Page 253 - Electrical Safety of Low Voltage Systems
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236    Chapter Fourteen






















                                  FIGURE 14.14 Test circuit to measure touch and step voltages in TN systems.

                                     The touch and step voltage measurements are carried out by simu-
                                  lating ground faults by means of a test current I t of low magnitude, but
                                  of at least 1% of the actual ground-fault current I G impressed across
                                  the facility grounding system R G and auxiliary current electrode(s).
                                  The auxiliary current electrode(s) will be buried at a sufficient distance
                                  from R G to be considered independent of it (Fig. 14.14).
                                     For the touch voltage measurement, a voltmeter will measure the
                                  potential differences between any accessible ECPs/EXCPs and two
                                                                      2
                                  electrodes with a contact surface of 200 cm , pressed against the soil
                                  with a force of 250 N and placed at the distance of 1 m from each
                                  other. For the step voltage measurement, a voltmeter will measure
                                  the potential difference across the same two test electrodes in various
                                  locations within the facility.
                                     The test electrodes must be placed radially with respect to the grid,
                                  so that they will not sit on the equipotential lines of the electric field,
                                  thereby measuring zero potential difference.
                                     Also in this case, we assume a linear relationship between test cur-
                                  rent and touch and step potentials and, therefore, obtain their values
                                  in correspondence of the actual fault current, as follows:

                                                                  I G
                                                          V T,S = V 1                 (14.16)
                                                                  I t

                                  where V 1 is the reading of the voltmeter.
                                     The reading V 1 , though, may include the unavoidable and un-
                                  wanted contribution of “stray” potentials existing across the earth and
                                  not produced by the test circuit. The subsequent disturbance voltage
                                  V d vectorially adds itself to the true values of touch and step potentials
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