Simple Harmonic Motion

Similar documents
Simple Harmonic Motion and Elasticity continued

Chapter 10. Simple Harmonic Motion and Elasticity

Chapter 10. Simple Harmonic Motion and Elasticity. Example 1 A Tire Pressure Gauge

Unit 2: Simple Harmonic Motion (SHM)

Simple Harmonic Motion Test Tuesday 11/7

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

Exam II Difficult Problems

Chapter 14. Oscillations. Oscillations Introductory Terminology Simple Harmonic Motion:

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

PHYSICS - CLUTCH CH 15: PERIODIC MOTION (NEW)

Oscillatory Motion SHM

Periodic Motion. Periodic motion is motion of an object that. regularly repeats

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

10.1 The Ideal Spring and Simple Harmonic Motion

Chapter 14 Oscillations. Copyright 2009 Pearson Education, Inc.

Chapter 5 Oscillatory Motion

Faculty of Computers and Information. Basic Science Department

Physics 1C. Lecture 12B

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

Exam III Physics 101: Lecture 19 Elasticity and Oscillations

Chapter 14 Oscillations. Copyright 2009 Pearson Education, Inc.

Lectures Chapter 10 (Cutnell & Johnson, Physics 7 th edition)

Chapter 15. Oscillatory Motion

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

Oscillations. Simple Harmonic Motion (SHM) Position, Velocity, Acceleration SHM Forces SHM Energy Period of oscillation Damping and Resonance

Chapter 14 Oscillations

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

OSCILLATIONS ABOUT EQUILIBRIUM

CHAPTER 6 WORK AND ENERGY

Chapter 12 Vibrations and Waves Simple Harmonic Motion page

Harmonic Oscillator. Mass-Spring Oscillator Resonance The Pendulum. Physics 109 Experiment Number 12

Lecture 18. In other words, if you double the stress, you double the resulting strain.

Chapter 11 Vibrations and Waves

Oscillations. Phys101 Lectures 28, 29. Key points: Simple Harmonic Motion (SHM) SHM Related to Uniform Circular Motion The Simple Pendulum

PHYSICS 1 Simple Harmonic Motion

Good Vibes: Introduction to Oscillations

ELASTICITY. values for the mass m and smaller values for the spring constant k lead to greater values for the period.

Study Sheet for Exam #3

Mass on a Horizontal Spring

Chapter 7 Hooke s Force law and Simple Harmonic Oscillations

Chapter 14 Periodic Motion

Chapter 14: Periodic motion

Harmonic Oscillator. Outline. Oscillatory Motion or Simple Harmonic Motion. Oscillatory Motion or Simple Harmonic Motion

PHYS 1114, Lecture 33, April 10 Contents:

Midterm 3 Review (Ch 9-14)

11/17/10. Chapter 14. Oscillations. Chapter 14. Oscillations Topics: Simple Harmonic Motion. Simple Harmonic Motion

!T = 2# T = 2! " The velocity and acceleration of the object are found by taking the first and second derivative of the position:

Chapter 14. PowerPoint Lectures for University Physics, Thirteenth Edition Hugh D. Young and Roger A. Freedman. Lectures by Wayne Anderson

本教材僅供教學使用, 勿做其他用途, 以維護智慧財產權

Physics Mechanics. Lecture 32 Oscillations II

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

CHAPTER 7: OSCILLATORY MOTION REQUIRES A SET OF CONDITIONS

Chapter 6. Work and Energy

Oscillations. Oscillations and Simple Harmonic Motion

CHAPTER 11 VIBRATIONS AND WAVES

CHAPTER 12 OSCILLATORY MOTION

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

Chapter 13. F =!kx. Vibrations and Waves. ! = 2" f = 2" T. Hooke s Law Reviewed. Sinusoidal Oscillation Graphing x vs. t. Phases.

Wave Motion: v=λf [m/s=m 1/s] Example 1: A person on a pier observes a set of incoming waves that have a sinusoidal form with a distance of 1.

Chapter 10. Solids & Liquids

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

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

PHYSICS - CLUTCH CH 15: PERIODIC MOTION (OSCILLATIONS)

SOLUTION a. Since the applied force is equal to the person s weight, the spring constant is 670 N m ( )( )

Chapter 15 Periodic Motion

DEVIL PHYSICS THE BADDEST CLASS ON CAMPUS IB PHYSICS

Mechanics Oscillations Simple Harmonic Motion

AP Physics. Harmonic Motion. Multiple Choice. Test E

Essential Physics I. Lecture 9:

Chapter 15 SIMPLE HARMONIC MOTION

PHYSICS. Chapter 15 Lecture FOR SCIENTISTS AND ENGINEERS A STRATEGIC APPROACH 4/E RANDALL D. KNIGHT Pearson Education, Inc.

Chapter 14 Oscillations

Chapters 10 & 11: Energy

Physics 207 Lecture 25. Lecture 25. HW11, Due Tuesday, May 6 th For Thursday, read through all of Chapter 18. Angular Momentum Exercise

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

2.4 Harmonic Oscillator Models

Exam 3 Review. Chapter 10: Elasticity and Oscillations A stress will deform a body and that body can be set into periodic oscillations.

Outline. Hook s law. Mass spring system Simple harmonic motion Travelling waves Waves in string Sound waves

Simple Harmonic Motion

Thursday March 30 Topics for this Lecture: Simple Harmonic Motion Kinetic & Potential Energy Pendulum systems Resonances & Damping.

PreClass Notes: Chapter 13, Sections

2.4 Models of Oscillation

Summary PHY101 ( 2 ) T / Hanadi Al Harbi

Chapter 16: Oscillations

In vertical circular motion the gravitational force must also be considered.

Raymond A. Serway Chris Vuille. Chapter Thirteen. Vibrations and Waves

Oscillations Simple Harmonic Motion

Power: Sources of Energy

Chapter 14. PowerPoint Lectures for University Physics, Thirteenth Edition Hugh D. Young and Roger A. Freedman. Lectures by Wayne Anderson

Unit 7: Oscillations

Chapter 13: Oscillatory Motions

Rutgers University Department of Physics & Astronomy. 01:750:271 Honors Physics I Fall Lecture 19. Home Page. Title Page. Page 1 of 36.

General Physics I. Lecture 12: Applications of Oscillatory Motion. Prof. WAN, Xin ( 万歆 )

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

General Physics (PHY 2130)

Physics General Physics. Lecture 24 Oscillating Systems. Fall 2016 Semester Prof. Matthew Jones

Practice Test SHM with Answers

Corso di Laurea in LOGOPEDIA FISICA ACUSTICA MOTO OSCILLATORIO

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

Phys101 Second Major-152 Zero Version Coordinator: Dr. W. Basheer Monday, March 07, 2016 Page: 1

Transcription:

3/5/07 Simple Harmonic Motion 0. The Ideal Spring and Simple Harmonic Motion HOOKE S AW: RESTORING FORCE OF AN IDEA SPRING The restoring force on an ideal spring is F x k x spring constant Units: N/m

3/5/07 0. The Ideal Spring and Simple Harmonic Motion Example A Tire Pressure Gauge The spring constant of the spring is 30 N/m and the bar indicator extends.0 cm. What force does the air in the tire apply to the spring? 0. The Ideal Spring and Simple Harmonic Motion F Applied x k x 30 N m0.00 m 6.4 N

3/5/07 0. The Ideal Spring and Simple Harmonic Motion Conceptual Example Are Shorter Springs Stiffer? A 0-coil spring has a spring constant k. If the spring is cut in half, so there are two 5-coil springs, what is the spring constant of each of the smaller springs? 0. Simple Harmonic Motion and the Reference Circle DISPACEMENT x Acos t 3

3/5/07 0. Simple Harmonic Motion and the Reference Circle amplitude A: the maximum displacement period T: the time required to complete one cycle frequency f: the number of cycles per second (measured in Hz) f T f T 0. Simple Harmonic Motion and the Reference Circle VEOCITY v x v T sin A sin t v max 4

3/5/07 0. Simple Harmonic Motion and the Reference Circle Example 3 The Maximum Speed of a oudspeaker Diaphragm The frequency of motion is.0 KHz and the amplitude is 0.0 mm. (a) What is the maximum speed of the diaphragm? (b) Where in the motion does this maximum speed occur? 0. Simple Harmonic Motion and the Reference Circle v x v T sin A sin t v max 3 3 (a) v A A f 0.00 m.0 0 Hz max.3m s (b) The maximum speed occurs midway between the ends of its motion. 5

3/5/07 0. Simple Harmonic Motion and the Reference Circle ACCEERATION a x a c A cos cos t a max 0. Simple Harmonic Motion and the Reference Circle FREQUENCY OF VIBRATION x Acos t a x A cos t F kx ma x ka ma f k m k m 6

3/5/07 SHM Kinematics m = 0.5 kg What is the Frequency? Period? s f 0.5 Hz What is the Angular Frequency? f k m r /s What is the Amplitude? x m 4 m What function is x(t)? cos x(t) x m cos(t) 4cos(t) What function is v(t)? sin What is V m? vm x m v(t) v m sin(t) 4sin(t) v(t).6sin(t) SHM Kinematics m = 0.5 kg What function is a(t)? What is a m? cos a m x m a(t) a m cos(t) 4cos(t) a(t) 39.5cos(t) What function is F(t)? cos What is F m? F m ma m m x m F(t) F m cos(t) F(t) (0.5) 4cos(t) F(t) 9.7cos(t) 7

3/5/07 0. Simple Harmonic Motion and the Reference Circle Example 6 A Body Mass Measurement Device The device consists of a spring-mounted chair in which the astronaut sits. The spring has a spring constant of 606 N/m and the mass of the chair is.0 kg. The measured period is.4 s. Find the mass of the astronaut. 0. Simple Harmonic Motion and the Reference Circle k mtotal k m total m total k T m chair m astro f T m k astro T 606 N m.4s 4 m chair.0 kg 77. kg 8

3/5/07 0.3 Energy and Simple Harmonic Motion DEFINITION OF EASTIC POTENTIA ENERGY The elastic potential energy is the energy that a spring has by virtue of being stretched or compressed. For an ideal spring, the elastic potential energy is PEelastic kx SI Unit of Elastic Potential Energy: joule (J) 0.3 Energy and Simple Harmonic Motion A compressed spring can do work. 9

3/5/07 0.3 Energy and Simple Harmonic Motion W elastic kx o kxf 0.3 Energy and Simple Harmonic Motion Example 8 Changing the Mass of a Simple Harmonic Oscilator A 0.0-kg ball is attached to a vertical spring. The spring constant is 8 N/m. When released from rest, how far does the ball fall before being brought to a momentary stop by the spring? 0

3/5/07 0.3 Energy and Simple Harmonic Motion E f E o mv f I mgh f f ky f mv o I mgh o o ky o kho mgh o mg h o k 8 N 0.0 kg9.8m s 0.4 m m Assignment pg. 3 #,3,3 pg. 33-36 #3,4,9,3,6,8,6,3,36,4

3/5/07 0.4 The Pendulum A simple pendulum consists of a particle attached to a frictionless pivot by a cable of negligible mass. g (small angles only) mg I (small angles only) 0.4 The Pendulum Example 0 Keeping Time Determine the length of a simple pendulum that will swing back and forth in simple harmonic motion with a period of.00 s. f T g T g 4 T g 4.00 s 9.80m s 0.48 m 4

3/5/07 cos(θ) θ g x m A 0.5 m long pendulum with a mass of kg is released from rest at θ = 0 o. Find x m, v m, a m, τ, f, ω, and the maximum Tension in the string. x m is the maximum arc length: x m 0o 360 0.75 m o v m is the velocity at the bottom: E i E f 0.5 9.8.4 s f 0.70 Hz.4 4.43 r /s.4 v mgh m gh (9.8)0.03 0.77 m/s mv m v m x m 0.77 m/s F x ma m T h = cos(θ) θ mgsin ma a m gsin 3.35 m /s h = 0.03 m mg a m x m 3.4 m/s Maximum tension is at the bottom: T +y +x mg F y ma c m v r T mg m v m T m( v m g) N 0.5 Damped Harmonic Motion In simple harmonic motion, an object oscillated with a constant amplitude. In reality, friction or some other energy dissipating mechanism is always present and the amplitude decreases as time passes. This is referred to as damped harmonic motion. 3

3/5/07 0.5 Damped Harmonic Motion ) simple harmonic motion &3) underdamped 4) critically damped 5) overdamped 0.6 Driven Harmonic Motion and Resonance When a force is applied to an oscillating system at all times, the result is driven harmonic motion. Here, the driving force has the same frequency as the spring system and always points in the direction of the object s velocity. 4

3/5/07 0.6 Driven Harmonic Motion and Resonance RESONANCE Resonance is the condition in which a time-dependent force can transmit large amounts of energy to an oscillating object, leading to a large amplitude motion. Resonance occurs when the frequency of the force matches a natural frequency at which the object will oscillate. 0.7 Elastic Deformation STRETCHING, COMPRESSION, AND YOUNG S MODUUS F Y A o Young s modulus has the units of pressure: N/m 5

3/5/07 0.7 Elastic Deformation 0.7 Elastic Deformation Example Bone Compression In a circus act, a performer supports the combined weight (080 N) of a number of colleagues. Each thighbone of this performer has a length of 0.55 m and an effective cross sectional area of 7.7 0-4 m. Determine the amount that each thighbone compresses under the extra weight. 6

3/5/07 0.7 Elastic Deformation F Y A o F YA o N0.55 m 540 5 4.0 9 4 9.4 0 N m 7.7 0 m m 0.7 Elastic Deformation SHEAR DEFORMATION AND THE SHEAR MODUUS x F S A o The shear modulus has the units of pressure: N/m 7

3/5/07 0.7 Elastic Deformation 0.7 Elastic Deformation Example 4 J-E---O You push tangentially across the top surface with a force of 0.45 N. The top surface moves a distance of 6.0 mm relative to the bottom surface. What is the shear modulus of Jell-O? x F S A o Fo S Ax 8

3/5/07 0.7 Elastic Deformation S Fo Ax S 0.45 N0.030 m 460 N m 3 0.070 m 6.0 0 m 0.7 Elastic Deformation VOUME DEFORMATION AND THE BUK MODUUS V P B V o The Bulk modulus has the units of pressure: N/m 9

3/5/07 0.7 Elastic Deformation 0.8 Stress, Strain, and Hooke s aw In general the quantity F/A is called the stress. The change in the quantity divided by that quantity is called the strain: V V o o x o HOOKE S AW FOR STRESS AND STRAIN Stress is directly proportional to strain. Strain is a unitless quantitiy. SI Unit of Stress: N/m 0

3/5/07 0.8 Stress, Strain, and Hooke s aw Assignment pg. 33 #4,7 pg. 36-38 #43,46,49,5,54,60,64,7