Page 20 - Basic PD Theory
P. 20

Basic PD Theory


               a complex phenomenon depending on the size, shape, internal gas pressure, and nature of the void surface and will deviate from
               cycle to cycle due to past space charge trapping [Section 2.4.2].

               2.4.4   Voltage Dependence
               Not only is the spark (partial discharge) an indication that a gas-filled void exists and thus a symptom of deterioration, but it also
               breaks down the carbon bonds of the organic resin and accelerates aging.  Because the magnitude of the voltage stress across a
               void is dependent upon the applied voltage, most partial discharges only occur on high voltage (line-end) coils.  Coils at the
               neutral end do not have sufficient voltage to ground stress to exceed the electrical breakdown stress for air or hydrogen. Some
               voids do not actually produce a pulse spark, but instead exhibit glow and pseudo-glow characteristics.  Most conventional partial
               discharge detectors do not detect this activity [1].  The model shown in Figure 11 is an extremely simple model, the frequency
               and magnitude of discharges in a void is a complex phenomenon depending on the size, shape, internal gas pressure, and nature
               of the void surface.

               2.4.5   Pulse Shape
               The magnitude of partial discharge depends on the void volume (W = 0.5CV ) and shape, as well   *  Rise-time is the time
                                                                          2
               as the proximities to the copper conductor and PD sensor, and the void gas pressure.  The   required for a pulse
                                                                                               to increase from
               relative  phase angle position  depends on the void size, surface conductivity, and winding   10% to 90% of its
               temperature.  The rise-time depends on the cross-sectional area and the strength of the electrical   pulse magnitude.
               field.
               The pulse from a partial discharge is unipolar and has an extremely fast rise-time (1-5ns) and short pulse-width (2-6ns) [1].  The
               period of oscillation, the rise-times and magnitudes of subsequent peaks vary for each pulse.  This normally depends upon the
               geometry of the machine, the location of the pulse and the insulation materials.  Since partial discharges are pulses, they will
               produce  energy across the frequency spectrum  from DC to GHz.  In addition to the spark  pulses, there are also slower
               detectable frequencies from ionic tails.  Therefore, it is possible to detect partial discharge activity across several frequency bands
               with advantages and disadvantages for each [1].  It also means that no one instrument can detect all of the energy dissipated due
               to a partial discharge.
               Most partial discharge detection devices only detect the initial pulse that has a rise-time of 1-5ns.  Based   *  Partial discharge:
               on rise-time, to a first approximation, the frequency characteristic of a pulse is      50-250MHz
                                                                                                 frequency
                       f = 1/T  = 1/(4*rise-time)                                                characteristic
               Thus, the rise-time range of 1-5ns for partial discharges corresponds to the frequency characteristic
               range of 50-250MHz.

               2.4.6   Pulse Travel
               Once a pulse occurs, it has to travel somewhere to be detected by a sensor.  High frequency pulses travel through a stator
               winding in three different ways:  transmission, capacitive coupling, and radiation.

               2.4.6.1  Transmission
               The most widely understood and predictable method for a pulse to travel is to transmit through the copper conductors, similar
               to the 50/60Hz power signal.  When high frequency pulses travel as transmission waves, they undergo severe distortion due to
               the inductance of the coils.  Inductance of a stator-winding coil, which is a normal and necessary characteristic for electrical
               production, is a property that develops an electromagnetic field by impeding a sudden change in current.  Though this has a
               positive effect on the low frequency 50/60Hz power signal, it does diminish the high frequency (50-250MHz) pulses of partial
               discharges.  The distortion is attenuation and an increase in the rise-time (lower frequency response).  In fact, the pulses are
               distorted beyond recognition as high frequency partial discharges after only a few coils are traversed.
               In spite of this phenomenon, two conditions make partial discharge detection possible: first, that aging, (i.e. development of a
               failure mechanism) normally affects all coils to some degree; and second, that partial discharges can only occur when there is
               sufficient voltage to ground stress to cause an electrical breakdown of the air in the void.  This latter aspect only occurs on high



                                                                                 www.irispower.com


                                                                                  17 | P ag e
   15   16   17   18   19   20   21   22   23   24   25