Chapter 13 Section 1 Sound Waves. Sound Waves What are they? – Longitudinal – Require medium.

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Chapter 13 Section 1 Sound Waves

Transcript of Chapter 13 Section 1 Sound Waves. Sound Waves What are they? – Longitudinal – Require medium.

Page 1: Chapter 13 Section 1 Sound Waves. Sound Waves What are they? – Longitudinal – Require medium.

Chapter 13

Section 1 Sound Waves

Page 2: Chapter 13 Section 1 Sound Waves. Sound Waves What are they? – Longitudinal – Require medium.

Sound Waves

• What are they?

– Longitudinal– Require medium

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Production

• Compression- region of a longitudinal wave in which the density and pressure are greater than normal (crests)

• Rarefaction- region of a longitudinal wave in which the density and pressure are less than normal (troughs)

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Characteristics of Sound Waves

• Frequency- the # of cycles per unit of time– Audible: 20 – 20,000 Hz– Infrasonic: less than 20 Hz– Ultrasonic: more than 20,00) Hz

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Characteristics of Sound Waves

• Frequency determines pitch– Frequency is a quantity of sound that can be

measured– Pitch is how different frequency are perceived by

our ears– Increase in frequency = Increase in pitch

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Click below to watch the Visual Concept.

Visual Concept

Resonance (Frequency)

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Characteristics of Sound Waves

• Ultrasonic can produce images– How?

• Ultrasonic waves are short• A portion of the wave is reflected when density

changes

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Characteristics of Sound

• Frequency is the number of waves per second. • You have heard of ultrasound. What is it?• Frequencies audible to humans are between 20

Hz and 20 000 Hz.– Middle C on a piano is 262 Hz.– The emergency broadcast signal is 1 000 Hz.

• Infrasound frequencies are lower than 20 Hz.• Ultrasound frequencies are greater than 20

000 Hz.

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Characteristics of Sound Waves

• Speed of sound – Depends on the medium– Depends on the temperature

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Speed of Sound

• Sound waves travel though solids, liquids and gases.– In which would the speed generally be greatest?

Why?• Solids. Because the molecules are more closely packed, the

particles respond more rapidly to compressions.

– How might the temperature of air affect the speed of sound waves? Why?

• Higher temperature increases the speed of the waves because the particles are moving faster and colliding more often.

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Speed of Sound

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Characteristics of Sound Waves

• Propagation– Travel in all three dimensions– Wave Fronts- indicate center areas of

compression– Rays- indicate direction of waves, perpendicular to

the wave fronts– Plane waves

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Spherical Waves• Sound propagates in three

dimensions.• The diagram shows:

– Crests or wave fronts (blue circles)– Wavelength ()– Rays (red arrows)

• Rays indicate the direction of propagation.

• How would these wave fronts appear different if they were much farther from the source?

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Spherical Waves

• Wave fronts and rays become more nearly parallel at great distances.

• Plane waves are simply very small segments of a spherical wave a long distance from the source.

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Doppler Effect

• Motion creates a change in frequency– Why?

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Doppler Effect• Why are the waves closer together on the left?

– Waves are closer because the vehicle moves to the left along with the previous wave.

• How will the sound be different for observer A and observer B?– Higher frequency

(pitch) for observer A

• Continued on the next slide….

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Doppler Effect• How would the wave

pattern change if the vehicle moved at a faster speed? How would it sound different?– At a higher speed, waves

would be even closer together and the pitch difference would be even greater.

• The Doppler effect is the observed change in frequency due to the motion of the source or observer.

Page 18: Chapter 13 Section 1 Sound Waves. Sound Waves What are they? – Longitudinal – Require medium.

Click below to watch the Visual Concept.

Visual Concept

Doppler Effect and Sound

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Sound Intensity

• Rate that energy flows through a given area– Intensity = (ΔE/Δt) = P .

area areaIntensity is Power ÷ area watt/m2

Equation for the area of a square = 4πr2

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Sound Intensity

• Vibrating objects do work on the air as they push against the molecules.

• Intensity is the rate of energy flow through an area.– What is “rate of energy flow” called?

• E/t is called power (P).

– Since the waves spread out spherically, you must calculate the area of a sphere. How?

• A = 4r2

– So, what is the equation for intensity?

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Sound Intensity

• SI unit: W/m2

• This is an inverse square relationship.– Doubling r reduces intensity by ¼.– What happens if r is halved?

• Intensity increases by a factor of 4.

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Intensity and Decibels• An intensity scale based on human perception of

loudness is often used.• The base unit of this scale is the bel. More

commonly, the decibel (dB) is used.– 0.1 bel = 1 dB,1 bel = 10 dB, 5 bels = 50 dB, etc.– The lowest intensity humans hear is assigned a value

of zero.

• The scale is logarithmic, so each increase of 1 bel is 10 times louder.– An increase in intensity of 3 bels is 1 000 times louder.

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Page 24: Chapter 13 Section 1 Sound Waves. Sound Waves What are they? – Longitudinal – Require medium.
Page 25: Chapter 13 Section 1 Sound Waves. Sound Waves What are they? – Longitudinal – Require medium.

Click below to watch the Visual Concept.

Visual Concept

Human Hearing

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Threshold of HearingSource Intensity

Intensity Level

# of Times Greater Than TOH

Threshold of Hearing (TOH) 1*10-12 W/m2 0 dB 100

Rustling Leaves 1*10-11 W/m2 10 dB 101

Whisper 1*10-10 W/m2 20 dB 102

Normal Conversation 1*10-6 W/m2 60 dB 106

Busy Street Traffic 1*10-5 W/m2 70 dB 107

Vacuum Cleaner 1*10-4 W/m2 80 dB 108

Large Orchestra 6.3*10-3 W/m2 98 dB 109.8

Walkman at Maximum Level 1*10-2 W/m2 100 dB 1010

Front Rows of Rock Concert 1*10-1 W/m2 110 dB 1011

Threshold of Pain 1*101 W/m2 130 dB 1013

Military Jet Takeoff 1*102 W/m2 140 dB 1014

Instant Perforation of Eardrum 1*104 W/m2 160 dB 1016

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Intensity

• Measured in decibels– Relative intensity– Dimensionless because it is a comparison unit

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Audible Sounds

• The softest sound humans can hear is called the threshold of hearing.– Intensity = 1 10-12 W/m2 or zero dB

• The loudest sound humans can tolerate is called the threshold of pain.– Intensity = 1.0 W/m2 or 120 dB

• Human hearing depends on both the frequency and the intensity.

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Vibration & Resonance

• Forced vibrations: The tendency of one object to force another adjoining or interconnected object into vibrational motion

• Sympathetic vibrations: a vibration produced in one body by the vibrations of exactly the same period in a neighboring body

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Forced Vibrations

• Sympathetic vibrations occur when a vibrating object forces another to vibrate as well.– A piano string vibrates the sound board.– A guitar string vibrates the bridge.

• This makes the sound louder and the vibrations die out faster.– Energy is transferred from the string to the sound

board or bridge.

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Vibration & Resonance

• Natural frequency: The frequency or frequencies at which an object tends to vibrate with when hit, struck, plucked, strummed or somehow disturbed

• Resonance:when one object vibrating at the same natural frequency of a second object forces that second object into vibrational motion.

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Resonance• The red rubber band links the 4

pendulums.• If a blue pendulum is set in motion,

only the other blue pendulum will have large-amplitude vibrations.– The others will just move a small

amount.

• Since the vibrating frequencies of the blue pendulums match, they are resonant.

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Resonance

• Large amplitude vibrations produced when the frequency of the applied force matches the natural frequency of receiver– One blue pendulum was the driving force and the

other was the receiver.

• Bridges have collapsed as a result of structural resonance.– Tacoma Narrows in the wind– A freeway overpass during an earthquake

Page 34: Chapter 13 Section 1 Sound Waves. Sound Waves What are they? – Longitudinal – Require medium.

Click below to watch the Visual Concept.

Visual Concept

Resonance (Frequency)

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Human Ear

• Transmits vibrations that cause nerve impulses

Pathway = Outer ear (ear canal)Eardrum3 bones (hammer, anvil, stirrup)CochleaBasilar membranes