How do we describe this? 10. Wave Motion. An initial shape… …so can we just let the normal modes oscillate at  n ? No! Because that initial shape can.

Slides:



Advertisements
Similar presentations
Ch 16 Wave Motion - I.
Advertisements

Meanings of the Derivatives. I. The Derivative at the Point as the Slope of the Tangent to the Graph of the Function at the Point.
Objectives Identify how waves transfer energy without transferring matter. Contrast transverse and longitudinal waves. Relate wave speed, wavelength, and.
Physics 1B03summer-Lecture 9 Test 2 - Today 9:30 am in CNH-104 Class begins at 11am.
Lecture 13 2 nd order partial differential equations Remember Phils Problems and your notes = everything Only.
Announcements 10/19/12 Prayer Learn Smart – info in Term project proposal due tomorrow Labs 4-5 also due tomorrow Exam 2: starting next Thurs a.
Sound Physics 202 Professor Lee Carkner Lecture 9.
Sound Physics 202 Professor Vogel (Professor Carkner’s notes, ed) Lecture 7.
Lecture 8 Topics Fourier Transforms –As the limit of Fourier Series –Spectra –Convergence of Fourier Transforms –Fourier Transform: Synthesis equation.
THIS LECTURE single From single to coupled oscillators.
Waves on a string THIS LECTURE Standing waves Standing waves Dispersive and non-dispersive waves Dispersive and non-dispersive waves.
Continuous String Take limit of h→0 and m/h→ r Wave Equation.
Earth’s Normal Modes. Fundamentals and Harmonics Remember, a guitar string can have a fundamental (lowest tone) and many harmonics (integer level multiples).
Longitudinal Waves In a longitudinal wave the particle displacement is parallel to the direction of wave propagation. The animation above shows a one-dimensional.
9.6 Other Heat Conduction Problems
Waves - I Chapter 16 Copyright © 2014 John Wiley & Sons, Inc. All rights reserved.
Longitudinal Standing Waves and Harmonic Series in Open and Closed Tubes Physics of Music, Spring 2015.
Position, Velocity, Acceleration, & Speed of a Snowboarder.
Mechanics & Mechanical wave phenomena
Chapter 18 Superposition and Standing Waves. Waves vs. Particles Waves are very different from particles. Particles have zero size.Waves have a characteristic.
Sound Waves Sound waves are divided into three categories that cover different frequency ranges Audible waves lie within the range of sensitivity of the.
FCI. Faculty of Computers and Information Fayoum University 2014/ FCI.
Waves Chapter 16:Traveling waves Chapter 18:Standing waves, interference Chapter 37 & 38:Interference and diffraction of electromagnetic waves.
Acoustic diffraction by an Oscillating strip. This problem is basically solved by a technique called Wiener Hopf technique.
The complex exponential function REVIEW. Hyperbolic functions.
Physics.
Fourier Series - Recap. Interpretation of Fourier series: expansion in an orthonormal basis. Analogy: orthonormal basis in 3-dimensional space:
MODULE 1 In classical mechanics we define a STATE as “The specification of the position and velocity of all the particles present, at some time, and the.
11/20/2015 Fourier Series Chapter /20/2015 Fourier Series Chapter 6 2.
Gratings and the Plane Wave Spectrum
Physics 1B03summer-Lecture 9
T T Standing Waves Progressive Waves Stretched string Newton’s 2nd Wave Equation.
Coupled Oscillations.
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.
Waves - I Chapter 16 Copyright © 2014 John Wiley & Sons, Inc. All rights reserved.
Q13. Oscillatory Motion Q14. Wave Motion
Motion Recognizing, Describing, and Measuring Motion.
1) depends on the speed of sound in the pipe 2) you hear the same frequency 3) you hear a higher frequency 4) you hear a lower frequency You blow into.
Wave Equation II and Solution. Length of the curved element.

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.
If wave 1 displaces a particle in the medium by D 1 and wave 2 simultaneously displaces it by D 2, the net displacement of the particle is simply D 1 +
Power Spectrum Analysis: Analysis of the power spectrum of the stream- function output from a numerical simulation of a 2- layer ocean model. Data Analysis.
WAVE PACKETS & SUPERPOSITION
Oscillations SHM 1 Simple harmonic motion defined Simple harmonic motion is the motion of any system in which the position of an object can be put in the.
Wave Motion Types of mechanical waves  Mechanical waves are disturbances that travel through some material or substance called medium for the waves. travel.
Wave Equation & Solutions Transverse Waves. Transverse wave on a string String Wave.
Transverse vs. Longitudinal Waves pg. 59. Objectives Compare the characteristics and behaviors of transverse waves and longitudinal waves. Physics terms.
Physics 141Mechanics Lecture 22 Waves Yongli Gao The propagation of oscillations, such as ripples on a pond, sound, radio, TV, is a physical phenomenon.
Foundations of Physics
University Physics: Waves and Electricity
University Physics: Waves and Electricity
Cart on Ramp Lab.
Progressive Waves Standing Waves T Stretched string Wave Equation
Copyright © 2014 John Wiley & Sons, Inc. All rights reserved.
© 2014 John Wiley & Sons, Inc. All rights reserved.
(Based on medium) 2. Mechanical Waves
Free oscillation modes Spheroidal mode (analogous to the P, SV and Rayleigh waves). Motions are parallel to the radial direction. Sensitive to gravity,
Developing Wave Equations
Combining Waves interference §
بسم الله الرحمن الرحيم FCI.
Intro to Oscillations Topics 4 and 10.
Coupled Oscillations 2/22/2019 Coupled Oscillators.
A Wave on a String String at rest.
Continua Continued More Useful: find Normal Mode solutions:
Wave Equation & Solutions
Two-Plate Waveguide Wave impedance TM mode
Consider a potential energy function as shown here.
Presentation transcript:

How do we describe this? 10. Wave Motion

An initial shape… …so can we just let the normal modes oscillate at  n ? No! Because that initial shape can do many things: 0 L To get the answer right, we have to get all the boundary conditions right!

Wave equation needs two spatial and two temporal boundary conditions. Clamped string: y(0,t) = 0 “a certain point in space for all time” y(L,t) = 0 Two spatial boundary conditions Two temporal boundary conditions Initial shape: y(x,0) = “a certain point in time for all space” rather than an analogous second point in time (which could work), try this: Initial velocity:

The velocities tell you how the normal modes move with different phase offset. But don’t do it this way!!!

French’s Fourier series! (spatial boundary conditions) Initially at rest? Then A n = 0