Physics 1251 The Science and Technology of Musical Sound - PowerPoint PPT Presentation

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Physics 1251 The Science and Technology of Musical Sound

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Sound in pipes can produce standing waves in the air column. ... Standing waves in a pipe are an example of the property of Interference of sound waves. ... – PowerPoint PPT presentation

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Title: Physics 1251 The Science and Technology of Musical Sound


1
Physics 1251The Science and Technology of
Musical Sound
  • Unit 3
  • Session 26 MWF
  • Sound in Pipes

2
Physics 1251 Unit 3 Session 26 Sound in Pipes
  • A standing wave on a string (tied at the ends) of
    length 3.0 m has two other nodes. What is the
    wavelength of the string wave?

There are 6 node-antinode distances. Therefore,
L 6 ? ?/4 3.0 m ? 2.0 m.
3
Physics 1251 Unit 3 Session 26 Pipes
  • 1' Lecture
  • Sound in pipes can produce standing waves in the
    air column.
  • Standing waves in air columns produce pressure
    nodes and displacement nodes (and antinodes) at
    different places.
  • A change in the acoustic impedance of the air
    column produces a reflection.
  • Organ pipes and the flute are examples of open or
    unstopped pipes.

4
Physics 1251 Unit 3 Session 26 Sound in Pipes
  • Standing Waves
  • Strings reflected waves combine to produce
    cancellation through destructive interference at
    nodes and constructive interference at antinodes.

String Wave Demonstration ? redux
5
Physics 1251 Unit 3 Session 26 Sound in Pipes
  • Standing Waves in a Cylindrical Pipe
  • A Closed or Stopped Pipe the pressure wave
    reflects without inversion, but the displacement
    wave inverts upon reflection.
  • Thus, a pressure anti-node will occur at the
    wall but, on the other hand, a displacement node
    will occur at the same place.

6
Physics 1251 Unit 3 Session 26 Sound in Pipes
  • Reflection of a Sound Wave in a Stopped Pipe
  • A pressure anti-node appears at a wall.

Pressure Wave
7
Physics 1251 Unit 3 Session 26 Sound in Pipes
  • Displacement Standing Wave
  • Visualization

8
Physics 1251 Unit 3 Session 26 Sound in Pipes
  • Reflection of a Sound Wave in a Stopped Pipe
  • A displacement node appears at a wall.

Displacement Anti-node
Displacement Wave
Displacement Node
?/4
?/4
9
Physics 1251 Unit 3 Session 26 Sound in Pipes
  • Comparison of Pressure and Displacement Standing
    Wave in a Double Stopped Pipe

?/4
?/4
Pressure Wave
Displacement Wave
10
Physics 1251 Unit 3 Session 26 Sound in Pipes
  • Standing waves in a pipe are an example of the
    property of Interference of sound
    waves.

11
Physics 1251 Unit 3 Session 26 Sound in Pipes
  • Recall
  • f ? v
  • Thus, f v/ ? L Nna ?/4
  • So f Nna v/4L
  • Nna 2 n fn 2 n v/4L
  • fn n v/2L
  • In double stopped pipe.

12
Physics 1251 Unit 3 Session 26 Sound in Pipes
  • Why does the sound wave reflect?

Because of an abrupt change in a property of the
medium.
13
Physics 1251 Unit 3 Session 26 Sound in Pipes
  • 80/20Acoustic Impedance
  • Z p/U
  • Acoustic Impedance is the ratio of the pressure p
    of a sound wave to the flow U ( u S) that
    results.
  • For a plane wave in a tube of cross section S
    (m2) in air the acoustic impedance is
  • Z ?v/S 415/ S rayl

14
Physics 1251 Unit 3 Session 26 Sound in Pipes
  • Acoustic Impedance and Reflection
  • The pressure that reflects is
  • pout R ? pin
  • R (Z2 Z1 )/ (Z2 Z1)
  • At an immoveable wall U 0
  • (no displacement) irrespective of the pressure
    and, thus,
  • Z ? 8
  • R 1

15
Physics 1251 Unit 3 Session 26 Sound in Pipes
  • But what about an open pipe?
  • Does the sound reflect?

Yes! Z p/U p drops suddenly near the end of
the pipe, since S ? 8. Thus, Z 0, R -1
16
Physics 1251 Unit 3 Session 26 Sound in Pipes
  • Comparison of Pressure Standing Wave in a Single
    Stopped and an Open Pipe

L
17
Physics 1251 Unit 3 Session 26 Sound in Pipes
  • 80/20For Stopped Pipe
  • Nna odd number 2n-1, n1,2,3,4
  • ?n 4L/ Nna 4L / (2n-1)
  • fstopped f2n-1 v/ ?n (2n-1) v/ 4L
  • 80/20Only odd harmonics of fstopped 1 v/4L.

18
Physics 1251 Unit 3 Session 26 Sound in Pipes
  • Comparison of Pressure Standing Wave in a Single
    Stopped and an Open Pipe

L
19
Physics 1251 Unit 3 Session 26 Sound in Pipes
  • Open versus Stopped Pipe
  • Demonstration

20
Physics 1251 Unit 3 Session 26 Sound in Pipes
  • 80/20For Open Pipe
  • Nna even number 2n, n1,2,3,4
  • ?n 4L / Nna 4L/(2n) 2L/ n
  • fopen fn v/ ?n n ? v/2L
  • 80/20All harmonics of fopen 1 v/2L 2
    fstopped 1

21
Physics 1251 Unit 3 Session 26 Sound in Pipes
  • End Correction for Open Pipe
  • d 0.6 a for a ? d 0 a for a gt ? / 4

a Radius
L d
d
22
Physics 1251 Unit 3 Session 26 Sound in Pipes
  • Organ Pipes

Open Pipes
23
Physics 1251 Unit 3 Session 26 Sound in Pipes
  • Organ Pipes
  • Pipe Organs use both
  • open and stopped pipes
  • in different ranks because
  • the timbre is different
  • for each.

Open Pipes
Stopped Pipes
24
Physics 1251 Unit 3 Session 26 Sound in Pipes
  • Transverse Flute

25
Physics 1251 Unit 3 Session 26 Sound in Pipes
  • Transverse Flute
  • 80/20The transverse flute is a cylindrical open
    pipe.

Mouthpiece is open
26
Physics 1251 Unit 3 Session 26 Sound in Pipes
  • Other Flute-like Instruments

Kaen
RenaissanceFlute
Penny whistle
Fife
27
Physics 1251 Unit 3 Session 26 Sound in Pipes
  • Stopped Pipe Flute-like Instruments

The Pan Pipe Only odd harmonics different
timbre Lower fundamental shorter pipe
28
Physics 1251 Unit 3 Session 26 Sound in Pipes
  • Summary
  • fopen fn n ? v/2L
  • fstopped f2n-1 (2n-1) v/ 4L
  • Stopped and open cylindrical pipes have different
    timbres.
  • Impedance Z p/U
  • An abrupt change in Z is responsible for the
    reflections that lead to standing waves in pipes.
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