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BASIC EQUATIONS OF MACROSCOPIC ELECTRODYNAMICS                            3




            Introduction

            There are two basic versions of Maxwell’s equations: microscopic or quantum form  and
            macroscopic or classical form. The first set is more fundamental and describes the microscopic
            fields while taking into account their quantum nature. The second set is more straightforward
            and fun because it averages all charges and fields in macroscopic media and allows us to ignore
            the quantum effects while giving us sophisticated enough  and closed to reality picture  of
            surrounding world. Maxwell’s equations are essential not only for understanding the world
            around us but  strikingly  successful  in  explaining and  predicting a broad range of
            electromagnetic phenomena.  Macroscopic Electrodynamics deals  with  fields averaged on a
            spatial and temporal scale that is quite large compared to the interatomic space (in average
            10 −10 m) and the time of atomic fluctuations (in average 10 −11 s).
            The scale of  both  values  is  negligible  from  engineer’s  perspective.  In  2014,  the  Intel
            Corporation start mass production of new chips using very sophisticated the 14 nm technology
            enabling the manufacture of monolithic integrated circuits (IC) with conductive line widths of a
            few tens of nanometers (close to 10 m ). Even this tiny width  is  two  orders  of  magnitude
                                          −8
            higher than the average space between atoms. It means that, so far, the successful IC circuitry
            analysis stays in the range of classic electrodynamics settings. Note that the next just coming
            step is the 10 nm process.



            1.1 MACROSCOPIC ELECTRODYNAMICS

            1.1.1  Duality of Electromagnetic Waves

            We know from quantum physics about electromagnetic wave duality. They are both waves and
            discrete particles,  photons.  Each  photon  carries  a portion  of  energy    = ℎ,  where  ℎ =
                         −34
             6.6260755 ∙ 10  [J∙s] is Planck’s constant and  is the electromagnetic field frequency. Even
            at ultra-high  frequency  of  1  THz  (1,000,000,000,000 Hertz)  a  single  photon  carries  just
            6.6260755 ∙ 10 −22  Joules, an extremely small amount in macroscopic world. For comparison,
























                                 Figure 1.1.1 Electromagnetic spectrum
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