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Fundamentals of Electrical Safety      19


                                  measures, active and passive, against this type of fault situation must
                                  be considered.


                                  2.3.1 Protection by Automatic Disconnection of Supply
                                  The automatic disconnection of the faulty circuit from its source is an
                                  active protective measure aimed to limit the persistence of prospective
                                  touch voltages on an ECP to a time that the human body can withstand
                                  without incurring harmful physiological effects. The protective device
                                  must promptly trip in accordance with the magnitude of the touch
                                  voltage: the higher this value, the faster it must trip. As explained
                                  in Chap. 5, the time–voltage safety curve describes the permissible
                                  prospective touch voltage for persons as a function of the contact
                                  duration in any type of earthing system (e.g., 50 V a.c. can be withstood
                                  for no more than 5 s).
                                     As later shown, maximum disconnection times of protective de-
                                  vices have been elaboratedasafunctionofthenominalvoltageandthe
                                  type grounding of the electrical system, rather than of the perspective
                                  touch voltage.
                                     Disconnection of supply upon faults is a measure that requires
                                  an efficient bonding of the ECPs to the earthing system so that pro-
                                  tective devices, by sensing the leakage to earth, can intervene at the
                                  inception of the ground fault even before a person comes in con-
                                  tact with energized objects. This protection is suitable if electrical
                                  items are equipped with bonding terminals (i.e., Class I equipment of
                                  Fig. 2.2). Under this point of view, the disconnection of supply can be
                                  considered as a preventive approach to safety.
                                     If the ground-fault current is high enough (e.g., TN systems), au-
                                  tomatic circuit breakers can be employed to switch off the faulty cir-
                                  cuit. RCDs may also be used to disconnect the voltage source upon
                                  ground faults (especially in TT systems). In this regard, it is important
                                  to underline the importance of the inclusion of the neutral conductor
                                  through the RCD’s toroid (Fig. 2.8).
                                     If the neutral is not included, any unbalanced load could cause
                                  nuisance tripping of the device. In fact, the vector sum of the phase
                                  currents circulating through the toroid would not be compensated by
                                  the neutral current, causing a nonzero result. If the system does not
                                  carrytheneutralconductor,thevectorsumofthelinecurrentsthrough
                                  the toroid is normally zero, even if the load is unbalanced, but becomes
                                  nonzero in the case of a ground fault, allowing the operation of the
                                  device.
                                     On the other hand, the protective conductor PE must be excluded
                                  from the RCD, otherwise the device would never trip. The fault cur-
                                  rents over the PE, in fact, would return to the source passing through
                                  the toroid, thereby causing the vector sum of the currents to be zero,
                                  despite the presence of the fault.
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