Wave Physics PHYS 2023 Tim Freegarde.

Slides:



Advertisements
Similar presentations
Wave Physics PHYS 2023 Tim Freegarde. 2 Coming up in Wave Physics... local and macroscopic definitions of a wavetransverse waves on a string: wave equation.
Advertisements

Types, characteristics, properties
Physics 1025F Vibrations & Waves
Chapter 16 Wave Motion.
A disturbance that propagates Examples Waves on the surface of water
Physics 102 Waves Moza M. Al-Rabban Professor of Physics Lecture 3 Traveling Waves.
This lecture A wide variety of waves
Chapter 16 Waves (I) What determines the tones of strings on a guitar?
08/28/2013PHY Lecture 011 Light is electromagnetic radiation! = Electric Field = Magnetic Field Assume linear, isotropic, homogeneous media.
Chapter 16 Wave Motion.
Waves are everywhere: Earthquake, vibrating strings of a guitar, light from the sun; a wave of heat, of bad luck, of madness… Some waves are man-made:
Waves Traveling Waves –Types –Classification –Harmonic Waves –Definitions –Direction of Travel Speed of Waves Energy of a Wave.
Lattice Vibrations, Part I
Longitudinal Waves In a longitudinal wave the particle displacement is parallel to the direction of wave propagation. The animation above shows a one-dimensional.
Waves - I Chapter 16 Copyright © 2014 John Wiley & Sons, Inc. All rights reserved.
Wave Motion II Sinusoidal (harmonic) waves Energy and power in sinusoidal waves.
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.
Light and Matter Tim Freegarde School of Physics & Astronomy University of Southampton Classical electrodynamics.
Separate branches of Mechanics and Biomechanics I. Periodic Motion. Mechanical waves. Acoustics.
Wave motion and its equations Harmonic waves Waves on a string
Wave Physics Tim Freegarde School of Physics & Astronomy University of Southampton.
1 P1X: Optics, Waves and Lasers Lectures, Lecture 2: Introduction to wave theory (II) Phase velocity: is the same as speed of wave: o Phase velocity:
Wave Physics Tim Freegarde School of Physics & Astronomy University of Southampton.
Wave Physics PHYS 2023 Tim Freegarde. 2 Coming up in Wave Physics... local and macroscopic definitions of a wavetransverse waves on a string: wave equation.
Chapter 16 Lecture One: Wave-I HW1 (problems): 16.12, 16.24, 16.27, 16.33, 16.52, 16.59, 17.6, Due.
1 Honors Physics 1 Summary and Review - Fall 2013 Quantitative and experimental tools Mathematical tools Newton’s Laws and Applications –Linear motion.
Wave Physics PHYS 2023 Tim Freegarde.
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
Waves - I Chapter 16 Copyright © 2014 John Wiley & Sons, Inc. All rights reserved.
Wave Physics PHYS 2023 Tim Freegarde. 2 Thermal waves (diffusion) xx+δx use physics/mechanics to write partial differential wave equation for system insert.
H. SAIBI October 28 th, ©2008 by W.H. Freeman and Company Fig. Deep-Ocean Assessment and Reporting of Tsunamis (NOAA) in North Pacific.
Wave Physics PHYS 2023 Tim Freegarde.
EVAT 554 OCEAN-ATMOSPHERE DYNAMICS TIME-DEPENDENT DYNAMICS; WAVE DISTURBANCES LECTURE 21.
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.
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.
Chapter 16. Waves - I Waves are of three main types:
Wave Motion & EM Waves (II)
Chapter 14: 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.
1 Semester Review EP I. 2 1 Vector Addition Graphical Algebraic.
Springs Hooke’s Law (Fs) Spring Constant (k)
Wave Physics PHYS 2023 Tim Freegarde. 2 Coming up in Wave Physics... local and macroscopic definitions of a wavetransverse waves on a string: wave equation.
PHYSICAL CHEMISTRY - ADVANCED MATERIALS Particles and Waves Two opposing concepts Particle theory Field theory Quantum Mechanics Position, mass, velocity,
EE Audio Signals and Systems Wave Basics Kevin D. Donohue Electrical and Computer Engineering University of Kentucky.
Chapter 13 Wave Motion.
Light and Matter Tim Freegarde School of Physics & Astronomy University of Southampton Wave mechanics.
VibrationsandWaves. Ch. 14 examines wave motion and the oscillating, vibrating motion that creates them. This oscillating motion is known as periodic.
1 Reading: Main GEM Taylor 16.1, 16.2, 16.3 (Thornton 13.4, 13.6, 13.7) THE NON-DISPERSIVE WAVE EQUATION.
Oscillatory Motion Physics 7(A). Learning Objectives Examine and describe oscillatory motion Examine and describe wave propagation in various types 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.
Unit 1 C Work Energy Power. Forms of Energy Mechanical Mechanical focus for now focus for now chemical chemical electromagnetic electromagnetic nuclear.
SIMPLE HARMONIC OSCILLATION
SIMPLE HARMONIC OSCILLATION
Kinematics of Simple Harmonic Motion
Electromagnetic Waves in Vacuum
Waves: Intro Periodoic motion.
PHYS 172: Modern Mechanics Fall 2011
Wave Physics PHYS 2023 Tim Freegarde.
Wave Physics PHYS 2023 Tim Freegarde.
Waves Chapter 16: Traveling waves
Copyright © 2014 John Wiley & Sons, Inc. All rights reserved.
© 2014 John Wiley & Sons, Inc. All rights reserved.
Lecture 30 Wave Equation and solution (Chap.47)
Phase Velocity & Group Velocity.
Elastic Properties of Solids: A Brief Introduction
Classical Physics Describes objects and their interactions on a macroscopic scale Mechanics Electromagnetism Thermodynamics Seemingly very successful “There.
Waves Characteristics
A disturbance that propagates Examples Waves on the surface of water
THE NON-DISPERSIVE WAVE EQUATION
Presentation transcript:

Wave Physics PHYS 2023 Tim Freegarde

Coming up in Wave Physics... today’s lecture: local and macroscopic definitions of a wave transverse waves on a string: wave equation travelling wave solutions other wave systems: electromagnetic waves in coaxial cables shallow-water gravity waves sinusoidal and complex exponential waveforms

Wave Physics Local/microscopic definition: a collective bulk disturbance in which what happens at any given position is a delayed response to the disturbance at adjacent points speed of propagation is derived particles (Lagrange) fields (Euler) static dynamic equilibrium eg Poisson’s equation SHM WAVES Macroscopic definition: a time-dependent feature in the field of an interacting body, due to the finite speed of propagation of a causal effect speed of propagation is assumed

Wave Physics Local/microscopic definition: a collective bulk disturbance in which what happens at any given position is a delayed response to the disturbance at adjacent points speed of propagation is derived What is the net force on the penguin? rest position For an elastic penguin, Hooke’s law gives separation displacement If the penguin has mass , Newton’s law gives pressure elasticity density where

Waves on long strings

Solving the wave equation shallow waves on a long thin flexible string use physics/mechanics to write partial differential wave equation for system travelling wave insert generic trial form of solution wave velocity find parameter values for which trial form is a solution

Travelling wave solutions consider a wave shape at which is merely translated with time use physics/mechanics to write partial differential wave equation for system where insert generic trial form of solution use chain rule for derivatives find parameter values for which trial form is a solution

General solutions wave equation is linear – i.e. if use physics/mechanics to write partial differential wave equation for system are solutions to the wave equation, then so is insert generic trial form of solution arbitrary constants find parameter values for which trial form is a solution note that two solutions to our example:

Particular solutions fit general solution to particular constraints – e.g. use physics/mechanics to write partial differential wave equation for system insert generic trial form of solution x find parameter values for which trial form is a solution

Plucked guitar string x

Wave propagation transverse motion of taut string use physics/mechanics to write partial differential wave equation for system e-m waves along coaxial cable shallow-water waves flexure waves string with friction travelling wave: general form sinusoidal insert generic trial form of solution complex exponential damped standing wave soliton speed of propagation find parameter values for which trial form is a solution dispersion relation string motion from initial conditions

Wave equations waves are collective bulk disturbances, whereby the motion at one position is a delayed response to the motion at neighbouring points use physics/mechanics to write partial differential wave equation for system propagation is defined by differential equations, determined by the physics of the system, relating derivatives with respect to time and position insert generic trial form of solution e.g. find parameter values for which trial form is a solution but note that not all wave equations are of the same form

Electromagnetic waves aliexpress.com NASA/DOE/Fermi LAT Collaboration Light Radio Gamma radiation

Waves along a coaxial cable V(x) V(x+δx) r a I x -δQ δQ x x+δx

Waves along a coaxial cable r a x -δQ δQ x x+δx

Waves along a coaxial cable r a I x x x+δx

Water waves Ocean waves Severn bore Kelvin ship wake Tsunami www.fluidconcept.co.uk/Images/Uploads/capetown1-400-279.jpg theguardian.com © Jason Hawkes / Getty Images © Reuters / Mainichi Shimbun Ocean waves Severn bore Kelvin ship wake Tsunami

Shallow-water waves ε1 ε2 h(x) volume = h(x) (δx+ε2-ε1) δy v1 v2 δx

Shallow-water waves h(x) volume = h(x) (δx+ε2-ε1) δy v1 δx x-δx x x+δx

Velocities of waves on a string x x phase velocity (group velocity) transverse string velocity