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1 Musical Acoustics Lecture 6 Waves - 1 Musical Acoustics, C. Bertulani

Lecture 6 Waves - 1faculty.tamuc.edu/cbertulani/music/lectures/Lec6/Lec6.pdfLecture 6 Waves - 1 Musical Acoustics, C. Bertulani . 2 Waves The wave carries the disturbance, but not

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Page 1: Lecture 6 Waves - 1faculty.tamuc.edu/cbertulani/music/lectures/Lec6/Lec6.pdfLecture 6 Waves - 1 Musical Acoustics, C. Bertulani . 2 Waves The wave carries the disturbance, but not

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Musical Acoustics

Lecture 6

Waves - 1

Musical Acoustics, C. Bertulani

Page 2: Lecture 6 Waves - 1faculty.tamuc.edu/cbertulani/music/lectures/Lec6/Lec6.pdfLecture 6 Waves - 1 Musical Acoustics, C. Bertulani . 2 Waves The wave carries the disturbance, but not

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Waves

The wave carries the disturbance, but not the water

Each point makes a simple harmonic vertical oscillation

position x

position y

Page 3: Lecture 6 Waves - 1faculty.tamuc.edu/cbertulani/music/lectures/Lec6/Lec6.pdfLecture 6 Waves - 1 Musical Acoustics, C. Bertulani . 2 Waves The wave carries the disturbance, but not

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–  Periodic wave – is regular frequency continuing for may cycles

–  Wave pulse - is a disturbance of short duration

Mechanical waves –  Require medium for propagation –  Waves move through medium –  Medium remains in place

Electromagnetic waves (light) do not require medium

Page 4: Lecture 6 Waves - 1faculty.tamuc.edu/cbertulani/music/lectures/Lec6/Lec6.pdfLecture 6 Waves - 1 Musical Acoustics, C. Bertulani . 2 Waves The wave carries the disturbance, but not

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Types of waves

Transversal: movement is perpendicular to the wave motion

wave

oscillation

Longitudinal: movement is in the direction of the wave motion

oscillation

Page 5: Lecture 6 Waves - 1faculty.tamuc.edu/cbertulani/music/lectures/Lec6/Lec6.pdfLecture 6 Waves - 1 Musical Acoustics, C. Bertulani . 2 Waves The wave carries the disturbance, but not

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Longitudinal (Compression) Waves

Sound waves are longitudinal waves Elements move parallel to wave motion

Page 6: Lecture 6 Waves - 1faculty.tamuc.edu/cbertulani/music/lectures/Lec6/Lec6.pdfLecture 6 Waves - 1 Musical Acoustics, C. Bertulani . 2 Waves The wave carries the disturbance, but not

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Transverse Waves Elements move perpendicular to wave motion

Page 7: Lecture 6 Waves - 1faculty.tamuc.edu/cbertulani/music/lectures/Lec6/Lec6.pdfLecture 6 Waves - 1 Musical Acoustics, C. Bertulani . 2 Waves The wave carries the disturbance, but not

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Snapshot of a Transverse Wave

wavelength

x

Page 8: Lecture 6 Waves - 1faculty.tamuc.edu/cbertulani/music/lectures/Lec6/Lec6.pdfLecture 6 Waves - 1 Musical Acoustics, C. Bertulani . 2 Waves The wave carries the disturbance, but not

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Snapshot of Longitudinal Wave

y could refer to pressure or density

λ

Page 9: Lecture 6 Waves - 1faculty.tamuc.edu/cbertulani/music/lectures/Lec6/Lec6.pdfLecture 6 Waves - 1 Musical Acoustics, C. Bertulani . 2 Waves The wave carries the disturbance, but not

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Describing a traveling wave

While the wave has traveled one wavelength, each point on the rope has made one period of oscillation.

λ: wavelength distance between two maxima. f: frequency of oscillations

vwave =λT= λ f

Page 10: Lecture 6 Waves - 1faculty.tamuc.edu/cbertulani/music/lectures/Lec6/Lec6.pdfLecture 6 Waves - 1 Musical Acoustics, C. Bertulani . 2 Waves The wave carries the disturbance, but not

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Speed of a Wave in a Vibrating String

v =Tµwhere µ =

mL

For different kinds of waves: (e.g. sound) •  Always a square root •  Numerator related to restoring force •  Denominator is some sort of mass density

L, m

screw tension T

Page 11: Lecture 6 Waves - 1faculty.tamuc.edu/cbertulani/music/lectures/Lec6/Lec6.pdfLecture 6 Waves - 1 Musical Acoustics, C. Bertulani . 2 Waves The wave carries the disturbance, but not

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Why does it matter?

λf = v

f =vλ

Higher tension T à higher frequency, because (for the same wavelength and same string) •  Reverse is true (smaller T, lower f)

Higher density μ à lower frequency

v =Tµ

or

change T or change μ

Page 12: Lecture 6 Waves - 1faculty.tamuc.edu/cbertulani/music/lectures/Lec6/Lec6.pdfLecture 6 Waves - 1 Musical Acoustics, C. Bertulani . 2 Waves The wave carries the disturbance, but not

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Sound wave speed

v = γpρ

γ = adiabatic index p = pressure ρ = density

Air: γ ~ 1.4, p ~ 1 atm ~ 100 Pa ρ ~ 1.2 kg/m³

à vair ~ 331 m/s

Page 13: Lecture 6 Waves - 1faculty.tamuc.edu/cbertulani/music/lectures/Lec6/Lec6.pdfLecture 6 Waves - 1 Musical Acoustics, C. Bertulani . 2 Waves The wave carries the disturbance, but not

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The lone Ranger put his ear to the ground

Speed of sound in several materials

Page 14: Lecture 6 Waves - 1faculty.tamuc.edu/cbertulani/music/lectures/Lec6/Lec6.pdfLecture 6 Waves - 1 Musical Acoustics, C. Bertulani . 2 Waves The wave carries the disturbance, but not

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The frequency of sound

•  We hear frequencies of sound as having different pitch.

•  A low frequency sound has a low pitch, like the rumble of a big truck.

•  A high-frequency sound has a high pitch, like a whistle or siren.

•  In speech, women have higher fundamental frequencies than men.

Page 15: Lecture 6 Waves - 1faculty.tamuc.edu/cbertulani/music/lectures/Lec6/Lec6.pdfLecture 6 Waves - 1 Musical Acoustics, C. Bertulani . 2 Waves The wave carries the disturbance, but not

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The wavelength of sound