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2' Waves, the Wave Equation, and Phase Velocity

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A simpler equation for a harmonic wave: E(x,t) = A cos([kx wt] q) ... Life will get even simpler in a few minutes! Definitions: Amplitude and Absolute phase ... – PowerPoint PPT presentation

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Title: 2' Waves, the Wave Equation, and Phase Velocity


1
2. Waves, the Wave Equation, and Phase Velocity
  • What is a wave?
  • Forward f(x-vt) vs. backward f(xvt)
    propagating waves
  • The one-dimensional wave equation

Phase velocity Complex numbers
2
What is a wave?
  • A wave is anything that moves.
  • To displace any function f(x)
  • to the right, just change its
  • argument from x to x-a,
  • where a is a positive number.
  • If we let a v t, where v is positive
  • and t is time, then the displacement
  • will increase with time.
  • So f(x-vt) represents a rightward, or forward,
  • propagating wave.
  • Similarly, f(xvt) represents a leftward, or
    backward,
  • propagating wave.
  • v will be the velocity of the wave.

3
The one-dimensional wave equation
has the simple solution
  • where f(u) can be any twice-differentiable
    function.

4
Proof that f(xvt) solves the wave equation
  • 1. Write f(xvt) as f(u), where uxvt. So
    and
  •  
  • 2. Now, use the chain rule
  •  
  • 3. So Þ
    and Þ
  •   
  • 4. Substituting into the wave equation

QED
5
The 1D wave equation for light waves
  • Well use cosine- and sine-wave solutions
  •  
  • or
  • where

6
A simpler equation for a harmonic wave
  • E(x,t) A cos(kx wt q)
  • Use the trigonometric identity
  • cos(uv) cos(u)cos(v) sin(u)sin(v)
  • to obtain
  • E(x,t) A cos(kx wt) cos(q) A sin(kx
    wt) sin(q)
  • which is the same result as before, as long as
  • A cos(q) B and
    A sin(q) C
  • Life will get even simpler in a few minutes!

7
Definitions Amplitude and Absolute phase
  • E(x,t) A cos(kx wt q)
  • A Amplitude
  • q Absolute phase (or initial phase)

8
Definitions
  • Spatial quantities


Temporal quantities
9
The Phase Velocity
  • How fast is the wave traveling? Velocity is a
    reference distance
  • divided by a reference time.

The phase velocity is the wavelength /
period v l / t In terms of the
k-vector, k 2p/ l, and the angular frequency,
w 2p/ t, this is v w / k
10
The Phase of a Wave
  • The phase is everything inside the cosine.
  • E(t) A cos(j), where j
    kx wt q
  • We give the phase a special name because it comes
    up so often.
  • In terms of the phase,
  • w j/t
  • k j/x
  • and
  • j/t
  • v
  • j/x

11
Electromagnetism is linear The principle of
Superposition holds.
  • If E1(x,t) and E2(x,t) are solutions to Maxwells
    equations,
  • then E1(x,t) E2(x,t) is also a solution.
  •  
  • Proof and
  •  
  •  
  • Typically, one sine wave plus another equals a
    sine wave.
  •  
  • This means that light beams can pass through each
    other.
  •  
  • It also means that waves can constructively or
    destructively interfere.

12
Complex numbers
Consider a point, P (x,y), on a 2D Cartesian
grid.
Let the x-coordinate be the real part and the
y-coordinate the imaginary part of a complex
number.
  • So, instead of using an ordered pair, (x,y), we
    write
  • P x i y
  • A cos(j) i A sin(j)
  • where i (-1)1/2

13
Euler's Formula
  • exp(ij) cos(j)
    i sin(j)
  • so the point, P A cos(j) i A sin(j), can be
  • written
  • P A exp(ij)
  • where
  • A Amplitude
  • j Phase

14
Proof of Euler's Formula
  • exp(ij) cos(j) i
    sin(j)
  • Using Taylor Series

15
Complex number theorems
16
More complex number theorems
  • 1. Any complex number, z, can be written
  • z Re z i Im z
  • So
  • Re z 1/2 ( z z )
  • and
  • Im z 1/2i ( z z )
  • where z is the complex conjugate of z ( i
    i )
  • 2. The "magnitude," z, of a complex number is
  • z2 z z
  • 3. To convert z into polar form, A exp(ij)
  • A2 Re z 2 Im z 2
  • tan(j) Im z / Re z

17
We can also differentiate exp(ikx) as if the
argument were real.
18
Waves using complex numbers
  • The electric field of a light wave can be
    written
  • E(x,t) A cos(kx wt q)
  • Since exp(ij) cos(j) i sin(j), E(x,t) can
    also be written
  • E(x,t) Re A expi(kx wt q)
  • or
  • E(x,t) 1/2 A expi(kx wt q) c.c.
  • where " c.c." means "plus the complex
  • conjugate of everything before the plus sign."

19
The 3D wave equation for the electric field
  • or
  • which has the solution
  •  
  • where
  • and

20
Waves using complex amplitudes
  • We can let the amplitude be complex
  • where we've separated out the constant stuff from
    the rapidly changing stuff.
  • The resulting "complex amplitude" is
  • So
  • How do you know if E0 is real or complex?
  • Sometimes people use the "", but not always.
  • So always assume it's complex.
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