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FEED LINE BASICS                                                        279



            analytically and numerically section of classical circuit theory. The logical connection is based
            as usual on the fundamental physical principle of energy conservation.
            Let us start from simple lumped circuit called cell and depicted in Figure 6.1.2a and assume
            that the voltage    is applied to the capacitor  C  while the current      flows through the
                           
                                                                       
            inductance ℒ. Then the energy stored in these elements according to (3.27) and (3.31) is
                                     ′
                                                    ′
                                     ∆ =  2     and   ℒ ∆ =  2                       (6.6)
                                            2              2
                                                    
            Here the total cell inductance ℒ and capacitance is expressed through so-called distributed
            parameters ℒ  and   as ℒ = ℒ ∆ and  =  ∆ (∆ <<  ) where ℒ  and   is the inductance-
                            ′
                                     ′
                                                ′
                                                                        ′
                                                                   ′
                       ′
            per-unit length in [Henry/m] and capacitance-per-unit length in [Farad/m], respectively. From
            the reactive energy balance (3.52) follows that the source of energy to support EM nonstop
            oscillations is not required if in free-of-loss system   =  , i.e.
                                                       
                                                            
                                   = ℒ    and   =   = �ℒ           (6.7)
                                 2
                               ′
                                      ′ 2
                                                            ′
                                                               ′
                                                   ⁄
                                                             ⁄
                                                      
                                              
                                       
                                                  
                                 
               Figure 6.1.2 a) Current and voltage illustration, b) Equivalent infinite transmission line
            The ratio in (6.7) is measured in Ohms and called the characteristic line impedance  . Now
                                                                                  
            we are capable to build an ideal  transmission line  just  connecting  the infinite  number of
            identical cells in cascade as shown in Figure 6.1.2b. Suppose that at some moment of time we
            inject the portion of EM energy into the first cell thereby forcing it to oscillate. Then a little bit
            later the energy of this oscillation transfers to the second connected cell and so on, i.e. the wave
            of voltage and current starts its propagation along the line. The circuit theory tells us that the
            speed of such wave  = 1 √ℒ  . Therefore, the wavenumber in line, wavelength in line and,
                                      ′
                                     ′
                                 ⁄
            characteristic impedance can be defined as ( =    and  =   )
                                                            2
                                                2
                                                      ∗
                                                                   ∗
                                                                  
                                                     
                                                            
                                                
                                                    ∗2 2    
                                                       
                                     = 1 √ℒ  = ��  ′  ′  =  ⎫
                                                     ′  ′   ′
                                                   4      ,
                                                              ⎪
                                                    ′         ⎪
                                                   ,  2
                                             ⁄
                                        =   =  =                        (6.8)
                                                     
                                                          ⎬
                                              =
                                                   ′          ⎪
                                                  ,  ⎪
                                     =   =  ⁄⁄     2  2 = 2  ⁄   2  ⎭
                                          
                                     
                   ′
            Here   ,  =  /∆  is  the  electric  and  magnetic  energy  stored-per-unit  length,
                         
            correspondingly,  is the frequency, and  =   /2 is the average power delivered to a single
                                                   ∗
                                                   
            cell. Note a very significant fact that the speed of wave  is inverse function of the energy stored
            in electric / magnetic field. Speaking metaphorically, a wave storing more EM energy while P
            =  const.  “gains weight”  and runs slower.  Continuing this analogy  we can see that
            simultaneously the wavelength  shrinks, i.e. the wave “becomes thin”. Sometimes, the lines
            like hollow waveguides with closed metal wall cannot offer a wave “enough room” to store
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