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Wave Motion & EM Waves (II)

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Presentation on theme: "Wave Motion & EM Waves (II)"— Presentation transcript:

1 Wave Motion & EM Waves (II)
Chih-Chieh Kang Electrooptical Eng.Dept. STUT

2 Sinusoidal Traveling Waves

3 Sinusoidal Waves Snapshot of a traveling sinusoidal wave (at a fixed time, t = 0), and 0=0 Vertical displacement of the traveling wave: Wavelength  :the distance between two successive crests or troughs. Amplitude A:one half the wave height or the distance from either the crest or the trough to the equilibrium points Phase  = 2z/

4 Sinusoidal Traveling Waves
A wave does not change its shape as it travels through space. For a traveling sinusoidal wave moving at a speed v, the wave function  at some later time t :

5 Phase Lead & Phase Lag (Ulaby)

6 Sinusoidal Traveling Waves
For the time a wave traveling a distance of one wavelength is called period T The frequency of a sinusoidal wave f

7 Sinusoidal Traveling Waves
The angular wave number (or propagation number) of a sinusoidal wave k  Wave function

8 Harmonic Traveling Waves
For a traveling sinusoidal wave (at a fixed point z = 0) angular frequency=2/T=2f  wave function

9 Speed of a Wave For a traveling wave, its waveform retains the same phase Phase velocity v : the velocity of the waveform as it moves across the medium

10 Mathematical Description of a Wave
Waves are solutions to the wave equation: 1-D waves :wave function, v:phase velocity - Where does wave equation come from? - What do solutions look like? - How much energy do they carry?

11 Wave Equation for a String
Each small piece of string obeys Newton’s Law: Small displacement, so Net force is proportional to curvature:

12 Wave Equation for a String
Newton’s 2nd Law… >>(mass density …leads to the wave equation with - wave function=transverse displacement - phase velocity <-restoring force <-inertia

13 Solutions of 1-D Wave Equation
Consider

14 Solutions of 1-D Wave Equation
 is a solution the same reason, is a solution is a solution too any linear combination of solutions is also a solution : superposition

15 Description of Traveling Waves
waves traveling in the +z direction no change in shape point P moving with time

16 1-D Harmonic Traveling Waves
1-D time-harmonic traveling waves propagating in the +z direction /v = 2f / f = 2/= k : Angular wave number

17 1-D Harmonic Traveling Waves
Complex representation of harmonic traveling waves propagating in +z direction  If

18 References F. T. Ulaby, Fundamentals of Applied Electromagnetics, Prentice Hall. J. D. Cutnell, and K. W. Johnson, Physics, Wiley.


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