SlideShare una empresa de Scribd logo
1 de 71
Chapter 17 The Principle of Linear Superposition and Interference Phenomena
AP Learning Objectives ,[object Object],[object Object],[object Object],[object Object],[object Object],[object Object],[object Object],[object Object]
Table of Contents ,[object Object],[object Object],[object Object],[object Object],[object Object],[object Object],[object Object]
Chapter 17:   The Principle of Linear Superposition and Interference Phenomena Section 1: The Principle of Linear Superposition
Superposition When the pulses merge, the Slinky assumes a shape that is the sum of the shapes of the individual pulses.
Superposition When the pulses merge, the Slinky assumes a shape that is the sum of the shapes of the individual pulses.
Principle of Superposition ,[object Object],[object Object]
17.1.1. The graph shows two waves at time  t  = 0 s, one moving toward the right at 2.0 cm/s and the other moving toward the left at 2.0 cm/s.  What will the amplitude be at  x  = 0 at time  t  = 0.5 s? a)  +1 cm b)  zero cm c)   1 cm d)   2 cm e)   3 cm
17.1.2. Two waves are traveling along a string.  The graph shows the position of the waves at time  t  = 0.0 s.  One wave with a maximum amplitude of 0.5 cm is traveling toward the right at 0.5 cm/s.  The second wave with a maximum amplitude of 2.0 cm is traveling toward the left at 2.0 cm/s.  At what elapsed time will the two waves completely overlap and what will the maximum amplitude be at that time? a)  2.0 s, 1.5 cm b)  1.3 s, 2.5 cm c)  1.0 s, 1.5 cm d)  1.0 s, 2.5 cm e)  1.3 s, 0.0 cm
Chapter 17:   The Principle of Linear Superposition and Interference Phenomena Section 2: Constructive and Destructive Interference of Sound Waves
Types of Interference ,[object Object],[object Object]
Constructive Interference When two waves always meet condensation-to-condensation and  rarefaction-to-rarefaction, they are said to be  exactly in phase   and  to exhibit  constructive interference.
Constructive Interference Animation courtesy of Dr. Dan Russell, Kettering University
Destructive Interference When two waves always meet condensation-to-rarefaction, they are  said to be  exactly out of phase   and to exhibit  destructive interference.
Sample Problem
Solution
Noise Cancelling Headphones
Coherent Waves If the wave patters do not shift relative to one another as time passes, the sources are said to be  coherent . For two wave sources vibrating in phase, a difference in path lengths that is zero or an integer number (1, 2, 3, . . ) of wavelengths leads to constructive  interference; a difference in path lengths that is a half-integer number (½ , 1 ½, 2 ½, . .) of wavelengths leads to destructive interference.
Example 1  What Does a Listener Hear? Two in-phase loudspeakers, A and B, are  separated by 3.20 m.  A listener is stationed at C, which is 2.40 m in front of speaker B. Both speakers are playing identical 214-Hz  tones, and the speed of sound is 343 m/s. Does the listener hear a loud sound, or no sound? Calculate the path length difference. Calculate the wavelength. Because the path length difference is equal to an integer (1)  number of wavelengths, there is constructive interference, which means there is a loud sound.
Conceptual Example 2  Out-Of-Phase Speakers To make a speaker operate, two wires must be connected between the  speaker and the amplifier.  To ensure that the diaphragms of  the two speakers vibrate in phase, it is  necessary to make these connections in exactly the same way.  If the wires for one speaker are not connected just as they are  for the other, the diaphragms will vibrate out of phase.  Suppose in the connections are  made so that the speaker diaphragms vibrate out of phase, everything else remaining the  same.  In each case, what kind of interference would result in the overlap point?
17.2.1. A radio station has a transmitting tower that transmits its signal (electromagnetic waves) uniformly in all directions on the west end of Main Street.  They are considering building a second, identical transmitter at the east end of Main Street, ten miles due east of the first transmitter.  The same signal is to be broadcast at the same time from both towers.  As you drive ten miles east to west on Main Street, what would you hear as you listen to the radio station broadcast from these two towers? a)  The signal gets stronger as you drive the first five miles, but then the signal decreases as you travel the final five miles. b)  The signal is somewhat stronger than when there was just one tower and there is no variation in signal strength as you drive the ten miles. c)  The signal alternates between increasing strength and decreasing strength as you drive the ten miles. d)  The signal is the same as it was with just one tower.  For the first five miles, you receive the signal from the east tower.  For the second five miles, you receive the signal from the west tower. e)  To answer this question, one must know the amplitude of the broadcast signal.
17.2.2. A tuning fork, like the one shown in the drawing, is tapped and begins to vibrate.  When you place it next to you ear as shown, you can hear a distinctive tone.  The dashed lines in the picture indicate possible axes of rotation.  Consider each if the five axes shown.  About which of these axes can you rotate the tuning fork without producing constructive or destructive interference at the ear as it is rotated? a)  A only b)  B only c)  C only d)  D only e)  D and E only
17.2.3. Two identical speakers are emitting a constant tone that has a wavelength of 0.50 m.  Speaker A is located to the left of speaker B.  At which of the following locations would complete destructive interference occur? a)  2.15 m from speaker A and 3.00 m from speaker B b)  3.75 m from speaker A and 2.50 m from speaker B c)  2.50 m from speaker A and 1.00 m from speaker B d)  1.35 m from speaker A and 3.75 m from speaker B e)  2.00 m from speaker A and 3.00 m from speaker B
Chapter 17:   The Principle of Linear Superposition and Interference Phenomena Section 3: Diffraction
Diffraction ,[object Object],[object Object]
Double/Multi- Slit Diffraction ,[object Object],[object Object],Picture  courtesy of Dr. John U Free, Eastern Nazarene College
Diffraction Patterns ,[object Object],[object Object],[object Object],[object Object],[object Object],[object Object],m=0 m=1 m=2 m=1 m=2 d
Double Slit Approximation ,[object Object],[object Object],d L x
17.3.1. A speaker is located inside a box and emits a constant tone.  There is a partition in the box that has a circular opening with the diameter shown.  There is only one opening in the box to the outside.  That opening is also circular with the diameter shown.  A man is slowly walking alongside the box in the direction shown.  What does the person hear, if anything, as he passes the outer circular opening?  Notes: Not all of the waves are shown and the walls do not absorb any sound. a)  As the man walks along side the box,  he hears the constant tone emitted by the  speaker and its intensity increases as he  is passing the circular opening. b)  As the man walks along side the box,  he only hears the constant tone emitted  by the speaker when he is front of the  circular opening. c)  At no time does the man hear any  sound from the speaker. d)  As the man walks along side the box, he hears the tone intensity alternating between its maximum and minimum values.
17.3.2. Consider the situation shown below.  You are walking north on a street approaching a small marching band that is traveling west to east.  The large, shaded rectangles in the drawing represent tall buildings.  At the moment shown, which instrument(s) do you hear first? a)  flute (f) b)  snare drum (sd) c)  bass drum (bd) d)  flute (f) and  snare drum (sd)
Chapter 17:   The Principle of Linear Superposition and Interference Phenomena Section 4: Beats
Beats ,[object Object],[object Object],[object Object],Animation courtesy of Dr. Dan Russell, Kettering University
Beat Frequency The  beat frequency  is the  difference  between the two sound frequencies.
17.4.1. Two waves, A and B, are superposed.  For which one of the following circumstances will beats result? a)  A and B are identical waves traveling in the same direction. b)  A and B are traveling with differing speeds. c)  A and B are identical waves traveling in the opposite directions. d)  A and B are waves with slightly differing frequencies, but otherwise identical. e)  A and B are waves with slightly differing amplitudes, but otherwise identical.
17.4.2. Which of the graphs shown represent the superposition of two different waves with the smallest difference in frequency between the two waves? a)  A b)  B c)  both A and B, since  the frequency difference  is the same in the two cases d)  This cannot be answered  since no frequency information is available.
17.4.3. Consider the following graphs, each showing the result waves from addition of two differing waves.  For which graph is the frequency difference between the two original waves the smallest? a)  1 b)  2 c)  3 d)  The frequency difference is the same for graphs 1 and 3 and is the smallest.
Chapter 17:   The Principle of Linear Superposition and Interference Phenomena Section 5: Transverse Standing Waves
Standing Wave ,[object Object],[object Object],[object Object],Animation courtesy of Dr. Dan Russell, Kettering University
[object Object],[object Object],[object Object],Standing waves
Standing Wave Patterns
Fixed End Standing Waves ,[object Object],[object Object],[object Object],[object Object],[object Object],[object Object],[object Object],[object Object]
Harmonics String fixed at both ends
Standing Waves
Conceptual Example 5  The Frets on a Guitar Frets allow a the player to produce a complete sequence of musical notes on a single string.  Starting with the fret at the top of the neck, each successive fret shows where the player should press to get the next note in the sequence. Musicians call the sequence the chromatic scale, and every thirteenth note  in it corresponds to one octave, or a doubling of the sound frequency.  The  spacing between the frets is greatest at the top of the neck and decreases with each additional fret further on down.  Why does the spacing decrease going  down the neck?
17.5.1. A transverse standing waves is present on a plucked guitar string.  What is the distance from the fixed end of a string to the nearest antinode? a)  λ /4 b)  λ /2 c)  2 λ /3 d)  3 λ /4 e)  λ
17.5.2. Which one of the following statements is true concerning the points on a string that sustain a standing wave? a)  All points undergo motion that is purely longitudinal. b)  All points vibrate with the same energy. c)  All points vibrate with different amplitudes. d)  All points undergo the same displacements. e)  All points vibrate with different frequencies.
17.5.3. A rope of length  L  is clamped at both ends.  Which one of the following is not a possible wavelength for standing waves on this rope? a)  L /2 b)  2 L /3 c)  L d)  2 L e)  4 L
17.5.4. Consider a wire under tension that is driven by an oscillator.  Initially, the wire is vibrating in its second harmonic mode.  How does the oscillation of the wire change as the frequency is slowly increased? a)  No standing wave may be observed until the frequency matches the third harmonic mode of the wire. b)  No standing wave may be observed until the frequency matches the first harmonic mode of the wire. c)  The observed oscillation of the wire not change until the frequency matches the third harmonic mode of the wire. d)  The observed oscillation of the wire will slowly change in fractions of the harmonic between the second and third harmonic modes. e)  The observed oscillation of the wire will slowly change in fractions of the harmonic between the second and first harmonic modes.
17.5.5. Which one of the following statements explains why a piano and a guitar playing the same musical note sound different? a)  The fundamental frequency is different for each instrument. b)  The two instruments have the same fundamental frequency, but different harmonic frequencies. c)  The two instruments have the same harmonic frequencies, but different fundamental frequencies. d)  The two instruments have the same fundamental frequency and the same harmonic frequencies, but the amounts of each of the harmonics is different for the two instruments..
17.5.6. The sound emitted from a strummed guitar string is either a resonant frequency or one of its harmonics.  Although the string is not being driven at its resonant frequency, no non-resonant waves are emitted.  Which one of the following statements best describes why non-resonant waves are not heard? a)  Non-resonant waves are not sound waves. b)  The non-resonant waves are too quickly damped out. c)  The musician has tuned the strings so that only resonant waves will occur. d)  Any non-resonant waves will destructively interfere with each other.
Chapter 17:   The Principle of Linear Superposition and Interference Phenomena Section 6: Longitudinal Standing Waves
Longitudinal Standing Waves A longitudinal standing wave pattern on a slinky.
[object Object],[object Object],[object Object],[object Object],[object Object],[object Object],[object Object],[object Object],Open-ended Standing Waves
Open-ended Standing Waves  Tube open at both ends
Example 6  Playing a Flute When all the holes are closed on one type of flute, the lowest note it can sound is middle C (261.6 Hz).  If the speed of sound is 343 m/s, and the flute is assumed to be a cylinder open at both ends, determine the distance L.
Mixed Standing Wave ,[object Object],[object Object],[object Object],[object Object],[object Object],[object Object],[object Object],[object Object],[object Object]
Tube open at one end
Sample Problem: ,[object Object],[object Object],[object Object]
Sample Problem ,[object Object],[object Object],[object Object]
Resonance ,[object Object],[object Object],[object Object],[object Object]
Resonance ,[object Object],[object Object],[object Object]
17.6.1. A soft drink bottle is 15 cm tall.  Joey blows across that top of the bottle just after drinking the last of his drink.  What is the approximate fundamental frequency of the tone that Joey generates? a)  230 Hz b)  570 Hz c)  680 Hz d)  810 Hz e)  1100 Hz
17.6.2. An aluminum rod of length  L  may be held at various points along its length, some of which are indicated in the drawing.  A small hammer is then used to tap the rod.  As a result, longitudinal standing waves are generated in the rod.  At which position should the rod be held to generate its second harmonic? a)  A b)  B c)  C d)  D e)  E
17.6.3. Which one of the following statements concerning standing waves within a pipe open only at one end is true? a)  The standing waves have a fundamental mode have a shorter wavelength than that for the same tube with both ends open. b)  The standing waves must be transverse waves, since longitudinal waves could not exit the tube. c)  The standing waves have a greater number of harmonics than which occur for the tube when both ends are open. d)  The standing waves have fewer harmonics than which occur for the tube when both ends are open. e)  The standing waves have a fundamental mode with a smaller frequency than that which occurs when both ends of the tube are open.
17.6.4. Given that the first three resonant frequencies of an organ pipe are 200, 600, and 1000 Hz, what can you conclude about the pipe? a)  The pipe is open at both ends and has a length of 0.95 m. b)  The pipe is closed at one end and has a length of 0.95 m. c)  The pipe is closed at one end and has a length of 0.475 m. d)  The pipe is open at both ends and has a length of 0.475 m. e)  It is not possible to have a pipe with this combination of resonant frequencies.
Chapter 17:   The Principle of Linear Superposition and Interference Phenomena Section 7: Complex Sound Waves
Pure Sounds ,[object Object],[object Object],[object Object],[object Object]
Complex Sounds ,[object Object],[object Object],[object Object]
The Oscilloscope ,[object Object]
The Fourier Transform ,[object Object],[object Object]
END

Más contenido relacionado

La actualidad más candente

La actualidad más candente (20)

Nuclear Chemistry-Augar effect-Internal conversion-Isomerism
Nuclear Chemistry-Augar effect-Internal conversion-IsomerismNuclear Chemistry-Augar effect-Internal conversion-Isomerism
Nuclear Chemistry-Augar effect-Internal conversion-Isomerism
 
Energetika Gelombang
Energetika GelombangEnergetika Gelombang
Energetika Gelombang
 
Interference And Youngs two Slit
Interference And Youngs two SlitInterference And Youngs two Slit
Interference And Youngs two Slit
 
Wave optics
Wave opticsWave optics
Wave optics
 
Classical and Quantum Theory of light.pdf
Classical and Quantum Theory of light.pdfClassical and Quantum Theory of light.pdf
Classical and Quantum Theory of light.pdf
 
Interference original
Interference originalInterference original
Interference original
 
Wave particle duality
Wave particle dualityWave particle duality
Wave particle duality
 
Interference of light
Interference of lightInterference of light
Interference of light
 
Diploma sem 2 applied science physics-unit 5-chap-2 photoelectric effect
Diploma sem 2 applied science physics-unit 5-chap-2 photoelectric effectDiploma sem 2 applied science physics-unit 5-chap-2 photoelectric effect
Diploma sem 2 applied science physics-unit 5-chap-2 photoelectric effect
 
1.3 refraction Fizik SPM - Pembiasan Gelombang
1.3 refraction Fizik SPM - Pembiasan Gelombang1.3 refraction Fizik SPM - Pembiasan Gelombang
1.3 refraction Fizik SPM - Pembiasan Gelombang
 
Interference
InterferenceInterference
Interference
 
Notafizik f5c1
Notafizik f5c1Notafizik f5c1
Notafizik f5c1
 
Chapter 7 interference
Chapter 7 interferenceChapter 7 interference
Chapter 7 interference
 
Ch 15 waves
Ch 15 wavesCh 15 waves
Ch 15 waves
 
Photoelectric Effect
Photoelectric EffectPhotoelectric Effect
Photoelectric Effect
 
Efek Fotolistrik
Efek FotolistrikEfek Fotolistrik
Efek Fotolistrik
 
physics intro
physics introphysics intro
physics intro
 
Wave functions
Wave functionsWave functions
Wave functions
 
Quantum mechanics I
Quantum mechanics IQuantum mechanics I
Quantum mechanics I
 
Wave nature of_light
Wave nature of_lightWave nature of_light
Wave nature of_light
 

Destacado

Ch 1: Introduction and Math Concepts
Ch 1:  Introduction and Math ConceptsCh 1:  Introduction and Math Concepts
Ch 1: Introduction and Math ConceptsScott Thomas
 
Learning object #2 - 2D wave interference
Learning object #2 - 2D wave interference Learning object #2 - 2D wave interference
Learning object #2 - 2D wave interference Emily Gresham
 
Interference of light in arabic
Interference of light in arabicInterference of light in arabic
Interference of light in arabicQahtannRose
 
Huygens Principle
Huygens PrincipleHuygens Principle
Huygens Principlekleybf
 
Huygens’ principle
Huygens’ principleHuygens’ principle
Huygens’ principlessyoung
 
Ch 21 Magnetic Fields and Forces
Ch 21 Magnetic Fields and ForcesCh 21 Magnetic Fields and Forces
Ch 21 Magnetic Fields and ForcesScott Thomas
 
Huygens' Principle
Huygens' PrincipleHuygens' Principle
Huygens' PrincipleCeleste Ng
 
Diffraction & Double Slit Experiment
Diffraction & Double Slit Experiment Diffraction & Double Slit Experiment
Diffraction & Double Slit Experiment dwsutherland
 
Pharmaceuticals: Bioequivalence & Clinical trials
Pharmaceuticals: Bioequivalence & Clinical trialsPharmaceuticals: Bioequivalence & Clinical trials
Pharmaceuticals: Bioequivalence & Clinical trialsFederico Karagulian
 
Pharmacokinetics of drugs administered by intravenous route
Pharmacokinetics of drugs administered by intravenous routePharmacokinetics of drugs administered by intravenous route
Pharmacokinetics of drugs administered by intravenous routeProf. Dr. Basavaraj Nanjwade
 
Chapter 11 Vocab 9th Grade--Waves and Their Parts
Chapter 11 Vocab 9th Grade--Waves and Their PartsChapter 11 Vocab 9th Grade--Waves and Their Parts
Chapter 11 Vocab 9th Grade--Waves and Their PartsLindsey
 
Bioavailability of drgs that follow nonlinear pharmacokinetics
Bioavailability of drgs that follow nonlinear pharmacokineticsBioavailability of drgs that follow nonlinear pharmacokinetics
Bioavailability of drgs that follow nonlinear pharmacokineticsMalla Reddy College of Pharmacy
 
3.3 electron configuration
3.3 electron configuration3.3 electron configuration
3.3 electron configurationZB Chemistry
 
Chapter 11 fluids vic
Chapter 11 fluids vicChapter 11 fluids vic
Chapter 11 fluids vicguest4f7c558
 
Physics 101 LO4 - Power and Intensity
Physics 101 LO4 - Power and IntensityPhysics 101 LO4 - Power and Intensity
Physics 101 LO4 - Power and IntensityLeslie Liu
 
Physical and chemical changes ppt
Physical and chemical changes pptPhysical and chemical changes ppt
Physical and chemical changes pptabecel22
 
Periodic table-shells-valence
Periodic table-shells-valencePeriodic table-shells-valence
Periodic table-shells-valenceabecel22
 

Destacado (20)

Ch 1: Introduction and Math Concepts
Ch 1:  Introduction and Math ConceptsCh 1:  Introduction and Math Concepts
Ch 1: Introduction and Math Concepts
 
Learning object #2 - 2D wave interference
Learning object #2 - 2D wave interference Learning object #2 - 2D wave interference
Learning object #2 - 2D wave interference
 
Interference of light in arabic
Interference of light in arabicInterference of light in arabic
Interference of light in arabic
 
Marx
Marx Marx
Marx
 
Topic 1 shm
Topic 1 shmTopic 1 shm
Topic 1 shm
 
Huygens Principle
Huygens PrincipleHuygens Principle
Huygens Principle
 
Huygens’ principle
Huygens’ principleHuygens’ principle
Huygens’ principle
 
Ch 21 Magnetic Fields and Forces
Ch 21 Magnetic Fields and ForcesCh 21 Magnetic Fields and Forces
Ch 21 Magnetic Fields and Forces
 
Huygens' Principle
Huygens' PrincipleHuygens' Principle
Huygens' Principle
 
Diffraction & Double Slit Experiment
Diffraction & Double Slit Experiment Diffraction & Double Slit Experiment
Diffraction & Double Slit Experiment
 
Pharmaceuticals: Bioequivalence & Clinical trials
Pharmaceuticals: Bioequivalence & Clinical trialsPharmaceuticals: Bioequivalence & Clinical trials
Pharmaceuticals: Bioequivalence & Clinical trials
 
Pharmacokinetics of drugs administered by intravenous route
Pharmacokinetics of drugs administered by intravenous routePharmacokinetics of drugs administered by intravenous route
Pharmacokinetics of drugs administered by intravenous route
 
Chapter 11 Vocab 9th Grade--Waves and Their Parts
Chapter 11 Vocab 9th Grade--Waves and Their PartsChapter 11 Vocab 9th Grade--Waves and Their Parts
Chapter 11 Vocab 9th Grade--Waves and Their Parts
 
Bioavailability of drgs that follow nonlinear pharmacokinetics
Bioavailability of drgs that follow nonlinear pharmacokineticsBioavailability of drgs that follow nonlinear pharmacokinetics
Bioavailability of drgs that follow nonlinear pharmacokinetics
 
3.3 electron configuration
3.3 electron configuration3.3 electron configuration
3.3 electron configuration
 
Chapter 11 fluids vic
Chapter 11 fluids vicChapter 11 fluids vic
Chapter 11 fluids vic
 
Physics 101 LO4 - Power and Intensity
Physics 101 LO4 - Power and IntensityPhysics 101 LO4 - Power and Intensity
Physics 101 LO4 - Power and Intensity
 
Physical and chemical changes ppt
Physical and chemical changes pptPhysical and chemical changes ppt
Physical and chemical changes ppt
 
Notes - Radiation Electromagnetic
Notes - Radiation ElectromagneticNotes - Radiation Electromagnetic
Notes - Radiation Electromagnetic
 
Periodic table-shells-valence
Periodic table-shells-valencePeriodic table-shells-valence
Periodic table-shells-valence
 

Similar a Ch 17 Linear Superposition and Interference

Physics by Younes Sina
Physics by Younes SinaPhysics by Younes Sina
Physics by Younes SinaYounes Sina
 
Programmed learning material
Programmed learning materialProgrammed learning material
Programmed learning material14162083
 
Programmed learning material
Programmed learning materialProgrammed learning material
Programmed learning material9924066834
 
7 superposition and standing waves
7 superposition and standing waves7 superposition and standing waves
7 superposition and standing wavesMissingWaldo
 
1.5 Interference of Waves
1.5 Interference of Waves1.5 Interference of Waves
1.5 Interference of Wavescgharyati
 
PHYSICS MAHARASHTRA STATE BOARD CHAPTER 6 - SUPERPOSITION OF WAVES EXERCISE S...
PHYSICS MAHARASHTRA STATE BOARD CHAPTER 6 - SUPERPOSITION OF WAVES EXERCISE S...PHYSICS MAHARASHTRA STATE BOARD CHAPTER 6 - SUPERPOSITION OF WAVES EXERCISE S...
PHYSICS MAHARASHTRA STATE BOARD CHAPTER 6 - SUPERPOSITION OF WAVES EXERCISE S...Pooja M
 
Standing waves (music)
Standing waves (music)Standing waves (music)
Standing waves (music)Anonymous0805
 
1.5 interference - Interferens Fizik SPM
1.5 interference - Interferens Fizik SPM1.5 interference - Interferens Fizik SPM
1.5 interference - Interferens Fizik SPMCikgu Fizik
 
chapter sound for class 9 ppt
chapter sound for class 9 ppt chapter sound for class 9 ppt
chapter sound for class 9 ppt Arpit Meena
 

Similar a Ch 17 Linear Superposition and Interference (20)

Physics by Younes Sina
Physics by Younes SinaPhysics by Younes Sina
Physics by Younes Sina
 
Programmed learning material
Programmed learning materialProgrammed learning material
Programmed learning material
 
Programmed learning material
Programmed learning materialProgrammed learning material
Programmed learning material
 
7 superposition and standing waves
7 superposition and standing waves7 superposition and standing waves
7 superposition and standing waves
 
Waves
WavesWaves
Waves
 
P6 lesson part one
P6 lesson part oneP6 lesson part one
P6 lesson part one
 
Waves 2
Waves  2Waves  2
Waves 2
 
1.5 Interference of Waves
1.5 Interference of Waves1.5 Interference of Waves
1.5 Interference of Waves
 
PHYSICS MAHARASHTRA STATE BOARD CHAPTER 6 - SUPERPOSITION OF WAVES EXERCISE S...
PHYSICS MAHARASHTRA STATE BOARD CHAPTER 6 - SUPERPOSITION OF WAVES EXERCISE S...PHYSICS MAHARASHTRA STATE BOARD CHAPTER 6 - SUPERPOSITION OF WAVES EXERCISE S...
PHYSICS MAHARASHTRA STATE BOARD CHAPTER 6 - SUPERPOSITION OF WAVES EXERCISE S...
 
Standing waves (music)
Standing waves (music)Standing waves (music)
Standing waves (music)
 
Introduction to Audiography/Sound
Introduction to Audiography/SoundIntroduction to Audiography/Sound
Introduction to Audiography/Sound
 
Lo7
Lo7Lo7
Lo7
 
Wave motion
Wave motionWave motion
Wave motion
 
1.5 interference - Interferens Fizik SPM
1.5 interference - Interferens Fizik SPM1.5 interference - Interferens Fizik SPM
1.5 interference - Interferens Fizik SPM
 
Arpit meena
Arpit meenaArpit meena
Arpit meena
 
chapter sound for class 9 ppt
chapter sound for class 9 ppt chapter sound for class 9 ppt
chapter sound for class 9 ppt
 
CLASS 9 _ SOUND.pptx
CLASS 9 _ SOUND.pptxCLASS 9 _ SOUND.pptx
CLASS 9 _ SOUND.pptx
 
Physics 17-2
Physics 17-2Physics 17-2
Physics 17-2
 
i AM YEDA
i AM YEDAi AM YEDA
i AM YEDA
 
Wave properties
Wave propertiesWave properties
Wave properties
 

Más de Scott Thomas

Final Review Worksheet
Final Review WorksheetFinal Review Worksheet
Final Review WorksheetScott Thomas
 
Ch 32 Radiation, Nuclear Energy, and Particles
Ch 32 Radiation, Nuclear Energy, and ParticlesCh 32 Radiation, Nuclear Energy, and Particles
Ch 32 Radiation, Nuclear Energy, and ParticlesScott Thomas
 
Ch 31 Nuclear Physics and Radioactivity
Ch 31 Nuclear Physics and RadioactivityCh 31 Nuclear Physics and Radioactivity
Ch 31 Nuclear Physics and RadioactivityScott Thomas
 
Ch 30 Nature of theAtom
Ch 30 Nature of theAtomCh 30 Nature of theAtom
Ch 30 Nature of theAtomScott Thomas
 
Ch 28 Special Relativity
Ch 28 Special RelativityCh 28 Special Relativity
Ch 28 Special RelativityScott Thomas
 
Ch 25 Light Reflection: Mirrors
Ch 25 Light Reflection: MirrorsCh 25 Light Reflection: Mirrors
Ch 25 Light Reflection: MirrorsScott Thomas
 
Ch 24 Electromagnetic Waves
Ch 24 Electromagnetic WavesCh 24 Electromagnetic Waves
Ch 24 Electromagnetic WavesScott Thomas
 
Ch 2 One Dimensional Kinematics
Ch 2 One Dimensional KinematicsCh 2 One Dimensional Kinematics
Ch 2 One Dimensional KinematicsScott Thomas
 
Ch 22 Electromagnetic Induction
Ch 22 Electromagnetic InductionCh 22 Electromagnetic Induction
Ch 22 Electromagnetic InductionScott Thomas
 
Ch 20 Electric Circuits
Ch 20 Electric CircuitsCh 20 Electric Circuits
Ch 20 Electric CircuitsScott Thomas
 
Ch19 Electric Potential Energy and Electric Potential
Ch19 Electric Potential Energy and Electric PotentialCh19 Electric Potential Energy and Electric Potential
Ch19 Electric Potential Energy and Electric PotentialScott Thomas
 
Ch 18 Electric Fields
Ch 18 Electric FieldsCh 18 Electric Fields
Ch 18 Electric FieldsScott Thomas
 
Ch 15 Thermodynamics
Ch 15 ThermodynamicsCh 15 Thermodynamics
Ch 15 ThermodynamicsScott Thomas
 
Ch 14 Ideal Gas Law & Kinetic Theory
Ch 14 Ideal Gas Law & Kinetic TheoryCh 14 Ideal Gas Law & Kinetic Theory
Ch 14 Ideal Gas Law & Kinetic TheoryScott Thomas
 
Ch 13 Transfer of Heat
Ch 13 Transfer of Heat Ch 13 Transfer of Heat
Ch 13 Transfer of Heat Scott Thomas
 
Ch 12 Temperature and Heat
Ch 12 Temperature and Heat Ch 12 Temperature and Heat
Ch 12 Temperature and Heat Scott Thomas
 
Ch 3 Two Dimensional Kinematics
Ch 3 Two Dimensional KinematicsCh 3 Two Dimensional Kinematics
Ch 3 Two Dimensional KinematicsScott Thomas
 
Ch 9 Rotational Dynamics
Ch 9 Rotational DynamicsCh 9 Rotational Dynamics
Ch 9 Rotational DynamicsScott Thomas
 
Ch 8 Rotational Kinematics
Ch 8 Rotational KinematicsCh 8 Rotational Kinematics
Ch 8 Rotational KinematicsScott Thomas
 

Más de Scott Thomas (20)

Final Review Worksheet
Final Review WorksheetFinal Review Worksheet
Final Review Worksheet
 
Ch 32 Radiation, Nuclear Energy, and Particles
Ch 32 Radiation, Nuclear Energy, and ParticlesCh 32 Radiation, Nuclear Energy, and Particles
Ch 32 Radiation, Nuclear Energy, and Particles
 
Ch 31 Nuclear Physics and Radioactivity
Ch 31 Nuclear Physics and RadioactivityCh 31 Nuclear Physics and Radioactivity
Ch 31 Nuclear Physics and Radioactivity
 
Ch 30 Nature of theAtom
Ch 30 Nature of theAtomCh 30 Nature of theAtom
Ch 30 Nature of theAtom
 
Ch 28 Special Relativity
Ch 28 Special RelativityCh 28 Special Relativity
Ch 28 Special Relativity
 
Ch 25 Light Reflection: Mirrors
Ch 25 Light Reflection: MirrorsCh 25 Light Reflection: Mirrors
Ch 25 Light Reflection: Mirrors
 
Ch 24 Electromagnetic Waves
Ch 24 Electromagnetic WavesCh 24 Electromagnetic Waves
Ch 24 Electromagnetic Waves
 
Ch 2 One Dimensional Kinematics
Ch 2 One Dimensional KinematicsCh 2 One Dimensional Kinematics
Ch 2 One Dimensional Kinematics
 
Ch 22 Electromagnetic Induction
Ch 22 Electromagnetic InductionCh 22 Electromagnetic Induction
Ch 22 Electromagnetic Induction
 
Ch 20 Electric Circuits
Ch 20 Electric CircuitsCh 20 Electric Circuits
Ch 20 Electric Circuits
 
Ch19 Electric Potential Energy and Electric Potential
Ch19 Electric Potential Energy and Electric PotentialCh19 Electric Potential Energy and Electric Potential
Ch19 Electric Potential Energy and Electric Potential
 
Ch 18 Electric Fields
Ch 18 Electric FieldsCh 18 Electric Fields
Ch 18 Electric Fields
 
Ch 15 Thermodynamics
Ch 15 ThermodynamicsCh 15 Thermodynamics
Ch 15 Thermodynamics
 
Ch 14 Ideal Gas Law & Kinetic Theory
Ch 14 Ideal Gas Law & Kinetic TheoryCh 14 Ideal Gas Law & Kinetic Theory
Ch 14 Ideal Gas Law & Kinetic Theory
 
Ch 13 Transfer of Heat
Ch 13 Transfer of Heat Ch 13 Transfer of Heat
Ch 13 Transfer of Heat
 
Ch 12 Temperature and Heat
Ch 12 Temperature and Heat Ch 12 Temperature and Heat
Ch 12 Temperature and Heat
 
Ch 3 Two Dimensional Kinematics
Ch 3 Two Dimensional KinematicsCh 3 Two Dimensional Kinematics
Ch 3 Two Dimensional Kinematics
 
First Day Info
First Day InfoFirst Day Info
First Day Info
 
Ch 9 Rotational Dynamics
Ch 9 Rotational DynamicsCh 9 Rotational Dynamics
Ch 9 Rotational Dynamics
 
Ch 8 Rotational Kinematics
Ch 8 Rotational KinematicsCh 8 Rotational Kinematics
Ch 8 Rotational Kinematics
 

Ch 17 Linear Superposition and Interference

  • 1. Chapter 17 The Principle of Linear Superposition and Interference Phenomena
  • 2.
  • 3.
  • 4. Chapter 17: The Principle of Linear Superposition and Interference Phenomena Section 1: The Principle of Linear Superposition
  • 5. Superposition When the pulses merge, the Slinky assumes a shape that is the sum of the shapes of the individual pulses.
  • 6. Superposition When the pulses merge, the Slinky assumes a shape that is the sum of the shapes of the individual pulses.
  • 7.
  • 8. 17.1.1. The graph shows two waves at time t = 0 s, one moving toward the right at 2.0 cm/s and the other moving toward the left at 2.0 cm/s. What will the amplitude be at x = 0 at time t = 0.5 s? a) +1 cm b) zero cm c)  1 cm d)  2 cm e)  3 cm
  • 9. 17.1.2. Two waves are traveling along a string. The graph shows the position of the waves at time t = 0.0 s. One wave with a maximum amplitude of 0.5 cm is traveling toward the right at 0.5 cm/s. The second wave with a maximum amplitude of 2.0 cm is traveling toward the left at 2.0 cm/s. At what elapsed time will the two waves completely overlap and what will the maximum amplitude be at that time? a) 2.0 s, 1.5 cm b) 1.3 s, 2.5 cm c) 1.0 s, 1.5 cm d) 1.0 s, 2.5 cm e) 1.3 s, 0.0 cm
  • 10. Chapter 17: The Principle of Linear Superposition and Interference Phenomena Section 2: Constructive and Destructive Interference of Sound Waves
  • 11.
  • 12. Constructive Interference When two waves always meet condensation-to-condensation and rarefaction-to-rarefaction, they are said to be exactly in phase and to exhibit constructive interference.
  • 13. Constructive Interference Animation courtesy of Dr. Dan Russell, Kettering University
  • 14. Destructive Interference When two waves always meet condensation-to-rarefaction, they are said to be exactly out of phase and to exhibit destructive interference.
  • 18. Coherent Waves If the wave patters do not shift relative to one another as time passes, the sources are said to be coherent . For two wave sources vibrating in phase, a difference in path lengths that is zero or an integer number (1, 2, 3, . . ) of wavelengths leads to constructive interference; a difference in path lengths that is a half-integer number (½ , 1 ½, 2 ½, . .) of wavelengths leads to destructive interference.
  • 19. Example 1 What Does a Listener Hear? Two in-phase loudspeakers, A and B, are separated by 3.20 m. A listener is stationed at C, which is 2.40 m in front of speaker B. Both speakers are playing identical 214-Hz tones, and the speed of sound is 343 m/s. Does the listener hear a loud sound, or no sound? Calculate the path length difference. Calculate the wavelength. Because the path length difference is equal to an integer (1) number of wavelengths, there is constructive interference, which means there is a loud sound.
  • 20. Conceptual Example 2 Out-Of-Phase Speakers To make a speaker operate, two wires must be connected between the speaker and the amplifier. To ensure that the diaphragms of the two speakers vibrate in phase, it is necessary to make these connections in exactly the same way. If the wires for one speaker are not connected just as they are for the other, the diaphragms will vibrate out of phase. Suppose in the connections are made so that the speaker diaphragms vibrate out of phase, everything else remaining the same. In each case, what kind of interference would result in the overlap point?
  • 21. 17.2.1. A radio station has a transmitting tower that transmits its signal (electromagnetic waves) uniformly in all directions on the west end of Main Street. They are considering building a second, identical transmitter at the east end of Main Street, ten miles due east of the first transmitter. The same signal is to be broadcast at the same time from both towers. As you drive ten miles east to west on Main Street, what would you hear as you listen to the radio station broadcast from these two towers? a) The signal gets stronger as you drive the first five miles, but then the signal decreases as you travel the final five miles. b) The signal is somewhat stronger than when there was just one tower and there is no variation in signal strength as you drive the ten miles. c) The signal alternates between increasing strength and decreasing strength as you drive the ten miles. d) The signal is the same as it was with just one tower. For the first five miles, you receive the signal from the east tower. For the second five miles, you receive the signal from the west tower. e) To answer this question, one must know the amplitude of the broadcast signal.
  • 22. 17.2.2. A tuning fork, like the one shown in the drawing, is tapped and begins to vibrate. When you place it next to you ear as shown, you can hear a distinctive tone. The dashed lines in the picture indicate possible axes of rotation. Consider each if the five axes shown. About which of these axes can you rotate the tuning fork without producing constructive or destructive interference at the ear as it is rotated? a) A only b) B only c) C only d) D only e) D and E only
  • 23. 17.2.3. Two identical speakers are emitting a constant tone that has a wavelength of 0.50 m. Speaker A is located to the left of speaker B. At which of the following locations would complete destructive interference occur? a) 2.15 m from speaker A and 3.00 m from speaker B b) 3.75 m from speaker A and 2.50 m from speaker B c) 2.50 m from speaker A and 1.00 m from speaker B d) 1.35 m from speaker A and 3.75 m from speaker B e) 2.00 m from speaker A and 3.00 m from speaker B
  • 24. Chapter 17: The Principle of Linear Superposition and Interference Phenomena Section 3: Diffraction
  • 25.
  • 26.
  • 27.
  • 28.
  • 29. 17.3.1. A speaker is located inside a box and emits a constant tone. There is a partition in the box that has a circular opening with the diameter shown. There is only one opening in the box to the outside. That opening is also circular with the diameter shown. A man is slowly walking alongside the box in the direction shown. What does the person hear, if anything, as he passes the outer circular opening? Notes: Not all of the waves are shown and the walls do not absorb any sound. a) As the man walks along side the box, he hears the constant tone emitted by the speaker and its intensity increases as he is passing the circular opening. b) As the man walks along side the box, he only hears the constant tone emitted by the speaker when he is front of the circular opening. c) At no time does the man hear any sound from the speaker. d) As the man walks along side the box, he hears the tone intensity alternating between its maximum and minimum values.
  • 30. 17.3.2. Consider the situation shown below. You are walking north on a street approaching a small marching band that is traveling west to east. The large, shaded rectangles in the drawing represent tall buildings. At the moment shown, which instrument(s) do you hear first? a) flute (f) b) snare drum (sd) c) bass drum (bd) d) flute (f) and snare drum (sd)
  • 31. Chapter 17: The Principle of Linear Superposition and Interference Phenomena Section 4: Beats
  • 32.
  • 33. Beat Frequency The beat frequency is the difference between the two sound frequencies.
  • 34. 17.4.1. Two waves, A and B, are superposed. For which one of the following circumstances will beats result? a) A and B are identical waves traveling in the same direction. b) A and B are traveling with differing speeds. c) A and B are identical waves traveling in the opposite directions. d) A and B are waves with slightly differing frequencies, but otherwise identical. e) A and B are waves with slightly differing amplitudes, but otherwise identical.
  • 35. 17.4.2. Which of the graphs shown represent the superposition of two different waves with the smallest difference in frequency between the two waves? a) A b) B c) both A and B, since the frequency difference is the same in the two cases d) This cannot be answered since no frequency information is available.
  • 36. 17.4.3. Consider the following graphs, each showing the result waves from addition of two differing waves. For which graph is the frequency difference between the two original waves the smallest? a) 1 b) 2 c) 3 d) The frequency difference is the same for graphs 1 and 3 and is the smallest.
  • 37. Chapter 17: The Principle of Linear Superposition and Interference Phenomena Section 5: Transverse Standing Waves
  • 38.
  • 39.
  • 41.
  • 42. Harmonics String fixed at both ends
  • 44. Conceptual Example 5 The Frets on a Guitar Frets allow a the player to produce a complete sequence of musical notes on a single string. Starting with the fret at the top of the neck, each successive fret shows where the player should press to get the next note in the sequence. Musicians call the sequence the chromatic scale, and every thirteenth note in it corresponds to one octave, or a doubling of the sound frequency. The spacing between the frets is greatest at the top of the neck and decreases with each additional fret further on down. Why does the spacing decrease going down the neck?
  • 45. 17.5.1. A transverse standing waves is present on a plucked guitar string. What is the distance from the fixed end of a string to the nearest antinode? a) λ /4 b) λ /2 c) 2 λ /3 d) 3 λ /4 e) λ
  • 46. 17.5.2. Which one of the following statements is true concerning the points on a string that sustain a standing wave? a) All points undergo motion that is purely longitudinal. b) All points vibrate with the same energy. c) All points vibrate with different amplitudes. d) All points undergo the same displacements. e) All points vibrate with different frequencies.
  • 47. 17.5.3. A rope of length L is clamped at both ends. Which one of the following is not a possible wavelength for standing waves on this rope? a) L /2 b) 2 L /3 c) L d) 2 L e) 4 L
  • 48. 17.5.4. Consider a wire under tension that is driven by an oscillator. Initially, the wire is vibrating in its second harmonic mode. How does the oscillation of the wire change as the frequency is slowly increased? a) No standing wave may be observed until the frequency matches the third harmonic mode of the wire. b) No standing wave may be observed until the frequency matches the first harmonic mode of the wire. c) The observed oscillation of the wire not change until the frequency matches the third harmonic mode of the wire. d) The observed oscillation of the wire will slowly change in fractions of the harmonic between the second and third harmonic modes. e) The observed oscillation of the wire will slowly change in fractions of the harmonic between the second and first harmonic modes.
  • 49. 17.5.5. Which one of the following statements explains why a piano and a guitar playing the same musical note sound different? a) The fundamental frequency is different for each instrument. b) The two instruments have the same fundamental frequency, but different harmonic frequencies. c) The two instruments have the same harmonic frequencies, but different fundamental frequencies. d) The two instruments have the same fundamental frequency and the same harmonic frequencies, but the amounts of each of the harmonics is different for the two instruments..
  • 50. 17.5.6. The sound emitted from a strummed guitar string is either a resonant frequency or one of its harmonics. Although the string is not being driven at its resonant frequency, no non-resonant waves are emitted. Which one of the following statements best describes why non-resonant waves are not heard? a) Non-resonant waves are not sound waves. b) The non-resonant waves are too quickly damped out. c) The musician has tuned the strings so that only resonant waves will occur. d) Any non-resonant waves will destructively interfere with each other.
  • 51. Chapter 17: The Principle of Linear Superposition and Interference Phenomena Section 6: Longitudinal Standing Waves
  • 52. Longitudinal Standing Waves A longitudinal standing wave pattern on a slinky.
  • 53.
  • 54. Open-ended Standing Waves Tube open at both ends
  • 55. Example 6 Playing a Flute When all the holes are closed on one type of flute, the lowest note it can sound is middle C (261.6 Hz). If the speed of sound is 343 m/s, and the flute is assumed to be a cylinder open at both ends, determine the distance L.
  • 56.
  • 57. Tube open at one end
  • 58.
  • 59.
  • 60.
  • 61.
  • 62. 17.6.1. A soft drink bottle is 15 cm tall. Joey blows across that top of the bottle just after drinking the last of his drink. What is the approximate fundamental frequency of the tone that Joey generates? a) 230 Hz b) 570 Hz c) 680 Hz d) 810 Hz e) 1100 Hz
  • 63. 17.6.2. An aluminum rod of length L may be held at various points along its length, some of which are indicated in the drawing. A small hammer is then used to tap the rod. As a result, longitudinal standing waves are generated in the rod. At which position should the rod be held to generate its second harmonic? a) A b) B c) C d) D e) E
  • 64. 17.6.3. Which one of the following statements concerning standing waves within a pipe open only at one end is true? a) The standing waves have a fundamental mode have a shorter wavelength than that for the same tube with both ends open. b) The standing waves must be transverse waves, since longitudinal waves could not exit the tube. c) The standing waves have a greater number of harmonics than which occur for the tube when both ends are open. d) The standing waves have fewer harmonics than which occur for the tube when both ends are open. e) The standing waves have a fundamental mode with a smaller frequency than that which occurs when both ends of the tube are open.
  • 65. 17.6.4. Given that the first three resonant frequencies of an organ pipe are 200, 600, and 1000 Hz, what can you conclude about the pipe? a) The pipe is open at both ends and has a length of 0.95 m. b) The pipe is closed at one end and has a length of 0.95 m. c) The pipe is closed at one end and has a length of 0.475 m. d) The pipe is open at both ends and has a length of 0.475 m. e) It is not possible to have a pipe with this combination of resonant frequencies.
  • 66. Chapter 17: The Principle of Linear Superposition and Interference Phenomena Section 7: Complex Sound Waves
  • 67.
  • 68.
  • 69.
  • 70.
  • 71. END