PC20312 Wave Optics
Section 1:
Electromagnetism and Waves
André-Marie Ampère
(1775-1836 )
Carl Friedrich Gauss 1777-1855
Images from Wikipedia
James Clerk Maxwell 1831-1879
Michael Faraday 1791-1867
Images from Wikipedia
Image adapted from Nick Strobel's Astronomy notes at www.astronomynotes.com
E
B k
John Henry Poynting (1852-1914)
S = -1 E × B
The Poynting vector is where a beam of light is pointing.
Image from Wikipedia
Plane wavefronts
Planar surfaces of constant phasek
E = E0 exp[i(kr-wt)]
Motion in +k direction
Plane wavefrontsPlanar surfaces of constant phase
kE = E0 exp[i(kr+wt)]
Motion in -k direction
Christiaan Huygens – 1629-95Pierre de Fermat – 1608-72
Images from Wikipedia
Huygens’ wavelets
Click to Huygens’ wavelets demo
Or go to
http://www.acoustics.salford.ac.uk/feschools/waves/diffract3.htm
Fig 1.1 Snell’s Law by Fermat
Image courtesy of A. Pedlar
Fig 1.2 Law of reflection by Fermat
h1
h2
x l - x
S
P
i r
l
0dx
dL
Tutorial problem:
• Write optical path length, L, between S and P as function of x
• Find
• i = r when
dx
dL
Fig 1.3 Refraction at a spherical surface
S P
Sosi
C
R
l oli
A
Imaging with a curved surface
S1 P1
S2
S3
P3
P2
C
Fig 1.4 Imaging with a lens
S P'P
So,1 Si,1
Si,2
So,2
Image formed by 1st surface acts as a virtual object for 2nd surfacen1 n2
n1
d