Page 62 - Maxwell House
P. 62

42                                                                 Chapter 1

                              Integral Form                     Differential Form

          8                      =                      =  
                                     
                                                                        
          9                      =                      =  
                                     0
                                                                        0
                                       We now placed in all equations the excitation charges
                         0             and currents discussed in the previous section. The
                                       constituency equations for these sources are not included
                                       because, as it has been mention before, the nature of them
                  q                    can  be  very complicated and they  could not follow
                 qv                    Maxwell’s equations. As we will demonstrate in Chapter
                                       2, in case of  monochromatic  field the  material
                                       parameters ,  ,  and    can be the  complex numbers
                                                          
                                                   
                                       having the real and imaginary parts while the imaginary
                                       part is responsible for the energy loss in materials.
               0
                                       Maxwell’s  House  summarizing  Maxwell’s  equations
                                       graphically in the frequency domain is shown in Figure
          Figure 1.8.1 Maxwell’s House   1.8.1  where for simplicity of drawing the excitation
            for monochromatic fields   sources  were omitted. In the  meantime, the  magnetic
                                       conductivity existence is uncertain, and we put it with the
        question mark. A look at Table 1.7 and 1.9 reveals that Maxwell’s equations can be solved
        either in time (using equations from Table 1.7) or frequency (using equations from Table 1.9)
        domain depending on which way is shorter or more natural.

        We are going to discuss in great details each of these approaches in following chapters. Just
        note that both  solutions  are interconnected  by Fourier’s transform or its inverse  form.  For
        example, Maxwell’s equations solution  (, )  in frequency domain corresponds in time
        domain to the vector

                                            ∞
                                  (, ) = ∫  (, ) exp()                 (1.88)
                                           −∞
        and vise verse.



        REFERENCES

        [1]    C. J. Cleveland, R.  K., Fundamental principles of energy, The Encyclopedia of Earth,
               2008, http://www.eoearth.org/view/article/152893.
        [2]    C. Benjamin, Conservation of Mass and Energy,
               http://www.lightandmatter.com/html_books/7cp/ch01/ch01.html.
        [3]    F. W. Hehl, Y. Obukhov, Foundations of Classical Electrodynamics: Charge, Flux
               and Metric, Birkhauser, Boston, 2003.
        [4]    A. Bossavit, Computational electromagnetism, San Diego, CA, Academic Press, 1998
        [5]    A. A. Sonin, The Physical Basis of Dimensional Analysis, 2  Edition, Department of
                                                                nd
               Mechanical Engineering MIT, Cambridge,
               http://web.mit.edu/2.25/www/pdf/DA_unified.pdf
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