Page 114 - MATLAB an introduction with applications
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Electrical Circuits ——— 99

                   The energy stored in an inductance is

                                    1      1
                                 E =   Li  =   L ( q   )  2
                                        2
                                    2      2
                   where q is the electrical charge.
                   The voltage drop in an inductance is

                                V i  = Li  = L q
                   Inductances in Series: Since the voltage drop through an inductor is proportional to the inductance L, we
                   have (Fig. 2.4 (a))

                                L eq = L 1  + L 2
                                                                                     L 1
                                 L 1             L 2



                                                                                     L 2
                            (a) Inductances in series                               (b) Inductances in parallel
                                                     Fig. 2.4 Inductances

                   Inductances in Parallel: Referring to Fig. 2.4 (b), we have
                                      LL
                                L eq  =   12
                                     L +  L 2
                                      1
                   Similarly, for n inductors
                                1  =  1  +  1  +  ... +  1
                               L eq  L 1  L 2  L n
                   Capacitance Elements: Capacitance C is a measure of the quantity of charge that can be stored for a given
                   voltage across the plates. The capacitance C of a capacitor is given by
                                    q
                                C =
                                    V c
                   where q is the quantity of charge stored and V c  is the voltage across the capacitor.
                           dq
                   Since i =    and V c  = q/C, we have
                            dt
                                     dV
                                  i =  C  c
                                      dt
                                    1
                   or             dV c  =   i dt
                                    C
                                    1
                   Hence        V c  =  ∫i c  dt
                                    C









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