Page 15 - Application Guide Semiconductor Fuse Link
P. 15

Short-circuit currents



        The r.m.s. value of the steady-state short-circuit current which would fl ow in the circuit if there
        were no fuse protection is called the prospective current (IEC) or the available short-circuit current
        (North America).

        In an a.c. circuit, the transient short-circuit current is given by

                             i     =         2I (sin(    t +   -   ) - sin (  -   )e - t/tan   )

        where  I      is the r.m.s. prospective (available) short-circuit current
                      is the supply angular frequency ( = 2  f )

                      is the electrical angle (point on the source voltage wave) at which the short-circuit
                      begins
                                                                               -1
                      is the power-factor angle of the circuit impedance ( = tan     L/R)
        The fi rst term in the above expression is the steady-state a.c. short-circuit current, while the second
        term is an exponentially-decaying transient d.c. component.


        If the short-circuit occurs at an instant when   =   the transient component is zero, and the short-
        circuit current will be a symmetric sine-wave (see Fig.5). The peak value is 1.414 ( 2) times the r.m.s.
        prospective (available) current.


        If       the short-circuit current will have an asymmetrical waveform with an exponentially-decaying
        d.c. component (see Fig.5). The maximum value of the fi rst asymmetrical peak current is obtained if
        the circuit is closed at the voltage zero (  =  ). It can reach 2.828 (2 2) times the r.m.s. symmetrical
        current in a purely inductive circuit, or about 2.5 times in a circuit with an X/R ratio of 10:1.


                        symmetrical                                         current  asymmetrical
                 current




                                                                       source
               source                                                  voltage
               voltage

                          time,’s                                                  time,’s
                      Fig.5 Symmetrical and asymmetrical short-circuit currents in an a.c. system

        For a fault in a d.c. circuit the prospective (available) short
        circuit current is the fi nal constant value VDC /R, where VDC is
        the source voltage and R is the resistance of the circuit. After a
        fault occurs, the current in the circuit increases exponentially,
        as shown in Fig.6, with a circuit time-constant L/R, where L is
        the circuit inductance.
        In this case the instantaneous short-circuit current is given by


                  i    =       I  1 - e -Rt/L
                                                                        Fig.6 Short-circit current in a d.c.
                                                                                     system

        where I = VDC /R. The heating effect of the fault current depends upon its r.m.s. value, which is
        given by


                                                          -2n
                                                     -n
                                                   2e     e      3
                             IRMS   =        I   1+ - - - - -
                                                   n       2n     2n
        where n = t/T and T = L/R is the circuit time constant. The variation of IRMS with time is also shown
        in Fig.6.
                                                                                                                   15
   10   11   12   13   14   15   16   17   18   19   20