Forced Oscillations Solution=Complementary Function +

Slides:



Advertisements
Similar presentations
Response Of Linear SDOF Systems To Harmonic Excitation
Advertisements

CHAPTER 4: HARMONIC RESPONSE WITH A SINGLE DEGREE OF FREEDOM
Lesson 1 - Oscillations Harmonic Motion Circular Motion
Resonance. External Force  Dynamical systems involve external forces. Arbitrary force F(q, t)Arbitrary force F(q, t) Small oscillations only F(t)Small.
Lab 5: Damped simple harmonic motion
ECE 201 Circuit Theory I1 Sinusoidal response of circuits The switch is closed at t = 0. Determine the current i(t) for t >= 0. i(t)
Van der Pol. Convergence  The damped driven oscillator has both transient and steady-state behavior. Transient dies outTransient dies out Converges to.
Resonance. External Force  External forces can be included in the Lagrangian. Arbitrary force F(q, t)Arbitrary force F(q, t) Small oscillations only.
Chapter 13 Oscillatory Motion.
 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.
Motion of a mass at the end of a spring Differential equation for simple harmonic oscillation Amplitude, period, frequency and angular frequency Energetics.
 Somnath Bharadwaj and Pratik Khastgir, Department of Physics and Meteorology, IIT Kharagpur, India  Somnath.
 Somnath Bharadwaj and Pratik Khastgir, Department of Physics and Meteorology, IIT Kharagpur, India Electromagnetic.
USSC3002 Oscillations and Waves Lecture 6 Forced Oscillations Wayne M. Lawton Department of Mathematics National University of Singapore 2 Science Drive.
Chapter 19 MECHANICAL VIBRATIONS
 Somnath Bharadwaj and Pratik Khastgir, Department of Physics and Meteorology, IIT Kharagpur, India  Somnath.
15.1 Motion of an Object Attached to a Spring 15.1 Hooke’s law 15.2.
Chapter 14 Outline Periodic Motion Oscillations Amplitude, period, frequency Simple harmonic motion Displacement, velocity, and acceleration Energy in.
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.
 Somnath Bharadwaj and Pratik Khastgir, Department of Physics and Meteorology, IIT Kharagpur, India  Somnath.
Chapter 1 - Vibrations Harmonic Motion/ Circular Motion Simple Harmonic Oscillators –Linear, Mass-Spring Systems –Initial Conditions Energy of Simple Harmonic.
1 Waves 2 Lecture 2 - Background from 1A Revision: Resonance and Superposition D Aims: ëContinue our review of driven oscillators: > Velocity resonance;
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.
CHAPTER - 3 FORCED OSCILLATOR Mrs. Rama Arora Assoc. Professor Deptt. Of Physics PGGCG-11 Chandigarh.
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.
Chapter 8 Vibration A. Free vibration  = 0 k m x
 Somnath Bharadwaj and Pratik Khastgir, Department of Physics and Meteorology, IIT Kharagpur, India Electromagnetic.
 Somnath Bharadwaj and Pratik Khastgir, Department of Physics and Meteorology, IIT Kharagpur, India Electromagnetic.
 Somnath Bharadwaj and Pratik Khastgir, Department of Physics and Meteorology, IIT Kharagpur, India Electromagnetic.
Lab 6: Forced Harmonic Motion  Driven harmonic oscillation Example: Atomic force microscope watch, circuit, …
APHY201 1/30/ Simple Harmonic Motion   Periodic oscillations   Restoring Force: F = -kx   Force and acceleration are not constant  
Damped Forced Oscillations Coupled Oscillations 1.
 Somnath Bharadwaj and Pratik Khastgir, Department of Physics and Meteorology, IIT Kharagpur, India  Somnath.
Forced Oscillation.
Damped Free Oscillations
Damped Oscillations 1.
Damped harmonic oscillator
K m b Damped SHM “Damping Constant” (kg/s) “Damping Parameter” (s -1 ) “Natural Frequency” (rad/s) EOM: damped oscillator.
1© Manhattan Press (H.K.) Ltd. Forced oscillation Resonance Resonance 7.8 Forced oscillation and resonance Experiments for forced oscillation and resonance.
Wave Equation & Solutions Transverse Waves. Transverse wave on a string String Wave.
Book Reference : Pages To Understand resonance 2.To be able to qualitatively explain how a system behaves at resonance and on either side of resonance.
A PRESENTATION ON VIBRATION
13.1 Harmonic Motion 1.
B. T remains the same and vmax doubles.
Lecture No. 2: Damped Oscillations, Driven Oscillations and Resonance
Physics 8.03 Vibrations and Waves
Resonance Learning Objectives To Understand resonance
The Electromagnetic Spectrum
Sinusoidal response of circuits
SHM: Damping Effects Pages
13.3 Resonance and Energy 1.
Sinusoidal Plane Waves
Damped Oscillations.
Forced Oscillations Damped
PHYSICS 1 Interference What happens when two waves are superposed?
Physics A First Course Vibrations, Waves, and Sound Chapter 19.
PHYSICS 1 External Forcing Why this particular type of force?
PHYSICS 1 Chain of Oscillators Maxima
Light -wave or particle?
ME321 Kinematics and Dynamics of Machines
Hour 12 Driven Harmonic Oscillators
PHYSICS 1 Resonance Electrical Circuits
X y y = x2 - 3x Solutions of y = x2 - 3x y x –1 5 –2 –3 6 y = x2-3x.
Chapter 15 Oscillations.
Wave Equation & Solutions
5.1 Oscillations Oscillation: any general movement that repeats itself
WEEKS 8-9 Dynamics of Machinery
Undamped Forced Oscillations
Sinusoidal response of circuits
Presentation transcript:

Forced Oscillations Solution=Complementary Function + Particular Integral

Solutions Complementary Functions are transients Steady State behaviour is decided by the Particular Integral

Solution with Damping

Amplitude and Phase (again)

Amplitude and Phase (again) -

Some Key Points High frequency and low frequency behaviour unchanged by damping Amplitude is finite throughout Maximum Amplitude at

PHYSICS 1 Average Energy Somnath Bharadwaj and Pratik Khastgir, Department of Physics and Meteorology, IIT Kharagpur, 721 302 India http://www.cts.iitkgp.ernet.in/~phy1/

Average Energy Plot

Mild Damping Maxima at

Mild Damping Maxima at Lorentzian Profile

FWHM FHWM=

Power

Average Power Using

Average Power

Mild Damping Lorentzian Profile

Average Power