Sine and Cosine are the y and x components of a point on the rim of a rotating wheel.

Slides:



Advertisements
Similar presentations
Chapter 14 Vibrations and Wave.
Advertisements

Physics 1025F Vibrations & Waves
Energy of the Simple Harmonic Oscillator
ISAT 241 ANALYTICAL METHODS III Fall 2004 D. J. Lawrence
Waves and Sound.
Wave Properties Chapter 14.
Chapter 15 - Waves Traveling Waves –Types –Classification –Harmonic Waves –Definitions –Direction of Travel Speed of Waves Energy of a Wave Standing Waves.
Chapter 13 VibrationsandWaves. Hooke’s Law F s = - k x F s = - k x F s is the spring force F s is the spring force k is the spring constant k is the spring.
PHYS 218 sec Review Chap. 15 Mechanical Waves.
By Bhaskar Department of Physics K L University. Lecture 2 (28 July) Interference.
Longitudinal Waves In a longitudinal wave the particle displacement is parallel to the direction of wave propagation. The animation above shows a one-dimensional.
When an object moves back and forth, it is called a vibration
Vibrations and Waves Chapter 12.
Ch11 Waves. Period (T): The shortest time interval during which motion repeats. Measures of a Wave Time (s)
Objectives Identify the conditions of simple harmonic motion.
WAVES AND WAVE PHENOMENA Physics 12 Source: Giancoli Chapter 11.
Chapter 13 Vibrations and Waves.
Wave Motion WOD are underlined. Wave Motion WAVE: A transfer of energy or propagation of a disturbance. A wave is the motion of a disturbance All waves.
Chapter 11 Elasticity And Periodic Motion. Goals for Chapter 11 To follow periodic motion to a study of simple harmonic motion. To solve equations of.
Chapter 13 Vibrations and Waves. Hooke’s Law F s = - k x F s is the spring force k is the spring constant It is a measure of the stiffness of the spring.
Phys203 Basic Principles of Contemporary Physics Waves, Optics, and Modern Physics Alexander Dzyubenko
Ch14 Waves. Wave Types Mechanical Waves: require a material medium to propagate. WaterRope SpringsSound 3 types of Mechanical Waves –Transverse –Longitudinal.
Physics 11 Vibrations and Waves Mr. Jean December 15 th, 2014.
Chapter 13 VibrationsandWaves. Hooke’s Law F s = - k x F s = - k x F s is the spring force F s is the spring force k is the spring constant k is the spring.
For this section we start with Hooke’s Law. But we already learned this. (partially)
Chapter 12: Vibrations and Waves Section 1: Simple harmonic motion Section 2: Measuring simple harmonic motion Section 3: Properties of waves Section 4:
For this section we start with Hooke’s Law. But we already learned this. (partially)
Chapter 11:Vibrartions and Waves
© 2005 Pearson Prentice Hall This work is protected by United States copyright laws and is provided solely for the use of instructors in teaching their.
Physics.
Chapter 11 Preview Objectives Hooke’s Law Sample Problem
Wave Mechanics Physics 1. What is a wave? A wave is: an energy-transferring disturbance moves through a material medium or a vacuum.
Wave Motion. Conceptual Example: Wave and Particle Velocity Is the velocity of a wave moving along a cord the same as the velocity of a particle of a.
Chapter 12: Vibration and Waves 12.1 Simple Harmonic Motion.
CP Physics Chapter 12 Waves. Hooke’s Law F spring = kx During the periodic motion At equilibrium, velocity reaches a maximum (b) At maximum displacement,
Hooke’s Law F s = - k x F s is the spring force k is the spring constant It is a measure of the stiffness of the spring A large k indicates a stiff spring.
Lecture Outline Chapter 13 College Physics, 7 th Edition Wilson / Buffa / Lou © 2010 Pearson Education, Inc.
Wave Properties! By Corey Dyer.
Physics Vibrations and Waves 11.1 Simple Harmonic Motion 11.2 Energy in SHM 11.3 Period and sinusoidal nature of SHM 11.4 The Simple Pendulum.
Chapter 16: Waves and Sound  We now leave our studies of mechanics and take up the second major topic of the course – wave motion (though it is similar.
Chapter 13: Vibrations and Waves
Wave Characteristics and Speed. a traveling disturbance that carries energy through matter or space matter moves horizontally or vertically just a little,
Part 1 – Wave Characteristics. What is a Wave? A disturbance that carries energy through matter or space.
© 2014 Pearson Education, Inc. This work is protected by United States copyright laws and is provided solely for the use of instructors in teaching their.
Chapter 16 Waves-I Types of Waves 1.Mechanical waves. These waves have two central features: They are governed by Newton’s laws, and they can exist.
1 Animations from: Wikipedia and WAVES Antonio J. Barbero, Mariano.
Chapter 16 Waves-I Types of Waves 1.Mechanical waves. These waves have two central features: They are governed by Newton’s laws, and they can exist.
Vibrations & Waves Chapter 25 - This will be phun!
Waves. Simple Harmonic Motion  periodic motion - a motion that ________itself again and again along the same path  simple harmonic motion (SHM) - a.
Waves and Sound. A disturbance or oscillation that travels through space and matter, accompanied by a transfer of energy. Big Idea 6: Waves can transfer.
Chapter 11 Vibrations and Waves.
Physics 207: Lecture 29, Pg 1 Lecture 29Goals: Chapter 20, Waves Chapter 20, Waves Final test review on Wednesday. Final exam on Monday, Dec 20, at 5:00.
Chapter 13 Wave Motion.
Chapter 14 Vibrations and Waves. Hooke’s Law F s = - k x F s is the spring force k is the spring constant It is a measure of the stiffness of the spring.
Reference Book is. Introduction mechanical waves electromagnetic wavesMechanical waves Waves are two main types : mechanical waves and electromagnetic.
Chapter 17 – Mechanical Waves and Sound Mechanical Waves Water waves have two features common to all waves: 1. A wave is a traveling disturbance.
Chapter 13 Vibrations and Waves. Hooke’s Law F s = - k x F s is the spring force k is the spring constant It is a measure of the stiffness of the spring.
Simple Harmonic Motion
College Physics, 7th Edition
Unit 10: Part 1 Waves.
Vibrations and Waves Chapter 13.
MECHANICAL WAVES AND SOUND
Chapter 13 Vibrations and Waves.
Mechanical Waves A mechanical wave is a physical disturbance in an elastic medium. Consider a stone dropped into a lake. Energy is transferred from stone.
11-3: PROPERTIES OF WAVES.
11-3: PROPERTIES OF WAVES.
Phys2120 Basic Principles of Contemporary Physics Waves, Optics, and Modern Physics Alexander Dzyubenko © 2014.
CHAPTER-16 T071,T062, T061.
Vibrations and Waves.
Wave Properties.
Presentation transcript:

Sine and Cosine are the y and x components of a point on the rim of a rotating wheel

Degree and radians on the unit circle s (m) = r (m) * θ (radians) arclength = radius * radians

Periodic Function

Sinusoidal wave Amplitudes

Wavelength (meters) Wavelength defined between any two points on wave that are one cycle apart (2*pi radians). e.g., Peaks Zeros crossing Troughs Sin(θ) where θ is an point. Wavelength of a sine wave, λ, can be measured between any two points with the same phase, such as between crests, or troughs, or corresponding zero crossings as shown.sine wavephasezero crossings

Wave Period T (s) and Linear Frequency 1/T (s -1 ) Wave parameters T: wave period (s) λ: wave length (m) f=1/T : linear frequency 1 (2π /s -1 or cycles/s) Wave Velocity or Speed: v (m/s) = λ/T = λ * f Angular wave number: k = 2π/ λ Angular frequency: ω = 2π/ T = 2π*f Wave solution: u(x,t) = A * sin( k*x – ω *t ) (m) The period of a wave is the time interval for the wave to complete one cycle (2*pi radians). What is this waves period?

Wave snapshot in space and time

F(x,t) amplitude in space/time Wavelength Wave period

Translation (space or time) of Sinusoidal wave Horizontal axis units are radians/2*pi. if f(θ=w*t) = sin( w*t ) = sin( 2π*(t/T) ) >> t=T >> sin(2 π) if f(θ=k*x) = sin( k*x ) = sin( 2π*(x/λ) ) >> x= λ >> sin(2 π)

Phase of sinusoidal wave Three phase power: three sinusoids phase separated by 120 ⁰.

Phase advance/delay and Unit circle Note minus sign in phase argument. The red sine phase is behind (negative) the blue line phase; hence, red sin function leads the blue sin function.

Wavefront: where and what is it ?

Pulse wave versus Sinusoidal wave A pulse is a compact disturbance in space/time. A sinusoidal wave is NOT compact, it is everywhere in space/time. A pulse can be ‘built’ up mathematically as a sum of sinusoidal waves.

Superposition of wave pulses Which is the space (x) axis and which the time (t) axis?

Waves move KE/PE energy (not mass) in time

Longitudinal (P) vs. Transverse (S) waves: vibration versus energy transport direction

Water and Rayleigh waves particle motions Elastic medium Rayleigh surface wave Synchronized P-SV motions Retrograde Circular particle motion Acoustic medium (water) Prograde circular particle motion

Two different wavelength waves added Together: beating phenomena Two 1-dimensional wave pulse traveling And superimposing their amplitudes

Huygen’s wavelets: secondary wavefronts propagated to interfere constructively and destructively to make new time advanced wavefront

Standing waves on a string. Fixed endpoint don’t move; wave is trapped.

Harmonic motion: two forces out of phase A mechanical wave propagates a pulse/sinusoid of KE+PE energy because the inertial forces load the springs by pushing and pulling on the springs which permits the wave energy to propagated in time.