Page 453 - Instrumentation Reference Book 3E
P. 453

436  Electrical measurements



























                                                                    a.c.   8.0.   a.c.
                                                                      iov  6WV  3WV
                                                                      d.c.   a.c.   d.c.
                                                                      1oov
                                                                      a.c.
            Figure 20.13  Multimeter. Courtesy Thorn EM1 Instruments Ltd.
            and thus                                  (w2L2)/(2R2), where L is its inductance and R its
                                                      resistance. Figure 20.16(b) shows a compensation
                0   1  1  dL  .2                      method for this error.
                   2  k  d0                            Although  the  moving-iron  instrument  is  a
              The  deflection  of  the  instrument  is  propor-   mean square indicating instrument errors can be
            tional to the mean square of the current and thus   introduced  when  measuring  the  rms  value  of  a
            the instrument provides a steady-state deflection   non-sinusoidal  voltage  waveform.  These  errors
            from an  a.c. current. The scales of  such instru-   are  caused  by  the  peak  flux  in  the  instrument
            ments  are  usually  calibrated  in  terms  of  rms   exceeding the maximum permitted  flux and also
            values  and  they  tend  to  be  non-linear,  being   by attenuation of  the harmonic current through
            cramped at the lower end.                 the instrument by the time constant of the meter,
              Friction  in  the  bearings  of  the  instrument   as shown in Figure 20.16(c).
            causes error. Hysteresis effects in the iron of the   Moving-iron  instruments  are capable  of  pro-
            instrument  give rise  to different  indications  for   viding an accuracy of better than 0.5 percent of
            increasing and decreasing current. Errors can also   FSD. As ammeters they have typical FSDs in the
            be caused by the presence of stray magnetic fields.   range of 0.1-30 A without shunts. The minimum
            Variation in ambient temperature causes changes   FSD when they are used as voltmeters is typically
            in the mechanical dimensions  of the instrument,   50V with a low input impedance of order 50 ON.
            alters the permeability of the iron, and changes the   Their  frequenc  response is limited by  their  high
            resistance of the coil. This last effect is the most   inductance and stray capacitance to low frequen-
            important.  Used  as  an  ammeter  the  change  in   cies, although instruments are available which will
            resistance  causes no error, but  when  used  as  a   measure  at  frequencies up  to  2500Hz.  Moving-
            voltmeter  the change in resistance of the copper   iron  instruments  have  relatively  high  power
            winding of +0.4%/K  causes the sensitivity of the   requirements  and  therefore  they  are  unsuitable
            voltmeter to change. This effect is usually reduced   for use in high-impedance ax. circuits.
            by using a resistance in series with the coil wound
            with a wire having a low temperature coefficient.   20.2.3  A.c. range extension using current and
            The inductance of the instrument can also cause   voltage transformers
            changes  in  its  sensitivity  with  frequency  when
            used  as  a  voltmeter.  This  is  shown  in  Figure   In  Section  20.2.1.1,  extension  of  the  range  of
            20.16(a).  At  a  given  angular  frequency  i~, the   permanent magnet-moving coil instruments using
            error  of  reading  of  the  voltmeter  is  given  by   current  shunt  and  resistive  voltage  multipliers
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