The Lightning Detection and Ranging (LDAR) system was developed at the Kennedy Space Center (KSC) in order to provide real time lightning safety information (Maier et al., 1995a). The LDAR is able to accurately locate lightning radiation sources in 3 spatial dimensions and time by measuring the arrival time of impulsive VHF events at seven stations.
The operating frequency of the LDAR is centered at 66 MHz with a 3 dB
bandwidth of 6 MHz. The 66 MHz VHF signal at each station is
logarithmically detected and transmitted to the central site via video
microwave links. Each of the analog signals is sampled at the central
site with a 100 MHz rate and with 8-bit resolution. The time and
amplitude of the peak signal within an 81.96 s window is
determined for each channel every 100
s. This data is output to
a data computation system which determines 3D source locations for
those points which are observed at the proper retardation times by
at least 4 stations.
The stations are positioned such that they are approximately
evenly-spaced from each other on the periphery of a circle
10 km in radius, with one station at the center (see
Figures 3.1-3.2). The median
location error within the LDAR network is only
50 m
(Maier et al., 1995a). Outside the network, the 3D location
errors are due primarily to radial errors which increase with range at
a rate faster than the linearly increasing transverse errors due to a
fixed bearing error of
0.5
.
The individual flashes analyzed in this dissertation were reported by LDAR
to be between 40-130 km range from the LDAR central station. The
median radial error at 40 km was directly measured by
Maier et al. (1995a) to be 1 km for regular VHF pulses
emitted from an aircraft which was equipped with a differential GPS
navigational system. Assuming an approximate
dependency of
radial errors on range (Boccippio et al., 1999), the median radial
error at 130 km range would be
10 km.
The detection efficiency of the LDAR instrument decreasees with
increasing source range. Climatologically-averaged areal source
density declines exponentially with ground range at an e-folding
length of 39-50 km (Boccippio et al., 1999). Thus, the detection
efficiency at 40-130 km range would be a factor of 3-30 less
than within the LDAR network.
One effect of the rapid drop in detection efficiency is that sources
which are closer than their calculated range will be overrepresented
relative to sources which are further away, resulting in a net outward
bias in radial locations. This will also result in an upward bias in
heights. Climatologically-averaged source density plots of LDAR
heights with respect to range indicate that heights are ``pushed up''
at increasing range with an approximate dependency, though this
effect is somewhat minor with only a
1 km increase in height
at 100 km range (Boccippio et al., 1999). Since most of the data
points analyzed will be within 100 km range, the systematic increase
in height will not be particularly important.