Lab 6: Forced Harmonic Motion  Driven harmonic oscillation Example: Atomic force microscope watch, circuit, …

Slides:



Advertisements
Similar presentations
Motion and Force A. Motion 1. Motion is a change in position
Advertisements

Lecture D31 : Linear Harmonic Oscillator
Lesson 1 - Oscillations Harmonic Motion Circular Motion
FCI. Prof. Nabila.M.Hassan Faculty of Computer and Information Basic Science department 2013/ FCI.
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.
Moza M. Al-Rabban Professor of Physics
Phy 212: General Physics II Chapter 15: Oscillations Lecture Notes.
Simple Harmonic Motion Physics 202 Professor Vogel (Professor Carkner’s notes, ed) Lecture 2.
Lab 5: Damped simple harmonic motion
Copyright © 2009 Pearson Education, Inc. Lecture 1 – Waves & Sound a) Simple Harmonic Motion (SHM)
Physics 101: Lecture 20, Pg 1 Lecture 20: Ideal Spring and Simple Harmonic Motion l New Material: Textbook Chapters 10.1 and 10.2.
Oscillations An oscillation is a repetitive to-and- fro movement. There are two types of vibration: free and forced. A forced vibration is produced when.
Oscillation.
Chapter 13 Oscillatory Motion.
S1-1 SECTION 1 REVIEW OF FUNDAMENTALS. S1-2 n This section will introduce the basics of Dynamic Analysis by considering a Single Degree of Freedom (SDOF)
13. Oscillatory Motion. Oscillatory Motion 3 If one displaces a system from a position of stable equilibrium the system will move back and forth, that.
Motion of a mass at the end of a spring Differential equation for simple harmonic oscillation Amplitude, period, frequency and angular frequency Energetics.
Harmonic Oscillation 1. If a force F acts on a spring, the length x changes. The change is proportional to the restoring force (Hooke’s Law). A spring.
Wave Motion II Sinusoidal (harmonic) waves Energy and power in sinusoidal waves.
Damped Oscillations (Serway ) Physics 1D03 - Lecture 35.
Chapter 13: Oscillatory Motions
Energy of the Simple Harmonic Oscillator. The Total Mechanical Energy (PE + KE) Is Constant KINETIC ENERGY: KE = ½ mv 2 Remember v = -ωAsin(ωt+ ϕ ) KE.
Oscillators. An oscillator is any measurable quantity capable of repetition. Examples: Volume of a loudspeaker Brightness of a bulb Amount of money in.
P Class 26: Outline Hour 1: Driven Harmonic Motion (RLC) Hour 2: Experiment 11: Driven RLC Circuit.
OSCILLATIONS Chapter 15. Simple Harmonic Motion (SHM) Systems.
Oscillators fall CM lecture, week 4, 24.Oct.2002, Zita, TESC Review simple harmonic oscillators Examples and energy Damped harmonic motion Phase space.
15.1 Motion of an Object Attached to a Spring 15.1 Hooke’s law 15.2.
Associate Professor: C. H.L IAO. Contents:  3.1 Introduction 99  3.2 Simple Harmonic Oscillator 100  3.3 Harmonic Oscillations in Two Dimensions 104.
Ch1 Examples.
Copyright © 2010 Pearson Education, Inc. Lecture Outline Chapter 13 Physics, 4 th Edition James S. Walker.
Copyright © 2009 Pearson Education, Inc. Chapter 14 Oscillations.
Simple Harmonic Oscillator and SHM A Simple Harmonic Oscillator is a system in which the restorative force is proportional to the displacement according.
SHM is the projection of uniform circular motion The ball mounted on the turntable moves in uniform circular motion, and its shadow, projected on a moving.
Chapter 14 - Oscillations
Chapter 12 Oscillations. 2 Mechanical oscillations: pendulum, string of a guitar, vocal cords, … More general oscillations: Electrical, optical, atomic,
11/11/2015Physics 201, UW-Madison1 Physics 201: Chapter 14 – Oscillations (cont’d)  General Physical Pendulum & Other Applications  Damped Oscillations.
Chapter 1 - Vibrations Harmonic Motion/ Circular Motion Simple Harmonic Oscillators –Linear, Mass-Spring Systems –Initial Conditions Energy of Simple Harmonic.
Simple Harmonic Motion and Elasticity The Ideal Spring and Simple Harmonic Motion spring constant Units: N/m.
Vibrations & Waves. In the example of a mass on a horizontal spring, m has a value of 0.80 kg and the spring constant, k, is 180 N/m. At time t = 0 the.
Simple Harmonic Motion: SHM
Fluid Dynamics How does conservation of mass apply in a fluid? How does conservation of energy apply in a fluid? What is laminar flow? What is turbulence.
PH 421: Oscillations - do not distribute
1 Honors Physics 1 Lecture 21 - F2013 Waves –Terms –Travelling waves –Waves on a string.
1FCI. Prof. Nabila.M.Hassan Faculty of Computer and Information Basic Science department 2012/2013 2FCI.
Vibrations and Waves Hooke’s Law Elastic Potential Energy Simple Harmonic Motion.
Ball in a Bowl: F g F N F g F N  F  F Simple Harmonic Motion (SHM) Stable Equilibrium (restoring force, not constant force)
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.
Oscillations Readings: Chapter 14.
Damped Free Oscillations
Physics 1D03 - Lecture 331 Harmonic Motion ( II ) (Serway 15.2, 15.3) Mass and Spring Energy in SHM.
Damped harmonic oscillator
Simple Harmonic Motion
1 10. Harmonic oscillator Simple harmonic motion Harmonic oscillator is an example of periodic motion, where the displacement of a particle from.
Graphical analysis of SHM
PA114 Waves and Quanta · Unit 1: Oscillations PA114 Waves and Quanta Unit 1: Oscillations and Oscillators (Introduction) Tipler, Chapter 14
Announcements Midterm Exam next Friday In class, ~1 hr. Closed book, one page of notes Bring a calculator (not phone, computer, iPad, etc.) Practice problems.
1© Manhattan Press (H.K.) Ltd. Forced oscillation Resonance Resonance 7.8 Forced oscillation and resonance Experiments for forced oscillation and resonance.
Waves and Quanta PA114 Unit 1: Oscillations and Oscillators
Applications of SHM and Energy
10. Harmonic oscillator Simple harmonic motion
PH421: Oscillations; do not distribute
Oscillations Readings: Chapter 14.
10.4 The Pendulum.
Motion and Force A. Motion 1. Motion is a change in position
Damped Oscillations.
Harmonic Motion (II) Mass and Spring Energy in SHM
Lecture Outline Chapter 13 Physics, 4th Edition James S. Walker
Chapter 15 Oscillations.
HARMONIC MOTION.
Chapter 15 - Oscillations
Presentation transcript:

Lab 6: Forced Harmonic Motion  Driven harmonic oscillation Example: Atomic force microscope watch, circuit, …

A constant energy flow at steady state

Forced harmonic oscillation (steady state)

Forced harmonic oscillation (cont.)

Amplitude of displacement: Amplitude of velocity:

Amplitude peaks at  0  resonance

v max peaks at  0  resonance

Phase changes sharply at resonance

Forced harmonic oscillation (log scale)

Energy that flows in (drive) The power P supplied by F is: The average over one cycle is power factor

Energy that flows out (dissipation) The power P dissipated by F d is: The average over one cycle is

Maximal power and quality factor Quality factor: Quality factor is also a measure of the “sharpness” of resonance

Lab 6: Forced Harmonic Motion For each measurement allow enough time for the system to reach steady state after you changed the rotation speed.

v max peaks at  0  resonance

How to measure phase? (Lock-in method) From data:

How to measure phase? (Lock-in method) Find out F 0 and A; Create a column with value Fx=F(t)  x(t); Sum over the column to find cos  Here N is the total number of the data points