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Physical Optics - 3. lecture


   Huygens Principle. Polarization of electromagnetic waves. Circular polarization


    Huygens principle is a simple intuitive picture of wave motion, valid for any type of waves.
    It can be used to understand the so calles Snell's law

    Mathematical formulation can be related to the Green's function method
 
      sc_0100.png

       sc_0100.png


    Snell's Law for refraction can be simply understood from Huygens principle as shown in the following drawings
    What can not be determined is which part of the wave is reflected and which part is refracted to the angle

      snell1.png

       snell1.png


    The following drawing shows that Snell's law is connected with the two wavelengths - rather than the speeds of propagations
    If the wavelength is shorter in medium 2, the propagation angle (measured from the normal)  is smaller
   

      snell2.png

       snell2.png


   For all waves where the phase velocity is independent of wavelength:   the frequency  =  velocity divided by wavelength
                       Since the frequency must remain unchanged in the two media, shorter  wavelength in medium 2 means lower velocity

                       Therefore, if the picture of refraction is as indicated, the velocity in medium 2 is smaller
                                                                     Thus index of refraction (inversely proportional to the spead) is larger for medium 2

      snell3.png

       snell3.png

   If light consisted of particles, Snell's law would be satisfied if particles would get a push forward, i.e. move
   with a larger velocity in medium 2. This was believed by Newton

      sc_0200.png

       sc_0200.png


    To determine how the electromagnetic wave behaves at the interface, we must add the "boundary conditions"
    to the analysis.
    The relations are shown in the following drawing
    The parallel component of E  and the normal component of B are continuous
     From Gauss law, the normal component of E is changed according to the relation below. 
     For most materials, B remains constant (permeability  changes  are roughly negligible)

      sc_0300.png

       sc_0300.png


   Thus the behaviour of the wave at the interface will be determined by the relations above.

   Electromagnetic waves are transverse waves. The wave can be polarized in any direction (perpendicular to propagation)
   Waves can be superposed - and decomposed

   It is thus enough to consider behaviour of waves with polarization(s) which allow simple analysis
   That means two simple waves - with E in the pane of incidence, and with E perpendicular to that plane
   This we shall explore next time

      sc_0400.png

       sc_0400.png


   More on polarization - intuitive pictures

      sc_0500.png

       sc_0500.png


   But in addition to the discussed "linear polarization" which can be decomposed into two perpendicular components
   There is also a possibility to have CIRCULAR polarization
                                                       (and elliptic - meaning that the two phase delayed perpendicular
                                                         motions have different amplitudes )

      sc_0600.png

       sc_0600.png


   Circular polarization and complex notation

      sc_0700.png

       sc_0700.png



    Next time:   More formal relations on polarization;
                        Notation - P-wave and S-wave  also TE-polarized and TM-polarized
                        Details of S-wave and P-wave reflection/refraction


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