drives at 21 m/s and toots his horn (just for fun; he doesn’t actually see her). His horn sounds at 650 Hz. How fast should Betty drive so that she hears the horn at 750 Hz? Assume the speed o’ sound is 343 m/s. 21 m/s vL FCI

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