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PHY2053 Lecture 27 Ch. 12.1 - 12.5: Sound Waves, Amplitude, Intensity

PHY2053 Lecture 27 - University of Florida...PHY2053, Lecture 4, Motion in a Plane Amplitude and intensity of sound • human register sound 13 orders of magnitude in intensity between

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Page 1: PHY2053 Lecture 27 - University of Florida...PHY2053, Lecture 4, Motion in a Plane Amplitude and intensity of sound • human register sound 13 orders of magnitude in intensity between

PHY2053 Lecture 27 Ch. 12.1 - 12.5: Sound Waves, Amplitude, Intensity

Page 2: PHY2053 Lecture 27 - University of Florida...PHY2053, Lecture 4, Motion in a Plane Amplitude and intensity of sound • human register sound 13 orders of magnitude in intensity between

PHY2053, Lecture 4, Motion in a Plane

Sound

• periodic variation of pressure - pressure waves• propagate through any material - gas, fluid or solid• compressions - areas of higher pressure• rarefactions - areas of lower pressure• sound source - object which oscillates within audible

range of frequencies• movement translates into pressure waves• pressure waves detected by eardrums (vibration)• audible range: 20 Hz to 20 kHz• infrasound - below 20 Hz, ultrasound - above 20 kHz

2

Page 3: PHY2053 Lecture 27 - University of Florida...PHY2053, Lecture 4, Motion in a Plane Amplitude and intensity of sound • human register sound 13 orders of magnitude in intensity between

PHY2053, Lecture 4, Motion in a Plane

Speed of sound waves• last lecture - dimensions of resonating system

determine wavelength, v = f × λ• transverse wave on a string:

• F - measure of restoring force• μ - measure of inertia of the system

• analogy for fluids:

3

Bulk Modulus

Density

Page 4: PHY2053 Lecture 27 - University of Florida...PHY2053, Lecture 4, Motion in a Plane Amplitude and intensity of sound • human register sound 13 orders of magnitude in intensity between

PHY2053, Lecture 4, Motion in a Plane

Speed of sound in gas and solids• for a gas, the bulk modulus is either the pressure (p)

(isothermal) or γp (adiabatic)

• temperature dependence:

• speed of sound along the length of a thin solid rod:

4

Young’s Modulus

Density

Page 5: PHY2053 Lecture 27 - University of Florida...PHY2053, Lecture 4, Motion in a Plane Amplitude and intensity of sound • human register sound 13 orders of magnitude in intensity between

PHY2053, Lecture 4, Motion in a Plane

Example problem:Dolphins emit ultrasonic waves with a frequency as high as 2.5 ×105 Hz. What is the wavelength of such a wave in seawater at 25 ºC? [the speed of sound in water at 0 ºC is 1493 m/s]

5

Page 6: PHY2053 Lecture 27 - University of Florida...PHY2053, Lecture 4, Motion in a Plane Amplitude and intensity of sound • human register sound 13 orders of magnitude in intensity between

PHY2053, Lecture 4, Motion in a Plane

Example problem:Dolphins emit ultrasonic waves with a frequency as high as 2.5 ×105 Hz. What is the wavelength of such a wave in seawater at 25 ºC? [the speed of sound in water at 0 ºC is 1493 m/s]

5

Page 7: PHY2053 Lecture 27 - University of Florida...PHY2053, Lecture 4, Motion in a Plane Amplitude and intensity of sound • human register sound 13 orders of magnitude in intensity between

PHY2053, Lecture 4, Motion in a Plane

Example problem:Dolphins emit ultrasonic waves with a frequency as high as 2.5 ×105 Hz. What is the wavelength of such a wave in seawater at 25 ºC? [the speed of sound in water at 0 ºC is 1493 m/s]

5

Page 8: PHY2053 Lecture 27 - University of Florida...PHY2053, Lecture 4, Motion in a Plane Amplitude and intensity of sound • human register sound 13 orders of magnitude in intensity between

p0 = !v⇢s0

I =p202⇢v

I ⇠ amplitude2

PHY2053, Lecture 4, Motion in a Plane

Amplitude and intensity of sound

6

Pressure amplitude Osc. object amplitude

mass density of mediumspeed of sound in medium

sound frequency

Page 9: PHY2053 Lecture 27 - University of Florida...PHY2053, Lecture 4, Motion in a Plane Amplitude and intensity of sound • human register sound 13 orders of magnitude in intensity between

PHY2053, Lecture 4, Motion in a Plane

Amplitude and intensity of sound• human register sound 13 orders of magnitude in

intensity between lowest intensity and pain threshold• if lowest intensity is 1, pain is 10 000 000 000 000• lowest sound intensity I0 = 10-12 W/m2

• ear registers intensity in orders of magnitude• intensity increase from 1 to 10 appears equivalent to

intensity increase from 10 to 100• a logarithmic scale is most appropriate, measure

sound intensity in decibels:

7

Page 10: PHY2053 Lecture 27 - University of Florida...PHY2053, Lecture 4, Motion in a Plane Amplitude and intensity of sound • human register sound 13 orders of magnitude in intensity between

PHY2053, Lecture 4, Motion in a Plane

Example problemThe amplitude of oscillation of a loud speaker is increased by 50%.a) By what percentage does the intensity increase?b) What is the change in intensity level (in dB)?

8

Page 11: PHY2053 Lecture 27 - University of Florida...PHY2053, Lecture 4, Motion in a Plane Amplitude and intensity of sound • human register sound 13 orders of magnitude in intensity between

PHY2053, Lecture 4, Motion in a Plane

Example problemThe amplitude of oscillation of a loud speaker is increased by 50%.a) By what percentage does the intensity increase?b) What is the change in intensity level (in dB)?

8

Page 12: PHY2053 Lecture 27 - University of Florida...PHY2053, Lecture 4, Motion in a Plane Amplitude and intensity of sound • human register sound 13 orders of magnitude in intensity between

PHY2053, Lecture 4, Motion in a Plane

Solution, continued

9

Page 13: PHY2053 Lecture 27 - University of Florida...PHY2053, Lecture 4, Motion in a Plane Amplitude and intensity of sound • human register sound 13 orders of magnitude in intensity between

PHY2053, Lecture 26, Interference and Diffraction

Standing Sound Waves• reminder from last time:• what happens when a standing wave gets “trapped”

between two boundaries? • superposition of incoming and reflected wave, while

taking into account boundary conditions• for example two fixed ends:

10

Page 14: PHY2053 Lecture 27 - University of Florida...PHY2053, Lecture 4, Motion in a Plane Amplitude and intensity of sound • human register sound 13 orders of magnitude in intensity between

PHY2053, Lecture 26, Interference and Diffraction

Unusual (but possible) Configuration

• one fixed end, one free end:

11

Page 15: PHY2053 Lecture 27 - University of Florida...PHY2053, Lecture 4, Motion in a Plane Amplitude and intensity of sound • human register sound 13 orders of magnitude in intensity between

PHY2053, Lecture 26, Interference and Diffraction

Example Problem• How long of a pipe is needed to have the lowest

resonant frequency of 440 Hz [pitch standard] ? Assume the pipe is open at both ends.

12

Page 16: PHY2053 Lecture 27 - University of Florida...PHY2053, Lecture 4, Motion in a Plane Amplitude and intensity of sound • human register sound 13 orders of magnitude in intensity between

PHY2053, Lecture 26, Interference and Diffraction

Example Problem• How long of a pipe is needed to have the lowest

resonant frequency of 440 Hz [pitch standard] ? Assume the pipe is open at both ends.

12

Page 17: PHY2053 Lecture 27 - University of Florida...PHY2053, Lecture 4, Motion in a Plane Amplitude and intensity of sound • human register sound 13 orders of magnitude in intensity between

PHY2053, Lecture 26, Interference and Diffraction

Example Problem• How long of a pipe is needed to have the lowest

resonant frequency of 440 Hz [pitch standard] ? Assume the pipe is open at both ends.

12

Page 18: PHY2053 Lecture 27 - University of Florida...PHY2053, Lecture 4, Motion in a Plane Amplitude and intensity of sound • human register sound 13 orders of magnitude in intensity between

PHY2053, Lecture 26, Interference and Diffraction

Example Problem• How long of a pipe is needed to have the lowest

resonant frequency of 440 Hz [pitch standard] ? Assume the pipe is open at both ends.

12

Page 19: PHY2053 Lecture 27 - University of Florida...PHY2053, Lecture 4, Motion in a Plane Amplitude and intensity of sound • human register sound 13 orders of magnitude in intensity between

PHY2053, Lecture 26, Interference and Diffraction

Example Problem• How long of a pipe is needed to have the lowest

resonant frequency of 440 Hz [pitch standard] ? Assume the pipe is open at both ends.

12

Page 20: PHY2053 Lecture 27 - University of Florida...PHY2053, Lecture 4, Motion in a Plane Amplitude and intensity of sound • human register sound 13 orders of magnitude in intensity between

PHY2053, Lecture 26, Interference and Diffraction

H-ITT from last lecture

13

Page 21: PHY2053 Lecture 27 - University of Florida...PHY2053, Lecture 4, Motion in a Plane Amplitude and intensity of sound • human register sound 13 orders of magnitude in intensity between

PHY2053, Lecture 4, Motion in a Plane

Timbre• no instrument produces only one harmonic• sounds produced are a superposition of harmonics• timbre / tone quality / tone color - spectrum of

harmonics specific to a particular instrument

14

Page 22: PHY2053 Lecture 27 - University of Florida...PHY2053, Lecture 4, Motion in a Plane Amplitude and intensity of sound • human register sound 13 orders of magnitude in intensity between

PHY2053, Lecture 4, Motion in a Plane

Timbre, continued

15

Page 23: PHY2053 Lecture 27 - University of Florida...PHY2053, Lecture 4, Motion in a Plane Amplitude and intensity of sound • human register sound 13 orders of magnitude in intensity between

PHY2053, Lecture 4, Motion in a Plane

Timbre, continued

15

Page 24: PHY2053 Lecture 27 - University of Florida...PHY2053, Lecture 4, Motion in a Plane Amplitude and intensity of sound • human register sound 13 orders of magnitude in intensity between

PHY2053, Lecture 4, Motion in a Plane

Timbre, continued

15

Page 25: PHY2053 Lecture 27 - University of Florida...PHY2053, Lecture 4, Motion in a Plane Amplitude and intensity of sound • human register sound 13 orders of magnitude in intensity between

PHY2053, Lecture 4, Motion in a Plane

Timbre, continued

15