The Physics of Sounds
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Transcript of The Physics of Sounds
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Content:
W hat is Sound?Properties of a Sound W ave
Speed of SoundConstructive and Destructive InterferenceDiffractionThe Doppler EffectIntensity
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S ound:y V ibratory disturbances in a gas, liquid, or solid
medium.y sound is the vibration of any substancey our ears gather these vibrations and allow us to
interpret them.
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A s sound waves travelthrough the material,
each molecule hitsanother and returns to its
original position
result is that regions of themedium become alternately more dense , when they are
called condensations,
less dense, when they are called
rarefactions.
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y Sound waves are often depicted in graphs like the onebelow, where the x-axis is time and the y-axis is pressure or the density of the medium through whichthe sound is travelling.
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Wav elength
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Period:
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Amp litude:A decibel is a
scientific unit thatmeasures the
intensity of sounds.
The softest sound
that a human canhear is the zeropoint. W hen thesound is twice asloud, the decibel
level goes up by six.
Humans speaknormally at 60
decibels.
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Speed of soundy sound waves travel the slowest through gases,y faster through liquids, andy fastest through solids.y Temperature also affects the speed of sound.
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G as e sy In a gas, it is particularly important to know the
temperature.y
This is because at lower temperatures, moleculescollide more often, giving the sound wave morechances to move around rapidly.
y A t freezing (0 Celcius), sound travels through air at
331 meters per second (about 740 mph). But, at 20C,room temperature, sound travels at 343 meters persecond (767 mph).
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S olid sy Sound travels fastest through solids.y This is because molecules in a solid medium are much
closer together, allowing sound waves to travel morequickly through ity sound waves travel over 17 times faster through steel
than through air.y The exact speed of sound in steel is 5,960 meters per
second (13,332 mph)!y But, this is only for the majority of solids. The speed of
sound in all solids are not faster than in all liquids.
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Con s tructi v e a nd De s tructi v eInterference of Sound Wav e s :
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B e a t s These periodic variations in loudness
are called b eats .
In this situation you will hear the loudness
rise and fall 2 timesper second because
440-438=2.So, there is a beatfrequency of 2 Hz.
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Diffra ction: A n obstacle is no matchfor a sound wave; the wave simply bendsaround it
This bending of a waveis called diffraction
The sound outside of the room has varyingintensity depending on where you stand
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y If we let angle x be the location of the first minimum
intensity point on either side of the center,y W be the wavelength, andy D be the width of the doorway, the equation
. For a c ir c ular opening , the equation is slightly different
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The Intensity of Three-Dimensional W aves:These circles
are called w avefronts
The space inbetween wavefronts is the w avelength
Rays indicate themotion of a set of
wavefronts.The intensity level of sound ismeasured in deci b els (dB).
threshold of hearing is
0 dB
threshold of pain is120 dB
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Threshold of pain
Threshold of hearing
Threshold of hearing formajority people
A uditory area
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Typical speech sounds
Typical music sounds
A uditory area of thehuman ear
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T he Do pp ler Effect: y change in pitch
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End