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Waves and Sound. Chapter 11. Ways to Transport. - PowerPoint PPT Presentation
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Chapter 11
Two ways to transport energy and momentum◦ Streaming particles◦ Flowing waves
Image right: Recent Cassini images of Saturn's moon Enceladus backlit by the sun show the fountain-like sources of the fine spray of material that towers over the south polar region. Image credit: NASA/JPL/Space Science Institute+ Full image and caption+ Movie: Enceladus plumes+ Browse version of image
Two ways to study◦ Psychological (mind) and physiological (body)
What we hear◦ Physical
What sound is – compression wave
Moving self-sustained disturbance of a medium
Medium◦ Field ◦ Substance
Mechanical wave – in material media
Atoms◦ Push together – repel◦ Pull apart – attract◦ Objects are made of atoms
When atoms are distorted they act like attached by springs
Displacement causes a wave
Self-sustaining disturbance Examples
◦ String◦ Liquid waves◦ Sound waves◦ Compression waves
The main difference between particle stream and wave is:◦ Medium stays in place as the wave progresses
Longitudinal ◦ Sustaining medium is displaced parallel to the
direction of propagation◦ Ex – Sound waves
Transverse◦ When the sustaining medium is displaced
perpendicular to the direction of propagation◦ Ex – Guitar string
Torsion◦ Variation of transverse waves
Water waves◦ Combination of Longitudinal and Transverse waves
Longitudinal – move back and forth
Transverse – moveup and down
Water – move in circle
One cycle of a wave Profile – outline or shape of the wavepulse
◦ Determined by the driver of the wave Speed – Determined by the medium Examples
◦ Gunshot◦ Grunt◦ Tsunami
Disturbance of waves with a beginning and end
Amplitude varies Carrier wavelength – Steady sinusoidal
oscillation
Ideal disturbance composed of endless repeats of the same profile wave
Period – how long it takes one profile to pass a point in space
Frequency – number of profile waves passing per second
Wavelength – λ (lambda) - distance in space over which the wavetrain executes one cycle
Amplitude – Height of the waves
v = fλ◦ V – velocity (m/s)◦ f – frequency (cycles/sec or Hz)◦ λ – wavelength (m)
Waves pass the length of a 4.5 m boat. It takes 1.5 seconds for the wave to go from end to end. If the waves are 0.5 seconds apart, what is the period, frequency and wavelength?
T = 0.5 seconds f = 1/T = 1/0.5 = 2.0 Hz v = L/t = 4.5 m/1.5 sec = 3.0 m/s λ = v/f = 3.0 m/s / 2.0 Hz = 1.5 m
Speed of the waves is determined by the properties of the medium, not in any way the motion of the source
Velocity of wave in string◦v = √FT/m/L◦v - velocity (m/s)◦FT = Tension (N)◦m /L – mass/unit length
What is the speed of a wave pulse in a 20 cm, 40 g guitar string with the tension of 19.6 N?◦ v = √FT/m/L◦ v - ?◦ FT = 19.6 N◦ m /L – .040 kg / 0.20 m = 0.020 kg/m
◦v = √FT/m/L = √19.6 N / 0.020 kg/m = 31 m/s
Reflected – carries all the original energy
Absorbed – Friction stops wave
Transmission – moving from one media to another◦ Velocity may change when
moving between medias
Solids – longitudinal elastic wave◦ Ex – Earth quake
Fluids – acoustic waves◦ Ex – sound waves
Parts◦ Rarefaction – distance between atoms is elongated◦ Compression – distance between atoms is squeezed◦ Direction of movement – in the direction of
oscillation Each atom is in SHM
Can be determined by the restoring force and its density◦ Use
Bulk Modulus Bernoulli’s equation Young’s Modulus
Dolphins use chirps to locate items underwater◦ Size of wave – 1.4 cm◦ Can “see” fish and other small items◦ Above our hearing range - 10⁵ Hz
Autofocus cameras Bats Medicine
◦ Tumor and Kidney stone destruction◦ Probe body
Joints Baby
Wave lengths below our hearing range (less than 20 Hz)
Examples◦ Elephants◦ Submarines◦ Subwoofers in Rock Bands
Vibrate our internal organs
http://www.pbs.org/wnet/nature/animalspredict/video2.html
Human hearing range – 20 Hz to 20 khz◦ Usually can not hear through entire range◦ Diminishes with age (above 20 years) and loud
noises
First considered in Rome◦ Marco Vitruvius Pollio – designed amphitheaters◦ Though sound travel through air like water waves
Sound needs a media to travel through◦ No sound in a vacuum◦ No sound in explosions in space
Speaker vibrates Creates pressure variations
◦ Quiet – less than 0.002 Pa◦ Loud – about 10 Pa
Loudness – depends on how far the air molecules move
Period and Frequency – depends on time for speaker to move through a cycle
Wavelength – distancebetween rarefactions
What is the wavelength of a tuning note (A440) which is 440 Hz. The speed of sound at room temperature is 343.9 m/s?
λ = v/f = 343.9 m/s / 440 Hz = 0.782 m
Waves can move through the same area of space and have a combined effect
Are not changed or scattered Superposition Principle -When two waves
overlap, the resultant is the algebraic sum of various contributions at each point
Jean Baptiste Joseph, Baron de Fourier
Proved that a periodic wave having a wavelength can be synthesized by a sum of harmonic waves
A wave profile is a result of overlapping sines and cosines
Waves move out in a circle or sphere In-phase at different distances As the wave moves out it becomes diffused
Power – Joules/sec – Watts P = Work/sec
Joules – Newton-meters Work = Force x Distance Measuring –
◦ Depends on area the detector ◦ Depends on the amount of time
The average power divided by the perpendicular area across which it is transported
I = Pav/A (Watt/meter²)
Area of spherical wave = 4ΠR²◦ The farther from the source, the greater the area,
therefore the less the intensity
An underwater explosion is detected 100 m away, where the intensity is 1.00 GW/m². About 1 second later the sound wave is recorded 1.5 km away from the explosion. What will its intensity be?
R1 = 100 m R2 = 1.5 kmI1 = 1.00 GW/m² Δt = 1 sec Power in first square = power in second square I1 4ΠR² = I2 4ΠR² I2 = (1 x 10⁹ W/m²) (100 m)² / (1500 m)² = 4.4 x 10⁶ W/m²
In 1636, Father Mersen used echoes to measure speed of sound
Speed of sound increases with temperature of air
Air temperatures aren’t constant◦ Velocity varies depending on the gas
Speed of sound does not depend on frequency ◦ All waves get there simultaneously
During a thunder storm, you hear thunder 3.50 seconds after you see a bolt of lightening. How far away, in meters and miles, did the lightening strike?
Three parts of ear◦ Outer – From outer ear to ear drum
Sound resonates in canal Amplifies waves from 3 kHz to 4 kHz
◦ Middle – links eardrum to 3 bones to oval window Increases sound pressure
◦ Inner – Transducer that converts pressure to electrical impulses Hairs in the cochlear vibrate at different frequencies
and amplitude
Human response to frequency Pure tone – sine wave Higher the frequency, the
higher the pitch◦ Varies in people◦ Increasing intensity makes you
think you also increased pitch Human voices
◦ Men 80 Hz – 240 Hz (700 Hz in song)
◦ Woman 140 Hz – 500 Hz (1100 Hz in song)
Waveform blend of:◦ Harmonic – fundamental tone (f)◦ Overtones – tones that are over the harmonic
May or may not be harmonics (2f, 3f, etc) Combination of harmonic and overtones makes the timbre
Intensity-level ◦ Number of factors of 10 that is its intensity is
above the threshold of sound◦ measured in bel (In honor of Alexander Graham
Bell)◦ Io(hearing) = 1.0 x 10 ¹² W/m²
Decibel (dB) – 1/10th of a bel◦ Unitless◦ β = 10 log10 I / Io
Condenses the range from 1.0 to a million millionth to 0dB to 120 dB
Log A/B = log A – log B
Log AB = log A + log B
β = 10 log I / Io
Δβ = 10 log I1 / I2 This means that if you have a 12-W system and
want to make it 2X louder, you have to increase the power to 120-W
Noise – Unrelated jumble of disturbances◦ Non-periodic◦ Continuous frequency
White noise – broad bandwidth of sounds out equal intensities◦ Ex – wind, pouring water, radio static
We can distinguish between wavepulses up to about 20 beats per second – then it becomes a hum
Interference caused in sound waves of different frequency
Used to tune guitars and pianos Carrier wave = f1 + f2 / 2 Beat frequency = f1 - f2
◦ f1 = higher f
Waves reflected back and forth in a finite medium
Very common◦ All instruments◦ Our speaking and singing voice◦ Ringing bells◦ Lasers
Nodes – when the resultant is zero Antinodes – midway between nodes Wavelength – twice the node-to-nodes
distance
First harmonic◦ Fundamental
2nd harmonic◦ 1st overtone
3rd harmonic◦ 2nd overtone
4th harmonic◦ 3rd overtone
5th harmonic◦ 4th overtone
Resonance in the system Amplifies the input Guitar
◦ Each string has a different tension and linear mass-density
◦ Fingering – Changes the length of the string – increases the fundamental frequency
L = ½ Nλ (N - whole number of nodes) fN = N/2L FT/m/L
Falsetto voice – increase tension to increase frequency
What must the tension on a 300 mm fiddle string be to be tuned to 660 Hz? The mass-length is 0.38 g/m.
FT = (m/L)(2Lf)² ==0.38 g/m (2 x 0.300 m x 660
Hz)² =72 N (about 16 lbs)
Strings are not loud◦ Sounding board
(piano)◦ Sounding box
(guitar and violin)◦ Pick-ups in
electric guitars
Made in air-filled chambers (wind pipe, trumpets, organ pipes)
Made by – vibrating reeds (saxophone), lips on mouth pieces(trumpet) , fluttering jet of air (flute)
Only frequencies that fit the standing wave mode will be sustained and amplified
◦ Open on both ends◦ Closed on both ends◦ Open on one end and closed on the other
Types of columns
◦ L = ¼ Nλ◦ fN = Nv/4L (v = speed of sound)
◦ L = ½ Nλ◦ fN = Nv/2L (v = speed of sound)
Blowing slow – fundamental Blowing fast – harmonics
Frequency of pitch changes from high to low
Eeeeeoooooo Think of bug in water swimming forward
fo = fsv + vo v + vs◦ The amount of frequency shift depends on who
is moving ◦ Uses – radar guns, weather tracking devices,
satellites, blood flow Doppler effect when bounced off an
approaching target and returned◦ fo = (v + vt) fs/ v - vt
◦ Red-shift of light – galaxies are moving away from us
◦ Based on recession rates and apparent size of universe – the Big Bang happened 15 thousand million years ago