Page 492 - Instrumentation Reference Book 3E
P. 492

The measurement of resistance, capacitance, and inductance 475




















                                                                            switch
                                                      Figure 20.68  Universal bridge.

                                                        Figure 20.68 shows a universal bridge for the
                                                      measurement  of R, C, and L. In the figure only
                                                      two decades of the inductive divider which con-
                                       0
                                        Detector
                                                      trol the voltages applied to the bank of identical
                                                      fixed  capacitors  and  resistors  are  shown.  The
                                                      balance condition for the bridge when connected
                                                      to measure capacitance is given by


                                                      and
             Figure 20.67  (a) Autotransformer ratio bridge;
             (b) double-wound transformer ratio bridge; (c) double ratio   1
             bridge.
             more nearly equal to the turns ratio. The bridge   When measuring inductance the current through
             has the disadvantage that the leakage inductance   the capacitor and inductor  are summed into the
             and winding resistance of each section is in series   current transformer and the value of capacitance
             with Z1  and Z2 and therefore the bridge is most   determined is the value which resonates with the
             suitable for the measurement of high impedances.   inductance. For an unknown inductance its meas-
               Figure 20.67(c) shows a double ratio transform-   ured  values  in  terms  of  its  parallel  equivalent
             er bridge in which the currents 11  and 12  are fed   circuit are given by
             into  a  second  double-wound  transformer.  The
             detector senses a null condition when there is zero
             flux in the core of the second transformer. Under
             these conditions for an ideal transformer   where the values of  C,  and R,  are given in the
                                                      above equations. The value  of  LU‘  is chosen  such
                                                      that it is a multiple of ten and therefore the values
                                                      of L,,  and  C,  are reciprocal. The values cf L,,
             and  the  second transformer  presents  zero  input   and R,,  can be converted to their series equiva-
             impedance. Therefore since               lent values using the equations in Section 20.7.2.
                                                        The transformer ratio bridge can also be config-
                                                      ured to measure low impedances, high impedances,
                                                      and  network  and  amplifier  characteristics.  The
             then                                     ampere turn balance used in ratio bridges is also
                 Z1  = nn’Z2;  /Z1/ = nn’1Zzl  and  iZ1 = LZ2   used in current comparators employed in the cali-
                                                      bration of current transformers and for intercom-
             By  using  the two  ratios  this bridge  extends  the   paring four-terminal impedances. Details of these
             range of measurement which can be covered by a   applications  can  be  found  in  Gregory  (1973):
             small number of standards.               Hague  and  Foord  (1971), and  Oliver  and  Cage
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