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leader
                                                                         leader










          Figure 2.1.2  Discharge mechanism of a negative downward flash   Figure 2.1.3  Discharge mechanism of a positive downward flash
                  (cloud-to-earth flash)                        (cloud-to-earth flash)


          300 km/h in steps of a few 10 m. The interval between the jerks   the leaders propagate from the exposed object on the surface
          amounts to a few 10 µs. When the leader has drawn close to   of the earth to the cloud, high objects can be struck several
          the earth (a few 100 m to a few 10 m), it causes the strength   times by one lightning discharge during a thunderstorm.
          of the electric field of objects on the surface of the earth in   Depending on the type of flash, each lightning discharge con-
          the vicinity of the leader (e.g. trees, gable ends of buildings)   sists of one or more partial lightning strikes. We distinguish
          to increase. The increase is great enough to exceed the dielec-  between short strokes with a duration of less than 2 ms and
          tric strength of the air. These objects involved reach out to the   long strokes with a duration of more than 2 ms. Further distinc-
          leader by growing positive streamers which then meet up with   tive features of partial lightning strikes are their polarity (nega-
          the leader, initiating the main discharge.   tive or positive) and their temporal position in the lightning
          Positive downward flashes can arise out of the lower, posi-  discharge  (first,  subsequent  or  superimposed).  The  possible
          tively charged area of a thundercloud (Figure  2.1.3). The
          ratio of the polarities is around 90 % negative lightning to
          10 % positive lightning. This ratio depends on the geographic
          location.
          On very high, exposed objects (e.g. wind turbines, radio masts,
          telecommunication towers, steeples) or on the tops of moun-
          tains,  upward  flashes  (earth-to-cloud  flashes)  can  occur.  It
          can be recognised by the upwards-reaching branches of the
          lightning discharge (Figure 2.1.4). In case of upward flashes,
          the high electric field strength required to trigger a leader is
          not achieved in the cloud, but rather by the distortion of the
          electric field on the exposed object and the associated high
          strength of the electric field. From this location, the leader and
          its charge channel propagate towards the cloud. Upward flash-
          es occur with both negative polarity (Figure 2.1.5) and with
          positive polarity (Figure 2.1.6). Since, with upward flashes,   Figure 2.1.4  Upward flash (earth-to-cloud flash)



          16  LIGHTNING PROTECTION GUIDE                             www.dehn-international.com
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