Hooke s law. F s =-kx Hooke s law

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

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

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

Ch 15 Simple Harmonic Motion

WAVES & SIMPLE HARMONIC MOTION

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

Oscillatory Motion SHM

Chapter 14 Oscillations. Copyright 2009 Pearson Education, Inc.

Chapter 14 Oscillations

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

Slide 1 / 70. Simple Harmonic Motion

Chapter 5 Oscillatory Motion

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

CHAPTER 6 WORK AND ENERGY

Simple Harmonic Motion Test Tuesday 11/7

CHAPTER 12 OSCILLATORY MOTION

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

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

Chapter 14 Oscillations. Copyright 2009 Pearson Education, Inc.

AP Physics. Harmonic Motion. Multiple Choice. Test E

PHYSICS 1 Simple Harmonic Motion

Chapter 13. Simple Harmonic Motion

Oscillatory Motion and Wave Motion

Chapter 15. Oscillatory 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 13. Hooke s Law: F = - kx Periodic & Simple Harmonic Motion Springs & Pendula Waves Superposition. Next Week!

Unit 2: Simple Harmonic Motion (SHM)

Chapter 12 Vibrations and Waves Simple Harmonic Motion page

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

Lecture 1 Notes: 06 / 27. The first part of this class will primarily cover oscillating systems (harmonic oscillators and waves).

Simple Harmonic Motion and Elasticity continued

Exam II Difficult Problems

T 2. Key take-aways: k m. Tuesday March 28

Chapter 07: Kinetic Energy and Work

DEVIL PHYSICS THE BADDEST CLASS ON CAMPUS AP PHYSICS

Mass on a Horizontal Spring

Chapter 11 Vibrations and Waves

Good Vibes: Introduction to Oscillations

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

Unit 7: Oscillations

Midterm 3 Review (Ch 9-14)

Oscillations. Oscillations and Simple Harmonic Motion


Physics 101 Discussion Week 12 Explanation (2011)

AP Physics C Mechanics

Oscillatory Motion. Solutions of Selected Problems

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

General Physics I Spring Oscillations

Chapter 14 Periodic Motion

PHYSICS - CLUTCH CH 15: PERIODIC MOTION (NEW)

Physics 231 Lecture 18

Force, Energy & Periodic Motion. Preparation for unit test

Chapter 7 Hooke s Force law and Simple Harmonic Oscillations

Chapter 14: Periodic motion

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

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

ENERGY. Conservative Forces Non-Conservative Forces Conservation of Mechanical Energy Power

Corso di Laurea in LOGOPEDIA FISICA ACUSTICA MOTO OSCILLATORIO

Physics 106 Group Problems Summer 2015 Oscillations and Waves

Chapter 6 Work and Energy

Chapter 6 Energy and Oscillations

1. [30] Y&F a) Assuming a small angle displacement θ max < 0.1 rad, the period is very nearly

Midterm Exam #1: Solutions

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

本教材僅供教學使用, 勿做其他用途, 以維護智慧財產權

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

Chapter 15. simple harmonic motion

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

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

10.1 The Ideal Spring and Simple Harmonic Motion

Static Equilibrium, Gravitation, Periodic Motion

Pre-Class. List everything you remember about circular motion...

Simple Harmonic Motion - 1 v 1.1 Goodman & Zavorotniy

Oscillations - AP Physics B 1984

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

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

CHAPTER 7: OSCILLATORY MOTION REQUIRES A SET OF CONDITIONS

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

The object of this experiment is to study systems undergoing simple harmonic motion.

Chapter 10. Simple Harmonic Motion and Elasticity

Work and Energy continued

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

Double Spring Harmonic Oscillator Lab

Mass on a Spring C2: Simple Harmonic Motion. Simple Harmonic Motion. Announcements Week 12D1

LECTURE 3 ENERGY AND PENDULUM MOTION. Instructor: Kazumi Tolich

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

CHAPTER 11 VIBRATIONS AND WAVES

Chapter 15 Oscillations

PHYS 1114, Lecture 33, April 10 Contents:

Simple Harmonic Motion

Name (please print): UW ID# score last first

Physics 1C. Lecture 12C

POTENTIAL ENERGY AND ENERGY CONSERVATION

Chapter 13: Oscillatory Motions

Solution Derivations for Capa #12

Grade 11/12 Math Circles Conics & Applications The Mathematics of Orbits Dr. Shahla Aliakbari November 18, 2015

Simple Harmonic Motion Practice Problems PSI AP Physics 1

Multiple-Choice questions

Ch 10 HW: Problem Spring Force

Transcription:

Hooke s law F s =-kx Hooke s law If there is no friction, the mass continues to oscillate back and forth. If a force is proportional to the displacement x, but opposite in direction, the resulting motion of the object is called: simple harmonic oscillation 1

displacement x a) Simple harmonic motion A b) c) time (s) Amplitude (A): maximum distance from equilibrium (unit: m) Period (T): Time to complete one full oscillation (unit: s) Frequency (f): Number of completed oscillations per second (unit: 1/s = 1 Herz [Hz]) f=1/t 2

displacement x 5cm Simple harmonic motion -5cm 2 4 6 8 10 time (s) a) what is the amplitude of the harmonic oscillation? b) what is the period of the harmonic oscillation? c) what is the frequency of the harmonic oscillation? a) Amplitude: 5 cm (0.05 m) b) period: time to complete one full oscillation: 4s c) frequency: number of oscillations per second=1/t=0.25 s 3

The spring constant k When the object hanging from the spring is not moving: F spring =-F gravity -kd =-mg k = mg/d k is a constant, so if we hang twice the amount of mass from the spring, d becomes twice larger: k=(2m)g/(2d)=mg/d 4

displacement x A displacement vs acceleration time (s) -A Newton s second law: F=ma -kx=ma a=-kx/m acceleration(a) ka/m -ka/m 5

example A mass of 1 kg is hung from a spring. The spring stretches by 0.5 m. Next, the spring is placed horizontally and fixed on one side to the wall. The same mass is attached and the spring stretched by 0.2 m and then released. What is the acceleration upon release? 1 st step: find the spring constant k F spring =-F gravity or -kd =-mg k = mg/d =1*9.8/0.5=19.6 N/m 2 nd step: find the acceleration upon release Newton s second law: F=ma -kx=ma a=-kx/m a=-19.6*0.2/1=-3.92 m/s 2 6

energy and velocity E kin (½mv 2 ) E pot,spring (½kx 2 ) Sum A 0 ½kA 2 ½kA 2 ½mv 2 0 ½mv 2 -A 0 ½k(-A) 2 ½kA 2 conservation of ME: ½m[v(x=0)] 2 =½kA 2 so v(x=0)=±a (k/m) 7

velocity more general Total ME at any displacement x: ½mv 2 +½kx 2 Total ME at max. displacement A: ½kA 2 Conservation of ME: ½kA 2 =½mv 2 +½kx 2 So: v=± [(A 2 -x 2 )k/m] position X velocity V acceleration a +A 0 -ka/m 0 ±A (k/m) 0 -A 0 ka/m 8

A x -A time (s) velocity v A (k/m) -A (k/m) ka/m a -ka/m 9

Generally: also add gravitational PE ME = KE + PE spring + PE gravity = ½mv 2 + ½kx 2 + mgh 10

An example A 0.4 kg object, connected to a light spring with a spring constant of 19.6 N/m oscillates on a frictionless horizontal surface. If the spring is compressed by 0.04 and then released determine: a) the maximum speed of the object b) the speed of the object when the spring is compressed by 0.015 m c) when it is stretched by 0.015 m d) for what value of x does the speed equal one half of the maximum speed? a) v= [(A 2 -x 2 )k/m] (speed is always positive!) maximum if x=0: [A 2 k/m]=0.04 (19.6/0.4)=0.28 m/s b) v= [(A 2 -x 2 )k/m] at x=-0.015 v= [((0.04) 2 -(-0.015) 2 )19.6/0.4]=0.26 m/s c) same as b) d) [(A 2 -x 2 )k/m]=0.28/2=0.14 x= (A 2-0.14 2 m/k)=0.035m 11

circular motion & simple harmonic motion A particle moves in a circular orbit with angular velocity ω, corresponding to a linear velocity v 0 =ωr=ωa A v 0 θ v x θ x The horizontal position as a function of time: x(t)=acosθ=acos(ωt) (θ=ωt) The horizontal velocity as a function of time: sinθ=-v x /v 0 v x (t)=-v 0 sinθ=-ωasin(ωt) t=0 Time to complete one circle (I.e. one period T): T=2πA/v 0 =2πA/ωA=2π/ω ω=2π/t=2πf (f: frequency) ω: angular frequency 12

Circular motion and simple harmonic motion The simple harmonic motion can be described by the projection of circular motion on the horizontal axis. x harmonic (t)=acos(ωt) v harmonic (t)=-ωasin(ωt) where A is the amplitude of the oscillation, and ω=2π/t=2πf, where T is the period of the harmonic motion and f=1/t the frequency. 13

For the case of a spring position X velocity V acceleration a +A 0 -ka/m 0 ±A (k/m) 0 -A 0 ka/m 1) velocity is maximum if v=±a (k/m) 2) circular motion: v spring (t)=-ωasinωt maximal if v spring =±ωa combine 1) & 2) ω= (k/m) Acceleration: a(t)=-(ka/m)cos(ωt)=-ω 2 Acos(ωt) 14

A x -A velocity v A (k/m) x harmonic (t)=acos(ωt) ω=2πf=2π/t= (k/m) v harmonic (t)=-ωasin(ωt) time (s) -A (k/m) ka/m a a harmonic (t)=-ω 2 Acos(ωt) -ka/m 15

Example A mass of 0.2 kg is attached to a spring with k=100 N/m. The spring is stretched over 0.1 m and released. a) What is the angular frequency (ω) of the corresponding circular motion? b) What is the period (T) of the harmonic motion? c) What is the frequency (f)? d) What are the functions for x,v and t of the mass as a function of time? Make a sketch of these. a) ω= (k/m)= ω= (100/0.2)=22.4 rad/s b) ω=2π/t T= 2π/ω=0.28 s c) ω=2πf f=ω/2π=3.55 Hz (=1/T) d) x harmonic (t)=acos(ωt)=0.1cos(0.28t) v harmonic (t)=-ωasin(ωt)=-0.028sin(0.28t) a harmonic (t)=-ω 2 Acos(ωt)=-0.0078cos(0.28t) 16

0.1 x -0.1 velocity v 0.028 0.28 0.56 time (s) -0.028 0.28 0.56 0.0078 a -0.0078 0.28 0.56 17