The Physical Pendulum Damped Oscillations Forced Oscillations

Slides:



Advertisements
Similar presentations
Harmonic Motion Chapter 13.
Advertisements

1 Simple harmonic motion displacement velocity = dx/dt acceleration = dv/dt LECTURE 3 CP Ch 14 CP449.
Problmes-1.
Simple pendulum Physical pendulum Diatomic molecule Damped oscillations Driven oscillations Lecture 24: General Oscillations.
Dr. Jie Zou PHY 1151G Department of Physics1 Chapter 13 Oscillations About Equilibrium (Cont.)
Chapter 14 Oscillations Chapter Opener. Caption: An object attached to a coil spring can exhibit oscillatory motion. Many kinds of oscillatory motion are.
P H Y S I C S Chapter 7: Waves and Vibrations Section 7B: SHM of a Pendulum.
Oscillation.
Measuring Simple Harmonic Motion
Measuring Simple Harmonic Motion
Harmonic Motion AP Physics C.
Physics 6B Oscillations Prepared by Vince Zaccone
Chapter 15– Oscillations I.Simple harmonic motion (SHM) - Velocity - Acceleration II. Force law for SHM - Simple linear harmonic oscillator - Simple linear.
Damped Oscillations (Serway ) Physics 1D03 - Lecture 35.
Chapter 13: Oscillatory Motions
Welastic = 1/2 kx02 - 1/2 kxf2 or Initial elastic potential energy minus Final elastic potential energy.
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.
Physics. Simple Harmonic Motion - 3 Session Session Objectives.
The Simple Pendulum A simple pendulum consists of a mass at the end of a lightweight cord. We assume that the cord does not stretch, and that its mass.
SHM occurs when an object oscillates back and forth over the same path. Examples 1. 2.
Copyright © 2010 Pearson Education, Inc. Lecture Outline Chapter 13 Physics, 4 th Edition James S. Walker.
Copyright © 2009 Pearson Education, Inc. Chapter 14 Oscillations.
Chapter 15 Oscillatory Motion.
Copyright © 2009 Pearson Education, Inc. Oscillations of a Spring Simple Harmonic Motion Energy in the Simple Harmonic Oscillator The Simple Pendulum Lecture.
When a weight is added to a spring and stretched, the released spring will follow a back and forth motion.
Simple Harmonic Motion. Restoring Forces in Spring  F=-kx  This implies that when a spring is compressed or elongated, there is a force that tries to.
Simple Harmonic Motion
Simple Harmonic Motion and Elasticity The Ideal Spring and Simple Harmonic Motion spring constant Units: N/m.
Chapter 15 Oscillations. Periodic motion Periodic (harmonic) motion – self-repeating motion Oscillation – periodic motion in certain direction Period.
Chapter 13. Simple Harmonic Motion A single sequence of moves that constitutes the repeated unit in a periodic motion is called a cycle The time it takes.
Oscillatory motion (chapter twelve)
Wednesday, Nov. 20, 2002PHYS , Fall 2002 Dr. Jaehoon Yu 1 PHYS 1443 – Section 003 Lecture #19 Monday, Nov. 20, 2002 Dr. Jaehoon Yu 1.Energy of.
When a weight is added to a spring and stretched, the released spring will follow a back and forth motion.
Periodic Motions.
Chapter 11: Harmonic Motion
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.
Oscillations. Definitions Frequency If an object vibrates or oscillates back and forth over the same path, each cycle taking the same amount of time,
Chapter 11 Vibrations and Waves. Simple harmonic motion Measuring simple harmonic motion Properties of waves Wave interactions.
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 Section 11.2 Apply properties of pendulums and springs A pendulum exhibits harmonic motion. A complete cycle is called an oscillation. The maximum.
Copyright © 2010 Pearson Education, Inc. Lecture Outline Chapter 13 Physics, 4 th Edition James S. Walker.
PHY 151: Lecture Motion of an Object attached to a Spring 12.2 Particle in Simple Harmonic Motion 12.3 Energy of the Simple Harmonic Oscillator.
Simple Harmonic Motion (SHM). Simple Harmonic Motion – Vibration about an equilibrium position in which a restoring force is proportional to displacement.
Units of N/m m 2 = N m = J  Total potential energy is Example: Problem A block (m = 1.7 kg) and a spring (k = 310 N/m) are on a frictionless incline.
PHYS 1443 – Section 003 Lecture #22
When a weight is added to a spring and stretched, the released spring will follow a back and forth motion.
Periodic Motion Oscillations: Stable Equilibrium: U  ½kx2 F  kx
Period of Simple Harmonic Motion
Simple Harmonic Motion
Oscillatory Motion.
Harmonic Motion AP Physics C.
Oscillations Readings: Chapter 14.
The Simple Pendulum A simple pendulum consists of a mass at the end of a lightweight cord. We assume that the cord does not stretch, and that its mass.
A mass m = 2.0 kg is attached to a spring having a force constant k = 990 N/m as in the figure. The mass is displaced from its equilibrium position.
Ch. 12 Waves pgs
Harmonic Motion AP Physics C.
Lecture Outline Chapter 13 Physics, 4th Edition James S. Walker
Measuring Simple Harmonic Motion
Harmonic Motion AP Physics C.
Differential Equations
VIBRATION.
VIBRATION.
Chapter 15 Oscillations.
Chapter 15: Oscillatory motion
Periodic Motion Oscillations: Stable Equilibrium: U  ½kx2 F  -kx
Harmonic Motion AP Physics C.
Harmonic Motion AP Physics C.
Simple Harmonic Motion
Simple Harmonic Motion and Wave Interactions
Presentation transcript:

The Physical Pendulum Damped Oscillations Forced Oscillations Chapter 12 – part C The Physical Pendulum Damped Oscillations Forced Oscillations

In-phase and quadrature components of motion     Interesting properties:            

The forced and damped harmonic oscillator       For X:…   For Y:…   From the last one and considering the relation between sin and cos:    

From the X equation, one can work out A:   Replacing cos j and sin j:  

Exercise 12.28 28. A very light rigid rod with a length of 0.500 m extends straight out from one end of a meter stick. The stick is suspended from a pivot at the far end of the rod and is set into oscillation. (a) Determine the period of oscillation. (b) By what percentage does the period differ from the period of a simple pendulum 1.00 m long?

Exercise 12.31 31. A pendulum with a length of 1.00 m is released from an initial angle of 15.0°. After 1 000 s, its amplitude has been reduced by friction to 5.50°. What is the value of b/2m?

Exercise 12.31 33. A 2.00-kg object attached to a spring moves without friction and is driven by an external force F = (3.00 N) sin(2πt). Assuming that the force constant of the spring is 20.0 N/m, determine (a) the period and (b) the amplitude of the motion.

Exercise 12.24 24. The angular position of a pendulum is represented by the equation θ = (0.032 0 rad) cos ωt, where θ is in radians and ω = 4.43 rad/s. Determine the period and length of the pendulum.

Exercise 12.36 36. Damping is negligible for a 0.150-kg object hanging from a light 6.30-N/m spring. A sinusoidal force with an amplitude of 1.70 N drives the system. At what frequency will the force make the object vibrate with an amplitude of 0.440 m?

Exercise 12.49 49. A horizontal plank of mass m and length L is pivoted at one end. The plank’s other end is supported by a spring of force constant k. The moment of inertia of the plank about the pivot is . The plank is displaced by a small angle θ from its horizontal equilibrium position and released. (a) Show that it moves with simple harmonic motion with an angular frequency . (b) Evaluate the frequency, assuming that the mass is 5.00 kg and that the spring has a force constant of 100 N/m.