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120                                                                Chapter 3


                                       () = ∯    x              (3.18)
                                     Σ
                                             
        Poynting’s vector is probably the  most  interesting  component of energy conservation law
        because  behind it  the quantum  nature of EM fields. Loosely speaking, this vector is the
        “macroscopic bridge” bonding classical Maxwell’s equations with quantum physics.

        3.1.6   Velocity of EM Waves Energy Transportation

                                        Poynting’s theorem as one  of the  key  theorem  of
                                        electrodynamics predicts not only the effect of
                                        electromagnetic energy transportation by EM  waves
                                        but allows to estimate the velocity of this transportation
                                        customary called energy velocity of EM wave. Let us
                                        refer to Figure 3.1.3 assuming that it takes some short
                                        period of time ∆ for the incoming EM energy ∆  to
                                                                                
                                        fill up the tiny volume ∆ = ∆ ∘ ∆. Then the balance
                                        of power contained inside this volume (see (3.15)) can
                                        be written as
           Figure 3.1.3 Volume ∆ filling
               up with energy flux              ∆ ⁄ ∆ = − ∬  ∘  =  ∘ ∆    (3.19)
                                                
                                                           ∆
        Taking into account that the volume is infinitesimal we obtain


                                ∫    ∘  ∆  ∆
                     ∆ ⁄ ∆ =  ∆  =  ∘ ∫    =  ∘ (  ∆)                  (3.20)
                                                
                                    ∆   ∆  ∆   ∆
                ∆
        The ratio   can be interpreted as the velocity vector    of the energy flux propagating in the
                ∆                               
        direction ∆. Therefore,

                                                             ⁄
                                 ∘ (  ∆) =  ∘ ∆    or       =     [m/s]               (3.21)
        Note that we implicitly assumed that the energy flux through the side surface of ∆ is small
        enough to be neglected and the medium of propagation is isotropic and non-dispersive. In this
        case, the Poynting’s vector direction shows the path and velocity of the energy flux, i.e.   ||.
        The detailed discussion of this subject is out of this book theme. More fundamental analysis of
        such issue the reader can find in [6].

        3.1.7   Linear Momentum of EM Fields. Radiation Pressure and Solar Sailing

        Feedback between Poynting’s theorem and conservation laws is much deeper than it seems at
        first glance. Let us come back for a while to the EM wave-particle duality we have touched in
                                                                      4
        Chapter 1. It is well-known that each photon carries a certain portion of energy   = ℎ = 
                                                                                   2
        traveling in vacuum at the ultimate speed of light and never stops. Meanwhile, it sounds creasy

        4  To avoid the confusion, we temporally use the common in physics notification of energy and frequency.
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