Physics 231 Lecture 28

Size: px
Start display at page:

Download "Physics 231 Lecture 28"

Transcription

1 Physics 231 Lecture 28 Main points of today s lecture: Reflection of waes. rigid end inerted wae free end non-inerted wae Standing waes on string: n 2L f n λn n 1, 2, 3,,, 2L n Standing wae in air columns: f n both ends open n 2L λ n 2L n one end open n 4L f n λn n 13,, 5,,, 4L n Resonance n 1,2,3,,,

2 Example Each of three tuning forks A, B, and C has a slightly different frequency. When A and B are sounded together, they produce a beat frequency of 2 Hz. When A and C are sounded together, the produce a beat frequency of 5 Hz. What is the beat frequency that occurs when B and C are sounded together? There are two possible answers. if fa fb fc 100Hz, 98 or 102 Hz 95 or 105 Hz fbeat,b C fb fc 3 or 7

3 reflection of wae at a boundary amplitude at fixed end is zero and reflected wae is inerted. Amplitude at free end is double and reflected wae is same polarity (in this case it is positie.

4 Superposition principle Two traeling pulse waes pass through each other without affec4ng each other. The resul4ng displacement is the superposi4on of the two indiidual waes.

5 Standing waes on a string Two traeling sinusoidal waes of the same frequency moing in opposite directions can superimposed so as to make a standing wae: Because the string is held at each end, those points are nodes of the oscillator motion, where the amplitude of motion anishes. Anti-nodes are the points where fundamental the motion is maximal. 1 st harmonic Motion with one antinode has λ/2 L, two antinodes has λl... The general relationship is: 2L n n F λ n ; f n n 1,2,3,,, n λ 2L 2L µ n higher harmonics n1 fund. E n2 2 nd Har. E n3 3 d Har. B n4 4 th Har. E n5 5 th Har. G #

6 Example A stretched string fixed at each end has a mass of 40.0 g and a length of 8.00 m. The tension in the string is 49.0 N. (a) Determine the positions of the nodes and antinodes for the 2 nd harmonic. (b) What is the ibration frequency for this harmonic? Second harmonic (n 0,4, and 8 m and anti-nodes at 2 and 6 m. f 2 2 2L F m/l 2) has nodes at 49N 0.04kg / 8m 98m / s Fig 14.18, p. 443 Slide 25 ans. f 2 λ 2 L 98m / s 8m 12.4Hz

7 Standing waes in an air columns: both ends open If one end of the air column is closed, a node must exist at this end since the moement of the air is restricted If the end is open, the elements of the air hae complete freedom of moement and an antinode exists n 2L f n λn n 1, 2, 3,,, 2L n

8 Interference: Standing Wae in a open pipe If two waes trael in opposite direc4ons and 12, the superposi4on of the two waes produces a standing wae: maxima and minima always appear at the same loca4on

9 Standing waes in an air columns: one end closed If one end of the air column is closed, a node must exist at this end since the moement of the air is restricted If the end is open, the elements of the air hae complete freedom of moement and an antinode exists n 4L f n λn n 13,, 5,,, 4L n

10 Quiz The fundamental frequencies of two air columns are the same. Column A is open at both ends, while column B is open at only one end. The length of column A is 0.60 m. What is the length of column B? a) 0.1 m b) 0.2 m c) 0.3 m d) 0.5 m e) 0.6 m f A f B fa 2L A fb 4L B fb fa 4L B 2L 4L A B L L /2 B A ans. LB 0.3m 2L A

11 Mach Cone What happens when we exceed the speed of sound with our source elocity? source < sound source > sound

12 Mach Cone µ

13 Mach Cone What happens when we exceed the speed of sound with our source elocity? Mach Cone Mach angle: sound Δt θ M sinθ M soundδt source Δt source Δt θ M sin 1 sound source Physics 231C 74

14 Mach Cone A apor cone is formed as this F/A-18F Super Hornet closes on Mach 1.(Hayman Tam)

15 Forced ibrations and resonance A system with a driing force will force a ibration at its frequency When the frequency of the driing force equals the natural frequency of the system, the system is said to be in resonance

16 Conceptual question A string is clamped at both ends and plucked so it ibrates in a standing mode between two extreme positions a and b. Let upward motion correspond to positie elocities.when the string is in position c, the instantaneous elocity of points along the string: a. is zero eerywhere. b. is positie eerywhere. c. is negatie eerywhere. d. depends on location.

Lecture 18. Sound Waves: Intensity, Interference, Beats and Doppler Effect.

Lecture 18. Sound Waves: Intensity, Interference, Beats and Doppler Effect. Lecture 18 Sound Waes: Intensity, Interference, Beats and Doppler Effect. Speed of sound Speed of soun in air, depends on temperature: = (331 + 0.60 T ) m/s where T in C Sound intensity leel β = 10log

More information

Superposition and Standing Waves

Superposition and Standing Waves Physics 1051 Lecture 9 Superposition and Standing Waves Lecture 09 - Contents 14.5 Standing Waves in Air Columns 14.6 Beats: Interference in Time 14.7 Non-sinusoidal Waves Trivia Questions 1 How many wavelengths

More information

S 1 S 2 A B C. 7/25/2006 Superposition ( F.Robilliard) 1

S 1 S 2 A B C. 7/25/2006 Superposition ( F.Robilliard) 1 P S S S 0 x S A B C 7/5/006 Superposition ( F.Robilliard) Superposition of Waes: As we hae seen preiously, the defining property of a wae is that it can be described by a wae function of the form - y F(x

More information

16 SUPERPOSITION & STANDING WAVES

16 SUPERPOSITION & STANDING WAVES Chapter 6 SUPERPOSITION & STANDING WAVES 6. Superposition of waves Principle of superposition: When two or more waves overlap, the resultant wave is the algebraic sum of the individual waves. Illustration:

More information

Physics 4C Spring 2016 Test 3

Physics 4C Spring 2016 Test 3 Physics 4C Spring 016 Test 3 Name: June 1, 016 Please show your work! Answers are not complete without clear reasoning. When asked for an expression, you must gie your answer in terms of the ariables gien

More information

Exam tomorrow on Chapter 15, 16, and 17 (Oscilla;ons and Waves 1 &2)

Exam tomorrow on Chapter 15, 16, and 17 (Oscilla;ons and Waves 1 &2) Exam tomorrow on Chapter 15, 16, and 17 (Oscilla;ons and Waves 1 &2) What to study: Quiz 6 Homework problems for Chapters 15 & 16 Material indicated in the following review slides Other Specific things:

More information

Chapter 14: Wave Motion Tuesday April 7 th

Chapter 14: Wave Motion Tuesday April 7 th Chapter 14: Wave Motion Tuesday April 7 th Wave superposition Spatial interference Temporal interference (beating) Standing waves and resonance Sources of musical sound Doppler effect Sonic boom Examples,

More information

Physics 11 Chapter 15/16 HW Solutions

Physics 11 Chapter 15/16 HW Solutions Physics Chapter 5/6 HW Solutions Chapter 5 Conceptual Question: 5, 7 Problems:,,, 45, 50 Chapter 6 Conceptual Question:, 6 Problems:, 7,, 0, 59 Q5.5. Reason: Equation 5., string T / s, gies the wae speed

More information

Chapter 16 Waves. Types of waves Mechanical waves. Electromagnetic waves. Matter waves

Chapter 16 Waves. Types of waves Mechanical waves. Electromagnetic waves. Matter waves Chapter 16 Waves Types of waves Mechanical waves exist only within a material medium. e.g. water waves, sound waves, etc. Electromagnetic waves require no material medium to exist. e.g. light, radio, microwaves,

More information

Wave Motion Wave and Wave motion Wave is a carrier of energy Wave is a form of disturbance which travels through a material medium due to the repeated periodic motion of the particles of the medium about

More information

10. Yes. Any function of (x - vt) will represent wave motion because it will satisfy the wave equation, Eq

10. Yes. Any function of (x - vt) will represent wave motion because it will satisfy the wave equation, Eq CHAPER 5: Wae Motion Responses to Questions 5. he speed of sound in air obeys the equation B. If the bulk modulus is approximately constant and the density of air decreases with temperature, then the speed

More information

Physics 11 Chapters 15: Traveling Waves and Sound and 16: Superposition and Standing Waves

Physics 11 Chapters 15: Traveling Waves and Sound and 16: Superposition and Standing Waves Physics 11 Chapters 15: Traeling Waes and Sound and 16: Superposition and Standing Waes We are what we beliee we are. Benjamin Cardozo We would accomplish many more things if we did not think of them as

More information

Old Exams - Questions Ch-16

Old Exams - Questions Ch-16 Old Exams - Questions Ch-16 T081 : Q1. The displacement of a string carrying a traveling sinusoidal wave is given by: y( x, t) = y sin( kx ω t + ϕ). At time t = 0 the point at x = 0 m has a displacement

More information

Oscillation the vibration of an object. Wave a transfer of energy without a transfer of matter

Oscillation the vibration of an object. Wave a transfer of energy without a transfer of matter Oscillation the vibration of an object Wave a transfer of energy without a transfer of matter Equilibrium Position position of object at rest (mean position) Displacement (x) distance in a particular direction

More information

Physics 231 Lecture 28

Physics 231 Lecture 28 Physics 31 Lecture 8 Cocepts or today s lecture Spherical waes P I 4πr Dopper shit + o ƒ' ƒ s Itererece o soud waes L L λ costructi e ( 0,1,) L 1 1 L ( + 1/ ) λ destructi e Stadig waes o strig: L λ L 1,,3,,,

More information

Physics 231 Lecture 27

Physics 231 Lecture 27 Physics 31 Lecture 7 Concepts for today s lecture Wae speed for a string / μ : tension; μ m /L. Sound intensity I β 10log 10 I 0 IP/A, I 0 μ 1x10-1 W/m Spherical waes Here P is the string tension I and

More information

Prashant Patil ( ) PRASHANT PATIL PHYSICS CLASSES NEET/JEE(Main) Date : 19/07/2017 TEST ID: 11 Time : 00:45:00 PHYSICS

Prashant Patil ( ) PRASHANT PATIL PHYSICS CLASSES NEET/JEE(Main) Date : 19/07/2017 TEST ID: 11 Time : 00:45:00 PHYSICS Prashant Patil (99709774) PRASHANT PATIL PHYSICS CLASSES NEET/JEE(Main) Date : 9/07/07 TEST ID: Time : 00:45:00 PHYSICS Marks : 80 5. STATIONARY WAVES Single Correct Answer Type. Stationary waes are set

More information

Longitudinal Waves. Reading: Chapter 17, Sections 17-7 to Sources of Musical Sound. Pipe. Closed end: node Open end: antinode

Longitudinal Waves. Reading: Chapter 17, Sections 17-7 to Sources of Musical Sound. Pipe. Closed end: node Open end: antinode Longitudinal Waes Reading: Chapter 7, Sections 7-7 to 7-0 Sources o Musical Sound Pipe Closed end: node Open end: antinode Standing wae pattern: Fundamental or irst harmonic: nodes at the ends, antinode

More information

Sound Waves. Sound waves are longitudinal waves traveling through a medium Sound waves are produced from vibrating objects.

Sound Waves. Sound waves are longitudinal waves traveling through a medium Sound waves are produced from vibrating objects. Sound Waves Sound waves are longitudinal waves traveling through a medium Sound waves are produced from vibrating objects Introduction Sound Waves: Molecular View When sound travels through a medium, there

More information

Physics 231 Lecture 25

Physics 231 Lecture 25 Physics 231 Lecture 25 Spherical waves P Main points of today s I = lecture: 2 4πr Wave Dopper speed shift for a string v + v o ƒ' = ƒ F v = v vs µ Interference of sound waves L Here F is the string tension

More information

Phys101 Lectures 28, 29. Wave Motion

Phys101 Lectures 28, 29. Wave Motion Phys101 Lectures 8, 9 Wave Motion Key points: Types of Waves: Transverse and Longitudinal Mathematical Representation of a Traveling Wave The Principle of Superposition Standing Waves; Resonance Ref: 11-7,8,9,10,11,16,1,13,16.

More information

Einstein Classes, Unit No. 102, 103, Vardhman Ring Road Plaza, Vikas Puri Extn., Outer Ring Road New Delhi , Ph. : ,

Einstein Classes, Unit No. 102, 103, Vardhman Ring Road Plaza, Vikas Puri Extn., Outer Ring Road New Delhi , Ph. : , PW W A V E S PW CONCEPTS C C Equation of a Travelling Wave The equation of a wave traveling along the positive x-ax given by y = f(x vt) If the wave travelling along the negative x-ax, the wave funcion

More information

Physics 101: Lecture 22 Sound

Physics 101: Lecture 22 Sound EXAM III Physics 101: Lecture 22 Sound Today s lecture will cover Textbook Chapter 12 Physics 101: Lecture 22, Pg 1 Standing Waves Fixed Endpoints Fundamental n=1 (2 nodes) l n = 2L/n f n = n v / (2L)

More information

PHYSICS 149: Lecture 24

PHYSICS 149: Lecture 24 PHYSICS 149: Lecture 24 Chapter 11: Waves 11.8 Reflection and Refraction 11.10 Standing Waves Chapter 12: Sound 12.1 Sound Waves 12.4 Standing Sound Waves Lecture 24 Purdue University, Physics 149 1 ILQ

More information

Exam 3 Review. F P av A. m V

Exam 3 Review. F P av A. m V Chapter 9: luids Learn the physics o liquids and gases. States o Matter Solids, liquids, and gases. Exam 3 Reiew ressure a ascal s rinciple change in pressure at any point in a conined luid is transmitted

More information

WAVES. Wave Equation. Waves Chap 16. So far this quarter. An example of Dynamics Conservation of Energy. Conservation theories. mass energy.

WAVES. Wave Equation. Waves Chap 16. So far this quarter. An example of Dynamics Conservation of Energy. Conservation theories. mass energy. Waes Chap 16 An example of Dynamics Conseration of Energy Conceptual starting point Forces Energy WAVES So far this quarter Conseration theories mass energy momentum angular momentum m E p L All conserations

More information

No Lecture on Wed. But, there is a lecture on Thursday, at your normal recitation time, so please be sure to come!

No Lecture on Wed. But, there is a lecture on Thursday, at your normal recitation time, so please be sure to come! Announcements Quiz 6 tomorrow Driscoll Auditorium Covers: Chapter 15 (lecture and homework, look at Questions, Checkpoint, and Summary) Chapter 16 (Lecture material covered, associated Checkpoints and

More information

General Physics I. Lecture 14: Sinusoidal Waves. Prof. WAN, Xin ( 万歆 )

General Physics I. Lecture 14: Sinusoidal Waves. Prof. WAN, Xin ( 万歆 ) General Physics I Lecture 14: Sinusoidal Waves Prof. WAN, Xin ( 万歆 ) xinwan@zju.edu.cn http://zimp.zju.edu.cn/~xinwan/ Motivation When analyzing a linear medium that is, one in which the restoring force

More information

A wave is a disturbance that propagates energy through a medium without net mass transport.

A wave is a disturbance that propagates energy through a medium without net mass transport. Waes A wae is a disturbance that propagates energy through a medium without net mass transport. Ocean waes proide example of transerse waes in which if we focus on a small olume of water, at a particular

More information

Chapter 16: Oscillatory Motion and Waves. Simple Harmonic Motion (SHM)

Chapter 16: Oscillatory Motion and Waves. Simple Harmonic Motion (SHM) Chapter 6: Oscillatory Motion and Waves Hooke s Law (revisited) F = - k x Tthe elastic potential energy of a stretched or compressed spring is PE elastic = kx / Spring-block Note: To consider the potential

More information

Chapter 16 Mechanical Waves

Chapter 16 Mechanical Waves Chapter 6 Mechanical Waves A wave is a disturbance that travels, or propagates, without the transport of matter. Examples: sound/ultrasonic wave, EM waves, and earthquake wave. Mechanical waves, such as

More information

Written homework due in class on Monday Online homework due on Tuesday by 8 am

Written homework due in class on Monday Online homework due on Tuesday by 8 am Homework #13 Written homework due in class on Monday Online homework due on Tuesday by 8 am Problem 15.35: use v sound = 343 m/s Final exam Thu May 14 from 1:30 to 3:30 pm (see info on blog) Boyden gym

More information

Einstein Classes, Unit No. 102, 103, Vardhman Ring Road Plaza, Vikas Puri Extn., Outer Ring Road New Delhi , Ph. : ,

Einstein Classes, Unit No. 102, 103, Vardhman Ring Road Plaza, Vikas Puri Extn., Outer Ring Road New Delhi , Ph. : , PW W A V E S Syllabus : Wave motion. Longitudinal and transverse waves, speed of wave. Dplacement relation for a progressive wave. Principle of superposition of waves, reflection of waves, Standing waves

More information

Lecture #8-6 Waves and Sound 1. Mechanical Waves We have already considered simple harmonic motion, which is an example of periodic motion in time.

Lecture #8-6 Waves and Sound 1. Mechanical Waves We have already considered simple harmonic motion, which is an example of periodic motion in time. Lecture #8-6 Waes and Sound 1. Mechanical Waes We hae already considered simple harmonic motion, which is an example of periodic motion in time. The position of the body is changing with time as a sinusoidal

More information

Chapter 14 Waves and Sound. Copyright 2010 Pearson Education, Inc.

Chapter 14 Waves and Sound. Copyright 2010 Pearson Education, Inc. Chapter 14 Waes and Sound Units of Chapter 14 Types of Waes Waes on a String Harmonic Wae Functions Sound Waes Sound Intensity The Doppler Effect We will leae out Chs. 14.5 and 14.7-14.9. 14-1 Types of

More information

Waves Part 3A: Standing Waves

Waves Part 3A: Standing Waves Waves Part 3A: Standing Waves Last modified: 24/01/2018 Contents Links Contents Superposition Standing Waves Definition Nodes Anti-Nodes Standing Waves Summary Standing Waves on a String Standing Waves

More information

Producing a Sound Wave. Chapter 14. Using a Tuning Fork to Produce a Sound Wave. Using a Tuning Fork, cont.

Producing a Sound Wave. Chapter 14. Using a Tuning Fork to Produce a Sound Wave. Using a Tuning Fork, cont. Producing a Sound Wave Chapter 14 Sound Sound waves are longitudinal waves traveling through a medium A tuning fork can be used as an example of producing a sound wave Using a Tuning Fork to Produce a

More information

Standing Waves (stationary waves) interference, nodes, antinodes, wavelength is twice the node-to-node distance

Standing Waves (stationary waves) interference, nodes, antinodes, wavelength is twice the node-to-node distance Standing Waes Doppler Eect Standing Waes (stationary waes) intererence, nodes, antinodes, waelength is twice the node-to-node distance Standing Waes on Strings - string ixed at both end undamental, harmonics,

More information

Downloaded from

Downloaded from Chapter 15 (Waves) Multiple Choice Questions Single Correct Answer Type Q1. Water waves produced by a motorboat sailing in water are (a) neither longitudinal nor transverse (b) both longitudinal and transverse

More information

Oscillations - AP Physics B 1984

Oscillations - AP Physics B 1984 Oscillations - AP Physics B 1984 1. If the mass of a simple pendulum is doubled but its length remains constant, its period is multiplied by a factor of (A) 1 2 (B) (C) 1 1 2 (D) 2 (E) 2 A block oscillates

More information

Physics 1501 Lecture 28

Physics 1501 Lecture 28 Phsics 1501 Lecture 28 Phsics 1501: Lecture 28 Toda s Agenda Homework #10 (due Frida No. 11) Midterm 2: No. 16 Topics 1-D traeling waes Waes on a string Superposition Power Phsics 1501: Lecture 28, Pg

More information

Standing Waves on Strings - string fixed at both end fundamental, harmonics, overtones, modes of vibration (Fig ) Node Antinode N A N A N

Standing Waves on Strings - string fixed at both end fundamental, harmonics, overtones, modes of vibration (Fig ) Node Antinode N A N A N PHYS2 Physics 1 FUNDAMENTALS Module 3 OSCILLATIONS & WAVES Text Physics by Hecht Chapter 11 WAVES Standing Waes Doppler Eect Sections: 11. 11.11 Examples: 11.12 11.13 11.14 11.15 CHECKLIST Standing Waes

More information

WAVES( SUB) 2. What is the property of the medium that is essential for the propagation of mechanical wave? Ans: Elasticity and inertia

WAVES( SUB) 2. What is the property of the medium that is essential for the propagation of mechanical wave? Ans: Elasticity and inertia WAES( SUB). What is meant by a wave? Ans: The disturbance set up in a medium is known as a wave. What is the property of the medium that is essential for the propagation of mechanical wave? Ans: Elasticity

More information

Class Average = 71. Counts Scores

Class Average = 71. Counts Scores 30 Class Average = 71 25 20 Counts 15 10 5 0 0 20 10 30 40 50 60 70 80 90 100 Scores Chapter 12 Mechanical Waves and Sound To describe mechanical waves. To study superposition, standing waves, and interference.

More information

Get Solution of These Packages & Learn by Video Tutorials on SOUND WAVES

Get Solution of These Packages & Learn by Video Tutorials on  SOUND WAVES Get Solution of These Packages & Learn by Video Tutorials on www.mathsbysuhag.com. PROPAGATION OF SOUND WAVES : Sound is a mechanical three dimensional and longitudinal wae that is created by a ibrating

More information

Transverse waves. Waves. Wave motion. Electromagnetic Spectrum EM waves are transverse.

Transverse waves. Waves. Wave motion. Electromagnetic Spectrum EM waves are transverse. Transerse waes Physics Enhanceent Prograe for Gifted Students The Hong Kong Acadey for Gifted Education and, HKBU Waes. Mechanical waes e.g. water waes, sound waes, seisic waes, strings in usical instruents.

More information

SIMPLE HARMONIC MOTION

SIMPLE HARMONIC MOTION WAVES SIMPLE HARMONIC MOTION Simple Harmonic Motion (SHM) Vibration about an equilibrium position in which a restoring force is proportional to the displacement from equilibrium TYPES OF SHM THE PENDULUM

More information

Lorik educatinal academy vidya nagar

Lorik educatinal academy vidya nagar Lorik educatinal academy vidya nagar ========================================================== PHYSICS-Wave Motion & Sound Assignment. A parachutist jumps from the top of a very high tower with a siren

More information

NARAYANA JUNIOR COLLEGE

NARAYANA JUNIOR COLLEGE SR IIT ALL STREAMS ADV MODEL DPT-6 Date: 18/04/2016 One (or) More Than One Answer Type: PHYSICS 31. A particle is executing SHM between points -X m and X m, as shown in figure-i. The velocity V(t) of the

More information

Simple Harmonic Motion

Simple Harmonic Motion Please get your personal iclicker from its pigeonhole on North wall. Simple Harmonic Motion 0 t Position: x = A cos(ω t + φ) Velocity: x t = (ω A) sin(ω t + φ) { max Acceleration: t = (ω2 A) cos(ω t +

More information

Physics 207 Lecture 28

Physics 207 Lecture 28 Goals: Lecture 28 Chapter 20 Employ the wae model Visualize wae motion Analyze functions of two ariables Know the properties of sinusoidal waes, including waelength, wae number, phase, and frequency. Work

More information

CLASS 2 CLASS 2. Section 13.5

CLASS 2 CLASS 2. Section 13.5 CLASS 2 CLASS 2 Section 13.5 Simple Pendulum The simple pendulum is another example of a system that exhibits simple harmonic motion The force is the component of the weight tangent to the path of motion

More information

Physics 248 Spring 2009

Physics 248 Spring 2009 Physics 248 Spring 2009 Lab 1: Transverse standing waves on a string and speed of sound in air Your TA will use this sheet to score your lab. It is to be turned in at the end of the lab. You must use complete

More information

Physics 111. Lecture 31 (Walker: ) Wave Superposition Wave Interference Standing Waves Physics of Musical Instruments Temperature

Physics 111. Lecture 31 (Walker: ) Wave Superposition Wave Interference Standing Waves Physics of Musical Instruments Temperature Physics 111 Lecture 31 (Walker: 14.7-8) Wave Superposition Wave Interference Physics of Musical Instruments Temperature Superposition and Interference Waves of small amplitude traveling through the same

More information

Physics 1C Lecture 14B. Today: End of Chapter 14 Start of Chapter 27

Physics 1C Lecture 14B. Today: End of Chapter 14 Start of Chapter 27 Physics 1C Lecture 14B Today: End of Chapter 14 Start of Chapter 27 ! Example Wave Interference! Two strings with linear densities of 5.0g/m are stretched over pulleys, adjusted to have vibrating lengths

More information

UNIVERSITY OF SASKATCHEWAN Department of Physics and Engineering Physics

UNIVERSITY OF SASKATCHEWAN Department of Physics and Engineering Physics UNIVERSITY OF SASKATCHEWAN Department of Physics and Engineering Physics Physics 111.6 MIDTERM TEST #3 January 25, 2007 Time: 90 minutes NAME: (Last) Please Print (Given) STUDENT NO.: LECTURE SECTION (please

More information

Chapter 15 Mechanical Waves

Chapter 15 Mechanical Waves Chapter 15 Mechanical Waves 1 Types of Mechanical Waves This chapter and the next are about mechanical waves waves that travel within some material called a medium. Waves play an important role in how

More information

13.3 Interference and Superposition. Interference and Superposition Constructive Interference Destructive Interference Standing Waves

13.3 Interference and Superposition. Interference and Superposition Constructive Interference Destructive Interference Standing Waves 13.3 Interference and Superposition Interference and Superposition Constructive Interference Destructive Interference Standing Waves Interference and Superposition When raindrops fall into still water,

More information

Chapter 16. Waves and Sound

Chapter 16. Waves and Sound Chapter 16 Waes and Sound 16.1 The Nature of Waes 1. A wae is a traeling disturbance. 2. A wae carries energy from place to place. 16.1 The Nature of Waes Transerse Wae 16.1 The Nature of Waes Longitudinal

More information

Standing waves [49 marks]

Standing waves [49 marks] Standing waves [49 marks] 1. The graph shows the variation with time t of the velocity v of an object undergoing simple harmonic motion (SHM). At which velocity does the displacement from the mean position

More information

Physics 240: Worksheet 24 Name:

Physics 240: Worksheet 24 Name: () Cowboy Ryan is on the road again! Suppose that he is inside one of the many caerns that are found around the Whitehall area of Montana (which is also, by the way, close to Wheat Montana). He notices

More information

General Physics (PHY 2130)

General Physics (PHY 2130) General Physics (PHY 2130) Lecture XII Sound sound waves Doppler effect Standing waves Light Reflection and refraction Lightning Review Last lecture: 1. Vibration and waves Hooke s law Potential energy

More information

Waves Encountering Barriers

Waves Encountering Barriers Waves Encountering Barriers Reflection and Refraction: When a wave is incident on a boundary that separates two regions of different wave speed, part of the wave is reflected and part is transmitted. Figure

More information

Chapter 17. Superposition & Standing Waves

Chapter 17. Superposition & Standing Waves Chapter 17 Superposition & Standing Waves Superposition & Standing Waves Superposition of Waves Standing Waves MFMcGraw-PHY 2425 Chap 17Ha - Superposition - Revised: 10/13/2012 2 Wave Interference MFMcGraw-PHY

More information

Class 35. Wave properties. PHY 231 Fall 2004 Prof. S. Billinge

Class 35. Wave properties. PHY 231 Fall 2004 Prof. S. Billinge Class 35 Wave properties Announcements Clicker scores were sent by message to LONCAPA. Please check and report problems to me ASAP Concepts overview 1. Wavelength, amplitude, frequency, period 2. Superposition

More information

General Physics (PHY 2130)

General Physics (PHY 2130) General Physics (PHY 2130) Lecture XII Sound sound waves Doppler effect Standing waves Light Reflection and refraction http://www.physics.wayne.edu/~apetrov/phy2130/ Lightning Review Last lecture: 1. Vibration

More information

WAVE MOTION AND SHM SECTON 3 SOLUTIONS. Ans.a

WAVE MOTION AND SHM SECTON 3 SOLUTIONS. Ans.a WAVE MOTION AND SHM SECTON 3 SOLUTIONS πf ω π. V = fλ= =, because πf = ω, = k. Ans.a π / λ k λ. While (a) and (b) are traelling waes, (d) is the superposition of two traelling waes, f(x-t) and f(x+t).

More information

1. Types of Waves. There are three main types of waves:

1. Types of Waves. There are three main types of waves: Chapter 16 WAVES I 1. Types of Waves There are three main types of waves: https://youtu.be/kvc7obkzq9u?t=3m49s 1. Mechanical waves: These are the most familiar waves. Examples include water waves, sound

More information

Superposition and Standing Waves

Superposition and Standing Waves 8 Superposition and Standing Waes CHPTER OUTLINE 8. Superposition and Intererence 8. Standing Waes 8.3 Standing Waes in a String Fixed at Both Ends 8. Resonance 8.5 Standing Waes in ir Columns 8.6 Standing

More information

PHYS Homework # 10 (Mendes, Fall 2015) due in class on Nov 20. 1) Exercise 15.4, p. 501, University Physics by Young & Freedman

PHYS Homework # 10 (Mendes, Fall 2015) due in class on Nov 20. 1) Exercise 15.4, p. 501, University Physics by Young & Freedman PHYS 98 - Homework # 10 (Mendes, Fall 015) due in class on Nov 0 1) Exercise 154, p 501, Universit Phsics b Young & Freedman IDENTIFY: f v SET UP: 10 mm 00010 m v 1500m/s 6 EXECUTE: f 15 10 Hz 00010 m

More information

jfpr% ekuo /kez iz.ksrk ln~xq# Jh j.knksm+nklth egkjkt

jfpr% ekuo /kez iz.ksrk ln~xq# Jh j.knksm+nklth egkjkt Phone : 93 93 7779, 9893 58881 Sount & Waves Page: 9 fo/u fopkjr Hkh# tu] ugha vkjehks dke] foifr ns[k NksM+s rqjar e/;e eu dj ';kea iq#"k flag ladyi dj] lgrs foifr vusd] ^cuk^ u NksM+s /;s; dks] j?kqcj

More information

Standing waves. The interference of two sinusoidal waves of the same frequency and amplitude, travel in opposite direction, produce a standing wave.

Standing waves. The interference of two sinusoidal waves of the same frequency and amplitude, travel in opposite direction, produce a standing wave. Standing waves The interference of two sinusoidal waves of the same frequency and amplitude, travel in opposite direction, produce a standing wave. y 1 (x, t) = y m sin(kx ωt), y 2 (x, t) = y m sin(kx

More information

Physics 101: Lecture 22 Sound

Physics 101: Lecture 22 Sound EXAM III Physics 101: Lecture 22 Sound Today s lecture will cover Textbook Chapter 12 Physics 101: Lecture 22, Pg 1 Speed of Sound Recall for pulse on string: v = sqrt(t / m) For fluids: v = sqrt(b/r)

More information

Standing Waves If the same type of waves move through a common region and their frequencies, f, are the same then so are their wavelengths, λ.

Standing Waves If the same type of waves move through a common region and their frequencies, f, are the same then so are their wavelengths, λ. Standing Waves I the same type o waves move through a common region and their requencies,, are the same then so are their wavelengths,. This ollows rom: v=. Since the waves move through a common region,

More information

Transverse Wave - Only in solids (having rigidity), in liquids possible only on the surface. Longitudinal Wave

Transverse Wave - Only in solids (having rigidity), in liquids possible only on the surface. Longitudinal Wave Wave is when one particle passes its motion to its neighbour. The Elasticity and Inertia of the medium play important role in the propagation of wave. The elasticity brings the particle momentarily at

More information

PHYSICS 220. Lecture 21. Textbook Sections Lecture 21 Purdue University, Physics 220 1

PHYSICS 220. Lecture 21. Textbook Sections Lecture 21 Purdue University, Physics 220 1 PHYSICS 220 Lecture 21 Sound Textbook Sections 13.1 13.7 Lecture 21 Purdue University, Physics 220 1 Overview Last Lecture Interference and Diffraction Constructive, destructive Diffraction: bending of

More information

Marketed and Distributed By FaaDoOEngineers.com

Marketed and Distributed By FaaDoOEngineers.com WAVES GUPTA CLASSES For any help contact: 995368795, 968789880 Nishant Gupta, D-, Prashant vihar, Rohini, Delhi-85 Waves Wave motion A wave motion is a kind of disturbance which is transferred from one

More information

Waves 2006 Physics 23. Armen Kocharian Lecture 3: Sep

Waves 2006 Physics 23. Armen Kocharian Lecture 3: Sep Waves 2006 Physics 23 Armen Kocharian Lecture 3: Sep 12. 2006 Last Time What is a wave? A "disturbance" that moves through space. Mechanical waves through a medium. Transverse vs. Longitudinal e.g., string

More information

Chapter 16 Waves in One Dimension

Chapter 16 Waves in One Dimension Chapter 16 Waves in One Dimension Slide 16-1 Reading Quiz 16.05 f = c Slide 16-2 Reading Quiz 16.06 Slide 16-3 Reading Quiz 16.07 Heavier portion looks like a fixed end, pulse is inverted on reflection.

More information

Chapter 18 Solutions

Chapter 18 Solutions Chapter 18 Solutions 18.1 he resultant wave function has the form y A 0 cos φ sin kx ω t + φ (a) A A 0 cos φ (5.00) cos (π /4) 9.4 m f ω π 100π π 600 Hz *18. We write the second wave function as hen y

More information

Physics 25 Section 2 Exam #1 February 1, 2012 Dr. Alward

Physics 25 Section 2 Exam #1 February 1, 2012 Dr. Alward 1.The tension in a taut rope is increased by a factor of 9, and the mass per length is reduced to one-fourth of its former value.. How does the speed of wave pulses on the rope change, if at all? A) The

More information

CHAPTER 11 VIBRATIONS AND WAVES

CHAPTER 11 VIBRATIONS AND WAVES CHAPTER 11 VIBRATIONS AND WAVES http://www.physicsclassroom.com/class/waves/u10l1a.html UNITS Simple Harmonic Motion Energy in the Simple Harmonic Oscillator The Period and Sinusoidal Nature of SHM The

More information

Magnetic fields & forces

Magnetic fields & forces Phys 102 Lecture 10 Magnetic fields & forces 1 Today we will... Learn about the magnetism Magnetic field B Magnetic force F on moing charge Apply these concepts! Charged particle motion in a magnetic field

More information

Chapter 16: Oscillations

Chapter 16: Oscillations Chapter 16: Oscillations Brent Royuk Phys-111 Concordia University Periodic Motion Periodic Motion is any motion that repeats itself. The Period (T) is the time it takes for one complete cycle of motion.

More information

Wave Motion A wave is a self-propagating disturbance in a medium. Waves carry energy, momentum, information, but not matter.

Wave Motion A wave is a self-propagating disturbance in a medium. Waves carry energy, momentum, information, but not matter. wae-1 Wae Motion A wae is a self-propagating disturbance in a medium. Waes carr energ, momentum, information, but not matter. Eamples: Sound waes (pressure waes) in air (or in an gas or solid or liquid)

More information

Section 1 Simple Harmonic Motion. The student is expected to:

Section 1 Simple Harmonic Motion. The student is expected to: Section 1 Simple Harmonic Motion TEKS The student is expected to: 7A examine and describe oscillatory motion and wave propagation in various types of media Section 1 Simple Harmonic Motion Preview Objectives

More information

Section 1 Simple Harmonic Motion. Chapter 11. Preview. Objectives Hooke s Law Sample Problem Simple Harmonic Motion The Simple Pendulum

Section 1 Simple Harmonic Motion. Chapter 11. Preview. Objectives Hooke s Law Sample Problem Simple Harmonic Motion The Simple Pendulum Section 1 Simple Harmonic Motion Preview Objectives Hooke s Law Sample Problem Simple Harmonic Motion The Simple Pendulum Section 1 Simple Harmonic Motion Objectives Identify the conditions of simple harmonic

More information

Lecture 30. Chapter 21 Examine two wave superposition (-ωt and +ωt) Examine two wave superposition (-ω 1 t and -ω 2 t)

Lecture 30. Chapter 21 Examine two wave superposition (-ωt and +ωt) Examine two wave superposition (-ω 1 t and -ω 2 t) To do : Lecture 30 Chapter 21 Examine two wave superposition (-ωt and +ωt) Examine two wave superposition (-ω 1 t and -ω 2 t) Review for final (Location: CHEM 1351, 7:45 am ) Tomorrow: Review session,

More information

Physics General Physics. Lecture 25 Waves. Fall 2016 Semester Prof. Matthew Jones

Physics General Physics. Lecture 25 Waves. Fall 2016 Semester Prof. Matthew Jones Physics 22000 General Physics Lecture 25 Waves Fall 2016 Semester Prof. Matthew Jones 1 Final Exam 2 3 Mechanical Waves Waves and wave fronts: 4 Wave Motion 5 Two Kinds of Waves 6 Reflection of Waves When

More information

1169T2/2001. Question 1 ( marks)

1169T2/2001. Question 1 ( marks) 1169T2/2001 1 Question 1 ( marks) a) Write the equations of two traelling waes, y 1 (x,t) and y 2 (x,t), which, when they superpose, produce a standing wae. State the amplitude, waelength and frequency

More information

Chapter 15. Mechanical Waves

Chapter 15. Mechanical Waves Chapter 15 Mechanical Waves A wave is any disturbance from an equilibrium condition, which travels or propagates with time from one region of space to another. A harmonic wave is a periodic wave in which

More information

Wave Phenomena Physics 15c. Lecture 9 Wave Reflection Standing Waves

Wave Phenomena Physics 15c. Lecture 9 Wave Reflection Standing Waves Wave Phenomena Physics 15c Lecture 9 Wave Reflection Standing Waves What We Did Last Time Energy and momentum in LC transmission lines Transfer rates for normal modes: and The energy is carried by the

More information

Content of the course 3NAB0 (see study guide)

Content of the course 3NAB0 (see study guide) Content of the course 3NAB0 (see study guide) 17 November diagnostic test! Week 1 : 14 November Week 2 : 21 November Introduction, units (Ch1), Circuits (Ch25,26) Heat (Ch17), Kinematics (Ch2 3) Week 3:

More information

Physics 107 TUTORIAL ASSIGNMENT #7

Physics 107 TUTORIAL ASSIGNMENT #7 Physics 07 TUTORIL SSIGNMENT #7 Cutnell & Johnson, 7 th edition Chapter 6: Problems 5, 65, 79, 93 Chapter 7: Problems 7,, 9, 37, 48 Chapter 6 5 Suppose that sound is emitted uniormly in all directions

More information

A longitudinal wave travels through a medium from left to right.

A longitudinal wave travels through a medium from left to right. 1. This question is about simple harmonic oscillations. A longitudinal wave travels through a medium from left to right. Graph 1 shows the variation with time t of the displacement x of a particle P in

More information

1) The K.E and P.E of a particle executing SHM with amplitude A will be equal to when its displacement is:

1) The K.E and P.E of a particle executing SHM with amplitude A will be equal to when its displacement is: 1) The K.E and P.E of a particle executing SHM with amplitude A will be equal to when its displacement is: 2) The bob of simple Pendulum is a spherical hallow ball filled with water. A plugged hole near

More information

The velocity (v) of the transverse wave in the string is given by the relation: Time taken by the disturbance to reach the other end, t =

The velocity (v) of the transverse wave in the string is given by the relation: Time taken by the disturbance to reach the other end, t = Question 15.1: A string of mass 2.50 kg is under a tension of 200 N. The length of the stretched string is 20.0 m. If the transverse jerk is struck at one end of the string, how long does the disturbance

More information

WAVES. 1.) A wave is a disturbance that moves through a medium. (You can t have water waves without water!)

WAVES. 1.) A wave is a disturbance that moves through a medium. (You can t have water waves without water!) WAVES 1.) A wave is a disturbance that moves through a medium. (You can t have water waves without water!) 2.) A wave produced by a force that is perpendicular to the direction of propagation of the wave

More information

N10/4/PHYSI/SPM/ENG/TZ0/XX PHYSICS STANDARD LEVEL PAPER 1. Monday 8 November 2010 (afternoon) 45 minutes INSTRUCTIONS TO CANDIDATES

N10/4/PHYSI/SPM/ENG/TZ0/XX PHYSICS STANDARD LEVEL PAPER 1. Monday 8 November 2010 (afternoon) 45 minutes INSTRUCTIONS TO CANDIDATES N1/4/PHYSI/SPM/ENG/TZ/XX 881654 PHYSICS STANDARD LEVEL PAPER 1 Monday 8 Noember 21 (afternoon) 45 minutes INSTRUCTIONS TO CANDIDATES Do not open this examination paper until instructed to do so. Answer

More information

AP Physics Problems Simple Harmonic Motion, Mechanical Waves and Sound

AP Physics Problems Simple Harmonic Motion, Mechanical Waves and Sound AP Physics Problems Simple Harmonic Motion, Mechanical Waves and Sound 1. 1977-5 (Mechanical Waves/Sound) Two loudspeakers, S 1 and S 2 a distance d apart as shown in the diagram below left, vibrate in

More information