AU2003213052A1

AU2003213052A1 - Lightning detection and data acquisition system

Info

Publication number: AU2003213052A1
Application number: AU2003213052A
Authority: AU
Inventors: Kenneth L Cummins; Martin J Murphy; Alburt E Pifer
Original assignee: Vaisala Inc
Current assignee: Vaisala Inc
Priority date: 2002-02-13
Filing date: 2003-02-13
Publication date: 2003-09-04
Also published as: JP2006504068A; WO2003069375A2; JP2009085965A; CN1646928A; JP2009109503A; CA2476199A1; JP4642105B2; EP1485721A2; WO2003069375A3; JP4445267B2

Description

WO 03/069375 PCT/US03/04351 LIGHTNING DETECTION AND DATA ACQUISITION SYSTEM BACKGROUND OF THE INVENTION This invention relates to lightning detection and data acquisition systems, and in 5 particular to systems that provide continuous lightning detection and are programmable to allow for user-selectable evaluation criteria. Lightning detection and data acquisition systems are used to detect the occurrence and determine the location of lightning discharges, and gather other data about the discharges. In traditional lightning detection systems, a plurality of sensors are placed 10 tens to hundreds of kilometers apart to remotely detect the electric and magnetic fields of lightning discharges. Such discharges may be between a cloud and the ground ("CG") or within a cloud ("IC"). Information from the sensors is transmitted to a central location, where analysis of the sensor data is performed. Typically, at least the time of occurrence and location of the discharges are determined from data provided by a plurality of 15 sensors. Remote sensors of lightning detection and data acquisition systems typically detect electric and magnetic fields of both CG and IC lightning flashes, which are composed of many discharges. It is often important to be able to distinguish between the two types of flashes. To that end, remote sensors often look at the low-frequency ("LF") 20 and very-low-frequency ("VLF") emissions from lightning discharges. The electrical signals produced by LF and VLF ("LF/VLF") detectors are ordinarily integrated prior to analysis to produce a waveform representation of the electric or magnetic discharge field, as the antenna inherently responds to the time derivative of the field. Analyzing signals representative of either an electric or magnetic field to distinguish CG and IC discharges 1 WO 03/069375 PCT/USO3/04351 is referred to as performing waveform analysis. There are several criteria for distinguishing between CG and IC events. One well known method for distinguishing lightning signals both in the LF and in the VLF range is to examine the time that passes from a peak in a representative signal to the instant it crosses a zero amplitude reference 5 point. This is referred to as a peak-to-zero ("PTZ") method of analysis. A relatively short PTZ time is a good indication that an IC discharge has occurred. Another well known method of distinguishment is referred to as a bipolar test wherein the representative signal is examined for a first peak and a subsequent peak of opposite polarity which is greater than a pre-determined fraction of the first peak. Such an 10 occurrence is another good indication of an IC discharge. Yet another test for IC discharges is the presence of subsequent peaks of the same polarity in a representative signal greater than the initial peak. This is predicated on the fact that some IC discharges have a number of small and fast leading electromagnetic pulses prior to a subsequent larger and slower pulse. In the absence of such criteria indicating that the discharge is an 15 IC discharge, it is ordinarily assumed to be a CG discharge. Even with the application of all established criterion for distinguishing between CG and IC events, some events are still misclassified. An alternative method of lightning detection is to monitor very high frequency ("VHF") radiation from lightning discharges. However, VHF detection systems must be 20 able to process information at extremely high data rates, as VHF pulse emissions in IC lightning occur approximately one tenth of a millisecond apart. Additionally, VHF systems can only detect lightning events that have direct line of sight to the sensor. One such system is currently in use by NASA at Kennedy Space Center in Florida. However, 2 WO 03/069375 PCT/USO3/04351 this system is further restricted to line of sight between the sensors and the central analyzer as it uses a real-time microwave communication system. Additionally, the VHF system in use by NASA has proven to be expensive to install and maintain. Previous lightning detection and data acquisition systems for detecting low 5 frequency electric field signals have been designed around a combination of two location methods, time-of-arrival ("TOA") and magnetic direction finding, with time-domain field waveform analysis. In most of these systems, the sensors are predominately analog devices. Using analog devices in lightning sensors requires the utilization of "track and hold" circuits to detect a qualifying event, capture a representative signal, and perform 10 waveform analysis on it. Due to an accumulation of delay periods in these "track and hold" circuits, these sensors have a large "re-arm" time, or "dead-time", during which the sensors do not record subsequent lightning events. Even more modem lightning detection and data acquisition systems that are substantially digital have some dead time. For example, the sensors in some such systems have a "dead-time" of 5 to 10 milliseconds, 15 and even the most current digital sensors have a "dead-time" of up to one millisecond. The latter are capable of detecting only a limited fraction of IC lightning discharges. This is due in part to the fact that several IC lightning discharges could occur in a single millisecond. CG lightning flashes, however, tend to have fewer discharges with relatively large periods of times between individual discharges. If a previous generation sensor is 20 designed to monitor both CG and IC electric field signals, a significant portion of time is occupied processing IC discharge events at the expense of recording CG events. Another aspect associated with sensor dead times and the TOA location method is the uncertainty in assuring that multiple remote sensors will respond to the same IC lightning event. Due 3 WO 03/069375 PCT/USO3/04351 to attenuation suffered by electromagnetic waves as they travel long distances over the earth, remote small amplitude events become difficult to detect. If different sensors produce time-of-arrival information from different events, the computed discharge location will have significant error. 5 Analog sensors operating at LF/VLF frequencies are difficult to tune for both CG and IC lightning discharges. The median amplitude of a CG field signal is about an order of magnitude greater than the median amplitude of an IC field signal. Optimizing the gain of one of these sensors to detect IC events often causes the sensor to become saturated with the much greater energy of nearby CG lightning discharges. Therefore, it is 10 customary to adjust the gain to accommodate both types of field signals, reducing a sensor's ability to detect IC events. As distant IC lightning discharges become attenuated by propagation over the ground, they become difficult to distinguish from background environmental noise. In order for the lightning detection system to provide useful information in a 15 timely manner, there must exist a method of transmitting sensor information to a central location. This central location must collect information from numerous remote sensors which is then correlated to establish the location, magnitude, and time of occurrence of lightning discharges. Existing detection systems generally have low-bandwidth communication systems, limiting the amount of information that a sensor can transmit to 20 the central analyzer. In many existing lightning detection networks, the sensors are connected to a central location by low-speed telephone modems, usually 2400 to 9600 bits per second. In the past, this communication restriction was not overly critical, as the 4 WO 03/069375 PCT/USO3/04351 large dead-time of previous generation analog sensors limited the amount of information that could be collected and sent to the central analyzer. Once the sensor information arrives at a central location, it must be analyzed. The information from each sensor is compared against incoming information from other 5 sensors. This correlation process attempts to find corresponding data to determine the location, magnitude, and time of occurrence of lightning discharges. However, current correlation techniques are not sufficient to handle large amounts of information when the time between discharges is more than an order of magnitude shorter than the travel time between sensors. In fact, if a lightning detection system made use of advanced 10 technologies to transmit and receive an increased amount of information, current central analyzers would be unable to process the information efficiently with current correlation techniques. The state of the art of lightning detection and data acquisition systems is generally represented, in part, by several patents. First, Krider et al. U.S. Patents 4,198,599 and 15 4,245,190 describe a network of gated wideband magnetic direction finding sensors. These sensors are sensitive to return strokes in CG lightning flashes. In U.S. Patent No. 4,198,599, discrimination and classification is accomplished by examining the shape of the time-domain field waveform. A short rise time (time from threshold to peak) results in a representative signal being placed in an analog track and hold circuit while further 20 analysis is performed. These sensors are designed with CG discharges being of primary interest. Any IC lightning discharges that are detected are discarded. However, both CG and IC events that meet the short rise time criteria and a simple test of event duration result in a significant amount of sensor dead-time. 5 WO 03/069375 PCT/USO3/04351 Second, Bent et al. U.S. Patents 4,543,580 and 4,792,806 disclose networks of sensors that measure TOA of electric field signals and employ this information to locate lightning. These sensors do not discriminate between IC and CG discharges. However, these sensors suffer the similar dead time issue as the magnetic direction sensors of the 5 Krider patents. When a number of IC discharge pulses occur in a short time, there is no assurance that multiple sensors will respond to same IC discharge event. Another patent of interest is Markson et al. U.S. Patent No. 6,246,367 wherein a lightning detection system utilizes an analog-to-digital converter ("ADC") to provide continuous processing of representative field signals. This eliminates the dead time issue 10 inherent in previous generation sensors. Markson describes using a bipolar comparator to distinguish between positive and negative polarity versions of a particular pulse that is inferred to be the first broadband radiation pulse in either a CG or an IC flash. Markson also uses a data correlation process and time-of-arrival difference location method. Markson explicitly uses a high pass filter to block most low frequency components of 15 representative field signals, which are not necessarily useful for detecting the initial pulse in the flash. Limitations of the Markson patent are the specific use of the HF frequency range and detection and processing of only the first pulse in each flash. Accordingly, there has been a need for improvement of lightning detection and data acquisition systems in several respects. First, an improved signal conditioning 20 method is needed. CG events are normally an order of magnitude larger than IC events at LF, due to the channel length and amount of current which flows during a CG return stroke. As mentioned previously, increasing the gain, or equivalently reducing the event threshold, results in CG events saturating an analog detection and evaluation system or 6 WO 03/069375 PCT/USO3/04351 the pick-up of significant amounts of noise. Reducing the gain, or equivalently increasing the event threshold, results in inefficient detection that masks IC events. There is a need to reduce the effect of this magnitude difference between CG and IC signals while removing unwanted noise components. An interesting aspect of both electric field and 5 magnetic field antennae is that they produce a signal which is proportional to the time derivative of the electromagnetic field they are detecting. These differentiating antennae actually reduce the magnitude disparity between IC and CG differential representative signals. However, current generation sensors invariably impose integration methods to convert the differentiated field signal to one representative of the electromagnetic field 10 without making use of the fact that the antenna itself reduces dynamic range requirements. Additionally, there is a need for an improved classification method for distinguishing between lightning types. Another need in the industry is the ability to program remote sensors with new or different waveform analysis techniques. There is also a need for improved data 15 compression and data decimation techniques to accommodate more IC as well as CG information. Additionally, new data correlation techniques are needed to handle increased information processing rates. These correlation techniques need to handle both time-of-arrival and direction information. Thus, a need exists for a complete lightning detection and data acquisition system 20 that combines new methods of signal conditioning, a user changeable system for event classification, new methods of data compression, and new data correlation techniques to efficiently detect CG and IC events and determine their location, magnitude, and time of occurrence. 7 WO 03/069375 PCT/USO3/04351 SUMMARY OF THE INVENTION The present invention meets the aforementioned needs by utilizing a plurality of remote programmable sensors (RPS) disposed in different geographic locations to detect, classify, package, and transmit in compressed form information regarding both CG and 5 IC lightning discharges. The information is collected at a central analyzer location where it is decompressed and correlated in order to determine the location, magnitude, and time of occurrence of the lightning discharges. An antenna designed to detect the electromagnetic field signal from a lightning discharge and produce a derivative representative field signal is used. The derivative signal has the benefit of reducing the 10 amplitude disparity between CG and IC field signals. A filter is used to increase the signal to noise ratio by passing the low frequency portions of the differentiated signal while discarding high frequency noise without integrating the principal components of the signal. Non-linear amplification further reduces the amplitude disparity between CG and IC signals by providing greater amplification for lower amplitude signals. The amplified 15 signals are then processed by an ADC to convert an amplified differential signal into a digital representation. This conversion allows a signal to be processed and stored digitally. The digital representation is then integrated by a digital processor to provide a signal representative of the electric or magnetic field. The digital differentiated field signal and the digital signal representative of the field itself are used by the digital 20 processor to classify the lightning event as either a CG or IC event. The analog-to-digital conversion coupled with digital storage permits continuous detection and evaluation of lightning discharges, which eliminates the "dead time" inherent in previous generation lightning detection systems. 8 WO 03/069375 PCT/USO3/04351 The present invention uses a novel data compression process to transmit data over low bandwidth communication channels. Numerous digital signal pulses representative of lightning discharges are grouped together in pulse trains. The largest pulse is designated as the reference pulse and its amplitude, time, and direction (if 5 available) are included in a data record. Other pulses in the pulse train are represented by a fractional amplitude of the reference pulse and a time-stamp relative to the time of the preceding or following pulse. This greatly reduces the information that must be transmitted to define all the pulses in the pulse train accurately. If the amount of transmitted information still exceeds the bandwidth of an associated communications 10 channel, then the RPS sensors in the lightning detection system can be programmed to transmit synchronized portions of the information, so that all sensors will report information about the same lightning events. Once received by the central analyzer, the information is unpacked and the original pulse amplitude, time, and direction (if available) information is reconstructed. 15 The unpacked pulse information is used to correlate lightning strike information from a plurality of sensor locations. This information is used to determine the magnitude, location, and time of occurrence of the lightning discharge. Accordingly, it is a principal object of the present invention to provide a novel and improved lightning detection and data acquisition system and method. 20 It is another object of the present invention to provide a lightning detection and data acquisition system and method with improved capability of distinguishing CG and IC lightning events. 9 WO 03/069375 PCT/USO3/04351 It is a further object of the present invention to provide a lightning detection and data acquisition system that reduces the amplitude disparity between CG and IC lightning representative field signals. It is an additional object of the present invention to provide a lightning detection 5 and data acquisition system and method that provides continuous detection and processing of electromagnetic field signals caused by lightning discharges. It is yet another object of the present invention to provide a lightning detection and data acquisition system and method for compression, decimation, and transmission of digital representations of lightning electromagnetic field signals. 10 It is yet a further object of the present invention to provide a lightning detection and data acquisition system and method for improved correlation of information from a plurality of remote programmable sensors to determine the location, magnitude, and time of occurrence of lightning strikes. It is a further object of the invention to provide a lightning detection and data 15 acquisition system in which the configuration of the sensors may be set or altered by remote access. The foregoing and other objects, features, and advantages of the invention will be more readily understood upon consideration of the following detailed description of the invention, taken in conjunction with the accompanying drawings. 10 WO 03/069375 PCT/USO3/04351 BRIEF DESCRIPTION OF THE DRAWINGS Figure 1 is an illustration of the physical arrangement of an exemplary system for acquiring data about cloud-to-ground and intra-cloud discharges according to the present invention. 5 Figure 2 is an illustration of a typical LF/VLF field waveform and corresponding time derivative waveform produced by a cloud-to-ground discharge. Figure 3 is an illustration of a typical LF/VLF field waveform and corresponding time derivative waveform produced by an IC discharge. Figure 4 shows empirically derived cumulative distributions of range-normalized 10 signal amplitude distributions of cloud-to-ground and IC discharges. Figure 5 is a functional block diagram of a preferred embodiment of a lightning detection and data acquisition system according to the present invention. Figure 6 is a structural block diagram of a preferred embodiment of a lightning detection and data acquisition system according to the present invention. 15 Figure 7 is a block diagram of an antenna filter network according to the present invention. Figure 8 is a graph of two exemplary frequency responses of the antenna filter network of Figure 7. Figure 9 is a graph of the gains of two non-linear amplifiers. 20 Figure 10A-10H is a flow chart of the operation of a preferred embodiment of a detection and data acquisition method for individual lightning discharge pulses according to the present invention. 11 WO 03/069375 PCT/USO3/04351 Figure 11 shows the time domain response of a digital filter according to the present invention for numerical integration of signals representative of the time derivative of the field. Figure 12 shows the frequency domain response of a digital filter according to the 5 present invention for numerical integration of signals representative of the time derivative of the field. Figure 13 illustrates the analysis performed on a general field waveform by a system according to the present invention. Figure 14 is a flow chart illustrating the process of grouping individual pulses into 10 pulse trains according to the invention. Figure 15 is a flow chart illustrating a "pre-trigger kibosh" test Figure 16 is a table depicting the time and amplitude of six electromagnetic pulses which, cumulatively, form a pulse train. Figure 17 is a table showing decimal and hexadecimal representations of the first 15 pulse of Figure 16. Figure 18 illustrates binary and hexadecimal representations of the largest pulse of Figure 16 compressed according to the invention. Figure 19 illustrates binary and hexadecimal representations of all pulses other than the largest pulse of the pulse train of FIG. 16. 20 Figures 20A-20D are a flowchart illustrating a compression process according to the invention. Figures 21A-21C are a flowchart illustrating a de-compression process according to the invention. 12 WO 03/069375 PCT/USO3/04351 Figure 22 is a time graph depicting the arrival of electromagnetic pulses at different remote programmable sensors as reconstructed through the de-compression process of Figures 21A-21C. Figure 23 is a table with the pulses of Figure 22 sorted by amplitude and sensor 5 location according to the invention. Figure 24 is a time-adjusted graph depicting a correlation process according to the invention. DETAILED DESCRIPTION OF THE INVENTION Referring to FIG. 1, a preferred embodiment of the lightning detection and data 10 acquisition system 10 is illustrated. Remote Programmable Sensors ("RPS") 12 are distributed tens to hundreds of kilometers apart. The remote sensors are used to detect electromagnetic fields generated by lightning discharges from clouds 22 as either CG lightning 14 or IC lightning 16. Communication link 18 allows the remote sensors 12 to send information to a central analyzer 20, where the locations, magnitudes, and times of 15 occurrence of the lightning discharges are determined. CG lightning discharges are generally ten times larger in magnitude than IC events in the VLF/LF frequency range. To prevent saturation of the analog components of the remote sensor 12, a means for reducing the amplitude disparity between CG representative signals and IC representative signals is provided. The sensors 12 also 20 possess a means for increasing the signal-to-noise ratio of the representative signals. Additionally, the sensors 12 convert the analog representative signals into digital signals which are then classified as either CG or IC lightning. Once the signals have been 13 WO 03/069375 PCT/USO3/04351 classified, the sensor determines whether groups of signals are sufficiently close together in time to be considered a train of pulses. For such pulse trains, the sensor packages the signal information into compressed data words and transmits the data words to the central analyzer 20. Isolated pulses are transmitted alone with a richer set of characterizing 5 features. If the communication link is insufficient to handle all the information, then the remote sensor 12 decimates the information, only sending synchronous portions of the information. The central analyzer 20 is used to receive the data words sent from the remote sensors 12 and decompress the words to obtain the lightning discharge information. 10 Applying correlation techniques, the information from a plurality of sensors 12 is used to determine the magnitude, location, and time of occurrence of lightning discharges 14, 16. Lightning flashes occur between opposite polarity charge accumulations. The lightning flash begins with small breakdown events as the air between the charge accumulations is ionized, forming conducting channels. In a CG flash, once a channel has 15 been formed from the cloud to the ground, large amounts of current flow between the cloud and the ground. The discharges carrying these large current flows are called return strokes. A typical CG lightning flash will have four return strokes. These strokes are typically tens of milliseconds apart. A waveform 30 of the field generated by a CG stroke is shown in FIG. 2. This figure illustrates an electromagnetic pulse with a first negative 20 peak 32, a first negative trough 34, a second negative peak 36, a zero crossing point 38, a first positive peak 40, a first positive trough 42, and a second positive peak 44. A second signal 46 demonstrates the electrical signal representative of the field wave after detection by an antenna 12 which is responsive to the time derivative of the field. 14 WO 03/069375 PCT/USO3/04351 The number of discharges in an IC flash is approximately ten times greater than the number of strokes in a CG flash. On the other hand, the median amplitude of electromagnetic fields caused by CG lightning strokes is approximately ten times greater than that caused by IC discharges. The time spacing between pulses in an IC discharges is 5 also much less than for CG lightning. The result is that IC discharges often occur as pulse trains. The largest amplitude electromagnetic field pulse generally occurs in the middle of these pulse trains. A waveform 50 of the field generated by an IC discharge is shown in HFIG. 3. This figure illustrates an electromagnetic field pulse train made up of numerous prominent pulses 52 and several small to moderate pulses 54. A second signal waveform 10 56 demonstrates the electrical signal representative of the time derivative of the field after detection by the (differentiating) antenna 12. Figure 4 shows empirically determined cumulative distributions of range normalized signal amplitudes of IC and CG discharges. Range-normalization results in signal amplitude values that are independent of the actual distance between the sensor and 15 the discharge. A first curve 70 in Figure 4 is a range-normalized representation of CG events. The domain is signal strength in LLP units range normalized to 100 km from the sensor location. Referring to the first curve 70, 50 percent of CG lightning events have an amplitude larger than 120 LLPUs and 50 percent are below 120 LLPUs. Approximately 80 percent of CG events have amplitudes less than 180 LLPUs and 20 percent are greater 20 than 180 LLPUs. A second curve 72 represents the range-normalized distribution of the large and prominent discharges within IC flashes, while a third curve 74 illustrates the range-normalized distribution of all IC discharges. Approximately 70 percent of all IC events are less than 1 LLP. This amplitude disparity requires a novel approach to 15 WO 03/069375 PCT/USO3/04351 lightning detection and processing if both CG and IC events are to be detected by the same sensor in the LF/VLF frequency range. Turning to FIG. 5, a block diagram illustrates the functional aspects of a lightning detection and data acquisition system according to the present invention. A 5 differentiating antenna 92 is used to detect either an electric field or a magnetic field generated by a lightning discharge. The antenna 92 outputs an analog signal representative of the detected field wave ("electrical detection signal") and sends it to the remote programmable sensor 94. The first stage of the remote sensor 94 is a signal conditioning circuit 96 used to reduce the amplitude disparity between CG representative 10 signals and IC representative signals, reduce noise, and convert the conditioned electrical detection signal to a digital representation. Once the representative signal has been conditioned, it is passed to the event classification stage 98 where the digital representative signal is evaluated to determine what type of event caused the electromagnetic field (either a CG or IC discharge). The remote sensor can be 15 programmed based on user-selectable criteria resulting in only signals of interest being accumulated. The accumulated signals of interest are processed by data compression software 100. If necessary, they are also processed by the data decimation stage 102 and then transmitted to the central analyzer 104 using any digital data transmission means. The central analyzer utilizes data decompression 105 and data correlation 106 followed 20 by location determination 108 to determine the magnitude, location, and time of occurrence of the lightning event. Referring to Figure 6, a structural block diagram of a preferred embodiment of a remote programmable sensor 110 is illustrated. The analog front end 112 accepts an 16 WO 03/069375 PCT/USO3/04351 analog representative signal from an electromagnetic antenna, filters the representative signal using the filter and amplification component 124 and passes the representative signal to an ADC 114 and an amplitude comparator 128 using a cross-point switch 126. The comparator 128 is used to determine whether the amplitude of the analog 5 representative signal exceeds a previously determined value, indicating the beginning of a "pulse". Upon determination that a pulse has begun, a Global Positioning System ("GPS") device 130 is used to provide a time-stamp which is stored in a time tag first-in first-out ("FIFO") 132 in a Field Programmable Gate Array ("FPGA") 116. The ADC 114 is used to provide continuous digitization of the signal provided by the cross-point switch 10 126. The ADC produces a digital signal with 12 bit resolution sampled at 20 MHz. The digitized signal is sent to a digital summer 134 inside the FPGA 116 mentioned above. The summer 134 is used to add groups of four digital samples producing a 5 MHz sample with a 14 bit resolution. These 14 bit digital samples are placed in a signal FIFO 136 in the FPGA 116. A clock signal provided by the FPGA is used to control the flow of digital 15 samples from the signal FIFO 136 to a ring buffer 138 residing in a synchronous dynamic random access memory device ("SD-RAM") 120. Access to the ring buffer 138 occurs by way of a dynamic memory access controller ("DMA") 140, part of a digital signal processor ("DSP") 118. The DMA controller 140 also transfers event time-stamps from the time tag FIFO 132 in the FPGA 116 to a time tag buffer 142 in the SD-RAM 120. A 20 central processor unit ("CPU") 144 inherent in the DSP 118 is used to evaluate data stored in the ring buffer 138 and time-stamp information stored in the time tag buffer 142. Data representing signals of interest are placed in a results buffer 146 in the SD-RAM 17 WO 03/069375 PCT/USO3/04351 120. The information then passes through a DSP-to-PC interface 148 to a host personal computer 122 where it is packaged for transmission. The signal conditioning and classification aspects of the remote programmable sensor 110 are addressed hereafter, and is illustrated by FIGs 7, 8, 9, and the flow chart in 5 HFIGs 10A-10H. Analog Processing The basic components of the antenna filter network 300 are shown in FIG.7. An antenna 301 provides a differentiated signal to a low pass filter 302 (four-pole or more) and high-pass filter 304. The filters are followed by an optional non-linear amplification 10 stage 306. Both electric field and magnetic field antennae produce signals that depend on the time derivatives of the field signals they monitor. Thus, this antenna 301 is referred to as a differentiating antenna. This differentiating property of the antenna 301 is important, as it has been discovered that differentiating electromagnetic signals reduces the amplitude disparity between CG and IC representative signals by a factor of two to four. 15 Previous generation lightning detection systems have not made use of this antenna property. In fact, most lightning detection systems integrate the antenna output to get a true representation of the electromagnetic field. The four-pole low pass filter 302 is used to provide a good transient response to the differentiated signal. The output of the low pass filter 302 is sent to a high pass filter 20 304 with a cut-off frequency around 300 hertz. The purpose of this filter is to remove any signals that are probably man-made such as 50/60 hertz power-line noise. In the frequency range between these two filters, no filtering is applied. This preserves the differentiated nature of the signal throughout the band where the signals of interest exist. 18 WO 03/069375 PCT/USO3/04351 This tuning of the filters effectively creates an analog leaky integrator that is tunable to allow frequencies below 0.5-1 MHz to pass through without being integrated. An optional component of the invention is the use of non-linear amplifiers 306 to further reduce the amplitude disparity between CG and IC representative signals. A first curve 310 of FIG. 8 5 shows the frequency response of the leaky filter network, including the differentiating antenna, in the preferred embodiment. A second curve 312 illustrates the frequency response of the leaky filter network wherein the time constant has been adjusted to remove excessive man-made radio frequency noise. The non-linear amplifier 306 of the preferred embodiment amplifies low 10 amplitude signals disproportionately more than high amplitude signals. Two types of non linear amplifiers that are well suited to this application are the logarithmic amplifier and the piece-wise linear amplifier. Both of these types of amplifiers can reduce the amplitude disparity between CG and IC signals by 12-24 dB. FIG. 9 illustrates the input-output characteristics of these non-linear amplifiers. A first curve 330 shows the response of a 15 logarithmic amplifier while a second curve 332 illustrates the response of a piece-wise linear amplifier. Referring to FIG. 10A, a differentiated representative analog signal is received from the antenna 92 of FIG. 5. Steps 150 and 151 are low-pass filtering necessary to remove high frequency noise from the representative signal, followed by high-pass 20 filtering used to remove power line noise. Optional non-linear amplification 152 is used to amplify low-amplitude signals disproportionately more than high amplitude signals, reducing the amplitude disparity between CG and IC signals. 19 WO 03/069375 PCT/USO3/04351 Data gathering Following non-linear amplification 152 in FIG. 10A, using the cross-point switch 154, analog information is sent to threshold comparison 156 and digitization 162. If a representative signal exceeds a pre-determined amplitude value, a "threshold crossing 5 time" is established in step 158 using the GPS device 130 of Figure 6 and placed into the time tag FIFO 132 per step 160. Simultaneous with threshold comparison 156, 12 bit resolution continuous digitization 162 at a rate of 20 MHz occurs at the ADC 114 of Figure. 6. In LF/VLF sensors, every four samples are added together in step 166 using the digital summer 134 of the FPGA 116. The result, a 5 MHz data sample stream with 10 14 bits of resolution, is stored per step 168 in the signal FIFO 136 of the FPGA 116. The process of moving samples through the FIFO 136 until they reach the end is shown by step 170. Control logic provided by the FPGA 116 and the DMA controller 140 are used to control the flow of digital samples from the signal FIFO 136 to the ring buffer of the SD-RAM 120; this is shown by step 172 of FIG. 10B. Implicit in the address of the data 15 sample within the ring buffer is the time stamp to the fraction of a second. A separate clock signal in the DSP 118 is used to regulate reading data samples from the ring buffer 138 into the CPU 144 of the DSP per steps 174. In practice, the transfer of data into the ring buffer at step 172 is always a few samples ahead (in time) of the transfer of data out of the ring buffer and into the DSP CPU at step 174. This time lag is represented 20 graphically by the "future buffer" 173 in FIG. 10B to symbolize the fact that this lag allows the DSP to examine a few samples on either side of the sample currently being examined at step 176. Step 178 provides the next time-stamp from the time tag buffer 142 to the CPU 144. Step 176 is the determination of whether the current data sample 20 WO 03/069375 PCT/USO3/04351 occurred at or after the threshold crossing time indicated by the time-stamp. If so, step 180 is used to determine whether the amplitude of the digitized signal has been below a threshold established for the end of an event. If so, the event which produced the pulse beginning with the time-stamp retrieved by step 178 is deemed to have ended, i.e., the 5 pulse is over. Step 182 is used to advance the time tag buffer to the next event of interest and proceed to pulse classification, step 184. If the result of step 180 is that the pulse is not deemed complete and we are just beginning a pulse, then steps 186 and 188 are used to find the time of the first data sample within the present pulse that had an absolute magnitude above the noise level. This time is not the same as the time-stamp retrieved in 10 step 178, as the time-stamp was recorded only after the current pulse exceeded a pre determined threshold magnitude (set higher than the noise floor). Steps 189 and 190 are used to generate a representative field signal by numerically adding the current data value to a weighted sum of all previous data values where the weighting is a function of the age of the samples. This process constitutes a 15 digital integrator to reconstruct the field signal over the band of interest using the differentiated field signal that has been passed through to this point. Figure 11 shows the time domain response 314 of the digital integrator according to the present invention. Figure 12 shows the frequency domain response 316 of the digital integrator according to the present invention. At the completion of step 192 of FIG. 10C, the data sample now 20 has three components: a time-stamp, the value of the derivative field signal, and the value of the representative field signal itself. A signal representative of an entire field pulse 293 after the digital integration is illustrated in FIG. 13. 21 WO 03/069375 PCT/USO3/04351 Peak and trough and zero-crossing determination Steps 194 and 196 are used to look for peaks and troughs in the representative field signal by searching the derivative signal for zero crossing points. In practice, the differentiated signal will contain some noise and will need to be smoothed 193 (digitally 5 filtered) in order to retain prominent peaks and troughs without flagging all small high frequency sign changes in the time derivative as significant peaks and troughs in the field signal. In a preferred embodiment, this smoothing will involve several samples on either side of the current sample. A first peak 294, a first trough 295, a second peak 296, and a zero crossing point 297 of the representative field signal 293 are shown in FIG. 13. The 10 number of peaks in the current pulse is recorded in step 200. In accordance with step 202, if the field representative signal has changed polarity, then a zero-crossing time is recorded in step 204 and a counter is incremented in step 206 of FIG. 10D. Once the data sample has been tested for peaks, troughs, and zero-crossing times, the next data sample is read into the DSP's CPU 144 in step 208 of FIG. 10D and the process returns to step 15 174 of FIG. 10B. The process steps illustrated by FIGs 10A, 10B, 10C, and 10D are used to detect signals of interest and gather information. Specifically, at the conclusion of step 208, the following information has been determined: (1) the number of peaks in the current pulse of the field representative signal; (2) the number of troughs in the current pulse; (3) the 20 time and amplitude of each peak and trough of the current pulse; (4) the number and times of zero crossings in the current pulse. 22 WO 03/069375 PCT/USO3/04351 Pulse Classification Once the pulse is determined to have terminated at step 180 of HFIG. 10B, then the process proceeds from step 184 to step 242 of FIG. O10E where pulse classification begins. Pulse classification begins by establishing a default value for the pulse as a IC event in 5 step 244. The overall pulse duration is evaluated in step 246. If the pulse is too short in duration or the largest amplitude of any peak within the pulse is too small, the event is presumed to be noise and is discarded in step 248, the counts of zero crossings, peaks, and troughs are zeroed at step 250, and the process returns to step 174 of FIG. 10B. If the pulse has sufficient duration, then it is evaluated for an excessive number of zero 10 crossings in step 252. Too many zero crossings are another indication of noise, in which case the pulse is discarded in step 248 and the process returns to step 174 of HFIG. 10B. A novel pulse classification process is illustrated by step 256, where the pulse is evaluated for a short time from the largest peak of the first polarity to the largest peak of opposite polarity. The result of this test must be temporarily saved (steps 257 and 258) because 15 after this test, all pulses proceed to the bipolar amplitude ratio test at step 260 of FIG. O10F. This pulse classification parameter is given by the time between the first peak 294 and the second peak 296. Pulses with a short time differential between these peaks are classified as IC pulses or leader pulses. 23 WO 03/069375 PCT/USO3/04351 Bi-polar amplitude ratio test Step 260 is used to determine if the largest of any subsequent opposite polarity peaks (299 of Figure 13) is greater than a pre-determined fraction of the largest peak of the initial polarity 294. In the event that the opposite polarity peak time difference (step 5 256 of FIG. 10E) was short, the bipolar amplitude ratio distinguishes between bipolar IC discharge pulses and leader pulses, which tend to be nearly unipolar. Thus, after step 260, the result of the opposite-polarity peak time test must be examined (steps 261, 263). If the bipolar amplitude ratio 260 was large and the opposite polarity peak time result was true (step 263), the pulse is classified as a bipolar IC pulse (step 265). If the bipolar amplitude 10 ratio is small and the opposite polarity peak time result was true (step 261), the pulse is classified as due to a leader (step 264). In the preferred embodiment, leader pulses are considered a special case of IC discharge pulses. Beyond steps 264 and 265, no further testing is required, and the IC discharge pulse information is saved 267 at step 284 of FIG. 10H. On the other hand, if the bipolar amplitude ratio is large, and the opposite 15 polarity peak time result was false (step 263), the pulse is classified as due to a distant CG stroke in step 270. Finally, if the bipolar amplitude ratio is small and the opposite polarity peak time result was false (step 261), the pulse is classified as due to a CG return stroke (not distant) at step 268. In either event, pulse classification continues at step 271. Optionally, if classification is used to eliminate IC discharges, the pulse may be discarded 20 in step 266 and the process returns to step 174 of FIG. 10B. 24 WO 03/069375 PCT/USO3/04351 Peak-to-zero test The first peak to zero time is evaluated at step 271 of FIG. 10F. If the peak-to-zero time 298 of FIG. 13 is relatively long in duration, the pulse retains its classification as a CG event. If the peak-to-zero time 298 is short, then the pulse is reclassified as a IC 5 event in step 262. In either event, pulse classification continues at step 274 of FIG. 10G. Second peak greater than first peak test Step 274 of FIG. 10G determines whether more than one peak of the same polarity (294, 296 of FIG. 13) occurs prior to an opposite polarity peak 299. If not, pulse classification ends at step 282. Otherwise an additional test 276 is used to determine 10 whether a second peak of the same polarity 296 within the pulse is sufficiently greater in amplitude than the first peak 294 of the pulse. If true, the pulse is reclassified as a cloud discharge in step 280. Otherwise, the pulse retains its classification as a CG discharge. In either case, classification ends at step 282 and the process proceeds to recording pulse information, step 284 of FIG. 10H. 25 WO 03/069375 PCT/USO3/04351 Save pulse information Step 284 of FIG. 10H begins the process of storing pulse information and event classification. In step 286, the pulse is defined by the following information: the threshold crossing time, the onset time; the first and second peak times; the first rise time; 5 the first and second peak amplitude; the peak-to-zero time; opposite polarity peak time and amplitude; field derivative at first zero crossing; pulse classification. In step 288, this information is stored in the results buffer 146 of the SD-RAM in FIG. 6. At this point, the process obtains a new data sample (step 289) and returns to step 174 of Fig 10B. At the same time, the pulse information saved to the results buffer at 288 is made available to 10 another process 290 that looks for and processes pulse trains. 26 WO 03/069375 PCT/USO3/04351 Pulse Train processing The flow chart of FIG. 14 illustrates the process of grouping individual pulses into pulse trains. Pulse train processing begins at step 412 and is initiated when pulse information has been stored in the results buffer 146 in step 288 of FIG. 10H. The time 5 between the most recent pulse and the previous pulse is evaluated in step 414. If the time interval between the two pulses exceeds a pre-determined amount, then the previous pulse is examined, step 416, to determine if it is part of an existing pulse train. If so, the existing pulse train is deemed to have ended, the data are compressed in step 422, the compressed data is sent to a host PC 122 in step 424, the previous pulse and its associated 10 pulse train are removed from the results buffer 146 in step 426, and the pulse train buffer is cleared in step 428. If the previous pulse is not part of an existing pulse train, the previous pulse is transferred to the host PC 122 in step 418 with all of the parameters saved at step 286 of HFIG. 10H, and it is then removed from the results buffer 146 in step 420. If the time interval evaluated in step 414 is found to be less than a pre-determined 15 amount, then the previous pulse is evaluated to determine if it belongs to an existing pulse train in step 430. If so, an optional PTK test is performed in step 432 and the amplitude of the newest pulse is evaluated to determine whether it is greater than any previous pulse in the current pulse train in step 436. If found to be larger than any previous pulse in the current pulse train, the newest pulse is flagged in step 438. Returning to step 430, if the 20 previous pulse is not part of a current pulse train, then a new pulse train is created starting with the previous pulse in step 434 and the process proceeds to steps 432, 436 and 438. The final step of this process is to move the newest pulse into the position of the second newest pulse in the results buffer 146 at step 440 and then return to step 412 awaiting the 27 WO 03/069375 PCT/USO3/04351 arrival of the next pulse. A maximum wait time is also used to make sure that pulses are transmitted to the central analyzer within a reasonable time period when there is little activity. In previous generation lightning detection systems, "pre-trigger kibosh" tests 5 consisted of determining whether a CG stroke was immediately preceded by an event of opposite polarity. If so, both the current pulse and previous pulse were discarded as they were deemed to have been most likely caused by an IC discharge or noise or interference. In these earlier systems, it was deemed more efficient to discard these pulses than tie up the analog hardware with further analysis. However, in the present invention it has been 10 found more effective to perform more thorough pre-trigger kibosh tests. Referring to FIG. 15, a flow chart illustrates the pre-trigger kibosh test referred to in FIG. 14. This test begins with step 450. The current pulse is evaluated in step 452 to determine whether it is a CG stroke. If not, the process returns to the pulse train processing algorithm step 466. However, if the current pulse is a CG stroke, then it is first transmitted to the host PC at 15 step 453 with the complete set of features saved at step 286 of FIG. 10H. Then, the previous pulse is examined in step 454 to determine whether it is an IC event. If not, the process returns to the pulse train processing algorithm at step 466. If the current pulse resulted from a CG stroke and the previous pulse was caused by an IC event, then the next step 456 of the algorithm is to determine whether the current pulse and previous 20 pulse have opposite polarity. If not, the process returns to the pulse train processing algorithm at step 466. If both pulses do have opposing polarity, the current pulse train is discarded in steps 458-464 and the process returns to step 412 of FIG. 14. 28 WO 03/069375 PCT/USO3/04351 As mentioned in the Summary of the Invention, RPS sensors are capable of detecting and evaluating at least an order of magnitude more lightning discharges than previous generation sensors. Therefore, an improved method for sending the lightning information to the central analyzer is required. The present invention uses a novel data 5 compression process for lightning discharges that occur in pulse trains according to the process of FIG. 14. The largest pulse is designated as the reference pulse and its amplitude, time, and direction (if available) are included in an 88 bit data record. Other pulses in the pulse train are represented by a fractional amplitude of the reference pulse with a time-stamp relative to the time of either the preceding or the following pulse, 10 represented by 24 bit data records. This greatly reduces the information that must be transmitted. Referring to FIG. 16, six electromagnetic pulses 470 are listed with their associated fractional second time 472, time in microseconds 474, and amplitude 476. These example pulses occur at midnight on August 6, 2001. The first pulse occurred 500 15 microseconds after midnight on this date and is represented in detail in FIG. 17. The full time stamp of the largest pulse in this example is 997056000 seconds since January 1, 1970 ("UNIX time"). A 32 bit hexadecimal representation 480 of this time stamp is: 3B6DDE00h. A fractional time count is derived by dividing the 500 microseconds by a predetermined unit of time, which is 50 nanoseconds in the preferred embodiment 20 because of the use of a 20-MHz ADC (each 50 nanosecond period being a "50 nanosecond count"). 500 microseconds divided by 50 nanoseconds produces a fractional time count of 10000. The hexadecimal representation 482 of this fractional time count is 2710h. The hexadecimal representation 484 of the amplitude of the first pulse 471 (4400 29 WO 03/069375 PCT/USO3/04351 counts) is 1130h. This particular sensor does not provide directional information, noted by assigning a value of three hundred and fifty nine point ninety-nine (359.99) degrees as the angle measurement. The hexadecimal representation 486 of this angle measurement is 7FFFh. A determination that this pulse was generated by a IC discharge is indicated with 5 a binary bit of "1" 488 (CG strokes would generate a "0" bit). Data Compression The illustrations of FIGs 18 and 19 and the flow-chart of FIGs. 20A-20D are used to illustrate the process of compressing pulse trains into data records. During the grouping of pulses (FIG. 14), the largest amplitude pulse is identified. 10 In this example, the second pulse 473 of FIG. 16 is the largest with an amplitude of 5100 counts. A binary representation of the largest amplitude pulse 473 including time, fraction of second count, amplitude, angle, classification, and an additional bit indicating whether fractional amplitudes of the smaller pulses are included is produced according to the invention. FIG. 18 shows the 88-bit compacted representation 490 of the largest pulse for 15 the present example according to the compression algorithm. A hexadecimal representation 492 of the largest amplitude pulse 473 is also shown with the binary representation 490 in FIG. 18. According to the invention, pulses in the same pulse train other than the largest amplitude pulse 473 are represented by fractional amplitudes relative to the largest pulse 20 473 and time differences relative to the preceding or following pulses. For each pulse prior to the largest pulse, the time difference is established by subtracting the 50 nanosecond time count of the current pulse from the 50 nanosecond time count of the 30 WO 03/069375 PCT/USO3/04351 pulse that follows it, resulting in a 13 bit signed binary number that is negative. Likewise, for each pulse after the largest, the time difference is given by subtracting the 50 nanosecond count of the current pulse from the 50-nanosecond count of the pulse that precedes it, resulting in a 13-bit signed value that is positive. For all pulses other than the 5 largest, the fractional amplitude of the pulse is calculated by multiplying the amplitude of the current pulse by 1000, dividing by the amplitude of the largest pulse, and rounding the result off to the nearest integer. This integer is then represented by a 10 bit binary number. A one bit binary flag is used to indicate whether the pulse is due to a CG event ("0") or an IC event ("1"). The 13 bit time difference, 1 bit classification flag, and 10 bit 10 fractional amplitude are concatenated together to generate binary representations 500 in FIG. 19 and their hexadecimal equivalents 502. Therefore, the six pulses of FIG. 16 are represented by the one 88-bit data record 490 of FIG. 18 for the largest amplitude pulse and the five 24-bit data records 500 of FIG. 19 for the five pulses other than the largest. Another optional embodiment of the invention will utilize a 15 bit signed time difference 15 value and an 8 bit fractional amplitude value rather than the 13 bit time difference and 10 bit fractional amplitude alluded to above. Other variations of this 24 bit data record scheme may be utilized to allow tradeoffs between maximum time interval and amplitude resolution. FIGs. 20A-20D are used to illustrate the compression process according to the 20 invention. In step 504 the position of the largest amplitude is identified. In step 506, the 32-bit time-stamp and 25-bit fifty nanosecond count of the largest pulse are stored. If amplitude fractions are to be used (step 508) in the representation of the other pulses in the pulse train, the amplitude fraction flag bit is set in step 512, otherwise it is cleared in 31 WO 03/069375 PCT/USO3/04351 step 510. The 14 bit binary representation of the amplitude of the largest pulse is stored is step 514. If direction information is provided (step 516), a 15 bit binary representation of the azimuth of the largest pulse is generated in step 520, otherwise the binary representation for 359.99 degrees is used in step 518. The process continues in step 522 5 of FIG. 20B where a flag indicating the type of event is set. A binary "1" indicates an IC event while a "0" indicates a CG event. A "current pulse" pointer is set to the data structure representing the pulse prior to the largest in step 524. A 13-bit value is generated for the time difference between the current pulse and the pulse immediately after it in the pulse train in steps 528 and 530. At step 532, the process determines 10 whether amplitude fractions are being used, and if so, a 10 bit value is generated for the amplitude fraction of the pulse immediately prior to the largest pulse in steps 534 and 536 and the classification bit is set in step 538 of Figure 20C. The pointer that was initialized in step 524 is then decremented at step 540 and the process loops to step 526 of Figure 20B until the pointer reaches the beginning of the pulse train. 15 Once the pointer has reached the beginning of the train, indicating that all pulses prior to the largest pulse have been encoded, the pointer is reset to the first pulse after the largest (step 542 of FIG. 20C). A 13-bit value is generated for the time difference between the largest pulse and the pulse prior to it in the pulse train in steps 546 and 548 of Figure 20C. At step 550 of FIG. 20D, the process determines whether amplitude 20 fractions are being used, and if so, a 10-bit value is generated for the amplitude fraction of the pulse immediately after the largest pulse in steps 552 and 554 and the classification bit is set in step 556 of Figure 20D. The pointer set in step 542 is then incremented in step 558 and the process loops to step 544 of FIG. 20C until the pointer reaches the end of 32 WO 03/069375 PCT/USO3/04351 the pulse train. When this occurs, the information has been compressed according to the invention and is ready to be transmitted to the central analyzer in step 560 of FIG 20D, at which point the process ends (step 562). Transmission of information between the remote programmable sensors 12 and 5 the central analyzer 20 occurs as packets or messages. These messages are made up of several 8 bit binary words. The size of the packet is variable with the number of pulses in a pulse train. The more pulses in a pulse train, the larger the message. Each message contains 11 bytes representing the largest pulse in the pulse train. The message also includes another 3 bytes for each additional pulse in the pulse train, if amplitude fractions 10 are being used. If not, the message includes one and three quarter (two in practice) bytes for each additional pulse in the pulse train. Occasionally, especially in sensors operating in the VHF frequency range, even the compression of pulse trains will be insufficient to allow all pulses to be transmitted over the available communications system in real time. In such situations, the sensor will 15 be capable of selecting portions of the pulses or pulse trains that occur in specific time periods and transmitting those only. More specifically, time is divided into short time periods referenced to the beginning of a second (for example, 50 millisecond periods). In the event of a backup of information in the communications system (as evidenced by data accumulating in an output buffer), data quantity is reduced to the first few events in a 20 collection of these time periods. For example, we may transmit only the first event from each of twenty 50-millisecond periods in one second. This "data decimation" algorithm is synchronized among all sensors in the network by way of the GPS time information, so 33 WO 03/069375 PCT/USO3/04351 that all sensors are guaranteed to transmit data corresponding to the same periods of time. Operation of the Central Analyzer is described hereafter. Data Decompression Once the information has been received by the central analyzer, it must be decompressed. 5 The flowchart of FIGS. 21A-21C represents the process necessary to decompress messages received from remote programmable sensors. The number of bytes in the message is determined in step 572 of FIG. 21A. The time-stamp of the largest pulse is extracted from the message in step 574 and the use of amplitude fractions is determined in step 578. The total number of pulses in the message is determined in step 580, if 10 amplitude fractions are not used and step 582 when amplitude fractions are used. This algorithm takes the number of bytes in the entire message determined in step 572 and subtracts eleven words, the number of words necessary to describe the largest amplitude pulse. The result is divided by the number of bytes necessary to represent a compressed pulse, two when amplitude fractions are not used and three when amplitude fractions are 15 used. A quantity of one is added to the quotient to produce the entire number of pulses in the pulse train. The amplitude of the largest pulse is determined in step 584 and the event classification is determined in step 586. A loop counter is initialized to zero in step 588 of FIG. 21B. The loop is used to step through all remaining pulses in the pulse train. 20 Each signed time difference is extracted from the compressed data stream at step 592 and added to the time stamp of either the largest pulse (step 602 the first time through the loop, as determined in the decision 594, or step 600 when the time difference changes sign as determined in the decision 596) or the time of the most recently decoded pulse 34 WO 03/069375 PCT/USO3/04351 (step 598) to generate the absolute time that each pulse occurred. Pulse classification is determined in step 604. Step 606 of FIG. 21C is used to determine whether amplitude fractions are included in the compressed data. If so, the actual amplitude of each pulse is reconstructed in step 608 and 610 of Figure 21C. The loop counter is incremented at 612, 5 and the process returns to step 590 of FIG. 21B. The loop continues until the loop counter equals the number of pulses determined in step 580 or step 582, indicating that all the pulses in the pulse train have been decompressed. At that point, the process ends at step 614 of FIG. 21C. Once the information has been decompressed, it is compared with information 10 from other remote programmable sensors 12 to determine the location, amplitude, and time of occurrence of the lightning events. With the increased information allowed by detecting pulse trains produced by the same lightning event, an improved correlation technique is required. 35 WO 03/069375 PCT/USO3/04351 Pulse Correlation Four pulse trains are illustrated in FIG. 22. A first pulse train 650 is detected by a remote programmable sensor 12 which is nearest to the site of lightning activity as indicated by the earliest time of arrival from the lightning event to the sensor and the 5 large number of pulses (thirteen). A second pulse train 652 is detected by a remote programmable sensor 12 located farther away from the lightning activity than the sensor which produced the first pulse train 650, as indicated by later arrival and fewer (eight) pulses of smaller amplitude. The remote programmable sensor 12 for the third pulse train 654 is located yet farther away from the lightning activity than the sensor producing the 10 second pulse train. The third pulse train 654 has only four pulses whose amplitudes are markedly less than those of the first or second pulse trains. A fourth pulse train 656 is detected by a remotely programmable sensor 12 which is the farthest away from the lightning activity. Only three pulses are evident in this pulse train. A unique correlation approach, according to the invention, provides high 15 confidence pulse source location using either three remote programmable sensors 12 or two remote programmable sensors 12 with direction information. If no direction information is provided by the remote programmable sensors 12, then a theoretical ideal subset of three sensors is chosen in order to provide an initial TOA-based location. This theoretical set of sensors is used to reduce the set of potential correlated pulses from other 20 sensors. To determine the necessary TOA differences, all the pulses in a time window for each sensor are sorted by decreasing signal amplitude producing the table of FIG. 23. Next, the three sensors having the largest pulses at the top of their amplitude-sorted lists are selected as the ideal subset previously mentioned. This choice is based on the fact 36 WO 03/069375 PCT/USO3/04351 that larger amplitude pulses are produced by lightning discharges that are substantially vertical and the largest pulse detected at one sensor is likely to be the largest pulse detected at another sensor. In the example of Fig. 22, the subset includes the remote programmable sensors 12 producing the first pulse train 650, second pulse train 652, and 5 third pulse train 654. These pulse trains were selected from the pulse trains reported by all sensors because they possessed the largest magnitude pulses. The largest pulses from each of the three ideal sensors are 1H, 2F, and 3C as shown in FIG. 23. Using the time differences between these three pulses, an estimated TOA-based location and time of occurrence are determined for the discharge. Next, expected values of the travel times 10 from the estimated discharge position to all sensors are determined and used to adjust the pulse trains in time by subtracting relative time differences alpha, beta, and gamma as shown in FIG. 24. The values of alpha, beta, and gamma used to slide the second pulse train 652, third pulse train 654, and fourth pulse train 656, respectively, are given by the difference between the time it takes the signal to reach each of the associated sensors 15 minus the time taken to reach the first sensor. After adjustment, the times of arrival of the largest amplitude pulses at the first three sensors coincide with pulse 4B of the fourth pulse train 656, as shown by the grouping of pulses 660 in FIG. 24. Likewise, the second largest correlated pulse corresponds with 4C of the fourth pulse train 656, as shown by the grouping 662 in FIG. 24, and finally, the third largest pulse corresponds with 4A of 20 the fourth pulse train 656, as shown by grouping 658. When at least one, and preferably more (as in FIG. 24) inter-pulse time intervals are found to match, the probability of having a proper correlation among the various sensors is very close to 1. If the pulse trains cannot be found to match as in FIG. 24, a different combination of pulses from 37 WO 03/069375 PCT/USO3/04351 three sensors from the amplitude-sorted lists in FIG. 23 is used to produce a new estimated discharge location, and the process starts over. This process may be repeated any number of times until pulses are exhausted, although in a preferred embodiment, the process might only be attempted three or four times. This correlation process has the 5 advantage that it also works well in the presence of regularly spaced pulses or pulses of similar amplitude. An alternative correlation process is used for lightning detection systems having at least 2 sensors with direction finding capability. The correlation process is the same as the method above except angle and time measurements from just two sensors are used to 10 produce an initial estimate of discharge position and time of occurrence, from which the travel time to other sensors can be estimated. Yet another extension of the correlation process is used to track the travel path of a progression of lightning discharges having a significant horizontal component to their motion. Identifying correlated pulses from different sensors with slightly different inter 15 pulse time intervals indicates pulse train expansion or contraction caused by horizontal movement of lightning during the production of the pulse train. Either of the first two correlation techniques may be used as long as a greater degree of timing uncertainty is allowed in the fine-scale pulse correlation in order to account for slightly different inter pulse intervals. If two or three sources can be located then a propagation speed and 20 direction may be estimated. These estimates may then be used to predict the contraction or expansion of pulse trains from other sensors in order to provide a further refinement to the correlation process. This correlation technique is useful to isolate different branches of a lightning discharge. TOA-based locations are determined throughout the processes 38 WO 03/069375 PCT/USO3/04351 described in preceding paragraphs, not only to get final, optimized positions in cases when there are more than three TOAs but also to get initial position estimates (start positions). In view of the foregoing, it can be seen that a system according to the invention 5 provides numerous advantages over prior art lightning detection and analysis systems. First, the system provides the ability to detect both CG and IC events while eliminating dead-time. Second, the remote programmable sensors have increased sensitivity to IC events without being swamped by CG events due to analysis of the differentiated and/or compressed waveform. Third, the system has the ability to transmit increased event 10 information over a limited broadband communication channel to a central analyzer using a novel compression and decompression scheme. Additionally, the system has the ability to correlate events that produce complex pulse trains at the central analyzer using a novel correlation technique, thereby allowing accurate TOA-based locations. The terms and expressions which have been employed in the foregoing specification are used therein as terms of description and not of limitation, and there is no intention in the use of such terms and expressions of excluding equivalents of the features shown and described or portions thereof, it being recognized that the scope of the invention is defined and limited only by the claims which follow. 39

Claims

1. A lightning detection system, comprising: a source of an electrical detection signal representative of the derivative of an electromagnetic field from a lightning discharge; an analog-to-digital converter, responsive to said electrical detection signal, for producing a digital detection signal representative of the derivative of said electromagnetic field; and a digital processor, responsive to said digital detection signal, for determining the type of lightning discharge that produced said electromagnetic field based on characteristics of said digital detection signal, said digital processor continually processing said digital detection signal so as to eliminate dead time between lightning events.

2. The lightning detection system of claim 1, further comprising a signal conditioning element responsive to said electrical detection signal for removing noise therefrom while maintaining the derivative state of components of said electrical detection signal deemed most significant and thereby producing a conditioned detection signal.

3. The lightning detection system of claim 2, wherein said signal conditioning element comprises a leaky analog integrator which substantially blocks signal components whose frequencies are above a cutoff threshold while substantially passing 40 WO 03/069375 PCT/USO3/04351 components of said electrical detection signal deemed most significant without integration thereof.

4. The lightning detection signal of claim 2, further comprising a non-linear amplifier, responsive to said conditioned detection signal, for producing an amplitude compressed conditioned detection signal having a reduced dynamic amplitude range prior to application to said analog-to-digital converter.

5. The lightning detection system of claim 4, wherein said non-linear amplifier is a logarithmic amplifier.

6. The lightning detection system of claim 4, wherein said non-linear amplifier is a piece-wise linear amplifier.

7. The lightning detection system of claim 1, further comprising a non-linear amplifier, responsive to said electrical detection signal, for reducing the dynamic amplitude range of said electrical detection signal prior to its application to said analog to-digital converter.

8. The lightning detection system of claim 7, wherein said non-linear amplifier is a logarithmic amplifier. 41 WO 03/069375 PCT/USO3/04351

9. The lightning detection system of claim 7, wherein said non-linear amplifier is a piece-wise linear amplifier.

10. The lightning detection system of claim 1, wherein said digital processor includes an integration element for digitally integrating said digital detection signal and thereby producing an integrated digital detection signal, said processor using both said digital detection signal representative of the derivative of said electromagnetic field and said integrated digital detection signal to determine the type of lightning discharge that produced said electromagnetic field.

11. The lightning detection system of claim 10, further comprising an amplifier, responsive to said electrical detection signal, for reducing the dynamic amplitude range of said electrical detection signal prior to its application to said analog-to-digital converter.

12. The lightning detection system of claim 11, wherein said amplifier is a logarithmic amplifier.

13. The lightning detection system of claim 11, wherein said amplifier is a piece-wise linear amplifier.

14. The lightning detection system of claim 10, further comprising a signal conditioning element responsive to said electrical detection signal for removing noise 42 WO 03/069375 PCT/USO3/04351 therefrom while maintaining the derivative state of the components of said detection signal deemed most significant prior to application to said analog-to-digital converter.

15. The lightning detection system of claim 14, wherein said signal conditioning element comprises a leaky analog integrator which substantially blocks signal components whose frequencies are above a cutoff threshold while substantially passing said components of said detection signal deemed most significant without integration thereof.

16. The lightning detection system of claim 10, wherein said digital processor employs said digital detection signal representative of the derivative of said electromagnetic field to identify maxima and minima of the waveform of said integrated digital detection signal, and identifies zero crossings of said integrated digital detection signal from said integrated digital detection signal itself.

17. The lightning detection system of claim 16, wherein said digital processor distinguishes between cloud-to-ground and intra-cloud lighting discharges.

18. The lightning detection system of claim 1, wherein said digital processor produces digital data characterizing lightning discharges, and said system further comprises a data transmission component for transmitting said characterizing data over a communications channel. 43 WO 03/069375 PCT/USO3/04351

19. The lightning detection system of claim 18, comprising a plurality of sources, associated analog-to-digital converters and associated digital processors, and a central analyzer for receiving said characterizing data, said central analyzer including a discharge correlation component for correlating pulses from said plurality of sources to determine the time and location of a discharge.

20. The lightning detection system of claim 19, wherein said transmission component includes a data compression component for reducing the amount of data needed to characterize a lightning discharge so as to decrease the time or bandwidth required to transmit a complete data set representative of a series of lightning discharges.

21. The lightning detection system of claim 20, wherein said data compression component minimally transmits, for each series of discharges, sufficient characterizing data to identify the amplitude of the largest pulse produced thereby and the time when said largest pulse occurred.

22. The lightning detection system of claim 20, wherein said data compression component includes a data decimation component for synchronously decimating said characterizing data when needed to accommodate the bandwidth of said communications channel.

23. A lightning detection system, comprising: 44 WO 03/069375 PCT/USO3/04351 a source of an electrical detection signal representative of an electromagnetic field from a lightning discharge; a non-linear amplifier, responsive to said electrical detection signal, for producing an amplitude compressed detection signal having a reduced amplitude dynamic range; and a signal processor responsive to said amplitude compressed detection signal for determining the type of lightning discharge that produced said electromagnetic field based on characteristics of said amplitude compressed detection signal.

24. The lightning detection system of claim 23, wherein said non-linear amplifier is a logarithmic amplifier.

25. The lightning detection system of claim 23, wherein said non-linear amplifier is a piece-wise linear amplifier.

26. The lightning detection system of claim 23, further comprising an analog-to digital converter, responsive to said amplitude compressed detection signal, for producing an amplitude compressed digital detection signal for application to said signal processor, and said signal processor comprises a digital processor.

27. The lightning detection system of claim 26, wherein said digital processor employs said amplitude compressed digital detection signal representative of said electromagnetic field to identify maxima and minima of the waveform of said amplitude 45 WO 03/069375 PCT/USO3/04351 compressed digital detection signal, and identifies zero crossings of said amplitude compressed digital detection signal.

28. The lightning detection system of claim 27, wherein said digital processor distinguishes between cloud-to-ground and intra-cloud lightning discharges.

29. The lightning detection system of claim 23, wherein said signal processor produces digital data characterizing lightning discharges that are identified, and said system further comprises a data transmission component for transmitting said characterizing data over a communications channel.

30. The lightning detection system of claim 29, wherein said transmission component includes a data compression component for reducing the amount of data needed to characterize a lightning discharge so as to decrease the time or bandwidth required to transmit a complete data set representative of a series of lightning discharges.

31. The lightning detection system of claim 30, wherein said data compression component minimally transmits, for each series of discharges, sufficient data to identify the amplitude of the largest pulse produced thereby and the time when said largest pulse occurred.

32. The lightning detection system of claim 29, wherein said data compression component further comprises a data decimation component for synchronously decimating 46 WO 03/069375 PCT/USO3/04351 said characterizing data when needed to accommodate the bandwidth of said communications channel.

33. The lightning detection system of claim 29, further comprising a central analyzer component for receiving and processing said characterizing data.

34. The lightning detection system of claim 33, comprising a plurality of sources, associated non-linear amplifiers, and associated digital processors, and wherein said central analyzer component includes a discharge correlation component for correlating pulses from said plurality of sources to determine the time and location of a discharge.

35. The lightning detection system of claim 23, wherein said source comprises an antenna.

36. A method for detecting lightning, comprising: producing in response to an electromagnetic field from a lightning discharge an electrical detection signal representative of the derivative of said electromagnetic field; producing, in response to said electrical detection signal, a digital detection signal representative of the derivative of said electromagnetic field; and determining the type of lightning discharge that produced said electromagnetic field based on characteristics of said digital detection signal while continually processing said digital detection signal so as to eliminate dead time between lightning events. 47 WO 03/069375 PCT/USO3/04351

37. The lightning detection method of claim 36, further comprising conditioning said electrical detection signal to remove noise therefrom while maintaining the derivative state of components of said electrical detection signal deemed most significant and thereby producing a conditioned detection signal.

38. The lightning detection method of claim 37, wherein said conditioning step comprises substantially blocking signal components whose frequencies are above a cutoff threshold while substantially passing a portion of said electrical detection signal deemed most significant without integration thereof.

39. The lightning detection method of Claim 37, further comprising producing from said electrical detection signal an amplitude compressed conditioned detection signal having a reduced amplitude dynamic range prior to producing said digital detection signal.

40. The lightning detection method of claim 39, wherein said amplitude compressed conditioned signal is produced by logarithmic amplification.

41. The lightning detection method of claim 39, wherein said amplitude compressed conditioned signal is produced by piece-wise linear amplification. 48 WO 03/069375 PCT/USO3/04351

42. The lightning detection method of claim 36, further comprising reducing the dynamic amplitude range of said electrical detection signal by non-linear amplification prior to producing said digital detection signal.

43. The lightning detection method of claim 42, wherein said reducing the dynamic amplitude range is accomplished by logarithmic amplification.

44. The lightning detection method of claim 42, wherein said non-linear amplification is accomplished by piece-wise linear amplification.

45. The lightning detection method of claim 36, further comprising digitally integrating said digital detection signal and thereby producing an integrated digital detection signal, and using both said digital detection signal representative of the derivative of said electromagnetic field and said integrated digital detection signal to determine the type of lightning discharge that produced said electromagnetic field.

46. The lightning detection method of claim 45, further comprising amplifying said electrical detection signal so as to reduce the dynamic amplitude range of said electrical detection signal prior to producing said digital detection signal.

47. The lightning detection method of claim 46, wherein said amplifying is accomplished by logarithmic amplification. 49 WO 03/069375 PCT/USO3/04351

48. The lightning detection method of claim 46, wherein said amplifying is accomplished by piece-wise linear amplification.

49. The lightning detection method of claim 45, further comprising removing noise from said electrical detection signal while maintaining the derivative state of components of said electrical detection signal deemed most significant prior to producing said digital detection signal.

50. The lightning detection method of claim 49, further comprising substantially blocking signal components whose frequencies are above a cutoff threshold while substantially passing components of said detection signal deemed most significant without integration thereof.

51. The lightning detection method of claim 45, further comprising using said digital detection signal representative of the derivative of said electromagnetic field to identify maxima and minima of the waveform of said integrated digital detection signal, and identifying zero crossings of said integrated digital detection signal from said integrated digital detection signal.

52. The lightning detection method of claim 51, further comprising distinguishing between cloud-to-ground and intra-cloud lightning discharges. 50 WO 03/069375 PCT/USO3/04351

53. The lightning detection method of claim 36, wherein said determining the type of lightning discharge includes producing digital data characterizing lightning discharges that are identified, and said method further comprises transmitting said characterizing data over a communications channel.

54. The lightning detection method of claim 53, comprising producing a plurality of electrical detection signals from different locations and correlating pulses from said plurality of detection signals to determine the time and location of a lightning discharge.

55. The lightning detection method of claim 53, wherein said transmitting includes reducing the amount of data needed to characterize a lightning discharge so as to decrease the time or bandwidth required to transmit a complete data set representative of a series of lightning discharges.

56. The lightning detection method of claim 55, further comprising minimally transmitting, for each series of discharges, sufficient data to identify the amplitude of the largest pulse in said characterizing data and the time when said largest pulse occurred.

57. The lightning detection method of claim 56, further comprising synchronously decimating said characterizing data where needed to accommodate the bandwidth of said communications channel.

58. A lightning detection method, comprising: 51 WO 03/069375 PCT/USO3/04351 producing in response to an electromagnetic field from a lightning discharge an electrical detection signal representative of the derivative of said field; amplifying said electrical detection signal so as to produce an amplitude compressed detection signal having a reduced dynamic range; and determining the type of lightning discharge that produced said electromagnetic field based on characteristics of said amplitude compressed detection signal.

59. The lightning detection method of claim 58, wherein said amplifying is accomplished by logarithmic amplification.

60. The lightning detection method of claim 58, wherein said amplifying is accomplished by piece-wise linear amplification.

61. The lightning detection method of claim 58, further comprising converting said amplitude compressed detection signal to digital form before determining the typeo f lightning discharge that produced said electromagnetic field.

62. The lightning detection method of claim 61, further comprising identifying maxima and minima and zero crossings of said digital amplitude compressed detection signal. 52 WO 03/069375 PCT/USO3/04351

63. The lightning detection method of claim 62, further comprising distinguishing between cloud-to-ground and intra-cloud lightning discharges based on said maxima and minima and zero crossings.

64. The lightning detection method of claim 58, further comprising producing from said amplitude compressed detection signal digital data characterizing lightning discharges that are identified and transmitting said characterizing data over a communications channel.

65. The lightning detection method of claim 64, further comprising reducing the amount of data needed to characterize a series of lightning discharges so as to decrease the time or bandwidth required to transmit said characterizing data.

66. The lightning detection method of claim 65, further comprising minimally transmitting, for each series of discharges sufficient data to identify the amplitude of the largest pulse in said characterizing data and the time when said largest pulse occurred.

67. The lightning detection method of claim 66, further comprising synchronously decimating said characterizing data when needed to accommodate the bandwidth of said communications channel. 53 WO 03/069375 PCT/USO3/04351

68. The lightning detection system of claim 64, further comprising producing a plurality of electrical detection signals and correlating pulses from said plurality of detection signals to determine the time and location of a discharge.

69. A lightning detection system, comprising: a source of an electrical detection signal representative of an electromagnetic field produced by a lightning discharge; an analog-to-digital converter, responsive to said electrical detection signal, for producing a digital detection signal; a digital processor for determining the type of lightning discharge that produced said electromagnetic field based on characteristics of said digital detection signal, said digital processor producing digital data characterizing lightning discharges that are identified; a data compression component for reducing the amount of data needed to characterize a lightning discharge so as to decrease the time or bandwidth required to transmit data representative of a series of lightning discharges; and a data transmission component for transmitting said characterizing data over a communications channel.

70. The lightning detection system of claim 69, wherein both said digital processor and said data compression component comprise a programmed digital processor. 54 WO 03/069375 PCT/USO3/04351

71. The lightning detection system of claim 69, wherein said data compression component produces, as data representative of said series of lightning discharges, data representative of the amplitude and data representative of the time of occurrence of the largest amplitude discharge in said series of lightning discharges.

72. The lightning detection system of claim 71, wherein said data compression component further produces, for one or more additional lightning discharges in said series of discharges, data representative of the time of occurrence of each said additional discharge with respect to the time of an adjacent discharge.

73. The lightning detection system of clam 72, wherein said data compression component further produces, for said one or more additional discharges in said series of discharges, data representative of the relative amplitude of each said additional discharge with respect to the amplitude of said largest amplitude discharge.

74. The lightning detection system of claim 73, wherein said data compression component further comprises a data decimation component for synchronously decimating said characterizing data when needed to accommodate the bandwidth of said communications channel.

75. The lightning detection system of claim 74, wherein said data decimation component comprises a component for determining whether the rate of electrical detection signals produced by said source in response to said series of lightning 55 WO 03/069375 PCT/USO3/04351 discharges exceeds the data transmission capacity of said communications channel and, in that event, selecting for transmission only data representing those electrical detection signals that occur during a periodically occurring time frame of predetermined length.

76. The lightning detection system of claim 69, further comprising a data decimation component for synchronously decimating said characterizing data when needed to accommodate the bandwidth of said communications channel.

77. The lightning detection system of claim 71, wherein said data decimation component comprises a component for determining whether the rate of electrical detection signals produced by said source in response to said series of lightning discharges exceeds the data transmission capacity of said communications channel and, in that event, selecting for transmission only data representing those electrical detection signals that occur during a periodically occurring time frame of predetermined length.

78. The lightning detection system of claim 69, further comprising a plurality of sources and respective analog-to-digital converters, digital processors, data compression components and data transmission components, and a central processor associated therewith for receiving said characterizing data, said central processor including a discharge correlation component for correlating sets of data representing series of discharges from respective said sources to determine the time and location of one or more discharges. 56 WO 03/069375 PCT/USO3/04351

79. The lightning detection system of claim 78, wherein said sets of data are correlated in time.

80. The lightning detection system of claim 79, wherein two distinct pairs of three said sets of data are operated on by a correlation operator, the time shift corresponding to the peak correlation value is taken to be the difference in propagation time from a given discharge to the respective sensors which serve as respective sources whose data is correlated, and the two time differences thus found are used to estimate the location of a discharge.

81. The lightning detection system of claim 79, wherein three said sets of data from respective sources are first compared to identify the data corresponding to the highest amplitude discharge represented in each set, the time differences between two distinct pairs of said data representing the highest amplitude discharge is taken to be the difference in propagation time from the highest amplitude discharge to the respective sensors, which serve as respective sources whose data is correlated, and the two time differences thus found are used to estimate the location of the said highest amplitude discharge.

82. The lightning detection system of claim 81, wherein said sets of data are shifted in the time domain so that data representing said highest amplitude discharge in each said set of data are coincident, and the corresponding time interval between adjacent discharges are compared for each set of data to estimate the reliability of the correlation. 57 WO 03/069375 PCT/US03/04351

83. The lightning detection system of claim 82, wherein said correlation is accepted as reliable where at least one corresponding said time interval from among all said sources agrees to within a predetermined maximum value.

84. The lightning detection system of claim 83, wherein said central processor further includes an optimization component which, when said data sets comprise redundant information regarding the location or time of occurrence of a discharge, applies an optimization algorithm to determine the optimum time and location pair.

85. The lightning detection system of claim 84, wherein said optimization algorithm employs a least-squares estimation of the optimum time and location pair based on propagation time data from at least four sensors which serve as respective sources.

86. The lightning detection system of claim 78, wherein when.said characterizing data includes information about the angle relative to two sensors which serve as respective sources with respect to a discharge, the location of said discharge is initially determined from said angles.

87. The lightning detection system of claim 86, wherein the arrival times of said discharge whose location is determined by said angles at a plurality of sensors which serve as respective sources are estimated from said location, said sets of data from said plurality of sensors are shifted in the time domain by relative differences in said arrival 58 WO 03/069375 PCT/USO3/04351 times, and the corresponding time intervals between adjacent discharges are compared for each set of data to estimate the reliability of said correlation.

88. The lightning detection system of claim 87, wherein said correlation is accepted as reliable where at least one corresponding said time interval for all said sensors agrees to within a predetermined maximum value.

89. A lightning detection system, comprising: an antenna for producing, in response to an electromagnetic field produced by a lightning discharge, an electrical detection signal representative of said field; an analog-to-digital converter, responsive to said electrical detection signal, for producing a digital detection signal; a digital processor for determining the type of lightning discharge that produced said electromagnetic field based on characteristics of said digital detection signal, said digital processor producing digital data characterizing lightning discharges that are identified; a data decimation component for synchronously decimating said characterizing data to reduce the data for transmission; and a data transmission component for transmitting said decimated characterizing data over a communications channel.

90. The lightning detection system of claim 89, wherein both said digital processor and said data decimation component comprise a programmed digital processor. 59 WO 03/069375 PCT/USO3/04351

91. The lightning detection system of claim 90, wherein said data decimation component comprises a component for determining whether the rate of electrical detection signals produced by said antenna in response to a series of lightning discharges exceeds the data transmission capacity of said communications channel and, in that event, selecting for transmission only data representing those discharges' electrical detection signals that occur during a periodically occurring time frame of predetermined length.

92. A lightning detection system, comprising: a plurality of sources of data representative of a series of lightning discharges; and a central analyzer for receiving and analyzing said data representative of a series of lightning discharges, said central analyzer including a discharge correlation component for correlating sets of data representing series of discharges from respective said sources to determine the time or location of one or more discharges.

93. The lightning detection system of claim 92, wherein said sets of data are correlated in time.

94. The lightning detection system of claim 93, wherein two distinct pairs of three said sets of data are operated on by a time correlation operator, the time shift corresponding to the peak correlation value is taken to be the difference in propagation time from a given discharge to the respective sensors which serve as respective sources whose data is correlated, and the two propagation time differences thus found are used to estimate the location of a discharge. 60 WO 03/069375 PCT/USO3/04351

95. The lightning detection system of claim 93, wherein three said sets of data from respective sources are first examined to identify the data corresponding to the highest amplitude discharge represented within each set, the time differences between two distinct pairs of said data representing the highest amplitude discharge is taken to be the difference in propagation time from the highest amplitude discharge to the respective sensors which serve as respective sources whose data is correlated, and the two propagation time differences thus found are used to estimate the location of the said highest amplitude discharge.

96. The lightning detection system of claim 95, wherein said sets of data are shifted in time so that data representing said highest amplitude discharge in each said set of data are coincident, and the corresponding time intervals between adjacent discharges are compared for each set of data to estimate the reliability of the correlation.

97. The lightning detection system of claim 96 wherein said correlation is accepted as reliable where at least one corresponding said time interval for all said sensors agrees to within a predetermined maximum value.

98. The lightning detection system of claim 92, wherein when said representative data includes information about the angles relative to two sensors which serve as respective sources with respect to a discharge, the location of said discharge is initially determined from said angles. 61 WO 03/069375 PCT/USO3/04351

99. The lightning detection system of claim 98, wherein the arrival times of an electromagnetic field produced by said discharge whose location is determined by said angles at a plurality of sensors which serve as respective sources are estimated from said location, said sets of data from said plurality of sensors are shifted in the time domain by relative differences in said arrival times, and the corresponding time intervals between adjacent discharges are compared for each set of data to estimate a reliability of said correlation.

100. The lightning detection system of claim 99, wherein said correlation is accepted as reliable where at least one corresponding said time interval for all said sensors agree to within a predetermined maximum value.

101. A method for detecting lightning, comprising: producing in response to an electromagnetic field produced by a lightning discharge an electrical detection signal representative of said electromagnetic field; producing a digital detection signal representative of said electrical detection signal; determining the type of lightning discharge that produced said electromagnetic field based on characteristics of said digital detection signal and producing digital data characterizing lightning discharges that are so determined; reducing the amount of data needed to characterize a lightning discharge so as to decrease the time or bandwidth required to transmit data representative of a series of lightning discharges; and 62 WO 03/069375 PCT/USO3/04351 transmitting said characterizing data over a communications channel.

102. The method of claim 101, wherein said reducing step produces data representative of the amplitude and data representative of the time of occurrence of the largest amplitude discharge in said series of lightning discharges.

103. The method of claim 102, wherein said reducing step further produces, for one or more additional lightning discharges in said series of discharges, data representative of the time of occurrence of each said additional discharge with respect to the time of occurrence of an adjacent discharge.

104. The method of claim 103, wherein said reducing step further produces, for said one or more additional discharges in said series of discharges, data representative of the relative amplitude of each said additional discharge with respect to the amplitude of said largest amplitude discharge.

105. The method of claim 104, wherein said reducing step further comprises synchronously decimating said characterizing data as needed to accommodate the bandwidth of said communications channel.

106. The method of claim 105, wherein said decimating step comprises determining whether the rate of electrical detection signals produced in response to said series of lightning discharges exceeds the data transmission capacity of said communications 63 WO 03/069375 PCT/USO3/04351 channel and, in that event, selecting for transmission only data representing those electrical detection signals that occur during a periodically occurring time frame of predetermined length.

107. The method of claim 101, further comprising synchronously decimating said characterizing data as needed to accommodate the bandwidth of said communications channel.

108. The method of claim 107, wherein said decimating step further comprises determining whether the rate of electrical detection signal produced in response to said series of lightning discharges exceeds the data transmission capacity of said communications channel and, in that event, selecting for transmission only data representing those discharges that occur during a periodically occurring time frame of predetermined length.

109. The method of claim 101, further comprising providing a plurality of electrical detection signals representative of an electromagnetic field from a lightning discharge and, for each said electrical detection signal, producing a digital detection signal, determining the type of lightning discharge that produced said electromagnetic field based on characteristics of said digital detection signal, producing digital data characterizing lightning discharges that are so determined, reducing the amount of data needed to characterize a lightning discharge so as to decrease the time or bandwidth required to transmit data representative of a series of lightning discharges, transmitting 64 WO 03/069375 PCT/USO3/04351 said characterizing data over a communications channel to a central location, and at said central location receiving said characterizing data and correlating sets of data to determine the time and location of one or more discharges, each said set of data corresponding to a unique source and an associated sensor location.

110. The method of claim 109, wherein said sets of data are correlated in time.

111. The method of claim 110, wherein two distinct pairs of three said sets of data are operated on by a correlation operator, the time shift corresponding to the peak correlation value is taken to be the difference in propagation time from a given discharge to the respective sensors which serve as respective sources whose data is correlated, and the two propagation time differences thus found are used to estimate the location of a discharge.

112. The method of claim 111, wherein three said sets of data are first compared to identify the data corresponding to the highest amplitude discharge represented in each set, the time differences between two distinct pairs of said data representing the highest amplitude discharge is taken to be the difference in propagation time from the highest amplitude discharge to the respective sensors which serve as respective sources whose data is correlated, and the two propagation time differences thus found are used to estimate the location of the said highest amplitude discharge.

113. The method of claim 112, wherein said sets of data are shifted in the time domain so that data representing said highest amplitude discharge in each said set of data are 65 WO 03/069375 PCT/USO3/04351 coincident, and the corresponding time intervals between adjacent discharges are compared for each set of data to estimate the reliability of the correlation.

114. The method of claim 113, wherein the correlation is accepted as reliable where at least one corresponding said time interval from among all said sensors agrees to within a predetermined maximum value.

115. The method of claim 109, wherein when said characterizing data includes information about the angle relative to two sensors which serve as respective sources with respect to a discharge, the location of said discharge is initially determined from said angles.

116. The method of claim 115, wherein the arrival times of said electromagnetic field produced by said discharge whose location is determined by said angles at a plurality of sensors which serve as respective sources are estimated from said location, said sets of data from said plurality of sensors which serve as respective sources are shifted in the time domain by relative differences in said arrival times, and the corresponding time intervals between adjacent discharges are compared for each set of data to estimate the reliability of the correlation value.

117. The method claim 116, wherein the correlation is accepted as reliable where at least one corresponding said time interval for all said sensors agree to within a predetermined maximum value. 66 WO 03/069375 PCT/USO3/04351

118. A method for detecting lightning, comprising: producing in response to an electromagnetic field produced by a lightning discharge, an electrical detection signal representative of said field; producing a digital detection signal responsive to said electrical detection signal; determining the type of lightning discharge that produced said electromagnetic field based on characteristics of said digital detection signal and producing digital data characterizing lightning discharges that are identified; synchronously decimating said characterizing data to reduce the data for transmission; and transmitting said decimated characterizing data over a communications channel.

119. The method of claim 118, wherein said data decimating step comprises determining whether the rate electrical detection signals produced in response to a series of lightning discharges exceeds the data transmission capacity of said communications channel and, in that event, selecting for transmission only data representing those electrical detection signals that occur during a periodically occurring time frame of predetermined length.

120. A method for detecting lightning, comprising: providing a plurality of sources of data representative of a series of lightning discharges; receiving said data representative of a series of lightning discharges at a central location; 67 WO 03/069375 PCT/USO3/04351 and correlating sets of data representing a series of discharges from respective said sources to determine the time or location of one or more discharges.

121. The method of claim 120, wherein said sets of data are correlated in time.

122. The method of claim 121, wherein two distinct pairs of three said sets of data are operated on by a correlation operator, the time shift corresponding to the peak correlation value is taken to be the difference in propagation time from a given discharge to respective sensors which serve as respective sources whose data is correlated, and the two propagation time differences thus found are used to estimate the location of a discharge.

123. The method of claim 121, wherein three said sets of data are first examined to identify the data corresponding to the highest amplitude discharge represented in each set, the corresponding time differences between two distinct pairs of said data representing the highest amplitude discharge are taken to be the difference in propagation time from the highest amplitude discharge to respective sensors which serve as respective sources whose data is correlated, and the two propagation time differences thus found are used to estimate said location of the said highest amplitude discharge.

124. The lightning detection system of claim 123, wherein said sets of data are shifted in time so that data representing said highest amplitude discharge in each said set of data 68 WO 03/069375 PCT/USO3/04351 are coincident, and the corresponding time intervals between adjacent discharges are compared for each set of data to estimate the reliability of the correlation.

125. The lightning detection system of claim 124, wherein the correlation is accepted as reliable where at least one corresponding said time interval for all said sources of data agrees to within a predetermined maximum value.

126. The method of claim 120, wherein when said data include information about the angles relative to the location of two said data sources with respect to a discharge, the location of said discharge is initially determined from said angles.

127. The method of claim 126, wherein the arrival times of said electromagnetic field produced by discharge whose location is determined by said angles at said two said data sources are estimated from said location, said sets of data from said plurality of data sources are shifted in the time domain by relative differences in said arrival times, and the corresponding time intervals between adjacent discharges are compared for each set of data to estimate a reliability of said correlation.

128. The method of claim 127, wherein the correlation is accepted as reliable where at least one corresponding said time interval for all said data sources agrees to within a predetermined maximum value. 69