@InProceedings{CamposSaWaCuKrOr:2010:DoAvDo,
author = "Campos, Leandro Zanella de Souza and Saba, Marcelo Magalh{\~a}es
Fares and Warner, T. A and Cummins, K. L and Krider, E. Philip and
Orville, R. E",
affiliation = "{Instituto Nacional de Pesquisas Espaciais (INPE)} and {Instituto
Nacional de Pesquisas Espaciais (INPE)} and {South Dakota School
of Mines and Technology} and {University of Arizona} and
{University of Arizona} and {Texas A\&M University}",
title = "Does the average downward speed of a lightning leader change as it
approaches the ground? An observational approach",
booktitle = "Proceedings...",
year = "2010",
organization = "International Lightning Detection Conference, 21.",
keywords = "Lightning Physics, Atmospheric Electricity, High-speed video
observations, Stepped-leader velocities, Positive leaders,
Positive lightning.",
abstract = "In the lightning literature, it is commonly assumed that the
stepped-leaders that initiate the first return stroke in negative
cloud-to-ground lightning flashes accelerate during the final
stages of their development, but there have been only a few
observational studies supporting this claim. Other studies have
reported a tendency for positive leaders to accelerate and
negative dart-leaders to decelerate. The aim of this investigation
is to determine how the average two-dimensional (2-D) downward
speed of lightning leaders changes as they approach the ground and
to see if any such changes depend on the leader type, polarity, or
instrumentation used to measure the speed. We have examined the
optical properties of leaders that were recorded using high-speed
video cameras at different sites in south and southeastern Brazil,
southern Arizona, and South Dakota, in conjunction with data
obtained by lightning locating systems. The GPS time-stamped
cameras were operated at frame rates ranging from 1000 to 11,854
frames per second. Our dataset consisted of 46 negative
steppedleaders, 53 negative dart-leaders, and 28 positive leaders.
Two different approaches were used in the data analysis; first,
the average downward speed of individual leaders was computed over
preset distance intervals above the ground, i.e. from 0 to 500 m,
500 to 1000 m, etc, and then the geometric mean (GM) was
calculated for all the cases in a given interval. We computed and
compared the GMs since the speeds of positive leaders and negative
dart-leaders follow a lognormal distribution (at the 0.05 level,
according to the Shapiro-Wilk test), and the negative
stepped-leaders have a similar distribution (according to the
Kolmogorov-Smirnov test). The GM of the positive leader speeds
increases by about a factor of 10 as they get closer to the ground
(i.e. from 104 to 105 m/s), and the GM speed of negative
stepped-leaders varies between 2.5x105 and 3.0x105 m/s. On the
other hand, the GM speed of negative dart-leaders shows a clear
decrease as they approach the ground. The second approach involved
analyzing the leaders individually over their measurable length,
and we found that: a) 82% of the 20 positive leaders accelerated,
7% decelerated, and 11% oscillated around an average speed; b) 46%
of the 46 negative stepped-leaders accelerated, 6% decelerated and
48% oscillated around an average speed; and c) 32.1% of the 53
negative dart-leaders accelerated, 54.7% decelerated, and 13.2%
oscillated around an average speed. We conclude that the
acceleration of negative stepped-leaders is not as strong as some
authors have assumed, but the tendencies for positive leaders to
accelerate and for negative dart-leaders to decelerate are clear
and agree with previous studies. We believe that the presented
behavior asymmetry between negative stepped- and positive leaders
might suggest microphysical differences in their propagation which
should be investigated further.",
conference-location = "Orlando",
conference-year = "19 - 20 Apr.",
targetfile = "campos_does.pdf",
urlaccessdate = "28 abr. 2024"
}