Page 47 - Maxwell House
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BASIC EQUATIONS OF MACROSCOPIC ELECTRODYNAMICS                           27


                                                             
                                           = ∯    ∘  = −                   (1.33)
                                          
                                               
            is the integral form of the continuity equation. But remember that this equation describes the
                                  movement of positive charges. If the current is defined as the flow
                        0         of electrons,   in (1.33) must be replaced by − . The deferential
                                              
                                                                          
                                  form of the continuity equation follows from (1.33) if we transform
                                  (see Appendix) the surface integral to volume one applying (1.30)
                 q                to the current density as
                 qv       -
                                                ∯   ∘  = ∫  ∘                     (1.34)
                                                       
                                  Replacing in (1.33)   = ∫   and grouping the terms we
                                                     
                                                            
                                                         
                                  obtain
                  Figure 1.6.7                       �  = 0              (1.35)
               Populated House of          ∫ � ∘    +  
                                        
                  Maxwell’s       Pronouncing the  “magic”  words,  we finally get  the  continuity
                Electrodynamics   equation in differential form

                                                   
                                              ∘    +   = 0                   (1.36)
                                                   
            Now, we can populate Maxwell’s House attic with new residents  ,   and  , as shown in
                                                                  
                                                                            0
                                                                     
            Figure 1.6.7.
                                              st
            1.6.11  Lorentz’s Force Equation and 1  Maxwell’s Equation
            Looking back at Lorentz force equation (1.11) we note that the magnetic field exerts the force
               on a moving charge that can be described through the equivalent electric field (1.15)
             
            as  =  x . That is not something occasional. The most remarkable fact is that magnetic
               
            and electric fields are in reality just different aspects of the same and inseparable phenomenon
            — the electromagnetic force. Imagine that a girl shown in Figure 1.6.6a is traveling on a train
            car touching a charged metal sphere and having a bunch of tools including her hair to measure
            electric and magnetic fields. Taking into account that the girl, the sphere, and all her instruments
            are at rest relative to each  other the  girl’s instruments  can detect only electrical  fields.
            Nevertheless, her friend standing with an identical set of tools on the platform while the train
            passes, will detect not only electric fields but magnetic fields too, because for the friend and
            his/her instruments the charged sphere in motion is equivalent to some current and the source
            of magnetic field. Eventually, nothing changes if the train stops and the girl’s friend starts
            running nearby the train car.

            We  will  use  such duality or  principle of relativity  sometimes  implicitly to bridge the  gap
            between static and time-varying  fields, static and  moving charges, electrical and  magnetic
            fields, et cetera. Electric and magnetic fields are just two faces of the same natural phenomenon
            like the ancient Roman two-faced god Janus, who looks simultaneously to the future and the
            past, symbolizing the transition from one condition to another . More details about such duality
                                                            10
            effects can be found in the special theory of relativity and are beyond the scope of this book.



            10  It looks like Romans believing in such god foresaw electromagnetic field propagation long ahead of
            Maxwell.
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