SIMPLE HARMONIC MOTION PREVIOUS EAMCET QUESTIONS ENGINEERING. the mass of the particle is 2 gms, the kinetic energy of the particle when t =

Size: px
Start display at page:

Download "SIMPLE HARMONIC MOTION PREVIOUS EAMCET QUESTIONS ENGINEERING. the mass of the particle is 2 gms, the kinetic energy of the particle when t ="

Transcription

1 SIMPLE HRMONIC MOION PREVIOUS EMCE QUESIONS ENGINEERING. he displacement of a particle executin SHM is iven by :y = 5 sin 4t +. If is the time period and 3 the mass of the particle is ms, the kinetic enery of the particle when t = 4 is iven by π ns : 4 [009 E] ) 0.4 Joules ) 0.5 Joules 3) 3 Joules 4) 0.3 Joules π Sol: he iven equation is y = 5sin 4t+ 3 () comparin with the equation y = sin ( ωt+ φ ) From the equation, π π π = = = s ω 4 π π When t =, y = 5sin ω = 4rads π = 5cos =.5m 3 KE.. = mω y = 0 3 ( 4 ) ( 5 ) (.5 ) = 0.3 J. particle is executin simple harmonic motion with an amplitude and time period. he displacement of the particle after period from its initial position is : [008 E] ) ) 4 3) 8 4) Zero ns : 4 Sol: fter a time period of or interal multiples of the particle comes to mean position. Hence displacement is zero. 3. he manitude of imum acceleration is times that of imum velocity of a simple harmonic oscillator. he time period of the oscillator in seconds is (007 E) ) 4 ) 3) 4) 0.5 ns : Sol: a = ω.() v = ω..() a = πv [iven ] = ( ) ω π ω ω = π = π π s ω = π =

2 4. he time period of a simple pendulum is. When the lenth is increased by 0cm, the period is. When the lenth is decreased by 0cm, its period is. hen relation between,, is ) = + ) = 3) = + 4) = Sol: he time period of a simple pendulum is l = π () When the lenth increases by 0cm then l + 0 = π () When the lenth decreases by 0cm then π l 0 = (3) Squarin () & (3) and addin l 0 l = π l = 4π = + = (004 E) 5. When a body of mass.0 k is suspended from a certain liht sprin hanin vertically, its lenth increases by 5cm. By suspendin.0 k block to the sprin and if the block is pulled throuh 0cm and released, the imum velocity of it in m/s is (cceleration due to ravity = 0 m/s ) (003E) ) 0.5 ) 3) 4) 4 Sol: Force = m = kx where k is force constant m k = = 00Nm x From law of conservation of enery kx = mv ( ) kx 00 0 V = = = m V = ms 6. body of mass m is suspended to an ideal sprin of force constant k. he expected chane in the position of the body due to an additional force F actin vertically downwards is : (005 E)

3 ) 3F k ) F k 3) 5F k 4) 4F k ns : Sol: If F is the force actin and K is the force constant. Let the chane in position of the body due to addition force is x. So F = kx F x = k 7. n object is attached to the bottom of a liht vertical sprin and set vibratin. he imum speed of the object is 5 cm/sec and the period is 68 milli seconds. he amplitude of the motion in centimeters is (003 E) ) 3.0 ).0 3).5 4).0 Sol: Given V = 5cms = 5 0 ms = s = 68 ms π V = = ω = = 5 0 m 3 =.5 cm 8. body executes S.H.M. under the action of a force F with a time period 4/5 seconds. If the force is chaned to F it executes S.H.M. with time period 3/5 seconds. If both the forces F and F act simultaneous in the same direction on the body. Its time period in seconds is (00 E) ) /5 ) 4/5 3) 5/4 4) 5/ π 4π mr Sol: Force F = mrω = mr = s the two forces are actin simultaneously Resultant force = F = F+ F = + [ Since m & r are constants) = = + = = s 6 9 5

4 9. If the displacement (x) and velocity (v) of a particle executin S.H.M. are related throuh the expression 4v = 5 - x then its time period is (00 E) ) π ) π 3) 4 π 4) 6 π Sol: Give expression is 4V = 5 x () Dividin equation () by 4 5 x V = V = x () Comparin () with V = ω x π ω = = = 4π s 0. wo particles P and Q start from oriin and execute S.H.M. alon x-axis with same amplitude but with periods 3 seconds and 6 seconds respectively. he ratio of the velocities of P and Q when they are at mean position is (00 E) ) : ) : 3) : 3 4) 3 : ns : Sol: Velocity of a particle executin S.H.M. V = ω y π π But ω = V = y s V V 6 V = = V : V = : 3. body is executin S.H.M. at a displacement x its P.E. is E and at a displacement y its P.E is E. he P.E at displacement (x+y) is ) E = E E ) E = E + E 3) E = E+ E 4) E = E E (00 E) Sol: he potential enery stored in a body E = kx K E = kx E =. x.() K E = ky E =. y.() Potential enery (E) at displacement (x+y) = ( ) k x+ y

5 From (), () and (3) k E = ( x+ y)...(3) k k k ( x + y) = ( x) + ( y) E = E + E. body of mass k executin S.H.M., its displacement y cm at t seconds is iven by y=6sin (00t + π /4). Its imum kinetic enery is (000 E) ) 6J ) 8J 3) 4J 4) 36J ns : Sol: Comparin the iven equation with y = sin ( ωt+ φ) π We et = 6 0 m, ω = 00 rads -, φ = 4 rad ( ) ( ) ( ) KE = mω = = 8 J 3. particle executin S.H.M. has an amplitude of 6 cm. Its acceleration at a distance of cm from the mean position is 8cm/s. he imum speed of particle is (000E) ) 8cm/s ) cm/s 3) 6 cm/s 4)4cm/s ns : a = ω y 8= ω Sol: ( ) ω = 4 ω = rads V = ω = 6 = cms MEDICL 4. simple pendulum is executin SHM with a period of 6sec between two extreme positions B and C about a point O. If the lenth of the arc BC is 0cm. how lon will the pendulum take the move from position C to a position D towards O exactly midway between C and O [009 M] ) 0.5sec ) sec 3).5 sec 4) 3 sec ns : Sol: ime period = s mplitude = 5 cm π he equation of SHM is y = sin t π = sin t π π sin = sin 6 6 t t = s 5. irl swins on a cradle in sittin position. If she stands, the time period of cradle [008 M]

6 ) decreases ) increases 3) remains constant 4) first increases then it remains constant ns : Sol: s the lenth of the pendulum decreases time period also decreases 6. he displacement of a particle of mass 3 m executin simple harmonic motion is iven by y = 3sin(0.t) in SI units. he kinetic enery of the particle at a point which is at a distance equal to of its amplitude from its mean position is (007 M) ) x 0 3 J ) 5 x 0 3 J 3) 0.48 x 0 3 J 4) 0.4 x 0 3 J ns : Sol: Given equation is y=3sin(0.t) comparin with standard equation y = sin ( ωt) 3 = 3 m, ω =0., m= 3 0 k KE. = mω ( x ) = ( 0. ) ( 3 ) 3 = J π 7. he simple harmonic motion of a particle is represented by the equation x = 4cos 88t+ 4. he ns : frequency (in Hz) and the initial displacement (in m) of the particle are (006 M) ) 4, ) 6, 3) 4,3 4) 6,3 Sol: Comparin the iven equation with x= cos( ωt+ φ ) i) ω t = 88t ω = 88 π n= 88 n= 4Hz ii) Initial displacement [t=0] π 4 x = 4cos = = 4 8. body executin S.H.M. has a imum velocity of and a imum acceleration of 4. Its amplitude in metres is (005 M) ) ) ) 0.5 J 4) 0.5 ns : 4 Sol: V ω =, a = ω V a ω () ω = = = = 0.5m 4 9. he equation of motion of particle executin SHM is a+ 6π x = 0. In this equation a is the linear acceleration in m/s, of the particle at a displacement x in meters. he time period of SHM, in seconds is (004 E) ) /4 ) / 3) 4) ns :

7 Sol: Given that 6π x 0 a+ = a= 6π x -ve sin indicates that acceleration and displacement are opposite in directions displacement ime period = π acceleration = π 6 = s π 0. he time period of a particle in simple harmonic motion is 8 seconds. t t = 0 it is at the mean position. he ratio of the distances travelled by it is the first and second seconds is: (003 M) ) ) 3) 4) 3 Sol: he equation of a particle executin S.H.M is y = sinωt distance traveled in s π y = sin = = S 8 π Distance traveled in seconds = y = sin = 8 S = Distance traveled in nd second = y - y = = S S = = /. he mass and diameter of a planet are two times those of earth. If a seconds pendulum is taken to it, the ns : 4 Sol: time period of the pendulum in seconds is (00 M) ) ) / 3) 4) We known that GM = R p M p R E = E M E R p

8 M E R E = = ME RE We know that time period of simple pendulum = l/ π = P E E p P = = s P. If two bodies of same mass are executin S.H.M. with frequencies in the ratio : and amplitudes in the ratio :3 then the ratio of their total eneries is (00M) ) : 3 ) : 9 3) : 4 4) : 6 ns : mω = ( ) m π n E n = = = E n 3 9 Sol: E = otal enery of a body executin SHM = 3. he time period of a liht loaded sprin is 3.5 seconds. On chanin the load by k, the period decreases by 0.5 seconds. he initial load on the sprin is (00 M) ) 3 (0/3) k ) 4 (0/3) k 3) 5 (0/3) k 4) 6 (0/3) k ns : m π k m = m 3.5 m = 3 m 0 On simplifyin m= 3 k 3 Sol: he time period of a mass loaded sprin = = 4. particle is executin simple harmonic motion with an amplitude of 4cm. t the mean position the velocity of the particle is 0 cm/s. he distance of the particle from the mean position when its speed becomes 5cm/s is (000 M) ) 3 cm ) 5 cm 3) 3cm 4) 5cm Sol: mplitude = 4 cm Maximum velocity V = 0cm/sec But V = aω

9 V 0 ω = = =.5rads a 4 Velocity V = ω a y 5 5= 6 y y = 3cm 5. particle executes simple harmonic motion with a period of s and amplitude m. he shortest time it takes to reach point ) ) 4 Sol: ime period = sec m from its mean position in seconds is (000 M) mplitude = metre Displacement = 3) 8 metre 4) 6

10 We know y = asinω t π = sin t 0 π sin 45 = sin t t = sec 8

OSCILLATIONS

OSCILLATIONS OSCIAIONS Important Points:. Simple Harmonic Motion: a) he acceleration is directly proportional to the displacement of the body from the fixed point and it is always directed towards the fixed point in

More information

f 1. (8.1.1) This means that SI unit for frequency is going to be s 1 also known as Hertz d1hz

f 1. (8.1.1) This means that SI unit for frequency is going to be s 1 also known as Hertz d1hz ecture 8-1 Oscillations 1. Oscillations Simple Harmonic Motion So far we have considered two basic types of motion: translational motion and rotational motion. But these are not the only types of motion

More information

Equations. A body executing simple harmonic motion has maximum acceleration ) At the mean positions ) At the two extreme position 3) At any position 4) he question is irrelevant. A particle moves on the

More information

Chapter 15 Oscillations

Chapter 15 Oscillations Chapter 5 Oscillations Any motion or event that repeats itself at reular intervals is said to be periodic. Oscillation: n eneral, an oscillation is a periodic fluctuation in the value of a physical quantity

More information

Oscillations Equations 0. Out of the followin functions representin otion of a particle which represents SHM I) y = sinωt cosωt 3 II) y = sin ωt III) IV) 3 y = 5cos 3ωt 4 y = + ωt+ ω t a) Only IV does

More information

Chapter 13 Oscillations about Equilibrium. Copyright 2010 Pearson Education, Inc.

Chapter 13 Oscillations about Equilibrium. Copyright 2010 Pearson Education, Inc. Chapter 13 Oscillations about Equilibrium Periodic Motion Units of Chapter 13 Simple Harmonic Motion Connections between Uniform Circular Motion and Simple Harmonic Motion The Period of a Mass on a Spring

More information

ONLINE: MATHEMATICS EXTENSION 2 Topic 6 MECHANICS 6.3 HARMONIC MOTION

ONLINE: MATHEMATICS EXTENSION 2 Topic 6 MECHANICS 6.3 HARMONIC MOTION ONINE: MATHEMATICS EXTENSION Topic 6 MECHANICS 6.3 HARMONIC MOTION Vibrations or oscillations are motions that repeated more or less reularly in time. The topic is very broad and diverse and covers phenomena

More information

Oscillations. PHYS 101 Previous Exam Problems CHAPTER. Simple harmonic motion Mass-spring system Energy in SHM Pendulums

Oscillations. PHYS 101 Previous Exam Problems CHAPTER. Simple harmonic motion Mass-spring system Energy in SHM Pendulums PHYS 101 Previous Exam Problems CHAPTER 15 Oscillations Simple harmonic motion Mass-spring system Energy in SHM Pendulums 1. The displacement of a particle oscillating along the x axis is given as a function

More information

spring mass equilibrium position +v max

spring mass equilibrium position +v max Lecture 20 Oscillations (Chapter 11) Review of Simple Harmonic Motion Parameters Graphical Representation of SHM Review of mass-spring pendulum periods Let s review Simple Harmonic Motion. Recall we used

More information

Chapter 14 (Oscillations) Key concept: Downloaded from

Chapter 14 (Oscillations) Key concept: Downloaded from Chapter 14 (Oscillations) Multiple Choice Questions Single Correct Answer Type Q1. The displacement of a particle is represented by the equation. The motion of the particle is (a) simple harmonic with

More information

g L Simple Pendulum, cont Simple Pendulum Period of Simple Pendulum Equations of Motion for SHM: 4/8/16 k m

g L Simple Pendulum, cont Simple Pendulum Period of Simple Pendulum Equations of Motion for SHM: 4/8/16 k m Simple Pendulum The simple pendulum is another example of simple harmonic motion The force is the component of the weiht tanent to the path of motion F t = - m sin θ Simple Pendulum, cont In eneral, the

More information

CHAPTER 12 OSCILLATORY MOTION

CHAPTER 12 OSCILLATORY MOTION CHAPTER 1 OSCILLATORY MOTION Before starting the discussion of the chapter s concepts it is worth to define some terms we will use frequently in this chapter: 1. The period of the motion, T, is the time

More information

Chapter K. Oscillatory Motion. Blinn College - Physics Terry Honan. Interactive Figure

Chapter K. Oscillatory Motion. Blinn College - Physics Terry Honan. Interactive Figure K. - Simple Harmonic Motion Chapter K Oscillatory Motion Blinn Collee - Physics 2425 - Terry Honan The Mass-Sprin System Interactive Fiure Consider a mass slidin without friction on a horizontal surface.

More information

1. Dimensions of force constant are (MHT-CET-2003) (a) M 1 L 0 T 2 (b) M 1 L 0 T 2. (c) M 0 L 1 T 2 (d) MLT 2

1. Dimensions of force constant are (MHT-CET-2003) (a) M 1 L 0 T 2 (b) M 1 L 0 T 2. (c) M 0 L 1 T 2 (d) MLT 2 1. Dimensions of force constant are (MHT-CET-2003) M 1 L 0 T 2 M 1 L 0 T 2 M 0 L 1 T 2 MLT 2 2. A bar magnet is in oscillatory motion its frequency is n magnetic field induction is 0.4 10 5 T when the

More information

1 A mass on a spring undergoes SHM. The maximum displacement from the equilibrium is called?

1 A mass on a spring undergoes SHM. The maximum displacement from the equilibrium is called? Slide 1 / 20 1 mass on a spring undergoes SHM. The maximum displacement from the equilibrium is called? Period Frequency mplitude Wavelength Speed Slide 2 / 20 2 In a periodic process, the number of cycles

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

AAPT UNITED STATES PHYSICS TEAM AIP 2009

AAPT UNITED STATES PHYSICS TEAM AIP 2009 2009 F = ma Exam 1 AAPT UNITED STATES PHYSICS TEAM AIP 2009 2009 F = ma Contest 25 QUESTIONS - 75 MINUTES INSTRUCTIONS DO NOT OPEN THIS TEST UNTI YOU ARE TOD TO BEGIN Use = 10 N/k throuhout this contest.

More information

AP Physics. Harmonic Motion. Multiple Choice. Test E

AP Physics. Harmonic Motion. Multiple Choice. Test E AP Physics Harmonic Motion Multiple Choice Test E A 0.10-Kg block is attached to a spring, initially unstretched, of force constant k = 40 N m as shown below. The block is released from rest at t = 0 sec.

More information

Physics 2101 S c e t c i cti n o 3 n 3 March 31st Announcements: Quiz today about Ch. 14 Class Website:

Physics 2101 S c e t c i cti n o 3 n 3 March 31st Announcements: Quiz today about Ch. 14 Class Website: Physics 2101 Section 3 March 31 st Announcements: Quiz today about Ch. 14 Class Website: http://www.phys.lsu.edu/classes/spring2010/phys2101 3/ http://www.phys.lsu.edu/~jzhang/teaching.html Simple Harmonic

More information

Chapter 13. Hooke s Law: F = - kx Periodic & Simple Harmonic Motion Springs & Pendula Waves Superposition. Next Week!

Chapter 13. Hooke s Law: F = - kx Periodic & Simple Harmonic Motion Springs & Pendula Waves Superposition. Next Week! Chapter 13 Hooke s Law: F = - kx Periodic & Simple Harmonic Motion Springs & Pendula Waves Superposition Next Week! Review Physics 2A: Springs, Pendula & Circular Motion Elastic Systems F = kx Small Vibrations

More information

EXERCISE - 01 NEETIIT.COM. d x dt. = 2 x 2 (4)

EXERCISE - 01 NEETIIT.COM. d x dt. = 2 x 2 (4) 1. The acceleration of a particle executing S.H.M. is (1) Always directed towards the equillibrium position () Always towards the one end (3) Continuously changing in direction () Maximum at the mean position.

More information

Faculty of Computers and Information. Basic Science Department

Faculty of Computers and Information. Basic Science Department 18--018 FCI 1 Faculty of Computers and Information Basic Science Department 017-018 Prof. Nabila.M.Hassan 18--018 FCI Aims of Course: The graduates have to know the nature of vibration wave motions with

More information

Oscillations. Simple Harmonic Motion of a Mass on a Spring The equation of motion for a mass m is attached to a spring of constant k is

Oscillations. Simple Harmonic Motion of a Mass on a Spring The equation of motion for a mass m is attached to a spring of constant k is Dr. Alain Brizard College Physics I (PY 10) Oscillations Textbook Reference: Chapter 14 sections 1-8. Simple Harmonic Motion of a Mass on a Spring The equation of motion for a mass m is attached to a spring

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

3. Can a simple pendulum vibrate at the centre of Earth? Ans : No, because at the centre of earth, g = 0

3. Can a simple pendulum vibrate at the centre of Earth? Ans : No, because at the centre of earth, g = 0 CHAPTER : 14 OSCILLATIONS 1 marks: 1. The length of a second s pendulum on the surface of earth is 1 m. What will be the length of a second s pendulum on the surface of moon? Ans : T = 2π, T remains same

More information

Double Spring Harmonic Oscillator Lab

Double Spring Harmonic Oscillator Lab Dylan Humenik and Benjamin Daily Double Spring Harmonic Oscillator Lab Objectives: -Experimentally determine harmonic equations for a double spring system using various methods Part 1 Determining k of

More information

PREMED COURSE, 14/08/2015 OSCILLATIONS

PREMED COURSE, 14/08/2015 OSCILLATIONS PREMED COURSE, 14/08/2015 OSCILLATIONS PERIODIC MOTIONS Mechanical Metronom Laser Optical Bunjee jumping Electrical Astronomical Pulsar Biological ECG AC 50 Hz Another biological exampe PERIODIC MOTIONS

More information

Another Method to get a Sine Wave. X = A cos θ V = Acc =

Another Method to get a Sine Wave. X = A cos θ V = Acc = LAST NAME FIRST NAME DATE PER CJ Wave Assignment 10.3 Energy & Simple Harmonic Motion Conceptual Questions 3, 4, 6, 7, 9 page 313 6, 7, 33, 34 page 314-316 Tracing the movement of the mass on the end of

More information

Experiment 1: Simple Pendulum

Experiment 1: Simple Pendulum COMSATS Institute of Information Technoloy, Islamabad Campus PHY-108 : Physics Lab 1 (Mechanics of Particles) Experiment 1: Simple Pendulum A simple pendulum consists of a small object (known as the bob)

More information

Physics 1C. Lecture 12B

Physics 1C. Lecture 12B Physics 1C Lecture 12B SHM: Mathematical Model! Equations of motion for SHM:! Remember, simple harmonic motion is not uniformly accelerated motion SHM: Mathematical Model! The maximum values of velocity

More information

PHYSICS - CLUTCH CH 15: PERIODIC MOTION (NEW)

PHYSICS - CLUTCH CH 15: PERIODIC MOTION (NEW) !! www.clutchprep.com CONCEPT: Hooke s Law & Springs When you push/pull against a spring (FA), spring pushes back in the direction. (Action-Reaction!) Fs = FA = Ex. 1: You push on a spring with a force

More information

The distance of the object from the equilibrium position is m.

The distance of the object from the equilibrium position is m. Answers, Even-Numbered Problems, Chapter..4.6.8.0..4.6.8 (a) A = 0.0 m (b).60 s (c) 0.65 Hz Whenever the object is released from rest, its initial displacement equals the amplitude of its SHM. (a) so 0.065

More information

Physics 20 Lesson 24 Simple Harmonic Motion Pendulums

Physics 20 Lesson 24 Simple Harmonic Motion Pendulums Physics 0 esson 4 Simple Harmonic Motion Pendulums Refer to Chapter 7 in Pearson for a discussion of simple harmonic motion. I. Simple Harmonic Motion A study of simple harmonic motion (SHM) will take

More information

Chapter 14 Periodic Motion

Chapter 14 Periodic Motion Chapter 14 Periodic Motion 1 Describing Oscillation First, we want to describe the kinematical and dynamical quantities associated with Simple Harmonic Motion (SHM), for example, x, v x, a x, and F x.

More information

Oscillations. Oscillations and Simple Harmonic Motion

Oscillations. Oscillations and Simple Harmonic Motion Oscillations AP Physics C Oscillations and Simple Harmonic Motion 1 Equilibrium and Oscillations A marble that is free to roll inside a spherical bowl has an equilibrium position at the bottom of the bowl

More information

Important because SHM is a good model to describe vibrations of a guitar string, vibrations of atoms in molecules, etc.

Important because SHM is a good model to describe vibrations of a guitar string, vibrations of atoms in molecules, etc. Simple Harmonic Motion Oscillatory motion under a restoring force proportional to the amount of displacement from equilibrium A restoring force is a force that tries to move the system back to equilibrium

More information

Page 1. Physics 131: Lecture 22. SHM and Circles. Today s Agenda. Position. Velocity. Position and Velocity. Acceleration. v Asin.

Page 1. Physics 131: Lecture 22. SHM and Circles. Today s Agenda. Position. Velocity. Position and Velocity. Acceleration. v Asin. Physics 3: ecture Today s enda Siple haronic otion Deinition Period and requency Position, velocity, and acceleration Period o a ass on a sprin Vertical sprin Enery and siple haronic otion Enery o a sprin

More information

Do not turn over until you are told to do so by the Invigilator.

Do not turn over until you are told to do so by the Invigilator. UNIVERSITY OF EAST ANGLIA School of Mathematics Main Series UG Examination 2016 17 ENGINEERING MATHEMATICS AND MECHANICS ENG-4004Y Time allowed: 2 Hours Attempt QUESTIONS 1 and 2, and ONE other question.

More information

Practice Test SHM with Answers

Practice Test SHM with Answers Practice Test SHM with Answers MPC 1) If we double the frequency of a system undergoing simple harmonic motion, which of the following statements about that system are true? (There could be more than one

More information

Chapter 15 Oscillations

Chapter 15 Oscillations Chapter 15 Oscillations Summary Simple harmonic motion Hook s Law Energy F = kx Pendulums: Simple. Physical, Meter stick Simple Picture of an Oscillation x Frictionless surface F = -kx x SHM in vertical

More information

Chapter 5 Oscillatory Motion

Chapter 5 Oscillatory Motion Chapter 5 Oscillatory Motion Simple Harmonic Motion An object moves with simple harmonic motion whenever its acceleration is proportional to its displacement from some equilibrium position and is oppositely

More information

8. What is the period of a pendulum consisting of a 6-kg object oscillating on a 4-m string?

8. What is the period of a pendulum consisting of a 6-kg object oscillating on a 4-m string? 1. In the produce section of a supermarket, five pears are placed on a spring scale. The placement of the pears stretches the spring and causes the dial to move from zero to a reading of 2.0 kg. If the

More information

Simple Harmonic Motion

Simple Harmonic Motion Chapter 9 Simple Harmonic Motion In This Chapter: Restoring Force Elastic Potential Energy Simple Harmonic Motion Period and Frequency Displacement, Velocity, and Acceleration Pendulums Restoring Force

More information

Mechanics Oscillations Simple Harmonic Motion

Mechanics Oscillations Simple Harmonic Motion Mechanics Oscillations Simple Harmonic Motion Lana Sheridan De Anza College Dec 3, 2018 Last time gravity Newton s universal law of gravitation gravitational field gravitational potential energy Overview

More information

AHL 9.1 Energy transformation

AHL 9.1 Energy transformation AHL 9.1 Energy transformation 17.1.2018 1. [1 mark] A pendulum oscillating near the surface of the Earth swings with a time period T. What is the time period of the same pendulum near the surface of the

More information

not to be republished NCERT OSCILLATIONS Chapter Fourteen MCQ I π y = 3 cos 2ωt The displacement of a particle is represented by the equation

not to be republished NCERT OSCILLATIONS Chapter Fourteen MCQ I π y = 3 cos 2ωt The displacement of a particle is represented by the equation Chapter Fourteen OSCILLATIONS MCQ I 14.1 The displacement of a particle is represented by the equation π y = 3 cos 2ωt 4. The motion of the particle is (a) simple harmonic with period 2p/w. (b) simple

More information

Chapter 12 Vibrations and Waves Simple Harmonic Motion page

Chapter 12 Vibrations and Waves Simple Harmonic Motion page Chapter 2 Vibrations and Waves 2- Simple Harmonic Motion page 438-45 Hooke s Law Periodic motion the object has a repeated motion that follows the same path, the object swings to and fro. Examples: a pendulum

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

DEVIL PHYSICS THE BADDEST CLASS ON CAMPUS AP PHYSICS

DEVIL PHYSICS THE BADDEST CLASS ON CAMPUS AP PHYSICS DEVIL PHYSICS THE BADDEST CLASS ON CAMPUS AP PHYSICS LSN 11-1: SIMPLE HARMONIC MOTION LSN 11-: ENERGY IN THE SIMPLE HARMONIC OSCILLATOR LSN 11-3: PERIOD AND THE SINUSOIDAL NATURE OF SHM Introductory Video:

More information

A. Incorrect! Frequency and wavelength are not directly proportional to each other.

A. Incorrect! Frequency and wavelength are not directly proportional to each other. MCAT Physics Problem Solving Drill 1: Waves and Periodic Motion Question No. 1 of 10 Question 1. Two waves on identical strings have frequencies in a ratio of 3 to. If their wave speeds are the same, then

More information

DEVIL PHYSICS THE BADDEST CLASS ON CAMPUS IB PHYSICS

DEVIL PHYSICS THE BADDEST CLASS ON CAMPUS IB PHYSICS DEVIL PHYSICS THE BADDEST CLASS ON CAMPUS IB PHYSICS TSOKOS LESSON 4-1 SIMPLE HARMONIC MOTION Introductory Video: Simple Harmonic Motion IB Assessment Statements Topic 4.1, Kinematics of Simple Harmonic

More information

Physics 161 Lecture 17 Simple Harmonic Motion. October 30, 2018

Physics 161 Lecture 17 Simple Harmonic Motion. October 30, 2018 Physics 161 Lecture 17 Simple Harmonic Motion October 30, 2018 1 Lecture 17: learning objectives Review from lecture 16 - Second law of thermodynamics. - In pv cycle process: ΔU = 0, Q add = W by gass

More information

Slide 1 / 70. Simple Harmonic Motion

Slide 1 / 70. Simple Harmonic Motion Slide 1 / 70 Simple Harmonic Motion Slide 2 / 70 SHM and Circular Motion There is a deep connection between Simple Harmonic Motion (SHM) and Uniform Circular Motion (UCM). Simple Harmonic Motion can be

More information

2015 (A) Roll No. INTERMEDIATE PART-I (11 th CLASS)

2015 (A) Roll No. INTERMEDIATE PART-I (11 th CLASS) Number: 647 (1) Liht year is a unit of:- () he resultant of two forces 30 N and 40 N actin parallel to each other is:- (3) A ball is allowed to fall freely from certain heiht. It covers a distance in first

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

AHL 9.1 Energy transformation

AHL 9.1 Energy transformation AHL 9.1 Energy transformation 17.1.2018 1. [1 mark] A pendulum oscillating near the surface of the Earth swings with a time period T. What is the time period of the same pendulum near the surface of the

More information

KINEMATICS PREVIOUS EAMCET BITS ENGINEERING PAPER

KINEMATICS PREVIOUS EAMCET BITS ENGINEERING PAPER KINEMATICS PREVIOUS EAMCET BITS ENGINEERING PAPER. A body is projected vertically upwards at time t = 0 and is seen at a heiht at time t and t seconds durin its fliht. The maximum heiht attained is [ =

More information

You may use your books and notes. Moreover, you are encouraged to freely discuss the questions..which doesn't mean copying answers.

You may use your books and notes. Moreover, you are encouraged to freely discuss the questions..which doesn't mean copying answers. Section: Oscillations Take-Home Test You may use your books and notes. Moreover, you are encouraged to freely discuss the questions..which doesn't mean copying answers. 1. In simple harmonic motion, the

More information

Good Vibes: Introduction to Oscillations

Good Vibes: Introduction to Oscillations Good Vibes: Introduction to Oscillations Description: Several conceptual and qualitative questions related to main characteristics of simple harmonic motion: amplitude, displacement, period, frequency,

More information

AP Physics 1 Multiple Choice Questions - Chapter 9

AP Physics 1 Multiple Choice Questions - Chapter 9 1 If an object of mass m attached to a light spring is replaced by one of mass 9m, the frequency of the vibrating system changes by what multiplicative factor? a 1/9 b 1/3 c 3 d 9 e 6 2 A mass of 0.40

More information

Simple Harmonic Motion Test Tuesday 11/7

Simple Harmonic Motion Test Tuesday 11/7 Simple Harmonic Motion Test Tuesday 11/7 Chapter 11 Vibrations and Waves 1 If an object vibrates or oscillates back and forth over the same path, each cycle taking the same amount of time, the motion is

More information

EXAM 1. WAVES, OPTICS AND MODERN PHYSICS 15% of the final mark

EXAM 1. WAVES, OPTICS AND MODERN PHYSICS 15% of the final mark EXAM 1 WAVES, OPTICS AND MODERN PHYSICS 15% of the final mark Autumn 2018 Name: Each multiple-choice question is worth 3 marks. 1. A light beam is deflected by two mirrors, as shown. The incident beam

More information

Vibrations and Waves MP205, Assignment 4 Solutions

Vibrations and Waves MP205, Assignment 4 Solutions Vibrations and Waves MP205, Assignment Solutions 1. Verify that x = Ae αt cos ωt is a possible solution of the equation and find α and ω in terms of γ and ω 0. [20] dt 2 + γ dx dt + ω2 0x = 0, Given x

More information

Chap 11. Vibration and Waves. The impressed force on an object is proportional to its displacement from it equilibrium position.

Chap 11. Vibration and Waves. The impressed force on an object is proportional to its displacement from it equilibrium position. Chap 11. Vibration and Waves Sec. 11.1 - Simple Harmonic Motion The impressed force on an object is proportional to its displacement from it equilibrium position. F x This restoring force opposes the change

More information

Unit 7: Oscillations

Unit 7: Oscillations Text: Chapter 15 Unit 7: Oscillations NAME: Problems (p. 405-412) #1: 1, 7, 13, 17, 24, 26, 28, 32, 35 (simple harmonic motion, springs) #2: 45, 46, 49, 51, 75 (pendulums) Vocabulary: simple harmonic motion,

More information

Lecture XXVI. Morris Swartz Dept. of Physics and Astronomy Johns Hopkins University November 5, 2003

Lecture XXVI. Morris Swartz Dept. of Physics and Astronomy Johns Hopkins University November 5, 2003 Lecture XXVI Morris Swartz Dept. of Physics and Astronomy Johns Hopins University morris@jhu.edu November 5, 2003 Lecture XXVI: Oscillations Oscillations are periodic motions. There are many examples of

More information

Simple harmonic motion the motion of springs is a very important topic in physics.

Simple harmonic motion the motion of springs is a very important topic in physics. Chapter 11 Potential and Kinetic Energy Together: Simple Harmonic Motion In This Chapter Using Hooke s law Working with simple harmonic motion Calculating simple harmonic motion velcoity Finding simple

More information

SIMPLE HARMONIC MOTION

SIMPLE HARMONIC MOTION SIMPLE HARMONI MOTION hallenging MQ questions by The Physics afe ompiled and selected by The Physics afe 1 Simple harmonic motion is defined as the motion of a particle such that A its displacement x from

More information

SOUND. Representative Sample Physics: Sound. 1. Periodic Motion of Particles PLANCESS CONCEPTS

SOUND. Representative Sample Physics: Sound. 1. Periodic Motion of Particles PLANCESS CONCEPTS Representative Sample Physics: Sound SOUND 1. Periodic Motion of Particles Before we move on to study the nature and transmission of sound, we need to understand the different types of vibratory or oscillatory

More information

Physics 101 Discussion Week 12 Explanation (2011)

Physics 101 Discussion Week 12 Explanation (2011) Physics 101 Discussion Week 12 Eplanation (2011) D12-1 Horizontal oscillation Q0. This is obviously about a harmonic oscillator. Can you write down Newton s second law in the (horizontal) direction? Let

More information

Circular_Gravitation_P1 [22 marks]

Circular_Gravitation_P1 [22 marks] Circular_Gravitation_P1 [ marks] 1. An object of mass m at the end of a strin of lenth r moves in a vertical circle at a constant anular speed ω. What is the tension in the strin when the object is at

More information

Exam II Difficult Problems

Exam II Difficult Problems Exam II Difficult Problems Exam II Difficult Problems 90 80 70 60 50 40 30 20 10 0 1 2 3 4 5 6 7 8 9 10 11 12 13 14 15 16 17 18 19 20 Two boxes are connected to each other as shown. The system is released

More information

CHAPTERS WAVES SOUND STATIONARY WAVES ACOUSTICSOF BUILDINGS

CHAPTERS WAVES SOUND STATIONARY WAVES ACOUSTICSOF BUILDINGS CET -IPUC: PHYSICS Unit VI : WAVES and SOUND CHAPTERS OSCILLATIONS WAVES SOUND STATIONARY WAVES ACOUSTICSOF BUILDINGS Particle acceleration: a = Aω 2 sinωt= ω 2 y Maximum acceleration: a max = A ω 2 The

More information

Distance travelled time taken and if the particle is a distance s(t) along the x-axis, then its instantaneous speed is:

Distance travelled time taken and if the particle is a distance s(t) along the x-axis, then its instantaneous speed is: Chapter 1 Kinematics 1.1 Basic ideas r(t) is the position of a particle; r = r is the distance to the origin. If r = x i + y j + z k = (x, y, z), then r = r = x 2 + y 2 + z 2. v(t) is the velocity; v =

More information

PHYSICS 1 Simple Harmonic Motion

PHYSICS 1 Simple Harmonic Motion Advanced Placement PHYSICS 1 Simple Harmonic Motion Student 014-015 What I Absolutely Have to Know to Survive the AP* Exam Whenever the acceleration of an object is proportional to its displacement and

More information

Mechanics Cycle 3 Chapter 12++ Chapter 12++ Revisit Circular Motion

Mechanics Cycle 3 Chapter 12++ Chapter 12++ Revisit Circular Motion Chapter 12++ Revisit Circular Motion Revisit: Anular variables Second laws for radial and tanential acceleration Circular motion CM 2 nd aw with F net To-Do: Vertical circular motion in ravity Complete

More information

A Level. A Level Physics. Oscillations (Answers) AQA, Edexcel. Name: Total Marks: /30

A Level. A Level Physics. Oscillations (Answers) AQA, Edexcel. Name: Total Marks: /30 Visit http://www.mathsmadeeasy.co.uk/ for more fantastic resources. AQA, Edexcel A Level A Level Physics Oscillations (Answers) Name: Total Marks: /30 Maths Made Easy Complete Tuition Ltd 2017 1. The graph

More information

PHY 140Y FOUNDATIONS OF PHYSICS Tutorial Questions #9 Solutions November 12/13

PHY 140Y FOUNDATIONS OF PHYSICS Tutorial Questions #9 Solutions November 12/13 PHY 4Y FOUNDAIONS OF PHYSICS - utorial Questions #9 Solutions Noveber /3 Conservation of Ener and Sprins. One end of a assless sprin is placed on a flat surface, with the other end pointin upward, as shown

More information

LAB 10 - HARMONIC MOTION AND THE PENDULUM

LAB 10 - HARMONIC MOTION AND THE PENDULUM L10-1 Name Date Partners LAB 10 - HARMONIC MOION AND HE PENDULUM θ L Groove marking the center of mass Photogate s = 0 s F tan mg θ OVERVIEW Figure 1 A body is said to be in a position of stable equilibrium

More information

LAB 10: HARMONIC MOTION AND THE PENDULUM

LAB 10: HARMONIC MOTION AND THE PENDULUM 163 Name Date Partners LAB 10: HARMONIC MOION AND HE PENDULUM Galileo reportedly began his study of the pendulum in 1581 while watching this chandelier swing in Pisa, Italy OVERVIEW A body is said to be

More information

Date: 31 March (1) The only reference material you may use is one 8½x11 crib sheet and a calculator.

Date: 31 March (1) The only reference material you may use is one 8½x11 crib sheet and a calculator. PH1140: Oscillations and Waves Name: SOLUTIONS AT END Conference: Date: 31 March 2005 EXAM #1: D2006 INSTRUCTIONS: (1) The only reference material you may use is one 8½x11 crib sheet and a calculator.

More information

Simple Harmonic Motion

Simple Harmonic Motion Pendula Simple Harmonic Motion diff. eq. d 2 y dt 2 =!Ky 1. Know frequency (& period) immediately from diff. eq.! = K 2. Initial conditions: they will be of 2 kinds A. at rest initially y(0) = y o v y

More information

Chapter 4. Oscillatory Motion. 4.1 The Important Stuff Simple Harmonic Motion

Chapter 4. Oscillatory Motion. 4.1 The Important Stuff Simple Harmonic Motion Chapter 4 Oscillatory Motion 4.1 The Important Stuff 4.1.1 Simple Harmonic Motion In this chapter we consider systems which have a motion which repeats itself in time, that is, it is periodic. In particular

More information

Simple Harmonic Motion Investigating a Mass Oscillating on a Spring

Simple Harmonic Motion Investigating a Mass Oscillating on a Spring 17 Investigating a Mass Oscillating on a Spring A spring that is hanging vertically from a support with no mass at the end of the spring has a length L (called its rest length). When a mass is added to

More information

Chapter 12. Recall that when a spring is stretched a distance x, it will pull back with a force given by: F = -kx

Chapter 12. Recall that when a spring is stretched a distance x, it will pull back with a force given by: F = -kx Chapter 1 Lecture Notes Chapter 1 Oscillatory Motion Recall that when a spring is stretched a distance x, it will pull back with a force given by: F = -kx When the mass is released, the spring will pull

More information

Chapter 10 Lecture Outline. Copyright The McGraw-Hill Companies, Inc. Permission required for reproduction or display.

Chapter 10 Lecture Outline. Copyright The McGraw-Hill Companies, Inc. Permission required for reproduction or display. Chapter 10 Lecture Outline Copyright The McGraw-Hill Companies, Inc. Permission required for reproduction or display. 1 Chapter 10: Elasticity and Oscillations Elastic Deformations Hooke s Law Stress and

More information

OSCILLATIONS.

OSCILLATIONS. OSCILLATIONS Periodic Motion and Oscillatory motion If a body repeats its motion along a certain path, about a fixed point, at a definite interval of time, it is said to have a periodic motion If a body

More information

C. points X and Y only. D. points O, X and Y only. (Total 1 mark)

C. points X and Y only. D. points O, X and Y only. (Total 1 mark) Grade 11 Physics -- Homework 16 -- Answers on a separate sheet of paper, please 1. A cart, connected to two identical springs, is oscillating with simple harmonic motion between two points X and Y that

More information

CHAPTER 7: OSCILLATORY MOTION REQUIRES A SET OF CONDITIONS

CHAPTER 7: OSCILLATORY MOTION REQUIRES A SET OF CONDITIONS CHAPTER 7: OSCILLATORY MOTION REQUIRES A SET OF CONDITIONS 7.1 Period and Frequency Anything that vibrates or repeats its motion regularly is said to have oscillatory motion (sometimes called harmonic

More information

Waves Part 1: Travelling Waves

Waves Part 1: Travelling Waves Waves Part 1: Travelling Waves Last modified: 15/05/2018 Links Contents Travelling Waves Harmonic Waves Wavelength Period & Frequency Summary Example 1 Example 2 Example 3 Example 4 Transverse & Longitudinal

More information

CIRCULAR MOTION, HARMONIC MOTION, ROTATIONAL MOTION

CIRCULAR MOTION, HARMONIC MOTION, ROTATIONAL MOTION CIRCULAR MOTION, HARMONIC MOTION, ROTATIONAL MOTION 1 UNIFORM CIRCULAR MOTION path circle distance arc Definition: An object which moves on a circle, travels equal arcs in equal times. Periodic motion

More information

4.1 KINEMATICS OF SIMPLE HARMONIC MOTION 4.2 ENERGY CHANGES DURING SIMPLE HARMONIC MOTION 4.3 FORCED OSCILLATIONS AND RESONANCE Notes

4.1 KINEMATICS OF SIMPLE HARMONIC MOTION 4.2 ENERGY CHANGES DURING SIMPLE HARMONIC MOTION 4.3 FORCED OSCILLATIONS AND RESONANCE Notes 4.1 KINEMATICS OF SIMPLE HARMONIC MOTION 4.2 ENERGY CHANGES DURING SIMPLE HARMONIC MOTION 4.3 FORCED OSCILLATIONS AND RESONANCE Notes I. DEFINING TERMS A. HOW ARE OSCILLATIONS RELATED TO WAVES? II. EQUATIONS

More information

KEELE UNIVERSITY PHYSICS/ASTROPHYSICS MODULE PHY OSCILLATIONS AND WAVES PRACTICE EXAM

KEELE UNIVERSITY PHYSICS/ASTROPHYSICS MODULE PHY OSCILLATIONS AND WAVES PRACTICE EXAM KEELE UNIVERSITY PHYSICS/ASTROPHYSICS MODULE PHY-10012 OSCILLATIONS AND WAVES PRACTICE EXAM Candidates should attempt ALL of PARTS A and B, and TWO questions from PART C. PARTS A and B should be answered

More information

AP Physics 1. April 11, Simple Harmonic Motion. Table of Contents. Period. SHM and Circular Motion

AP Physics 1. April 11, Simple Harmonic Motion. Table of Contents. Period. SHM and Circular Motion AP Physics 1 2016-07-20 www.njctl.org Table of Contents Click on the topic to go to that section Period and Frequency SHM and UCM Spring Pendulum Simple Pendulum Sinusoidal Nature of SHM Period and Frequency

More information

PHYS 124 Section A01 Final Examination Autumn 2006

PHYS 124 Section A01 Final Examination Autumn 2006 PHYS 14 Section A1 Final Examination Autumn 6 Name : S Student ID Number : Instructor : Marc de Montiny Time : Monday, December 18, 6 9: 11: AM Room : Tory Lecture (Turtle) TL-B Instructions : This booklet

More information

Name Lesson 7. Homework Work and Energy Problem Solving Outcomes

Name Lesson 7. Homework Work and Energy Problem Solving Outcomes Physics 1 Name Lesson 7. Homework Work and Energy Problem Solving Outcomes Date 1. Define work. 2. Define energy. 3. Determine the work done by a constant force. Period 4. Determine the work done by a

More information

Oscillatory Motion and Wave Motion

Oscillatory Motion and Wave Motion Oscillatory Motion and Wave Motion Oscillatory Motion Simple Harmonic Motion Wave Motion Waves Motion of an Object Attached to a Spring The Pendulum Transverse and Longitudinal Waves Sinusoidal Wave Function

More information

Physics 231. Topic 7: Oscillations. Alex Brown October MSU Physics 231 Fall

Physics 231. Topic 7: Oscillations. Alex Brown October MSU Physics 231 Fall Physics 231 Topic 7: Oscillations Alex Brown October 14-19 2015 MSU Physics 231 Fall 2015 1 Key Concepts: Springs and Oscillations Springs Periodic Motion Frequency & Period Simple Harmonic Motion (SHM)

More information

Simple Harmonic Motion and Elasticity continued

Simple Harmonic Motion and Elasticity continued Chapter 10 Simple Harmonic Motion and Elasticity continued Spring constants & oscillations Hooke's Law F A = k x Displacement proportional to applied force Oscillations position: velocity: acceleration:

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