Physics 41 Homework #2 Chapter 16. fa. Here v is the speed of the wave. 16. The speed of a wave on a massless string would be infinite!

Size: px
Start display at page:

Download "Physics 41 Homework #2 Chapter 16. fa. Here v is the speed of the wave. 16. The speed of a wave on a massless string would be infinite!"

Transcription

1 Physics 41 Hoewor # Chapter 1 Serway 7 th Conceptual: Q: 3,, 8, 11, 1, Probles P: 1, 3, 5, 9, 1, 5, 31, 35, 38, 4, 5, 57 Conceptual 3. (i) d=e, f, c, b, a (ii) Since, the saller the (the coefficient of x), the larger the wavelength. Thus, the ran according to wavelength is: d, a = b = c, e, f (iii) frequency: the larger oega (coefficient of t) the larger the frequency: f, e, d=b, a=c (iv) period is inverseley proportional to frequency so reverse (iii) (v) v Therefore the ratio of the t coefficient to the x coefficient gives the velocity: d, b = e, f, 3, 3. Higher tension aes wave speed higher. Greater linear density aes the wave ove ore slowly. va 8. Yes, aong other things it depends on. v ax A fa. Here v is the speed of the wave. 11. Each eleent of the rope ust support the weight of the rope below it. The tension increases T with height. (It increases linearly, if the rope does not stretch.) Then the wave speed v increases with height. 1. The speed of a wave on a assless string would be infinite! Probles P: 1, 3, 5, 9, 1, 5, 31, 35, 38, 4, 5, At t = 0, a transverse pulse in a wire is described by the function y x 3 where x and y are in eters. Write the function y(x, t) that describes this pulse if it is traveling in the positive x direction with a speed of 4.50 /s. P1.1 Replace x by x vt x 4.5 t (see plots) to get y x t Two points A and B on the surface of the Earth are at the sae longitude and 0.0 apart

2 in latitude. Suppose that an earthquae at point A creates a P wave that reaches point B by traveling straight through the body of the Earth at a constant speed of 7.80 /s. The earthquae also radiates a Rayleigh wave, which travels along the surface of the Earth in an analogous way to a surface wave on water, at 4.50 /s. (a) Which of these two seisic waves arrives at B first? What is the tie difference between the arrivals of the two waves at B? Tae the radius of the Earth to be 370. P1.3 (a) The longitudinal wave travels a shorter distance and is oving faster, so it will arrive at point B first. The transverse taes ore tie and carries ore energy! The wave that travels through the Earth ust travel a distance of R sin sin at a speed of Therefore, it taes /s s 817 s The wave that travels along the Earth s surface ust travel a distance of s R R rad at a speed of /s Therefore, it taes s The tie difference is 5 s 11.1 in 5. (a) Let u 10 t 3 x du dx at a point of constant phase 4 dt dt y dx 10 dt s The velocity is in the positive x -direction , sin c 4 (c) 3 : 0.7 f 10 : f 5.00 H z y vy cos 10 t 3 x t 4 (d) vy, ax s P1.9 y sin.11 x 3. t in SI units A.00 c

3 .11 rad rad s f 0.57 H z 3. v f s P1.1 (a) y () t = x () FIG. P1.1(a) 18.0 rad T s f 1.0 s f 1.0 s 75.4 rad s v f 1.0 s s (c) y A sin x t specializes to y 0.00 sin 18.0 x 75.4 ts sin at x 0, t 0 we require rad so yx, t 0.00 sin 18.0 x 75.4 t s rad 5. An astronaut on the Moon wishes to easure the local value of the free-fall acceleration by tiing pulses traveling down a wire that has an object of large ass suspended fro it. Assue a wire has a ass of 4.00 g and a length of 1.0, and that a 3.00-g object is suspended fro it. A pulse requires 3.1 s to traverse the length of the wire. Calculate gmoon fro these data. (You ay ignore the ass of the wire when calculating the tension in it.) T M g M gl L P1.5 T M g is the tension; v L t is the wave speed. M gl L Then, t 3 L g and g Mt g s 1.4 s

4 31. A steel wire and a 0.0- copper wire, both with diaeters, are connected end to end and stretched to a tension of 150 N. How long does it tae a transverse wave to travel the entire length of the two wires? P1.31 The total tie is the su of the two ties. L In each wire t L v T Let A represent the cross-sectional area of one wire. The ass of one wire can be written both as V AL and also as L. Then we have Thus, d t L 4T A d 4 1 For copper, t For steel, t s s 4150 The total tie is s 35. Sinusoidal waves 5.00 c in aplitude are to be transitted along a string that has a linear ass density of g/. If the source can deliver a axiu power of 300 W and the string is under a tension of 100 N, what is the highest frequency at which the source can operate? P1.35 A g Therefore, 1 P 300 W T 100 N P A v: T v 50.0 s 34 rad s f 55.1 H z P A v

5 38. The wave function for a wave on a taut string is y(x, t) = (0.350 )sin(10 t 3 x + /4) where x is in eters and t in seconds. (a) What is the average rate at which energy is transitted along the string if the linear ass density is 75.0 g/? What is the energy contained in each cycle of the wave? *P1.38 Coparing y 0.35sin 10t 3x 4 with y A sin x t A sin t x we 3 10 s have, 10 s, A Then v 3.33 s f f 3. (a) The rate of energy transport is P Av g 10 s s 15.1 W. The energy per cycle is E P T A g 10 s J. 4. *P1.4 The linear wave equation is Therefore, y 1 y x v t if b x vt y e y then bve b x vt y and be b xvt t x y b v e b xvt t y y v t x y and be b xvt x b, deonstrating that x vt e is a solution 5. Review proble. A bloc of ass M, supported by a string, rests on an incline aing an angle with the horizontal (Fig. P1.5). The length of the string is L and its ass is <<M. Derive an expression for the tie interval required for a transverse wave to travel fro one end of the string to the other. P1.5 Assuing the incline to be frictionless and taing the positive x-direction to be up the incline: F x T M g sin 0 or the tension in the string is T M gsin The speed of transverse waves in the string is then T M gsin v L M gl sin The tie interval for a pulse to travel the string s length is t L L L v M gl sin M gsin

Chapter 16 Solutions

Chapter 16 Solutions Chapter 16 Solutions 16.1 Replace x by x vt = x 4.5t to get y = 6 [(x 4.5t) + 3] 16. y (c) y (c) y (c) 6 4 4 4 t = s t = 1 s t = 1.5 s 0 6 10 14 x 0 6 10 14 x 0 6 10 14 x y (c) y (c) 4 t =.5 s 4 t = 3

More information

PHYS 102 Previous Exam Problems

PHYS 102 Previous Exam Problems PHYS 102 Previous Exa Probles CHAPTER 16 Waves Transverse waves on a string Power Interference of waves Standing waves Resonance on a string 1. The displaceent of a string carrying a traveling sinusoidal

More information

PH 221-2A Fall Waves - I. Lectures Chapter 16 (Halliday/Resnick/Walker, Fundamentals of Physics 9 th edition)

PH 221-2A Fall Waves - I. Lectures Chapter 16 (Halliday/Resnick/Walker, Fundamentals of Physics 9 th edition) PH 1-A Fall 014 Waves - I Lectures 4-5 Chapter 16 (Halliday/Resnick/Walker, Fundaentals of Physics 9 th edition) 1 Chapter 16 Waves I In this chapter we will start the discussion on wave phenoena. We will

More information

m A 1 m mgd k m v ( C) AP Physics Multiple Choice Practice Oscillations

m A 1 m mgd k m v ( C) AP Physics Multiple Choice Practice Oscillations P Physics Multiple Choice Practice Oscillations. ass, attached to a horizontal assless spring with spring constant, is set into siple haronic otion. Its axiu displaceent fro its equilibriu position is.

More information

Electromagnetic Waves

Electromagnetic Waves Electroagnetic Waves Physics 4 Maxwell s Equations Maxwell s equations suarize the relationships between electric and agnetic fields. A ajor consequence of these equations is that an accelerating charge

More information

Question 1. [14 Marks]

Question 1. [14 Marks] 6 Question 1. [14 Marks] R r T! A string is attached to the dru (radius r) of a spool (radius R) as shown in side and end views here. (A spool is device for storing string, thread etc.) A tension T is

More information

Physics 140 D100 Midterm Exam 2 Solutions 2017 Nov 10

Physics 140 D100 Midterm Exam 2 Solutions 2017 Nov 10 There are 10 ultiple choice questions. Select the correct answer for each one and ark it on the bubble for on the cover sheet. Each question has only one correct answer. (2 arks each) 1. An inertial reference

More information

F = 0. x o F = -k x o v = 0 F = 0. F = k x o v = 0 F = 0. x = 0 F = 0. F = -k x 1. PHYSICS 151 Notes for Online Lecture 2.4.

F = 0. x o F = -k x o v = 0 F = 0. F = k x o v = 0 F = 0. x = 0 F = 0. F = -k x 1. PHYSICS 151 Notes for Online Lecture 2.4. PHYSICS 151 Notes for Online Lecture.4 Springs, Strings, Pulleys, and Connected Objects Hook s Law F = 0 F = -k x 1 x = 0 x = x 1 Let s start with a horizontal spring, resting on a frictionless table.

More information

For a situation involving gravity near earth s surface, a = g = jg. Show. that for that case v 2 = v 0 2 g(y y 0 ).

For a situation involving gravity near earth s surface, a = g = jg. Show. that for that case v 2 = v 0 2 g(y y 0 ). Reading: Energy 1, 2. Key concepts: Scalar products, work, kinetic energy, work-energy theore; potential energy, total energy, conservation of echanical energy, equilibriu and turning points. 1.! In 1-D

More information

Physics 41 HW Set 1 Chapter 15 Serway 7 th Edition

Physics 41 HW Set 1 Chapter 15 Serway 7 th Edition Physics HW Set Chapter 5 Serway 7 th Edition Conceptual Questions:, 3, 5,, 6, 9 Q53 You can take φ = π, or equally well, φ = π At t= 0, the particle is at its turning point on the negative side of equilibriu,

More information

Simple Harmonic Motion

Simple Harmonic Motion Siple Haronic Motion Physics Enhanceent Prograe for Gifted Students The Hong Kong Acadey for Gifted Education and Departent of Physics, HKBU Departent of Physics Siple haronic otion In echanical physics,

More information

9 HOOKE S LAW AND SIMPLE HARMONIC MOTION

9 HOOKE S LAW AND SIMPLE HARMONIC MOTION Experient 9 HOOKE S LAW AND SIMPLE HARMONIC MOTION Objectives 1. Verify Hoo s law,. Measure the force constant of a spring, and 3. Measure the period of oscillation of a spring-ass syste and copare it

More information

Simple Harmonic Motion

Simple Harmonic Motion Reading: Chapter 15 Siple Haronic Motion Siple Haronic Motion Frequency f Period T T 1. f Siple haronic otion x ( t) x cos( t ). Aplitude x Phase Angular frequency Since the otion returns to its initial

More information

Lecture #8-3 Oscillations, Simple Harmonic Motion

Lecture #8-3 Oscillations, Simple Harmonic Motion Lecture #8-3 Oscillations Siple Haronic Motion So far we have considered two basic types of otion: translation and rotation. But these are not the only two types of otion we can observe in every day life.

More information

Periodic Motion is everywhere

Periodic Motion is everywhere Lecture 19 Goals: Chapter 14 Interrelate the physics and atheatics of oscillations. Draw and interpret oscillatory graphs. Learn the concepts of phase and phase constant. Understand and use energy conservation

More information

PHYS 1443 Section 003 Lecture #21 Wednesday, Nov. 19, 2003 Dr. Mystery Lecturer

PHYS 1443 Section 003 Lecture #21 Wednesday, Nov. 19, 2003 Dr. Mystery Lecturer PHYS 443 Section 003 Lecture # Wednesday, Nov. 9, 003 Dr. Mystery Lecturer. Fluid Dyanics : Flow rate and Continuity Equation. Bernoulli s Equation 3. Siple Haronic Motion 4. Siple Bloc-Spring Syste 5.

More information

Problem Set 14: Oscillations AP Physics C Supplementary Problems

Problem Set 14: Oscillations AP Physics C Supplementary Problems Proble Set 14: Oscillations AP Physics C Suppleentary Probles 1 An oscillator consists of a bloc of ass 050 g connected to a spring When set into oscillation with aplitude 35 c, it is observed to repeat

More information

In this chapter we will start the discussion on wave phenomena. We will study the following topics:

In this chapter we will start the discussion on wave phenomena. We will study the following topics: Chapter 16 Waves I In this chapter we will start the discussion on wave phenoena. We will study the following topics: Types of waves Aplitude, phase, frequency, period, propagation speed of a wave Mechanical

More information

which proves the motion is simple harmonic. Now A = a 2 + b 2 = =

which proves the motion is simple harmonic. Now A = a 2 + b 2 = = Worked out Exaples. The potential energy function for the force between two atos in a diatoic olecules can be expressed as follows: a U(x) = b x / x6 where a and b are positive constants and x is the distance

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

Physics 120 Final Examination

Physics 120 Final Examination Physics 120 Final Exaination 12 August, 1998 Nae Tie: 3 hours Signature Calculator and one forula sheet allowed Student nuber Show coplete solutions to questions 3 to 8. This exaination has 8 questions.

More information

Discussion Examples Chapter 13: Oscillations About Equilibrium

Discussion Examples Chapter 13: Oscillations About Equilibrium Discussion Exaples Chapter 13: Oscillations About Equilibriu 17. he position of a ass on a spring is given by x 6.5 c cos t 0.88 s. (a) What is the period,, of this otion? (b) Where is the ass at t 0.5

More information

Phys102 First Major-143 Zero Version Coordinator: xyz Sunday, June 28, 2015 Page: 1

Phys102 First Major-143 Zero Version Coordinator: xyz Sunday, June 28, 2015 Page: 1 Coordinator: xyz Sunday, June 28, 2015 Page: 1 Q1. A transverse sinusoidal wave propagating along a stretched string is described by the following equation: y (x,t) = 0.350 sin [1.25x + 99.6t], where x

More information

PH 221-1D Spring Oscillations. Lectures Chapter 15 (Halliday/Resnick/Walker, Fundamentals of Physics 9 th edition)

PH 221-1D Spring Oscillations. Lectures Chapter 15 (Halliday/Resnick/Walker, Fundamentals of Physics 9 th edition) PH 1-1D Spring 013 Oscillations Lectures 35-37 Chapter 15 (Halliday/Resnick/Walker, Fundaentals of Physics 9 th edition) 1 Chapter 15 Oscillations In this chapter we will cover the following topics: Displaceent,

More information

NAME NUMBER SEC. PHYCS 101 SUMMER 2001/2002 FINAL EXAME:24/8/2002. PART(I) 25% PART(II) 15% PART(III)/Lab 8% ( ) 2 Q2 Q3 Total 40%

NAME NUMBER SEC. PHYCS 101 SUMMER 2001/2002 FINAL EXAME:24/8/2002. PART(I) 25% PART(II) 15% PART(III)/Lab 8% ( ) 2 Q2 Q3 Total 40% NAME NUMER SEC. PHYCS 101 SUMMER 2001/2002 FINAL EXAME:24/8/2002 PART(I) 25% PART(II) 15% PART(III)/Lab 8% ( ) 2.5 Q1 ( ) 2 Q2 Q3 Total 40% Use the followings: Magnitude of acceleration due to gravity

More information

PHYSICS - CLUTCH CH 05: FRICTION, INCLINES, SYSTEMS.

PHYSICS - CLUTCH CH 05: FRICTION, INCLINES, SYSTEMS. !! www.clutchprep.co INTRO TO FRICTION Friction happens when two surfaces are in contact f = μ =. KINETIC FRICTION (v 0 *): STATIC FRICTION (v 0 *): - Happens when ANY object slides/skids/slips. * = Point

More information

m A 9. The length of a simple pendulum with a period on Earth of one second is most nearly (A) 0.12 m (B) 0.25 m (C) 0.50 m (D) 1.0 m (E) 10.

m A 9. The length of a simple pendulum with a period on Earth of one second is most nearly (A) 0.12 m (B) 0.25 m (C) 0.50 m (D) 1.0 m (E) 10. P Physics Multiple Choice Practice Oscillations. ass, attache to a horizontal assless spring with spring constant, is set into siple haronic otion. Its axiu isplaceent fro its equilibriu position is. What

More information

Systems of Masses. 1. Ignoring friction, calculate the acceleration of the system below and the tension in the rope. and (4.0)(9.80) 39.

Systems of Masses. 1. Ignoring friction, calculate the acceleration of the system below and the tension in the rope. and (4.0)(9.80) 39. Systes of Masses. Ignoring friction, calculate the acceleration of the syste below and the tension in the rope. Drawing individual free body diagras we get 4.0kg 7.0kg g 9.80 / s a?? g and g (4.0)(9.80)

More information

Physics 207 Lecture 18. Physics 207, Lecture 18, Nov. 3 Goals: Chapter 14

Physics 207 Lecture 18. Physics 207, Lecture 18, Nov. 3 Goals: Chapter 14 Physics 07, Lecture 18, Nov. 3 Goals: Chapter 14 Interrelate the physics and atheatics of oscillations. Draw and interpret oscillatory graphs. Learn the concepts of phase and phase constant. Understand

More information

Name Period. What force did your partner s exert on yours? Write your answer in the blank below:

Name Period. What force did your partner s exert on yours? Write your answer in the blank below: Nae Period Lesson 7: Newton s Third Law and Passive Forces 7.1 Experient: Newton s 3 rd Law Forces of Interaction (a) Tea up with a partner to hook two spring scales together to perfor the next experient:

More information

CHECKLIST. r r. Newton s Second Law. natural frequency ω o (rad.s -1 ) (Eq ) a03/p1/waves/waves doc 9:19 AM 29/03/05 1

CHECKLIST. r r. Newton s Second Law. natural frequency ω o (rad.s -1 ) (Eq ) a03/p1/waves/waves doc 9:19 AM 29/03/05 1 PHYS12 Physics 1 FUNDAMENTALS Module 3 OSCILLATIONS & WAVES Text Physics by Hecht Chapter 1 OSCILLATIONS Sections: 1.5 1.6 Exaples: 1.6 1.7 1.8 1.9 CHECKLIST Haronic otion, periodic otion, siple haronic

More information

Page 1. Physics 131: Lecture 22. Today s Agenda. SHM and Circles. Position

Page 1. Physics 131: Lecture 22. Today s Agenda. SHM and Circles. Position Physics 3: ecture Today s genda Siple haronic otion Deinition Period and requency Position, velocity, and acceleration Period o a ass on a spring Vertical spring Energy and siple haronic otion Energy o

More information

15 Newton s Laws #2: Kinds of Forces, Creating Free Body Diagrams

15 Newton s Laws #2: Kinds of Forces, Creating Free Body Diagrams Chapter 15 ewton s Laws #2: inds of s, Creating ree Body Diagras 15 ewton s Laws #2: inds of s, Creating ree Body Diagras re is no force of otion acting on an object. Once you have the force or forces

More information

27 Oscillations: Introduction, Mass on a Spring

27 Oscillations: Introduction, Mass on a Spring Chapter 7 Oscillations: Introduction, Mass on a Spring 7 Oscillations: Introduction, Mass on a Spring If a siple haronic oscillation proble does not involve the tie, you should probably be using conservation

More information

OSCILLATIONS AND WAVES

OSCILLATIONS AND WAVES OSCILLATIONS AND WAVES OSCILLATION IS AN EXAMPLE OF PERIODIC MOTION No stories this tie, we are going to get straight to the topic. We say that an event is Periodic in nature when it repeats itself in

More information

CE573 Structural Dynamics [Fall 2008]

CE573 Structural Dynamics [Fall 2008] CE573 Structural Dynaics [Fall 2008] 1) A rigid vehicle weighing 2000 lb, oving horizontally at a velocity of 12 ft/sec, is stopped by a barrier consisting of wire ropes stretched between two rigid anchors

More information

26 Impulse and Momentum

26 Impulse and Momentum 6 Ipulse and Moentu First, a Few More Words on Work and Energy, for Coparison Purposes Iagine a gigantic air hockey table with a whole bunch of pucks of various asses, none of which experiences any friction

More information

VIBRATING SYSTEMS. example. Springs obey Hooke s Law. Terminology. L 21 Vibration and Waves [ 2 ]

VIBRATING SYSTEMS. example. Springs obey Hooke s Law. Terminology. L 21 Vibration and Waves [ 2 ] L 1 Vibration and Waves [ ] Vibrations (oscillations) resonance pendulu springs haronic otion Waves echanical waves sound waves usical instruents VIBRATING SYSTEMS Mass and spring on air trac Mass hanging

More information

A body of unknown mass is attached to an ideal spring with force constant 123 N/m. It is found to vibrate with a frequency of

A body of unknown mass is attached to an ideal spring with force constant 123 N/m. It is found to vibrate with a frequency of Chapter 14 [ Edit ] Overview Suary View Diagnostics View Print View with Answers Chapter 14 Due: 11:59p on Sunday, Noveber 27, 2016 To understand how points are awarded, read the Grading Policy for this

More information

= T. Oscillations and Waves. Example of an Oscillating System IB 12 IB 12

= T. Oscillations and Waves. Example of an Oscillating System IB 12 IB 12 Oscillation: the vibration of an object Oscillations and Waves Eaple of an Oscillating Syste A ass oscillates on a horizontal spring without friction as shown below. At each position, analyze its displaceent,

More information

CHAPTER 15: Vibratory Motion

CHAPTER 15: Vibratory Motion CHAPTER 15: Vibratory Motion courtesy of Richard White courtesy of Richard White 2.) 1.) Two glaring observations can be ade fro the graphic on the previous slide: 1.) The PROJECTION of a point on a circle

More information

Flipping Physics Lecture Notes: Free Response Question #1 - AP Physics Exam Solutions

Flipping Physics Lecture Notes: Free Response Question #1 - AP Physics Exam Solutions 2015 FRQ #1 Free Response Question #1 - AP Physics 1-2015 Exa Solutions (a) First off, we know both blocks have a force of gravity acting downward on the. et s label the F & F. We also know there is a

More information

Chapter 4 FORCES AND NEWTON S LAWS OF MOTION PREVIEW QUICK REFERENCE. Important Terms

Chapter 4 FORCES AND NEWTON S LAWS OF MOTION PREVIEW QUICK REFERENCE. Important Terms Chapter 4 FORCES AND NEWTON S LAWS OF MOTION PREVIEW Dynaics is the study o the causes o otion, in particular, orces. A orce is a push or a pull. We arrange our knowledge o orces into three laws orulated

More information

NB1140: Physics 1A - Classical mechanics and Thermodynamics Problem set 2 - Forces and energy Week 2: November 2016

NB1140: Physics 1A - Classical mechanics and Thermodynamics Problem set 2 - Forces and energy Week 2: November 2016 NB1140: Physics 1A - Classical echanics and Therodynaics Proble set 2 - Forces and energy Week 2: 21-25 Noveber 2016 Proble 1. Why force is transitted uniforly through a assless string, a assless spring,

More information

Physics 2210 Fall smartphysics 20 Conservation of Angular Momentum 21 Simple Harmonic Motion 11/23/2015

Physics 2210 Fall smartphysics 20 Conservation of Angular Momentum 21 Simple Harmonic Motion 11/23/2015 Physics 2210 Fall 2015 sartphysics 20 Conservation of Angular Moentu 21 Siple Haronic Motion 11/23/2015 Exa 4: sartphysics units 14-20 Midter Exa 2: Day: Fri Dec. 04, 2015 Tie: regular class tie Section

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

Physics 18 Spring 2011 Homework 3 - Solutions Wednesday February 2, 2011

Physics 18 Spring 2011 Homework 3 - Solutions Wednesday February 2, 2011 Phsics 18 Spring 2011 Hoework 3 - s Wednesda Februar 2, 2011 Make sure our nae is on our hoework, and please bo our final answer. Because we will be giving partial credit, be sure to attept all the probles,

More information

Physics 41 HW Set 1 Chapter 15 Serway 8 th ( 7 th )

Physics 41 HW Set 1 Chapter 15 Serway 8 th ( 7 th ) Conceptual Q: 4 (7), 7 (), 8 (6) Physics 4 HW Set Chapter 5 Serway 8 th ( 7 th ) Q4(7) Answer (c). The equilibrium position is 5 cm below the starting point. The motion is symmetric about the equilibrium

More information

Antenna Theory Exam No. 1 October 9, 2000

Antenna Theory Exam No. 1 October 9, 2000 ntenna Theory Exa No. 1 October 9, 000 Solve the following 4 probles. Each proble is 0% of the grade. To receive full credit, you ust show all work. If you need to assue anything, state your assuptions

More information

5/09/06 PHYSICS 213 Exam #1 NAME FEYNMAN Please write down your name also on the back side of the last page

5/09/06 PHYSICS 213 Exam #1 NAME FEYNMAN Please write down your name also on the back side of the last page 5/09/06 PHYSICS 13 Exa #1 NAME FEYNMAN Please write down your nae also on the back side of the last page 1 he figure shows a horizontal planks of length =50 c, and ass M= 1 Kg, pivoted at one end. he planks

More information

Axis. Axis. Axis. Solid cylinder (or disk) about. Hoop about. Annular cylinder (or ring) about central axis. central axis.

Axis. Axis. Axis. Solid cylinder (or disk) about. Hoop about. Annular cylinder (or ring) about central axis. central axis. Instructor(s): Acosta, inzler PHYSICS DEPATMENT PHY 048, Spring 04 Final Exa March 4, 04 Nae (print, last first): Signature: On y honor, I have neither given nor received unauthorized aid on this exaination.

More information

Chapter 11 Simple Harmonic Motion

Chapter 11 Simple Harmonic Motion Chapter 11 Siple Haronic Motion "We are to adit no ore causes of natural things than such as are both true and sufficient to explain their appearances." Isaac Newton 11.1 Introduction to Periodic Motion

More information

Simple Harmonic Motion of Spring

Simple Harmonic Motion of Spring Nae P Physics Date iple Haronic Motion and prings Hooean pring W x U ( x iple Haronic Motion of pring. What are the two criteria for siple haronic otion? - Only restoring forces cause siple haronic otion.

More information

2009 Academic Challenge

2009 Academic Challenge 009 Acadeic Challenge PHYSICS TEST - REGIONAL This Test Consists of 5 Questions Physics Test Production Tea Len Stor, Eastern Illinois University Author/Tea Leader Doug Brandt, Eastern Illinois University

More information

Department of Physics Preliminary Exam January 3 6, 2006

Department of Physics Preliminary Exam January 3 6, 2006 Departent of Physics Preliinary Exa January 3 6, 2006 Day 1: Classical Mechanics Tuesday, January 3, 2006 9:00 a.. 12:00 p.. Instructions: 1. Write the answer to each question on a separate sheet of paper.

More information

Question number 1 to 8 carries 2 marks each, 9 to 16 carries 4 marks each and 17 to 18 carries 6 marks each.

Question number 1 to 8 carries 2 marks each, 9 to 16 carries 4 marks each and 17 to 18 carries 6 marks each. IIT-JEE5-PH-1 FIITJEE Solutions to IITJEE 5 Mains Paper Tie: hours Physics Note: Question nuber 1 to 8 carries arks each, 9 to 16 carries 4 arks each and 17 to 18 carries 6 arks each. Q1. whistling train

More information

α(t) = ω 2 θ (t) κ I ω = g L L g T = 2π mgh rot com I rot

α(t) = ω 2 θ (t) κ I ω = g L L g T = 2π mgh rot com I rot α(t) = ω 2 θ (t) ω = κ I ω = g L T = 2π L g ω = mgh rot com I rot T = 2π I rot mgh rot com Chapter 16: Waves Mechanical Waves Waves and particles Vibration = waves - Sound - medium vibrates - Surface ocean

More information

1 k. 1 m. m A. AP Physics Multiple Choice Practice Work-Energy

1 k. 1 m. m A. AP Physics Multiple Choice Practice Work-Energy AP Physics Multiple Choice Practice Wor-Energy 1. A ass attached to a horizontal assless spring with spring constant, is set into siple haronic otion. Its axiu displaceent fro its equilibriu position is

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

Ocean 420 Physical Processes in the Ocean Project 1: Hydrostatic Balance, Advection and Diffusion Answers

Ocean 420 Physical Processes in the Ocean Project 1: Hydrostatic Balance, Advection and Diffusion Answers Ocean 40 Physical Processes in the Ocean Project 1: Hydrostatic Balance, Advection and Diffusion Answers 1. Hydrostatic Balance a) Set all of the levels on one of the coluns to the lowest possible density.

More information

00 Elasticity Mechanical Properties of olids tress and train. When a weight of 0kg is suspended fro a copper wire of length 3 and diaeter 0.4. Its length increases by.4c. If the diaeter of the wire is

More information

Reading from Young & Freedman: For this topic, read the introduction to chapter 25 and sections 25.1 to 25.3 & 25.6.

Reading from Young & Freedman: For this topic, read the introduction to chapter 25 and sections 25.1 to 25.3 & 25.6. PHY10 Electricity Topic 6 (Lectures 9 & 10) Electric Current and Resistance n this topic, we will cover: 1) Current in a conductor ) Resistivity 3) Resistance 4) Oh s Law 5) The Drude Model of conduction

More information

Tutorial Exercises: Incorporating constraints

Tutorial Exercises: Incorporating constraints Tutorial Exercises: Incorporating constraints 1. A siple pendulu of length l ass is suspended fro a pivot of ass M that is free to slide on a frictionless wire frae in the shape of a parabola y = ax. The

More information

Q1. The displacement of a string carrying a traveling sinusoidal wave is given by:

Q1. The displacement of a string carrying a traveling sinusoidal wave is given by: Coordinator: A. Mekki Saturday, Noveber, 008 Page: 1 Q1. The displaceent of a string carrying a traveling sinusoidal wave is given by: y( x, t) = y sin( kx ω t + ϕ). At tie t = 0 the point at x = 0 has

More information

T m. Fapplied. Thur Oct 29. ω = 2πf f = (ω/2π) T = 1/f. k m. ω =

T m. Fapplied. Thur Oct 29. ω = 2πf f = (ω/2π) T = 1/f. k m. ω = Thur Oct 9 Assignent 10 Mass-Spring Kineatics (x, v, a, t) Dynaics (F,, a) Tie dependence Energy Pendulu Daping and Resonances x Acos( ωt) = v = Aω sin( ωt) a = Aω cos( ωt) ω = spring k f spring = 1 k

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

UNIVERSITY OF SASKATCHEWAN Department of Physics and Engineering Physics

UNIVERSITY OF SASKATCHEWAN Department of Physics and Engineering Physics UNIVERSITY OF SASKATCHEWAN Departent of Physics and Engineering Physics 017 Saskatchewan High School Physics Scholarship Copetition Wednesday May 10, 017 Tie allowed: 90 inutes This copetition is based

More information

Monitoring and system identification of suspension bridges: An alternative approach

Monitoring and system identification of suspension bridges: An alternative approach Monitoring and syste identification of suspension bridges: An alternative approach Erdal Şafak Boğaziçi University, Kandilli Observatory and Earthquake Reseach Institute, Istanbul, Turkey Abstract This

More information

Q5 We know that a mass at the end of a spring when displaced will perform simple m harmonic oscillations with a period given by T = 2!

Q5 We know that a mass at the end of a spring when displaced will perform simple m harmonic oscillations with a period given by T = 2! Chapter 4.1 Q1 n oscillation is any otion in which the displaceent of a particle fro a fixed point keeps changing direction and there is a periodicity in the otion i.e. the otion repeats in soe way. In

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

Faraday's Law Warm Up

Faraday's Law Warm Up Faraday's Law-1 Faraday's Law War Up 1. Field lines of a peranent agnet For each peranent agnet in the diagra below draw several agnetic field lines (or a agnetic vector field if you prefer) corresponding

More information

PHYS 1443 Section 003 Lecture #22

PHYS 1443 Section 003 Lecture #22 PHYS 443 Section 003 Lecture # Monda, Nov. 4, 003. Siple Bloc-Spring Sste. Energ of the Siple Haronic Oscillator 3. Pendulu Siple Pendulu Phsical Pendulu orsion Pendulu 4. Siple Haronic Motion and Unifor

More information

WileyPLUS Assignment 3. Next Week

WileyPLUS Assignment 3. Next Week WileyPLUS Assignent 3 Chapters 6 & 7 Due Wednesday, Noveber 11 at 11 p Next Wee No labs of tutorials Reebrance Day holiday on Wednesday (no classes) 24 Displaceent, x Mass on a spring ωt = 2π x = A cos

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

Phys102 First Major-112 Zero Version Coordinator: Wednesday, March 07, 2012 Page: 1

Phys102 First Major-112 Zero Version Coordinator: Wednesday, March 07, 2012 Page: 1 Coordinator: Wednesday, March 07, 01 Page: 1 Q1. A transverse sinusoidal wave, travelling in the positive x direction along a string, has an aplitude of 0 c. The transverse position of an eleent of the

More information

ROTATIONAL MOTION FROM TRANSLATIONAL MOTION

ROTATIONAL MOTION FROM TRANSLATIONAL MOTION ROTATIONAL MOTION FROM TRANSLATIONAL MOTION Velocity Acceleration 1-D otion 3-D otion Linear oentu TO We have shown that, the translational otion of a acroscopic object is equivalent to the translational

More information

(Newton s 2 nd Law for linear motion)

(Newton s 2 nd Law for linear motion) PHYSICS 3 Final Exaination ( Deeber Tie liit 3 hours Answer all 6 questions You and an assistant are holding the (opposite ends of a long plank when oops! the butterfingered assistant drops his end If

More information

1B If the stick is pivoted about point P a distance h = 10 cm from the center of mass, the period of oscillation is equal to (in seconds)

1B If the stick is pivoted about point P a distance h = 10 cm from the center of mass, the period of oscillation is equal to (in seconds) 05/07/03 HYSICS 3 Exa #1 Use g 10 /s in your calculations. NAME Feynan lease write your nae also on the back side of this exa 1. 1A A unifor thin stick of ass M 0. Kg and length 60 c is pivoted at one

More information

9. h = R. 10. h = 3 R

9. h = R. 10. h = 3 R Version PREVIEW Torque Chap. 8 sizeore (13756) 1 This print-out should have 3 questions. ultiple-choice questions ay continue on the next colun or page find all choices before answering. Note in the dropped

More information

UNIVERSITY OF SASKATCHEWAN Department of Physics and Engineering Physics

UNIVERSITY OF SASKATCHEWAN Department of Physics and Engineering Physics UNIVERSITY OF SASKATCHEWAN Departent of Physics and Engineering Physics 05 Saskatchewan High School Physics Scholarship Copetition May, 05 Tie allowed: 90 inutes This copetition is based on the Saskatchewan

More information

Quiz 5 PRACTICE--Ch12.1, 13.1, 14.1

Quiz 5 PRACTICE--Ch12.1, 13.1, 14.1 Nae: Class: Date: ID: A Quiz 5 PRACTICE--Ch2., 3., 4. Multiple Choice Identify the choice that best copletes the stateent or answers the question.. A bea of light in air is incident at an angle of 35 to

More information

CHAPTER 1 MOTION & MOMENTUM

CHAPTER 1 MOTION & MOMENTUM CHAPTER 1 MOTION & MOMENTUM SECTION 1 WHAT IS MOTION? All atter is constantly in MOTION Motion involves a CHANGE in position. An object changes position relative to a REFERENCE POINT. DISTANCE is the total

More information

Chapter 5, Conceptual Questions

Chapter 5, Conceptual Questions Chapter 5, Conceptual Questions 5.1. Two forces are present, tension T in the cable and gravitational force 5.. F G as seen in the figure. Four forces act on the block: the push of the spring F, sp gravitational

More information

L 2. AP Physics Free Response Practice Oscillations ANSWERS 1975B7. (a) F T2. (b) F NET(Y) = 0

L 2. AP Physics Free Response Practice Oscillations ANSWERS 1975B7. (a) F T2. (b) F NET(Y) = 0 AP Physics Free Response Practice Oscillations ANSWERS 1975B7. (a) 60 F 1 F g (b) F NE(Y) = 0 F1 F1 = g / cos(60) = g (c) When the string is cut it swings fro top to botto, siilar to the diagra for 1974B1

More information

Waves Solutions to the Wave Equation Sine Waves Transverse Speed and Acceleration

Waves Solutions to the Wave Equation Sine Waves Transverse Speed and Acceleration Waves Solutions to the Wave Equation Sine Waves Transverse Speed and Acceleration Lana Sheridan De Anza College May 17, 2018 Last time pulse propagation the wave equation Overview solutions to the wave

More information

PY241 Solutions Set 9 (Dated: November 7, 2002)

PY241 Solutions Set 9 (Dated: November 7, 2002) PY241 Solutions Set 9 (Dated: Noveber 7, 2002) 9-9 At what displaceent of an object undergoing siple haronic otion is the agnitude greatest for the... (a) velocity? The velocity is greatest at x = 0, the

More information

FOUNDATION STUDIES EXAMINATIONS January 2016

FOUNDATION STUDIES EXAMINATIONS January 2016 1 FOUNDATION STUDIES EXAMINATIONS January 2016 PHYSICS Seester 2 Exa July Fast Track Tie allowed 2 hours for writing 10 inutes for reading This paper consists of 4 questions printed on 11 pages. PLEASE

More information

PH 221-3A Fall Waves - II. Lectures Chapter 17 (Halliday/Resnick/Walker, Fundamentals of Physics 8 th edition)

PH 221-3A Fall Waves - II. Lectures Chapter 17 (Halliday/Resnick/Walker, Fundamentals of Physics 8 th edition) PH 221-3A Fall 2010 Waves - II Lectures 27-28 Chapter 17 (Halliday/Resnick/Walker, Fundaentals of Physics 8 th edition) 1 Chapter 17 Waves II In this chapter we will study sound waves and concentrate on

More information

Course Information. Physics 1C Waves, optics and modern physics. Grades. Class Schedule. Clickers. Homework

Course Information. Physics 1C Waves, optics and modern physics. Grades. Class Schedule. Clickers. Homework Course Inforation Physics 1C Waves, optics and odern physics Instructor: Melvin Oaura eail: oaura@physics.ucsd.edu Course Syllabus on the web page http://physics.ucsd.edu/ students/courses/fall2009/physics1c

More information

In this chapter we will study sound waves and concentrate on the following topics:

In this chapter we will study sound waves and concentrate on the following topics: Chapter 17 Waves II In this chapter we will study sound waves and concentrate on the following topics: Speed of sound waves Relation between displaceent and pressure aplitude Interference of sound waves

More information

Equilibrium & Elasticity

Equilibrium & Elasticity PHYS 101 Previous Exam Problems CHAPTER 12 Equilibrium & Elasticity Static equilibrium Elasticity 1. A uniform steel bar of length 3.0 m and weight 20 N rests on two supports (A and B) at its ends. A block

More information

National 5 Summary Notes

National 5 Summary Notes North Berwick High School Departent of Physics National 5 Suary Notes Unit 3 Energy National 5 Physics: Electricity and Energy 1 Throughout the Course, appropriate attention should be given to units, prefixes

More information

SRI LANKAN PHYSICS OLYMPIAD MULTIPLE CHOICE TEST 30 QUESTIONS ONE HOUR AND 15 MINUTES

SRI LANKAN PHYSICS OLYMPIAD MULTIPLE CHOICE TEST 30 QUESTIONS ONE HOUR AND 15 MINUTES SRI LANKAN PHYSICS OLYMPIAD - 5 MULTIPLE CHOICE TEST QUESTIONS ONE HOUR AND 5 MINUTES INSTRUCTIONS This test contains ultiple choice questions. Your answer to each question ust be arked on the answer sheet

More information

EN40: Dynamics and Vibrations. Midterm Examination Tuesday March

EN40: Dynamics and Vibrations. Midterm Examination Tuesday March EN4: Dynaics and ibrations Midter Exaination Tuesday Marc 4 14 Scool of Engineering Brown University NAME: General Instructions No collaboration of any kind is peritted on tis exaination. You ay bring

More information

Q1. For a given medium, the wavelength of a wave is:

Q1. For a given medium, the wavelength of a wave is: Phys10 First Major-091 Zero Version Coordinator: M Sunday, Noveber 15, 009 Page: 1 Q1. For a given ediu, the wavelength of a wave is: A) inversely proportional to the frequency B) independent of the frequency

More information

The Lagrangian Method vs. other methods (COMPARATIVE EXAMPLE)

The Lagrangian Method vs. other methods (COMPARATIVE EXAMPLE) The Lagrangian ethod vs. other ethods () This aterial written by Jozef HANC, jozef.hanc@tuke.sk Technical University, Kosice, Slovakia For Edwin Taylor s website http://www.eftaylor.co/ 6 January 003 The

More information

Chem/Biochem 471 Exam 3 12/18/08 Page 1 of 7 Name:

Chem/Biochem 471 Exam 3 12/18/08 Page 1 of 7 Name: Che/Bioche 47 Exa /8/08 Pae of 7 Please leave the exa paes stapled toether. The forulas are on a separate sheet. This exa has 5 questions. You ust answer at least 4 of the questions. You ay answer ore

More information

Definition of Work, The basics

Definition of Work, The basics Physics 07 Lecture 16 Lecture 16 Chapter 11 (Work) v Eploy conservative and non-conservative forces v Relate force to potential energy v Use the concept of power (i.e., energy per tie) Chapter 1 v Define

More information

MECHANICS of FLUIDS INSTRUCTOR'S SOLUTIONS MANUAL TO ACCOMPANY FOURTH EDITION. MERLE C. POTTER Michigan State University DAVID C.

MECHANICS of FLUIDS INSTRUCTOR'S SOLUTIONS MANUAL TO ACCOMPANY FOURTH EDITION. MERLE C. POTTER Michigan State University DAVID C. INSTRUCTOR'S SOLUTIONS MANUAL TO ACCOMPANY MECHANICS of FLUIDS FOURTH EDITION MERLE C. POTTER Michigan State University DAVID C. WIGGERT Michigan State University BASSEM RAMADAN Kettering University Contents

More information

PHYSICS 2210 Fall Exam 4 Review 12/02/2015

PHYSICS 2210 Fall Exam 4 Review 12/02/2015 PHYSICS 10 Fall 015 Exa 4 Review 1/0/015 (yf09-049) A thin, light wire is wrapped around the ri of a unifor disk of radius R=0.80, as shown. The disk rotates without friction about a stationary horizontal

More information