-Damped and Forces Oscillations -Resonance AP Physics C Mrs. Coyle.

Slides:



Advertisements
Similar presentations
Oscillations and Simple Harmonic Motion:
Advertisements

Coulomb or Dry Friction Damping.
Ch 3.8: Mechanical & Electrical Vibrations
Damped Oscillators SHO’s: Oscillations  “Free oscillations” because once begun, they will never stop! In real physical situations & for real physical.
Self-Inductance and Circuits
Lesson 1 - Oscillations Harmonic Motion Circular Motion
Oscillations Simple Harmonic Motion Velocity and Acceleration in SHM
FCI. Prof. Nabila.M.Hassan Faculty of Computer and Information Basic Science department 2013/ FCI.
Chapter 13 Periodic Motion. Special Case: Simple Harmonic Motion (SHM)
SHM SHM australia
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.
Ch 3.9: Forced Vibrations We continue the discussion of the last section, and now consider the presence of a periodic external force:
Damped Harmonic Motion State what is meant by damping. If a mass on the end of a spring is pulled down and released it will continue to oscillate.
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.
 All objects have a NATURAL FREQUENCY at which they tend to vibrate. This frequency depends on the material the object is made of, the shape, and many.
Oscillations and Waves Forced Oscillations and Resonance.
1© Manhattan Press (H.K.) Ltd. 7.9 Examples of forced vibration.
Damped Oscillations (Serway ) Physics 1D03 - Lecture 35.
Chapter 19 MECHANICAL VIBRATIONS
Chapter 12 Oscillatory Motion. Periodic Motion Periodic motion is motion of an object that regularly repeats The object returns to a given position after.
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.
Chapter 12 Oscillatory Motion.
Vibration and Waves AP Physics Chapter 11.
Welastic = 1/2 kx02 - 1/2 kxf2 or Initial elastic potential energy minus Final elastic potential energy.
Vibrations and Waves AP Physics Lecture Notes m Vibrations and Waves.
Simple Pendulum A simple pendulum also exhibits periodic motion A simple pendulum consists of an object of mass m suspended by a light string or.
Chapter 15 Oscillatory Motion.
Chapter 15 Oscillatory Motion. Intro Periodic Motion- the motion of an object that regularly repeats There is special case of periodic motion in which.
. Physics 207, Lecture 19, Nov. 5 Goals: Chapter 14 Chapter 15
Copyright © 2010 Pearson Education, Inc. Lecture Outline Chapter 13 Physics, 4 th Edition James S. Walker.
Monday, Dec. 1, 2003PHYS , Fall 2003 Dr. Jaehoon Yu 1 PHYS 1443 – Section 003 Lecture #23 Monday, Dec. 1, 2003 Dr. Jaehoon Yu 1.Simple Harmonic.
Chapter 14 - Oscillations
1 Lecture D32 : Damped Free Vibration Spring-Dashpot-Mass System Spring Force k > 0 Dashpot c > 0 Newton’s Second Law (Define) Natural Frequency and Period.
11/11/2015Physics 201, UW-Madison1 Physics 201: Chapter 14 – Oscillations (cont’d)  General Physical Pendulum & Other Applications  Damped Oscillations.
Chapter 15 Oscillatory Motion. Periodic Motion Periodic motion is motion of an object that regularly repeats The object returns to a given position after.
CHAPTER - 3 FORCED OSCILLATOR Mrs. Rama Arora Assoc. Professor Deptt. Of Physics PGGCG-11 Chandigarh.
Periodic Motion 1 Chapter 15 Oscillatory Motion April 17 th, 2006.
PH 421: Oscillations - do not distribute
Chapter 8 Vibration A. Free vibration  = 0 k m x
Oscillatory motion (chapter twelve)
Chapter 15 Oscillatory Motion.
1FCI. Prof. Nabila.M.Hassan Faculty of Computer and Information Basic Science department 2012/2013 2FCI.
Damped and Forced Oscillations
Chapter 15 Oscillatory Motion.
Simple Harmonic Motion
CHAPTER 23 WAVES 23.1 Harmonic Motion pp
Oscillations Readings: Chapter 14.
Damped Free Oscillations
Damped harmonic oscillator
Simple Harmonic Motion (SHM). Simple Harmonic Motion – Vibration about an equilibrium position in which a restoring force is proportional to displacement.
DEFINITION ENERGY TRANSFER As the object oscillates it will exchange kinetic energy and potential energy. At the midpoint, kinetic energy will be highest.
-Simple Pendulum -Damped and Forced Oscillations -Resonance AP Physics C Mrs. Coyle Mrs. Coyle.
1© Manhattan Press (H.K.) Ltd. Forced oscillation Resonance Resonance 7.8 Forced oscillation and resonance Experiments for forced oscillation and resonance.
PHY 151: Lecture Motion of an Object attached to a Spring 15.2 Particle in Simple Harmonic Motion 15.3 Energy of the Simple Harmonic Oscillator.
PHY238Y Lecture 3 Damped oscillations Forced oscillations. Resonance References: Halliday, Resnick, Walker: Fundamentals of Physics, 6 th edition, John.
Voronkov Vladimir Vasilyevich
Lecture No. 2: Damped Oscillations, Driven Oscillations and Resonance
MAE 82 – Engineering Mathematics
Ch 3.9: Forced Vibrations We continue the discussion of the last section, and now consider the presence of a periodic external force:
Oscillations Readings: Chapter 14.
Vibrations & Waves Part 1: Periodic Motion.
SHM: Damping Effects Pages
Damped Oscillations.
Damped and driven oscillations
Lecture Outline Chapter 13 Physics, 4th Edition James S. Walker
ME321 Kinematics and Dynamics of Machines
VIBRATIONS NATURAL VIBRATIONS DAMPED VIBRATIONS FORCED VIBRATIONS.
Physics : Oscillatory Motion
Chapter 15: Oscillatory motion
Free and Damped Oscillations
Presentation transcript:

-Damped and Forces Oscillations -Resonance AP Physics C Mrs. Coyle

Objectives Identify and analyze forced and damped oscillations. Develop a qualitative understanding of resonance Identify situations in which a system will resonate in response to a sinusoidal external force.

Damped Oscillations Non conservative forces are present (ex:friction, resistive forces, damping forces by a “dashpot” device). The amplitude and thus the mechanical energy is reduced over time.

Solution: Damped Oscillation- Ex 1  F x = -k x – bv = ma Equation of Motion:

Damped Oscillation The amplitude is reduced over time and eventually the oscillation stops.

Damped Oscillation- Ex 2 Resistive (retarding force), R R = - b v where b is a constant called the damping coefficient  F x = -k x – bv x = ma x Equation of Motion: Solution viscous liquid

Types of Damping A.Underdamped If R max = bv max < kA B.Critically damped When b reaches a critical value b c such that b c / 2 m = k/m=  0 2, the system will not oscillate (quick return to equilibrium). is called the natural frequency C.Overdamped If R max = bv max > kA and b/2m >  0 (return to equilibrium without oscillation).

Video of dampers zrzI zrzI

Forced vibrations: when an external force causes a system to oscillate External Force  F x =

Amplitude of a forced (driven) oscillation: –  0 is the natural frequency of the undamped oscillator

How can a damped system have an undamped motion (no decrease in amplitude)? To compensate for the loss of mechanical energy due to the resistive force, apply a forced vibration of equal energy.

Resonance: increase in amplitude due to addition of an external force. When the frequency of the driving force is near the natural frequency (   ) an increase in amplitude occurs The natural frequency   is also called the resonance frequency of the system

At resonance the applied force and v are both proportional to sin (  t +  ), so force and velocity are in phase. The power transferred to the oscillator (P=F. v) is a maximum at resonance.

Takoma Narrows Bridge: collapses in November, 1940, under 42mph winds (opened in July 1940) u7Ok u7Ok