y (m)

Size: px
Start display at page:

Download "y (m)"

Transcription

1 4 Spring 99 Problem Set Optional Problems Physics February, 999 Handout Sinusoidal Waes. sinusoidal waes traeling on a string are described by wae Two Waelength is waelength of wae?ofwae? In terms of amplitude A, period T and waelength, of a sinusoidal traeling wae isy(x; t) Acos, ( x, t T ). form 5 Frequency is frequency of wae?ofwae? Using same expression as in part (, we hae for wae f 3 T f T relation between frequency f, waelength, and wae for a sinusoidal wae isf. Sowehae speed f 4:77 :6 cm :6 cm f :9 :34 cm :6 cm both waes are traeling on same string, y must hae Since speed. same Phase Dierence d) is phase dierence between waes? phase of wae is 5x,3t; phase of wae x,t. phase dierence is is 5x, 3t, (x, t) 3x,8t Superposition e) superposition of se waes is y3(x; t) y(x; t)+y(x; t). Find an relating alues of x and t for which superposition y3(x; t) equation always zero. (This is called destructie interference). is y(x; t) cos(5x, 3t) and y(x; t) cos(x, t). In functions equations, y and x are in cm and t is in. se Speed c) is speed of waes on string? Comparing this expression with that of wae,we see that or x 5x cm:6 cm For wae,we hae x x cm:34 cm, t 3t T Hz 4:77 Hz For wae,we hae t t T Hz :9 Hz

2 a phase shift of n into a wae, where n is an odd integer, Introducing sign of wae. Since both wae and wae hae same changes sum of two waes will be zero wheneer phase amplitude, is relation between x and t which makes sum of two waes This zero. Speed of Transerse Waes. aluminum wire has 3 tions as shown. Section has radius r, tion An has radius r, and tion 3 has radius 3r. are ratios of of a transerse wae propagating in three tions? speeds : : 3 3 : : (A) 9 : 4 : (B) : / : /3 (C) elocity of wae is related to mass per unit, and tension,, by: p.for a wire of density and length, r, r. We see that / r. refore, : : 3 r : radius :3r::3 and correct answer is (C). r Pulse on a String 3. plot shows a pulse on a string at time t. wae speed is quantitatiely transerse elocity (\chunk speed") of Sketch as a function of x at t. Label your axes clearly and be sure to string use relation between transerse elocity and slope appropriate We dierence between waes is n. Thus we hae 3x,8t n ms,. p : p 3 (D): : : 3 (E) gie units. for a traeling wae moing in +x direction: y y, From this relation and graph gien aboe we hae:

3 If wae speed is 5m/s, describe in detail motion which should gien to end of string to produce this pulse. be steep part of pulse must hae been made rst since is farst from source. waeform traels.5 m horizontally it 5m/s in going from minimum to maximum displacement so this must at / of a ond. wae n traels.5 m horizontally at 5m/s take going from maximum to minimum displacement which takes / of a in refore, to produce waeform shown, end of string ond. be raised cm at a uniform elocity of cm/.s m/s and must lowered cm at a uniform elocity of cm/.5s.m/s. n How is answer changed if wae speed is m/s? If wae speed is now m/s, n to produce waeform indicated, end of string must be raised cm at a uniform of cm/.5s m/s and n lowered cm at a uniform elocity elocity of cm/.5s.4m/s. Wae Propagation 5. time t awae pulse looks as shown. It is propagating in +x At Propagation in t does pulse look like as a function of x at time.5 onds later? a At a time.5s later, pulse will hae traeled d t 5 along +x axis, so it will look same but be translated 5 m. This m Wae Pulses 4. want to produce a wae pulse on a string that is moing to right You direction with elocity m/s..8 and that has form shown in gure x (m) is shown below: 3

4 Propagation in x does pulse look like as a function of time x m? at This is trickier. One good way to handle this is to make marks on original cure showing time at which that part of tick wae will cross x. For example, on original axis at x you put a tick mark labeled s, at x, myou would put a tick would labeled s, and so on, because those are times when that point mark cure gets to x. You can n redraw graph with y s. t on Note that pulse looks reersed since leading edge will reach axes. point onxaxis at earlier times relatie to trailing edge. a Wae Equation 6. a wae described by y(x; t) f(x, t) that is traelling Consider Proe that slope of string at any point x is equal in magnitude ratio of \chunk speed" (transerse elocity) to wae speed to f(z) f(x,t) where z x, t, n slope of f(x, t) is: Gien aboe wehae that From and we recognize that, desired. as we let z (x,t) and y f(x, t) f(z). Again along a string. at that point x (m) Use a similar argument to show that y(x; t) satises wae equation, y y for any (reasonable) function f. () : Similarly, we can write: (,): u, where u is chunk speed. Thus, we hae,u t (s) f ( ) ( ) ( ) We follow similar steps for time deriaties: (,) f : f ( ) (, ) (, ) f : 4

5 since f f, refore, Howeer, Superposition 7. wae equation for transerse waes on a spring (or string) obeys Show that following ariation on wae equation obeys of superposition: principle sin(x) y We start with two solutions, y (x; t) and y (x; t), to wae equation aboe. Because y are both solutions: modied sin(x) y sin(x) y y see if y(x; t) Ay + By is also a solution. We'll start with left Let's of equation: side sin(x) A sin(x) y A y + B + Bsin(x) y Show that following ariation on wae equation does not obey principle of superposition: y sin y We'll try same method. If y (x; t) and y (x; t) are solutions, n y Asin sin + B y sin A y 6 B sin + B + f f : part of this equation is reponsible for it not obeying superposition? of superposition. That is, if y(x; t) and y(x; t) are solutions of principle wae equation, n y(x; t)+y(x; t) is a solution, too. y and y sin y Let's see if y(x; t) Ay + By is a solution. y [Ay + By] A y and sin(x) y does a sum of solutions fail to satisfy this wae equation? Because of Why sine, which is applied to y(x; t) (or more precisely, to its deriatie). that sine operation is not linear: sin( + sin( 6 sin(a +. [Ay + By] [Ay + By] So y(x; t) is a solution, too, and this wae equation obeys superposition. 5

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

PHYS1169: Tutorial 8 Solutions

PHYS1169: Tutorial 8 Solutions PHY69: Tutorial 8 olutions Wae Motion ) Let us consier a point P on the wae with a phase φ, so y cosϕ cos( x ± ωt) At t0, this point has position x0, so ϕ x0 ± ωt0 Now, at some later time t, the position

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

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

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

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

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

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

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

y(x,5) (cm) x (m)

y(x,5) (cm) x (m) Spring 99 Problem Set Optional Problems Physics February 9, 999 Handout Wave Propagation and Reection. pulse has shape shown in gure as it travels at 00 Asawtooth along a stretched wire. At t = 0, leading

More information

Get Solution of These Packages & Learn by Video Tutorials on WAVES ON A STRING

Get Solution of These Packages & Learn by Video Tutorials on  WAVES ON A STRING WVES ON STRING WVES Wae motion is the phenomenon that can be obsered almost eerywhere around us, as well it appears in almost eery branch o physics. Surace waes on bodies o mater are commonly obsered.

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

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 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

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

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

Last Name First Name Date

Last Name First Name Date Last Name irst Name Date 16.1 The Nature of Waes 16.2 Periodic Waes 16.3 The Speed of a Wae in a String Conceptual Questions 1,2,3,7, 8, 11 page 503 Problems 2, 4, 6, 12, 15, 16 page 501-502 Types of Waes

More information

Honors Classical Physics I

Honors Classical Physics I Honors Classical Physics I PHY141 ecture 32 ound Waes Please set your clicker to channel 21 ecture 32 1 Bosch 36W column loudspeaker polar pattern Monsoon Flat Panel speaker: (5 db grid) 400 Hz: Real oudspeakers

More information

E : Ground-penetrating radar (GPR)

E : Ground-penetrating radar (GPR) Geophysics 3 March 009 E : Ground-penetrating radar (GPR) The EM methods in section D use low frequency signals that trael in the Earth by diffusion. These methods can image resistiity of the Earth on

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

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

1 f. result from periodic disturbance same period (frequency) as source Longitudinal or Transverse Waves Characterized by

1 f. result from periodic disturbance same period (frequency) as source Longitudinal or Transverse Waves Characterized by result from periodic disturbance same period (frequency) as source Longitudinal or Transverse Waves Characterized by amplitude (how far do the bits move from their equilibrium positions? Amplitude of MEDIUM)

More information

Transmission lines using a distributed equivalent circuit

Transmission lines using a distributed equivalent circuit Cambridge Uniersity Press 978-1-107-02600-1 - Transmission Lines Equialent Circuits, Electromagnetic Theory, and Photons Part 1 Transmission lines using a distributed equialent circuit in this web serice

More information

Modern Physics. Unit 1: Classical Models and the Birth of Modern Physics Lecture 1.2: Classical Concepts Review of Particles and Waves

Modern Physics. Unit 1: Classical Models and the Birth of Modern Physics Lecture 1.2: Classical Concepts Review of Particles and Waves Modern Physics Unit 1: Classical Models and the Birth of Modern Physics Lecture 1.: Classical Concepts Reiew of Particles and Waes Ron Reifenberger Professor of Physics Purdue Uniersity 1 Equations of

More information

A possible mechanism to explain wave-particle duality L D HOWE No current affiliation PACS Numbers: r, w, k

A possible mechanism to explain wave-particle duality L D HOWE No current affiliation PACS Numbers: r, w, k A possible mechanism to explain wae-particle duality L D HOWE No current affiliation PACS Numbers: 0.50.-r, 03.65.-w, 05.60.-k Abstract The relationship between light speed energy and the kinetic energy

More information

Spring 2000 HIGHER STILL. Physics. Student Materials Advanced Higher. Summary Notes Unit 3 Wave Phenomena. Physics (AH): Mechanics - Student Materials

Spring 2000 HIGHER STILL. Physics. Student Materials Advanced Higher. Summary Notes Unit 3 Wave Phenomena. Physics (AH): Mechanics - Student Materials Spring 2000 HIGHER STILL Physics Student Materials Adanced Higher Summary Notes Unit 3 Wae Phenomena Physics (AH): Mechanics - Student Materials WAVE PHENOMENA The Content Statements for this unit are

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

1. Linear Motion. Table of Contents. 1.1 Linear Motion: Velocity Time Graphs (Multi Stage) 1.2 Linear Motion: Velocity Time Graphs (Up and Down)

1. Linear Motion. Table of Contents. 1.1 Linear Motion: Velocity Time Graphs (Multi Stage) 1.2 Linear Motion: Velocity Time Graphs (Up and Down) . LINEAR MOTION www.mathspoints.ie. Linear Motion Table of Contents. Linear Motion: Velocity Time Graphs (Multi Stage). Linear Motion: Velocity Time Graphs (Up and Down).3 Linear Motion: Common Initial

More information

LECTURE 3 3.1Rules of Vector Differentiation

LECTURE 3 3.1Rules of Vector Differentiation LETURE 3 3.1Rules of Vector Differentiation We hae defined three kinds of deriaties inoling the operator grad( ) i j k, x y z 1 3 di(., x y z curl( i x 1 j y k z 3 d The good news is that you can apply

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

UNDERSTAND MOTION IN ONE AND TWO DIMENSIONS

UNDERSTAND MOTION IN ONE AND TWO DIMENSIONS SUBAREA I. COMPETENCY 1.0 UNDERSTAND MOTION IN ONE AND TWO DIMENSIONS MECHANICS Skill 1.1 Calculating displacement, aerage elocity, instantaneous elocity, and acceleration in a gien frame of reference

More information

Chapter 24 & 26. Electromagnetic Waves & Wave Properties. 1. A wave is a traveling disturbance. 2. A wave carries energy from place to place.

Chapter 24 & 26. Electromagnetic Waves & Wave Properties. 1. A wave is a traveling disturbance. 2. A wave carries energy from place to place. Chapter 4 & 6 Electromagnetic Waes & Wae Properties DR JJ UiTM-Cutnell & Johnson 7th ed. 6. The Nature of Waes. A wae is a traeling disturbance.. A wae carries energy from place to place. Waes trael to

More information

Physics Department Tutorial: Motion in a Circle (solutions)

Physics Department Tutorial: Motion in a Circle (solutions) JJ 014 H Physics (9646) o Solution Mark 1 (a) The radian is the angle subtended by an arc length equal to the radius of the circle. Angular elocity ω of a body is the rate of change of its angular displacement.

More information

Chapter 14 PROBLEM SOLUTIONS Since vlight v sound, the time required for the flash of light to reach the observer is negligible in

Chapter 14 PROBLEM SOLUTIONS Since vlight v sound, the time required for the flash of light to reach the observer is negligible in Chapter 4 PRBLEM LUTN 4. ince light sound, the time required or the lash o light to reach the obserer is negligible in comparison to the time required or the sound to arrie. Thus, we can ignore the time

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

Sound, Decibels, Doppler Effect

Sound, Decibels, Doppler Effect Phys101 Lectures 31, 32 Sound, Decibels, Doppler Effect Key points: Intensity of Sound: Decibels Doppler Effect Ref: 12-1,2,7. Page 1 Characteristics of Sound Sound can trael through any kind of matter,

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

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

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

DO PHYSICS ONLINE. WEB activity: Use the web to find out more about: Aristotle, Copernicus, Kepler, Galileo and Newton.

DO PHYSICS ONLINE. WEB activity: Use the web to find out more about: Aristotle, Copernicus, Kepler, Galileo and Newton. DO PHYSICS ONLINE DISPLACEMENT VELOCITY ACCELERATION The objects that make up space are in motion, we moe, soccer balls moe, the Earth moes, electrons moe, - - -. Motion implies change. The study of the

More information

N12/4/PHYSI/SPM/ENG/TZ0/XX. Physics Standard level Paper 1. Tuesday 13 November 2012 (afternoon) 45 minutes INSTRUCTIONS TO CANDIDATES

N12/4/PHYSI/SPM/ENG/TZ0/XX. Physics Standard level Paper 1. Tuesday 13 November 2012 (afternoon) 45 minutes INSTRUCTIONS TO CANDIDATES N1/4/PHYSI/SPM/ENG/TZ0/XX 8816504 Physics Standard leel Paper 1 Tuesday 13 Noember 01 (afternoon) 45 minutes INSTRUCTIONS TO CANDIDATES Do not open this examination paper until instructed to do so. Answer

More information

LINEAR SUPERPOSITION AND INTERFERENCE PHENOMENA

LINEAR SUPERPOSITION AND INTERFERENCE PHENOMENA CHAPTER 7 THE PRINCIPE OF INEAR SUPERPOSITION AND INTERFERENCE PHENOMENA ANSWERS TO FOCUS ON CONCEPTS QUESTIONS. (d) I we add pulses and 4 as per the principle o linear superposition, the resultant is

More information

Physics 102 Homework Solutions: Ch 16

Physics 102 Homework Solutions: Ch 16 Physics 0 Hoework Solutions: Ch 6. SSM REASONING Since light behaes as a wae, its speed, requency, and waelength λ are related to according to = λ (Equation 6.). We can sole this equation or the requency

More information

Chapter 1: Kinematics of Particles

Chapter 1: Kinematics of Particles Chapter 1: Kinematics of Particles 1.1 INTRODUCTION Mechanics the state of rest of motion of bodies subjected to the action of forces Static equilibrium of a body that is either at rest or moes with constant

More information

Physics 231 Lecture 28

Physics 231 Lecture 28 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:

More information

A. unchanged increased B. unchanged unchanged C. increased increased D. increased unchanged

A. unchanged increased B. unchanged unchanged C. increased increased D. increased unchanged IB PHYSICS Name: DEVIL PHYSICS Period: Date: BADDEST CLASS ON CAMPUS CHAPTER B TEST REVIEW. A rocket is fired ertically. At its highest point, it explodes. Which one of the following describes what happens

More information

The number of marks is given in brackets [ ] at the end of each question or part question. The total number of marks for this paper is 72.

The number of marks is given in brackets [ ] at the end of each question or part question. The total number of marks for this paper is 72. ADVANCED GCE UNIT 76/ MATHEMATICS (MEI Mechanics MONDAY MAY 7 Additional materials: Answer booklet (8 pages Graph paper MEI Examination Formulae and Tables (MF Morning Time: hour minutes INSTRUCTIONS TO

More information

PHYSICS (B) v 2 r. v r

PHYSICS (B) v 2 r. v r PHYSICS 1. If Q be the amount of liquid (iscosity ) flowing per second through a capillary tube of radius r and length l under a pressure difference P, then which of the following relation is correct?

More information

Each of the following questions (1-15) is worth 6 points

Each of the following questions (1-15) is worth 6 points Name: ----------------------------------------------- S. I. D.: ------------------------------------ Physics 0 Final Exam (Version A) Summer 06 HIS EXAM CONAINS 36 QUESIONS. ANSWERS ARE ROUNDED. PICK HE

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

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

SUPERPOSITION AND STANDING WAVES 16

SUPERPOSITION AND STANDING WAVES 16 SUPERPOSITION AND STANDING WAVES 6 Q6.. Reason: Where there is a change in ediu in particular a change in the wae speed then reflection can occur. Assess: Light traels at different speeds in water and

More information

Unit 11: Vectors in the Plane

Unit 11: Vectors in the Plane 135 Unit 11: Vectors in the Plane Vectors in the Plane The term ector is used to indicate a quantity (such as force or elocity) that has both length and direction. For instance, suppose a particle moes

More information

TRAVELING WAVES. Conceptual Questions v a v b v c. Wave speed is independent of wave amplitude (a)

TRAVELING WAVES. Conceptual Questions v a v b v c. Wave speed is independent of wave amplitude (a) TRAVELING WAVES 0 Conceptual Questions 0.1. a b c. Wae speed is independent o wae amplitude. 0.. (a) T T T 0 cm/s (b) 100 cm/s 4 T 4m (c) cm/s (d) so the speed is unchanged: 00 cm/s. /4 4L 0.3. The constant

More information

3. Use absolute value notation to write an inequality that represents the statement: x is within 3 units of 2 on the real line.

3. Use absolute value notation to write an inequality that represents the statement: x is within 3 units of 2 on the real line. PreCalculus Review Review Questions 1 The following transformations are applied in the given order) to the graph of y = x I Vertical Stretch by a factor of II Horizontal shift to the right by units III

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

Magnetic Fields Part 3: Electromagnetic Induction

Magnetic Fields Part 3: Electromagnetic Induction Magnetic Fields Part 3: Electromagnetic Induction Last modified: 15/12/2017 Contents Links Electromagnetic Induction Induced EMF Induced Current Induction & Magnetic Flux Magnetic Flux Change in Flux Faraday

More information

Chapter 9. Electromagnetic Waves

Chapter 9. Electromagnetic Waves Chapter 9. Electromagnetic Waves 9.1 Waves in One Dimension 9.1.1 The Wave Equation What is a "wave?" Let's start with the simple case: fixed shape, constant speed: How would you represent such a string

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

ONLINE: MATHEMATICS EXTENSION 2 Topic 6 MECHANICS 6.6 MOTION IN A CIRCLE

ONLINE: MATHEMATICS EXTENSION 2 Topic 6 MECHANICS 6.6 MOTION IN A CIRCLE ONLINE: MAHEMAICS EXENSION opic 6 MECHANICS 6.6 MOION IN A CICLE When a particle moes along a circular path (or cured path) its elocity must change een if its speed is constant, hence the particle must

More information

SOUND AND HEARING. = BkA and Bk is constant gives pmax1 / A1 = pmax2 / A2 p Pa p. = BkA and solve for A. fba. 10 Pa) (1480 m s) 10 Pa) (1000 Hz)

SOUND AND HEARING. = BkA and Bk is constant gives pmax1 / A1 = pmax2 / A2 p Pa p. = BkA and solve for A. fba. 10 Pa) (1480 m s) 10 Pa) (1000 Hz) OUND AND HEARING 6 6 IDENTIFY and ET UP: Eq() gies the waelength in terms o the requency Use Eq(6) to relate the pressure and displacement amplitudes EXECUTE: (a) λ = / = (44 m/s)/000 Hz = 044 m (b) p

More information

(a) Taking the derivative of the position vector with respect to time, we have, in SI units (m/s),

(a) Taking the derivative of the position vector with respect to time, we have, in SI units (m/s), Chapter 4 Student Solutions Manual. We apply Eq. 4- and Eq. 4-6. (a) Taking the deriatie of the position ector with respect to time, we hae, in SI units (m/s), d ˆ = (i + 4t ˆj + tk) ˆ = 8tˆj + k ˆ. dt

More information

By signing this exam you certify to adhere to the Cornell academic integrity code.

By signing this exam you certify to adhere to the Cornell academic integrity code. Page1of17 PHYS214 Prelim I October 6 1998 Name: Signature: Section # and TA: The exam is out of 100 points. INSTRUCTIONS By signing this exam you certify to adhere to the Cornell academic integrity code.

More information

Physics Kinematics: Projectile Motion. Science and Mathematics Education Research Group

Physics Kinematics: Projectile Motion. Science and Mathematics Education Research Group F FA ACULTY C U L T Y OF O F EDUCATION E D U C A T I O N Department of Curriculum and Pedagogy Physics Kinematics: Projectile Motion Science and Mathematics Education Research Group Supported by UBC Teaching

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

Doppler shifts in astronomy

Doppler shifts in astronomy 7.4 Doppler shift 253 Diide the transformation (3.4) by as follows: = g 1 bck. (Lorentz transformation) (7.43) Eliminate in the right-hand term with (41) and then inoke (42) to yield = g (1 b cos u). (7.44)

More information

Section 7.2 Addition and Subtraction Identities. In this section, we begin expanding our repertoire of trigonometric identities.

Section 7.2 Addition and Subtraction Identities. In this section, we begin expanding our repertoire of trigonometric identities. Section 7. Addition and Subtraction Identities 47 Section 7. Addition and Subtraction Identities In this section, we begin expanding our repertoire of trigonometric identities. Identities The sum and difference

More information

DYNAMICS. Kinematics of Particles Engineering Dynamics Lecture Note VECTOR MECHANICS FOR ENGINEERS: Eighth Edition CHAPTER

DYNAMICS. Kinematics of Particles Engineering Dynamics Lecture Note VECTOR MECHANICS FOR ENGINEERS: Eighth Edition CHAPTER 27 The McGraw-Hill Companies, Inc. All rights resered. Eighth E CHAPTER 11 VECTOR MECHANICS FOR ENGINEERS: DYNAMICS Ferdinand P. Beer E. Russell Johnston, Jr. Kinematics of Particles Lecture Notes: J.

More information

5.1: Graphing Sine and Cosine Functions

5.1: Graphing Sine and Cosine Functions 5.1: Graphing Sine and Cosine Functions Complete the table below ( we used increments of for the values of ) 4 0 sin 4 2 3 4 5 4 3 7 2 4 2 cos 1. Using the table, sketch the graph of y sin for 0 2 2. What

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

Residual migration in VTI media using anisotropy continuation

Residual migration in VTI media using anisotropy continuation Stanford Exploration Project, Report SERGEY, Noember 9, 2000, pages 671?? Residual migration in VTI media using anisotropy continuation Tariq Alkhalifah Sergey Fomel 1 ABSTRACT We introduce anisotropy

More information

Instructor Quick Check: Question Block 12

Instructor Quick Check: Question Block 12 Instructor Quick Check: Question Block 2 How to Administer the Quick Check: The Quick Check consists of two parts: an Instructor portion which includes solutions and a Student portion with problems for

More information

is a What you Hear The Pressure Wave sets the Ear Drum into Vibration.

is a What you Hear The Pressure Wave sets the Ear Drum into Vibration. is a What you Hear The ear converts sound energy to mechanical energy to a nerve impulse which is transmitted to the brain. The Pressure Wave sets the Ear Drum into Vibration. electroencephalogram v S

More information

Math 144 Activity #9 Introduction to Vectors

Math 144 Activity #9 Introduction to Vectors 144 p 1 Math 144 ctiity #9 Introduction to Vectors Often times you hear people use the words speed and elocity. Is there a difference between the two? If so, what is the difference? Discuss this with your

More information

MA 266 Review Topics - Exam # 2 (updated)

MA 266 Review Topics - Exam # 2 (updated) MA 66 Reiew Topics - Exam # updated Spring First Order Differential Equations Separable, st Order Linear, Homogeneous, Exact Second Order Linear Homogeneous with Equations Constant Coefficients The differential

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

REVIEW AND SYNTHESIS: CHAPTERS 9 12

REVIEW AND SYNTHESIS: CHAPTERS 9 12 REVIEW AND SYNTHESIS: CHAPTERS 9 Reiew Exercises. Strategy The magnitude of the buoyant force on an object in water is equal to the weight of the water displaced by the object. (a) Lead is much denser

More information

MCAT Physics - Problem Drill 06: Translational Motion

MCAT Physics - Problem Drill 06: Translational Motion MCAT Physics - Problem Drill 06: Translational Motion Question No. 1 of 10 Instructions: (1) Read the problem and answer choices carefully () Work the problems on paper as 1. An object falls from rest

More information

(a) During the first part of the motion, the displacement is x 1 = 40 km and the time interval is t 1 (30 km / h) (80 km) 40 km/h. t. (2.

(a) During the first part of the motion, the displacement is x 1 = 40 km and the time interval is t 1 (30 km / h) (80 km) 40 km/h. t. (2. Chapter 3. Since the trip consists of two parts, let the displacements during first and second parts of the motion be x and x, and the corresponding time interals be t and t, respectiely. Now, because

More information

Sound, Decibels, Doppler Effect

Sound, Decibels, Doppler Effect Phys Lectures 3, 33 Sound, Decibels, Doppler Eect Key points: ntensity o Sound: Decibels Doppler Eect Re: -,,7. Page Characteristics o Sound Sound can trael through any kind o matter, but not through a

More information

A-Level Mathematics TRIGONOMETRY. G. David Boswell - R2S Explore 2019

A-Level Mathematics TRIGONOMETRY. G. David Boswell - R2S Explore 2019 A-Level Mathematics TRIGONOMETRY G. David Boswell - R2S Explore 2019 1. Graphs the functions sin kx, cos kx, tan kx, where k R; In these forms, the value of k determines the periodicity of the trig functions.

More information

Conservation of Momentum in Two Dimensions

Conservation of Momentum in Two Dimensions Conseration of Momentum in Two Dimensions Name Section Linear momentum p is defined as the product of the mass of an object and its elocity. If there is no (or negligible) external force in a collision,

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

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

Honors Algebra 2 Chapter 14 Page 1

Honors Algebra 2 Chapter 14 Page 1 Section. (Introduction) Graphs of Trig Functions Objectives:. To graph basic trig functions using t-bar method. A. Sine and Cosecant. y = sinθ y y y y 0 --- --- 80 --- --- 30 0 0 300 5 35 5 35 60 50 0

More information

VISUAL PHYSICS ONLINE RECTLINEAR MOTION: UNIFORM ACCELERATION

VISUAL PHYSICS ONLINE RECTLINEAR MOTION: UNIFORM ACCELERATION VISUAL PHYSICS ONLINE RECTLINEAR MOTION: UNIFORM ACCELERATION Predict Obsere Explain Exercise 1 Take an A4 sheet of paper and a heay object (cricket ball, basketball, brick, book, etc). Predict what will

More information

Linear Momentum and Collisions Conservation of linear momentum

Linear Momentum and Collisions Conservation of linear momentum Unit 4 Linear omentum and Collisions 4.. Conseration of linear momentum 4. Collisions 4.3 Impulse 4.4 Coefficient of restitution (e) 4.. Conseration of linear momentum m m u u m = u = u m Before Collision

More information

1-D Kinematics Problems

1-D Kinematics Problems x (m) Name: AP Physics -D Kinemics Problems 5. Answer the following based on the elocity s. time graph. 6 8 4-4 -8 - straight cured 4 6 8 a. Gie a written description of the motion. t (s) Object moes in

More information

General Physics I Spring Oscillations

General Physics I Spring Oscillations General Physics I Spring 2011 Oscillations 1 Oscillations A quantity is said to exhibit oscillations if it varies with time about an equilibrium or reference value in a repetitive fashion. Oscillations

More information

Faculty of Computers and Information Fayoum University 2017/ 2018 Physics 2 (Waves)

Faculty of Computers and Information Fayoum University 2017/ 2018 Physics 2 (Waves) Faculty of Computers and Information Fayoum University 2017/ 2018 Physics 2 (Waves) 3/10/2018 1 Using these definitions, we see that Example : A sinusoidal wave traveling in the positive x direction has

More information

Transmission Line Transients

Transmission Line Transients 8 5 Transmission Line Transients CHAPTER OBJECTIES After reading this chapter, you should be able to: Proide an analysis of traelling waes on transmission lines Derie a wae equation Understand the effect

More information

42 TRAVELING WAVES (A) (B) (C) (D) (E) (F) (G)

42 TRAVELING WAVES (A) (B) (C) (D) (E) (F) (G) 42 TRAVELING WAVES 1. Wave progagation Source Disturbance Medium (D) Speed (E) Traveling waves (F) Mechanical waves (G) Electromagnetic waves (D) (E) (F) (G) 2. Transverse Waves have the classic sinusoidal

More information

Motion in Two and Three Dimensions

Motion in Two and Three Dimensions PH 1-1D Spring 013 Motion in Two and Three Dimensions Lectures 5,6,7 Chapter 4 (Halliday/Resnick/Walker, Fundamentals of Physics 9 th edition) 1 Chapter 4 Motion in Two and Three Dimensions In this chapter

More information

Physics 111. Help sessions meet Sunday, 6:30-7:30 pm in CLIR Wednesday, 8-9 pm in NSC 098/099

Physics 111. Help sessions meet Sunday, 6:30-7:30 pm in CLIR Wednesday, 8-9 pm in NSC 098/099 ics Announcements day, ember 7, 2007 Ch 2: graphing - elocity s time graphs - acceleration s time graphs motion diagrams - acceleration Free Fall Kinematic Equations Structured Approach to Problem Soling

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

Medical Imaging Physics Spring Quarter Week 3-2

Medical Imaging Physics Spring Quarter Week 3-2 Medical Imaging Physics Spring Quarter Week 3-2 Ultrasound Daor Balzar balzar@du.edu www.du.edu/~balzar Outline Ultrasound Light, Eyes and Vision Reading assignment: CSG 12; D 15 Homework D 12: 5,6 and

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

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

JURONG JUNIOR COLLEGE Physics Department Tutorial: Motion in a Circle

JURONG JUNIOR COLLEGE Physics Department Tutorial: Motion in a Circle JURONG JUNIOR COLLEGE Physics Department Tutorial: Motion in a Circle Angular elocity 1 (a) Define the radian. [1] (b) Explain what is meant by the term angular elocity. [1] (c) Gie the angular elocity

More information

Physics 2A Chapter 3 - Motion in Two Dimensions Fall 2017

Physics 2A Chapter 3 - Motion in Two Dimensions Fall 2017 These notes are seen pages. A quick summary: Projectile motion is simply horizontal motion at constant elocity with ertical motion at constant acceleration. An object moing in a circular path experiences

More information