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Waves & Sound W. Sautter 2007
Transverse waves (light) Longitudinal waves (sound) Types of Wave Motion These are also called Compressional Waves
Comparing Transverse & Longitudinal Waves Rarefaction = low Pressure Compression = high Pressure Crest Trough Compression ...
Wavelength  Frequency    Properties of Transverse Waves Velocity Wavelength  Frequency    Velocity v x =
Constructive interference Destructive interference Partially Constructive interference Interference of Waves Wave A Wave A...
Sound Intensity Intensity = Power / Area Sound Source Sound radiates out from a source as concentric spheres and follows a...
Sound Intensity Inverse Square means as distance from the source doubles, the intensity 1/4 the original. If distance trip...
Decibels dB = 10 log ( I / I 0  ) I = the intensity of the sound to be evaluated I 0  = intensity of lowest sound that can...
<ul><li>SINCE LOGS ARE POWERS OF 10 THEY ARE USED JUST LIKE THE POWERS OF 10 ASSOCIATED WITH SCIENTIFIC NUMBERS. </li></ul...
<ul><li>A LOGARITHM (LOG) IS A POWER OF 10. IF A NUMBER IS WRITTEN AS 10 X  THEN ITS LOG IS X. </li></ul><ul><li>FOR EXAMP...
Sound Intensity Whisper 20 decibels Plane 120 decibels Conversation 60 decibels Siren 100 decibels
Tension, String Density & Frequency The frequency of a string depends on the Tension (N) and string  Linear  Density in ki...
The Doppler Effect V  (air)  = 341 m/s at 20  o C If observer is moving towards the source, V (observer)   = + If observer...
Slower at low temp Faster at high temp Speed of Sound Changes with Temperature
Speed of Sound Changes with Temperature V  =  331.5  =  .6 T 0 C
Doppler Effect  ( moving source moving observer ) Moving  Toward source Moving  Toward observer Observed Frequency Is higher
Doppler Effect  ( moving source moving observer ) Moving  Away from observer Moving  Away from source Observed Frequency I...
Doppler Effect  ( moving source stationary observer ) Moving  Away from observer Observer At rest Observed Frequency Is lo...
Doppler Effect  ( moving source stationary observer ) Moving  Toward observer Observer At rest Observed Frequency Is higher
Open End Columns 1 / 2   1    3 / 2   Fundamental     = 2 L Second Harmonic     =  L Third Harmonic     =  2/3 L
Open End Columns d = diameter of tube L = length of tube at first resonant point If d is small compared to L (which is oft...
Open End Columns Since  V =     f  If velocity is constant then as    decreases, f  increases  In the same ratio Second ...
Closed End Columns 1 / 4   3 / 4   5 / 4   Fundamental     = 4 L Second Harmonic     = 4/3 L Third Harmonic     =  4...
Closed End Columns d = diameter of tube L = length of tube at first resonant point If d is small compared to L (which is o...
Since  V =     f  If velocity is constant then as    decreases, f  increases  In the same ratio Second Harmonic     = 4...
Waves in a String Fundamental     = 2 L Second Harmonic     =  L Third Harmonic     =  2 / 3  L Fourth Harmonic     = ...
Since  V =     f  If velocity is constant then as    decreases, f  increases  In the same ratio Second Harmonic     =  ...
Waves from a Distant source = crest = trough Barrier with Two slits In phase waves Emerge from slits Constructive  interfe...
THE END
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Soundwaves 100212173149-phpapp02

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Transcript of "Soundwaves 100212173149-phpapp02"

  1. 1. Waves & Sound W. Sautter 2007
  2. 2. Transverse waves (light) Longitudinal waves (sound) Types of Wave Motion These are also called Compressional Waves
  3. 3. Comparing Transverse & Longitudinal Waves Rarefaction = low Pressure Compression = high Pressure Crest Trough Compression Rarefaction Compression Compression Rarefaction Rarefaction Trough Crest
  4. 4. Wavelength  Frequency  Properties of Transverse Waves Velocity Wavelength  Frequency  Velocity v x =
  5. 5. Constructive interference Destructive interference Partially Constructive interference Interference of Waves Wave A Wave A Wave A Wave B Wave B Wave B
  6. 6. Sound Intensity Intensity = Power / Area Sound Source Sound radiates out from a source as concentric spheres and follows an Inverse Square function
  7. 7. Sound Intensity Inverse Square means as distance from the source doubles, the intensity 1/4 the original. If distance triples, the intensity is 1/9 the original and so on. The surface area of a sphere is given by 4  r 2 Power is measured in watts ( 1 joule / second) Intensity = Power / Area = watts/ 4  r 2 Or Watts / meter 2
  8. 8. Decibels dB = 10 log ( I / I 0 ) I = the intensity of the sound to be evaluated I 0 = intensity of lowest sound that can be heard (1 x 10 -12 watts / meter 2 )
  9. 9. <ul><li>SINCE LOGS ARE POWERS OF 10 THEY ARE USED JUST LIKE THE POWERS OF 10 ASSOCIATED WITH SCIENTIFIC NUMBERS. </li></ul><ul><li>WHEN LOG VALUES ARE ADDED, THE NUMBERS THEY REPRESENT ARE MULTIPLIED. </li></ul><ul><li>WHEN LOG VALUES ARE SUBTRACTED, THE NUMBERS THEY REPRESENT ARE DIVIDED </li></ul><ul><li>WHEN LOGS ARE MULTIPLIED, THE NUMBERS THEY REPRESENT ARE RAISED TO POWERS </li></ul><ul><li>WHEN LOGS ARE DIVIDED, THE ROOTS OF NUMBERS THEY REPRESENT ARE TAKEN. </li></ul>Decibels are logarithmic functions
  10. 10. <ul><li>A LOGARITHM (LOG) IS A POWER OF 10. IF A NUMBER IS WRITTEN AS 10 X THEN ITS LOG IS X. </li></ul><ul><li>FOR EXAMPLE 100 COULD BE WRITTEN AS 10 2 THEREFORE THE LOG OF 100 IS 2. </li></ul><ul><li>IN PHYSICS CALCULATIONS OFTEN SMALL NUMBERS ARE USED LIKE .0001 OR 10 -4 . THE LOG OF .0001 IS THEREFORE –4. </li></ul><ul><li>FOR NUMBERS THAT ARE NOT NICE EVEN POWERS OF 10 A CALCULATOR IS USED TO FIND THE LOG VALUE. FOR EXAMPLE THE LOG OF .00345 IS –2.46 AS DETERMINED BY THE CALCULATOR. </li></ul>Decibels are logarithmic functions
  11. 11. Sound Intensity Whisper 20 decibels Plane 120 decibels Conversation 60 decibels Siren 100 decibels
  12. 12. Tension, String Density & Frequency The frequency of a string depends on the Tension (N) and string Linear Density in kilograms per meter (Kg/m). Light strings under high tension yield high frequencies. Heavy strings under low tension yield low frequencies. T _ m / L f =
  13. 13. The Doppler Effect V (air) = 341 m/s at 20 o C If observer is moving towards the source, V (observer) = + If observer is moving towards the source, V (observer) = - If source is moving towards the observer, V (source) = - If source is moving towards the observer, V (source) = + f = f v + v _________ v + v observer observer source source air air + + ( (
  14. 14. Slower at low temp Faster at high temp Speed of Sound Changes with Temperature
  15. 15. Speed of Sound Changes with Temperature V = 331.5 = .6 T 0 C
  16. 16. Doppler Effect ( moving source moving observer ) Moving Toward source Moving Toward observer Observed Frequency Is higher
  17. 17. Doppler Effect ( moving source moving observer ) Moving Away from observer Moving Away from source Observed Frequency Is lower
  18. 18. Doppler Effect ( moving source stationary observer ) Moving Away from observer Observer At rest Observed Frequency Is lower
  19. 19. Doppler Effect ( moving source stationary observer ) Moving Toward observer Observer At rest Observed Frequency Is higher
  20. 20. Open End Columns 1 / 2  1  3 / 2  Fundamental  = 2 L Second Harmonic  = L Third Harmonic  = 2/3 L
  21. 21. Open End Columns d = diameter of tube L = length of tube at first resonant point If d is small compared to L (which is often true) then: = 2 ( L + .8d )  fundamental  fundamental ~ 2 L ~
  22. 22. Open End Columns Since V =  f If velocity is constant then as  decreases, f increases In the same ratio Second Harmonic  = L Fundamental  = 2 L Third Harmonic  = 2/3 L Third Harmonic  =3 f fund Fundamental f = f fund Second Harmonic f = 2 f fund
  23. 23. Closed End Columns 1 / 4  3 / 4  5 / 4  Fundamental  = 4 L Second Harmonic  = 4/3 L Third Harmonic  = 4/5 L
  24. 24. Closed End Columns d = diameter of tube L = length of tube at first resonant point If d is small compared to L (which is often true) then: = 4 ( L + .4 d )  fundamental  fundamental ~ 4 L ~
  25. 25. Since V =  f If velocity is constant then as  decreases, f increases In the same ratio Second Harmonic  = 4/3 L Fundamental  = 4 L Third Harmonic  = 4/5 L Third Harmonic  = 5 f fund Fundamental f = f fund Second Harmonic f = 3 f fund Closed End Columns
  26. 26. Waves in a String Fundamental  = 2 L Second Harmonic  = L Third Harmonic  = 2 / 3 L Fourth Harmonic  = ½ L Node Node VIBRATIONAL MODES
  27. 27. Since V =  f If velocity is constant then as  decreases, f increases In the same ratio Second Harmonic  = L Fundamental  = 2 L Third Harmonic  = 2/3 L Third Harmonic  = 3 f fund Fundamental f = f fund Second Harmonic f = 2 f fund Waves in a String
  28. 28. Waves from a Distant source = crest = trough Barrier with Two slits In phase waves Emerge from slits Constructive interference Destructive interference Interference of Waves
  29. 29. THE END
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