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Propagation of waves

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Imagine a disturbane that results in waves propagating equally in all directions. E.g. sound wave source in air or water, light source in a dielectric medium etc. ... – PowerPoint PPT presentation

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Title: Propagation of waves


1
Propagation of waves
  • Friday October 18, 2002

2
Propagation of waves in 3D
  • Imagine a disturbane that results in waves
    propagating equally in all directions
  • E.g. sound wave source in air or water, light
    source in a dielectric medium etc..
  • The generalization of the wave equation to
    3-dimensions is straight forward if the medium is
    homogeneous
  • Let ? amplitude of disturbance (could be
    amplitude of E-field also)

3
Propagation of waves in 3D
? depends on x, y and z such that it satisfies
the wave equation
or,
where in cartesian co-ordinates,
4
1. Special Case Plane Waves along x
  • Suppose ?(x, y, z, t)?(x, t) (depends only on x)
  • Then ? f(kx-?t) g(kx?t)
  • Then for a given position xo, ? has the same
    value for all y, z at any time to.
  • i.e. the disturbance has the same value in the
    y-z plane that intersects the x-axis at xo.
  • This is a surface of constant phase

5
Plane waves along x
Planes perpendicular to the x-axis are wave
fronts by definition
6
2. Plane waves along an arbitrary direction (n)
of propagation
  • Now ? will be constant in plane perpendicular to
    n if wave is plane
  • For all points P in plane

P
P
d
7
2. Plane waves along an arbitrary direction (n)
of propagation
For all points P in plane
or, for the disturbance at P
8
2. Plane waves along an arbitrary direction (n)
of propagation
If wave is plane, ? must be the same everywhere
in plane ? to n
This plane is defined by
P
P
d
is equation of a plane ? to n, a distance d from
the origin
9
2. Plane waves along an arbitrary direction (n)
of propagation
is the equation of a plane wave propagating in
k-direction
10
3. Spherical Waves
  • Assume has spherical symmetry
    about origin (where source is located)
  • In spherical polar co-ordinates

z
?
r
y
f
x
11
3. Spherical Waves
  • Given spherical symmetry, ? depends only on r,
    not f or ?
  • Consequently, the wave equation can be written,

12
3. Spherical Waves
Now note that,
13
3. Spherical Waves
But,
is just the wave equation, whose solution is,
i.e. amplitude decreases as 1/ r !! Wave fronts
are spheres
14
4. Cylindrical Waves (e.g. line source)
The corresponding expression is,
for a cylindrical wave traveling along positive ?
15
Electromagnetic waves
  • Consider propagation in a homogeneous medium (no
    absorption) characterized by a dielectric
    constant

?o permittivity of free space
16
Electromagnetic waves
Maxwells equations are, in a region of no free
charges,
Gauss law electric field from a charge
distribution
No magnetic monopoles
Electromagnetic induction (time varying magnetic
field producing an electric field)
Magnetic fields being induced By currents and a
time-varying electric fields
µo permeability of free space (medium is
diamagnetic)
17
Electromagnetic waves
For the electric field E,
or,
i.e. wave equation with v2 1/µo?
18
Electromagnetic waves
Similarly for the magnetic field
i.e. wave equation with v2 1/µo?
In free space, ? ? ?o ?o
(? 1)
c 3.0 X 108 m/s
19
Electromagnetic waves
In a dielectric medium, ? n2 and
? ? ?o n2 ?o
20
Electromagnetic waves Phase relations
The solutions to the wave equations,
can be plane waves,
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