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where cos ϕ=Power factor of the circuit.


                  Note: Power factor, cosf is lagging for an inductive circuit and is leading
               for a capacitive circuit.




                                              3.2.6 R–L–C Series Circuit

               Consider a circuit consisting of resistance R, inductance L, and capacitance C
               connected in series with each other across an ac supply. The circuit has been

               shown in Fig. 3.25.
























                                      Figure 3.25 (a) R–L–C series circuit; (b) phasor diagram


                  The circuit draws a current I. Due to flow of current I, there are voltage
               drops across R, L, and C which are given by


                   i.  drop across resistance R is V  = IR
                                               R
                  ii.  drop across inductance L is V  = IX L
                                                L
                  iii.  drop across capacitance C is V  = IX C
                                                 C

               where I, V , V , and V  are the RMS values.
                                 L
                            R
                                           C
                  The phasor diagram depends on the magnitude of V  and V , which
                                                                                          C
                                                                                 L
               obviously depends upon X  and X . Let us consider the different cases.
                                                         C
                                               L
               (a) When X  > X , i.e., when inductive reactance is more than the capacitive
                              L
                                     C
               reactance.
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