From Last Time… Wave Properties - Department of...
Transcript of From Last Time… Wave Properties - Department of...
Fri. Sep 17 Phy107 Lecture 6
From Last Time… Wave Properties
• Amplitude is the maximum displacement ofstring above the equilibrium position
• Wavelength, λ, is the distance between twosuccessive points that behave identically
• Period: required to complete one cycle• Frequency = 1/Period = rate at which cycles
are completed
• Velocity = Wavelength/Period,v = λ / T, or v = λf
Fri. Sep 17 Phy107 Lecture 6
Hour Exam #1 Scores
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15 30 45 60 75 90 105
HOUR EXAM 1 SCORES
# SC
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SCORE ( % )
Mean = 65%Min = 27 %Max = 93%
65% =high BC
Fri. Sep 17 Phy107 Lecture 6
Quality of Sound – Tuning Fork
• Tuning fork producesonly thefundamentalfrequency
Fri. Sep 17 Phy107 Lecture 6
Quality of Sound – Flute
• The same note playedon a flute soundsdifferently
• The second harmonic isvery strong
• The fourth harmonic isclose in strength to thefirst
Fri. Sep 17 Phy107 Lecture 6
Quality of Sound – Clarinet
• The fifth harmonic isvery strong
• The first and fourthharmonics are verysimilar, with the thirdbeing close to them
Fri. Sep 17 Phy107 Lecture 6
Timbre
• In music, the characteristic sound of anyinstrument is referred to as the quality ofsound, or the timbre of the sound
• The quality depends on the mixture ofharmonics in the sound
Fri. Sep 17 Phy107 Lecture 6
Pitch
• Pitch is related mainly, although notcompletely, to the frequency of the sound
• Pitch is not a physical property of the sound• Frequency is the stimulus and pitch is the
response– It is a psychological reaction that allows humans
to place the sound on a scale
Fri. Sep 17 Phy107 Lecture 6
Frequency Response Curves
• Bottom curve is thethreshold of hearing– Threshold of hearing is
strongly dependent onfrequency
– Easiest frequency tohear is about 3000 Hz
• When the sound isloud (top curve,threshold of pain) allfrequencies can beheard equally well
Fri. Sep 17 Phy107 Lecture 6
Combining waves• Two traveling waves can meet and pass through
each other without being destroyed or evenaltered
• Waves obey the Superposition Principle– If two or more traveling waves are moving through a
medium, the resulting wave is found by addingtogether the displacements of the individual wavespoint by point
– Constructive interference: waves reinforce– Destructive interference: waves tend to cancel
Fri. Sep 17 Phy107 Lecture 6
Constructive Interference in a String
• Two pulses are traveling inopposite directions
• The net displacement whenthey overlap is the sum ofthe displacements of thepulses
• Note that the pulses areunchanged after theinterference
Fri. Sep 17 Phy107 Lecture 6
Constructive Interference
• Two waves, a and b, havethe same frequency,amplitude, and start point– Are in phase
• The combined wave, c, hasthe same frequency and agreater amplitude
Combined wave
+
=
Fri. Sep 17 Phy107 Lecture 6
Destructive Interference in aString
• Two pulses are traveling inopposite directions
• The net displacement whenthey overlap thedisplacements of the pulsessubtract
• Note that the pulses areunchanged after theinterference
Fri. Sep 17 Phy107 Lecture 6
Destructive Interference
• Two waves, a and b, havethe same amplitude andfrequency
• They are 1/2 wavelengthout of phase
• When they combine, thewaveforms cancel
+
=
Fri. Sep 17 Phy107 Lecture 6
Interference of sound waves
• Interference arises when waves change their‘phase relationship’.
• Can vary phase relationship of two waves bychanging physical location of speaker.
Constructive Destructive
‘in-phase’ ‘1/2 λ phase diff’
Fri. Sep 17 Phy107 Lecture 6
Example
• Speed of sound ~ 340 m/s• So f=340 Hz gives λ=v/f = 1 meter• Change of 1/2 wavelength is 1/2 meter.
Fri. Sep 17 Phy107 Lecture 6
Spherical Waves
• A spherical wavepropagates radiallyoutward from theoscillating sphere
• The energypropagates equallyin all directions
Fri. Sep 17 Phy107 Lecture 6
Representations of Waves
• Wave fronts are theconcentric arcs– The distance between
successive wave fronts isthe wavelength
• Rays are the radial linespointing out from thesource andperpendicular to thewave fronts
Fri. Sep 17 Phy107 Lecture 6
Shock Waves and Sonic Booms
• A shock waveresults when thesource velocityexceeds the speedof the wave itself
• The circlesrepresent thewave frontsemitted by thesource
Fig 14.11, p. 439
Slide 15
Fri. Sep 17 Phy107 Lecture 6
Sonic Boom
• What happens if the source of soundapproaching the listener is equal toor faster than the speed of sound
• Each successive wave is superimposedon the previous one
– If the speed is exceeded• No sound received till after the source
passes the listener - then a sonic boom- followed by normal sound from thesource
• Conical bow wake• Much like triangular
bow wake behind aduck swimming in apond
Fri. Sep 17 Phy107 Lecture 6
Superposition of Unequal FrequencyWaves
• Consider two harmonic waves A and B meeting atx=0.– Same amplitudes, but ω2 = 1.15 ω1.
• The displacement versus time for each is shownbelow:
What does C(t) = A(t) + B(t) look like??
A(ω1t)
B(ω2t)
Fri. Sep 17 Phy107 Lecture 6
Superposition & Interference• Consider two harmonic waves A and B meeting at x = 0.
– Same amplitudes, but ω2 = 1.15 x ω1.• The displacement versus time for each is shown below:
A(ω1t)
C(t) = A(t) + B(t)CONSTRUCTIVEINTERFERENCE
DESTRUCTIVEINTERFERENCE
B(ω2t)
Fri. Sep 17 Phy107 Lecture 6
Beats
( ) ( )tcostcosA2)tcos(A)tcos(A HL21 ωω=ω+ω
( )ω ω ωL = −12 1 2 ( )21H 2
1ω+ω=ω
The ‘beat’ freqency is exactly half the difference of the twosource freqeuncies.
The ‘pitch’ is the average (half the sum) of the two sourcefrequencies
where and
cos(ωLt)
Fri. Sep 17 Phy107 Lecture 6
Doppler Effect
• A Doppler effect is experienced wheneverthere is relative motion between a source ofwaves and an observer.– When the source and the observer are moving
toward each other, the observer hears a higherfrequency
– When the source and the observer are movingaway from each other, the observer hears alower frequency
• Although the Doppler Effect is commonlyexperienced with sound waves, it is aphenomena common to all waves
Fri. Sep 17 Phy107 Lecture 6
Doppler Effect, Case 1• An observer is moving
toward a stationarysource
• Due to his movement,the observer detectsan additional numberof wave fronts
• The frequency heard isincreased
Fig 14.8, p. 435
Slide 12
Fri. Sep 17 Phy107 Lecture 6
Doppler Effect, Case 2
• An observer ismoving away from astationary source
• The observerdetects fewer wavefronts per second
• The frequencyappears lower
Fig 14.9, p. 436
Slide 13