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Physics 221, April 5

Key Concepts: Traveling sound waves Standing sound waves Water waves The Doppler effect. Physics 221, April 5. Traveling sound waves. For a traveling sound wave in we have for the pressure variations : ∆P( x,t ) = ∆ P max sin ( kx - ωt + φ)

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Physics 221, April 5

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  1. Key Concepts: • Traveling sound waves • Standing sound waves • Water waves • The Doppler effect Physics 221, April 5

  2. Traveling sound waves For a traveling sound wave in we have for the pressure variations: ∆P(x,t) = ∆Pmaxsin(kx - ωt + φ) For the displacements from the equilibrium position we have: ∆s(x,t) = ∆smaxcos(kx - ωt + φ) The speed of a sound wave through a medium does not depend on the frequency of the wave. The speed of sound at standard temperature and pressure is 343 m/s. The energy carried by a sound wave is proportional to the square of its amplitude. Sound levels β are measured using a logarithmic scale. β = 10 log10(I/I0) The units of β are decibels (dB).  I0 = 10-12 W/m2 is the reference intensity. MULTIPLY the intensity by 10 < = > ADD another 10 dB to the sound level

  3. You hear the sound of the ring of a distant cannon 5 seconds after seeing the flash. How far are you from the cannon? • ~500 m • ~1700 m • ~70 m • no way to tell 30

  4. Extra credit:100 dB corresponds to what intensity, in W/m2? • 10-12 W/m2 • 10-19 W/m2 • 10-2 W/m2 • 10+10 W/m2 • none of these 10 dB: Rustling or falling leaves 50 dB: Conversation. 100 dB: Hearing damage after about 15 minutes. 30

  5. Beats Intensity modulations are produced when waves of slightly different frequencies are superimposed. The beat frequency is equal to the difference frequency | f1 - f2|. Demonstration: A speaker box containing two oscillators, one fixed and the other variable. By tuning the variable oscillator we can produce audio beats.

  6. Extra credit:Two flutists are tuning up. If the conductor hears the beat frequency increasing, are the two flute frequencies getting closer together or father apart? • Closer • Farther apart • No way to tell 30

  7. Interference Demonstration: Two speakers and a sine wave generator. The speakers are driven by the same signal and can move in or 180 degrees out of phase. Like all waves, two or more sound waves traveling trough the same medium will interfere.  We can have constructive and destructive interference. Assume s1 = 5 m and s2 = 4 m. The path difference ∆ = 1 m. If ∆ = m*λ with m = integer, then we have constructive interference. Constructive interference: λ =∆/m, f = v/λ = mv/∆. Destructive interference: λ =∆/(m + ½), f = v/λ = (m + ½)v/∆.

  8. If ∆ = 1 m and the speed of sound is 340 m/s, which statement is correct? • At the frequency f = 680 Hz the sound at the position of the listener is loud. • At the frequency f = 1190 Hz the sound at the position of the listener is very soft. • At the frequency f = 340 Hz the sound at the position of the listener is loud. • All of the above statements are correct. 30

  9. Constructive interference: λ =∆/m, f = v/λ = mv/∆.Destructive interference: λ =∆/(m + ½), f = v/λ = (m + ½)v/∆. Here ∆ = 1 m. If f*∆/v is an integer, we have constructive interference, if it is an integer plus ½, we have destructive interference. Case 1: f = 680 Hz, f*∆/v = 680/340 = 2. Case 2: f = 1190 Hz, f*∆/v = 1190/340 = 3.5. Case 1: f = 340 Hz, f*∆/v = 340/340 = 1.

  10. Standing sound waves We can create a standing wave in a tube, which is open on both ends, and in a tube, which is open on one end and closed on the other end.  Open and closed endsreflect waves differently.  Demonstration: Singing Tubes

  11. Extra Credit:How will the harmonics of an open tube compare with those of a stringed instrument (with the same fundamental)? • Totally different frequencies • The same frequencies 30

  12. f = v/λ While the wavelengths of the standing waves on the string and in the tube are the same, the speed of the sound waves is different from the speed of waves on a string.

  13. Fourier Series The quality of a sound depends on the relative intensities of the waves with the natural frequencies.  It depends on the spectrum of the sound.  The sound quality of a musical instrument is called its timbre. Any wave pattern can be produced by superimposing the appropriate sinusoidal waves.  Fast computer algorithms exist that calculate the required frequencies and amplitudes.

  14. The same note, two different instruments

  15. You’re listening to a computer-generated tone which contains two frequencies, f1 = 100 Hz and f6 = 600 Hz.What frequency do you (likely) perceive? • 100 Hz • 600 Hz • Something totally different. 30

  16. 600 Hz = 6*100 Hz 600 Hz is a higher harmonic of 100 Hz The wavelength of the 100 Hz wave is 6 times longer than the wavelength of the 100 Hz wave. A pattern composed of a superposition of both waves has a repetition rate or frequency of 100 Hz.

  17. Doppler effect The perceived pitch of a sound wave also changes if the observer or the source is moving.  If both source and observer are in motion, then the apparent frequency of the sound wave reaching the observer is f = f0(v + vo)/(v - vs) if the observer and the source are approaching each other, andf = f0(v - vo)/(v + vs) if the observer and the source are receding from each other. v = speed of sound vo = speed of observer vs = speed of source Demonstration: The Doppler Rocket

  18. Extra credit:A train whistle is blown by the driver who hears the sound at 650 Hz. If the train is heading towards a station at 20.0 m/s, what will the whistle sound like to a waiting commuter? Take the speed of sound to be 340 m/s. • 691 Hz • 614 Hz • 650 Hz • 688 Hz 30

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