Simple Harmonic Motion

Slides:



Advertisements
Similar presentations
Kinematics of simple harmonic motion (SHM)
Advertisements

Horizontal Spring-Block Oscillators
Physics 101: Lecture 22 Simple Harmonic Motion
Chapter 5 Kinetic Energy
SHM -1.
Adapted from Holt book on physics
Simple Harmonic Motion
Physics 101: Lecture 21, Pg 1 Lecture 21: Ideal Spring and Simple Harmonic Motion l New Material: Textbook Chapters 10.1, 10.2 and 10.3.
UB, Phy101: Chapter 10, Pg 1 Physics 101: Lecture 17 Simple Harmonic Motion l Today’s lecture will cover Textbook Sections
Problmes-1.
Chapter 14 Oscillations Chapter Opener. Caption: An object attached to a coil spring can exhibit oscillatory motion. Many kinds of oscillatory motion are.
Physics 101: Lecture 20, Pg 1 Lecture 20: Ideal Spring and Simple Harmonic Motion l New Material: Textbook Chapters 10.1 and 10.2.
Simple Harmonic Motion
Physics 6B Oscillations Prepared by Vince Zaccone
Physics 101: Lecture 20, Pg 1 Physics 101: Lecture 20 Elasticity and Oscillations l Today’s lecture will cover Textbook Chapter Exam III.
CHAPTER 10 Elasticity and Oscillations
Describing Periodic Motion AP Physics. Hooke’s Law.
Energy And SHM. Energy of Spring Spring has elastic potential energy PE = ½ kx 2 If assuming no friction, the total energy at any point is the sum of.
Physics 101: Lecture 19, Pg 1 Physics 101: Lecture 19 Elasticity and Oscillations Exam III.
Simple Harmonic Motion
Vibrations and Waves AP Physics Lecture Notes m Vibrations and Waves.
Chapter 11 - Simple Harmonic Motion
Periodic Motion. Definition of Terms Periodic Motion: Motion that repeats itself in a regular pattern. Periodic Motion: Motion that repeats itself in.
Simple Harmonic Motion. l Vibrations è Vocal cords when singing/speaking è String/rubber band l Simple Harmonic Motion è Restoring force proportional.
Chapter 12 Simple Harmonic Motion Photo by Mark Tippens A TRAMPOLINE exerts a restoring force on the jumper that is directly proportional to the average.
Oscillations - SHM. Oscillations In general an oscillation is simply aback and forth motion Since the motion repeats itself, it is called periodic We.
Simple Harmonic Motion
Physics 101: Lecture 19, Pg 1 Physics 101: Lecture 19 Elasticity and Oscillations Exam III.
Copyright © 2009 Pearson Education, Inc. Oscillations of a Spring Simple Harmonic Motion Energy in the Simple Harmonic Oscillator The Simple Pendulum Lecture.
Physics 101: Lecture 20, Pg 1 Physics 101: Lecture 20 Elasticity and Oscillations Today’s lecture will cover Textbook Chapter Exam III Tuned.
Physics 101: Lecture 20, Pg 1 Physics 101: Lecture 20 Elasticity and Oscillations Today’s lecture will cover Textbook Chapter Exam III Hour.
Chapter 11: Harmonic Motion
APHY201 1/30/ Simple Harmonic Motion   Periodic oscillations   Restoring Force: F = -kx   Force and acceleration are not constant  
Phys 250 Ch14 p1 Chapter 13: Periodic Motion What we already know: Elastic Potential Energy energy stored in a stretched/compressed spring Force: Hooke’s.
Physics 1D03 - Lecture 331 Harmonic Motion ( II ) (Serway 15.2, 15.3) Mass and Spring Energy in SHM.
Physics 101: Lecture 18, Pg 1 Physics 101: Lecture 18 Elasticity and Oscillations Exam III.
Lecture 18: Elasticity and Oscillations I l Simple Harmonic Motion: Definition l Springs: Forces l Springs: Energy l Simple Harmonic Motion: Equations.
Simple Harmonic Motion Periodic Motion Simple periodic motion is that motion in which a body moves back and forth over a fixed path, returning to each.
Physics 101: Lecture 18, Pg 1 Physics 101: Lecture 18 Elasticity and Oscillations Exam III.
Physics 101: Lecture 19, Pg 1 Physics 101: Lecture 19 Elasticity and Oscillations II Exam III.
Chapter 14 Springs A TRAMPOLINE exerts a restoring force on the jumper that is directly proportional to the average force required to displace the mat.
Simple Harmonic Motion (SHM). Simple Harmonic Motion – Vibration about an equilibrium position in which a restoring force is proportional to displacement.
Simple Harmonic Motion Wenny Maulina Simple harmonic motion  Simple harmonic motion (SHM) Solution: What is SHM? A simple harmonic motion is the motion.
Chapter 10 Waves and Vibrations Simple Harmonic Motion SHM.
Physics 101: Lecture 20, Pg 1 Physics 101: Lecture 20 Elasticity and Oscillations l Today’s lecture will cover Textbook Chapter
Harmonic Motion AP Physics C.
AP Physics Lecture Notes
Simple Harmonic Motion
Periodic Motion Oscillations: Stable Equilibrium: U  ½kx2 F  kx
Oscillations An Introduction.
Physics 101: Lecture 19 Elasticity and Oscillations II
Physics 101: Lecture 20 Elasticity and Oscillations
Harmonic Motion (III) Physics 1D03 - Lecture 33.
PHYS 1441 – Section 004 Lecture #22
Oscillations © 2014 Pearson Education, Inc..
Physics 101: Lecture 20 Elasticity and Oscillations
Oscillatory Motion Serway & Jewett (Chapter 15).
Simple Harmonic Motion
PhET mass spring applet
Physics 101: Lecture 19 Elasticity and Oscillations
Oscillations An Introduction.
A quick heads up on You will be able to derive it soon… Enquiry:
SCI 340 L25 SHM Things that vibrate
Harmonic Motion (II) Mass and Spring Energy in SHM
Simple Harmonic Motion
Simple Harmonic Motion Lesson 2
OBJECTIVE QUESTIONS FOR NEET AIIMS JIPMER
Aim: How do we explain the motion of a particle attached to a spring?
Simple Harmonic Motion and Wave Interactions
Physics 101: Lecture 19 Elasticity and Oscillations
Presentation transcript:

Simple Harmonic Motion 1

Simple Harmonic Motion Vibrations Vocal cords when singing/speaking String/rubber band Simple Harmonic Motion Restoring force proportional to displacement Springs F = -kx 11

Question II A mass on a spring oscillates back & forth with simple harmonic motion of amplitude A. A plot of displacement (x) versus time (t) is shown below. At what points during its oscillation is the magnitude of the acceleration of the block biggest? 1. When x = +A or -A (i.e. maximum displacement) 2. When x = 0 (i.e. zero displacement) 3. The acceleration of the mass is constant +A t -A x 17

Potential Energy in Spring Force of spring is Conservative F = -k x W = -1/2 k x2 Work done only depends on initial and final position Define Potential Energy PEspring = ½ k x2 Force work x 20

***Energy in SHM*** A mass is attached to a spring and set to motion. The maximum displacement is x=A Energy = PE + KE = constant! = ½ k x2 + ½ m v2 At maximum displacement x=A, v = 0 Energy = ½ k A2 + 0 At zero displacement x = 0 Energy = 0 + ½ mvm2 Since Total Energy is same ½ k A2 = ½ m vm2 vm = sqrt(k/m) A x PES m x x=0 25

Question 3 A mass on a spring oscillates back & forth with simple harmonic motion of amplitude A. A plot of displacement (x) versus time (t) is shown below. At what points during its oscillation is the speed of the block biggest? 1. When x = +A or -A (i.e. maximum displacement) 2. When x = 0 (i.e. zero displacement) 3. The speed of the mass is constant +A t -A x 29

Question 4 A spring oscillates back and forth on a frictionless horizontal surface. A camera takes pictures of the position every 1/10th of a second. Which plot best shows the positions of the mass. 1 2 3 EndPoint Equilibrium EndPoint EndPoint Equilibrium EndPoint EndPoint Equilibrium EndPoint 38

Springs and Simple Harmonic Motion X=0 X=A X=-A X=A; v=0; a=-amax X=0; v=-vmax; a=0 X=-A; v=0; a=amax X=0; v=vmax; a=0 X=A; v=0; a=-amax 32

What does moving in a circle have to do with moving back & forth in a straight line ?? x = R cos q = R cos (wt) since q = w t y x -R R  1 2 3 4 5 6 x 8 8 q R 7 7 34

SHM and Circles

Simple Harmonic Motion: x(t) = [A]cos(t) v(t) = -[A]sin(t) a(t) = -[A2]cos(t) x(t) = [A]sin(t) v(t) = [A]cos(t) a(t) = -[A2]sin(t) OR xmax = A vmax = A amax = A2 Period = T (seconds per cycle) Frequency = f = 1/T (cycles per second) Angular frequency =  = 2f = 2/T For spring: 2 = k/m 36

Example A 3 kg mass is attached to a spring (k=24 N/m). It is stretched 5 cm. At time t=0 it is released and oscillates. Which equation describes the position as a function of time x(t) = A) 5 sin(wt) B) 5 cos(wt) C) 24 sin(wt) D) 24 cos(wt) E) -24 cos(wt) Example: Given m,k and A and x(0), choose x(t), v(t), a(t), Calculate v_max and a_max, period, energy, K, U 39

Example A 3 kg mass is attached to a spring (k=24 N/m). It is stretched 5 cm. At time t=0 it is released and oscillates. What is the total energy of the block spring system? Example: Given m,k and A and x(0), choose x(t), v(t), a(t), Calculate v_max and a_max, period, energy, K, U 43

Example A 3 kg mass is attached to a spring (k=24 N/m). It is stretched 5 cm. At time t=0 it is released and oscillates. What is the maximum speed of the block? Example: Given m,k and A and x(0), choose x(t), v(t), a(t), Calculate v_max and a_max, period, energy, K, U 46

Example A 3 kg mass is attached to a spring (k=24 N/m). It is stretched 5 cm. At time t=0 it is released and oscillates. How long does it take for the block to return to x=+5cm? Example: Given m,k and A and x(0), choose x(t), v(t), a(t), Calculate v_max and a_max, period, energy, K, U 49

Pendulum Motion For small angles T = mg Tx = -mg (x/L) Note: F proportional to x! S Fx = m ax -mg (x/L) = m ax ax = -(g/L) x Recall for SHO a = -w2 x w = sqrt(g/L) T = 2 p sqrt(L/g) Period does not depend on A, or m! L T m x mg 37

Example: Clock If we want to make a grandfather clock so that the pendulum makes one complete cycle each sec, how long should the pendulum be?

Question 1 Suppose a grandfather clock (a simple pendulum) runs slow. In order to make it run on time you should: 1. Make the pendulum shorter 2. Make the pendulum longer 38

Summary Simple Harmonic Motion Springs Pendulum (Small oscillations) Occurs when have linear restoring force F= -kx x(t) = [A] cos(wt) v(t) = -[Aw] sin(wt) a(t) = -[Aw2] cos(wt) Springs F = -kx U = ½ k x2 w = sqrt(k/m) Pendulum (Small oscillations) w = sqrt(L/g) 50