5. Field Observing Systems

5.1 Radar Systems  [Table of Contents]

5.1.1 NCAR S-Pol Research Radar

The NCAR S-Pol research radar is a polarimetric Doppler radar developed at NCAR/ATD. The radar system is designed to be transported to the research field campaign location. The entire system is packaged into standard sized sea containers that are used as the antenna support structure at the research site. The structure and pedestal are designed to work properly in winds up to 30 m/s. If needed, a CP-2 inflatable radome can be used to enclose the radar.

The S-Pol radar uses a high performance modern transmitter, low sidelobe parabolic antenna, modern dual channel receiver, and a NCAR designed VME data system. The transmitter, built by Westinghouse, is an ASR-9 based unit using an air-cooled klystron and produces a one-Megawatt, one-microsecond pulse. Polarization switching is accomplished using a NCAR built mechanical switch that provides 49 dB transmit isolation, which is comparable to a dual transmitter configuration. Dual receivers, each providing 40 dB isolation is required for cross-polar measurements. The 8.5 m reflector is a high compliance aluminum structure providing –30 dB first sidelobes and at least –35 dB integrated cross-polar isolation. Pulse pair and dual polarization processing is performed by a NCAR designed VME-based Integrated Radar Acquisition system (VIRAQ). The VIRAQ processor uses a dual range 90 dB digital IF system with multiple C44 DSP chips that are controlled by a 486 CPU host running DOS. Refer to Table 5.1 for a detailed list of component specifications.

Between 100-128 samples are need to obtain accurate, reliable polarimetric measurements. Thus, it is recommended to use a PRF of 960 Hz at a scan rate of 6 deg/sec.  This scan rate is needed to utilize the ground clutter filter.  

Table 5.1. Technical specifications for the NCAR S-Pol radar.

Transmitter  
Wavelength 11.00 cm
Pulse width 0.3 - 1.4 µsec-tapered
PRF 0 - 1300 Hz
Peak power >1 MW
Staggered pulse Yes
Random phase jitter for 2nd trip suppression Yes
Interference Meets radio frequency management Subsection 5.2.3, Criteria C
Receivers (2)  
Noise power -115.5 dBm
Radar Noise figure 2.9 dB
Dynamic range 90 dB
Bandwidth 0.738 MHz
Digital IF Linear floating point processing
I-Q image rejection 50 dB
Minimum detectable dBZ at 50km/1km -15 dBZ/-52 dBZ at -6 dB SNR
Polarization switching  
Polarization H-V alternating or H only
Mechanical switch isolation 47 dB measured
Ferrite switch isolation 28 dB
Antenna  
Gain 44.5 dB including wave guide loss
Diameter 8.5 m
Beamwidth 0.91 degrees
First sidelobe better than -30 dB
Isolation (ICPR) better than -35 dB
Scan rate Up to 18°/s each axis, 30°/s with pulley change
Wind limit for operation 30 m/s (60 m/s w/ radome)
Data system  
Number of range gates 4000
Gate spacing 37.5 – 1000 m
Number of samples 16 – 1000
Clutter filter Single polarization only, 50 dB
Times series (I/Q) capability Yes
Real time scientific display NCAR Zebra
Recorded variables PHH, PVV, V, W, R(1)HV, |R(1)VH|, |R(2)|, PhiDP, PhoHV, NCP, ZH, ZDR, LDR, Kdp
Recording medium Exabyte, Dorade format

 
5.1.2 CSU-CHILL Research Radar
   [Table of Contents]

The CSU-CHILL research radar is a portable polarimetric, Doppler radar system stationed at Colorado State University. The system is packaged into shipping crates and assembled similarly to the S-Pol radar. The antenna for the system is housed inside a CP-2 inflatable radome.

The CSU-CHILL radar utilizes modern dual transmitters, high performance parabolic antenna, dual receivers, and programmable signal processor. The transmitting system consists of two klystron-based transmitters, each producing ~1.0 megawatt, one microsecond pulse. The antenna is an 8.5 meter, parabolic antenna with a half-power beamwidth of one degree. The main beam and sidelobe patterns at horizontal and vertical polarizations are well matched. The matched dual receivers have noise power levels of approximately -115 dBm. Information processing is handled by a programmable Lassen SP20 signal processor and recorded to 8 mm Exabyte cassette tapes. See Table 5.2 for a detailed list of specifications.

Between 100-128 samples are need to obtain accurate, reliable polarimetric measurements. Thus, it is recommended to use a PRF of 960 Hz at a scan rate of 6 deg/sec.  This scan rate is needed to utilize the ground clutter filter and match well with the S-Pol radar measurements.

Table 5.2. Technical specifications for the CSU CHILL radar.

Antenna  
Shape Parabolic
Diameter 8.5 m
Feed type Scalar
Gain 43 dB (includes waveguide loss)
3 dB Beamwidth 1.1 deg
Maximum sidelobe -27 dB (In worst f plane)
Inter-channel isolation -45 dB (limited by orothomode transducer)
ICPR (two-way) -34 dB
Transmitters  
Wavelength 11.01 cm
Peak Power 800 - 1000 kW
Final PA Type VA-87B/C (Klystron)
PRT Range 800 - 2500 ms
Pulse width 0.3 - 1.0 ms
Available Polarizations Horizontal, Vertical, slant 45o/135o , right/left circular
Receivers/DSP  
Noise Figure ~3.4 dB
Noise Power @SNR=1 ~ -114.0 dBm
Dynamic range ~96 dB
Bandwidth 750 KHz with programmable filter
Output Range Resolution 45 m minimum, adjustable upward in 15 m intervals
Maximum range gates estimated to be > 3000

5.1.3 NWS WSR-88D Operational Weather Radar  [Table of Contents]

The WSR-88D (KHGX) radar stationed in League City, TX will provide continuous surveillance scans of the research area. These surveillance scans will consist of scans at a sequence of constant elevation angles of radar reflectivity and radial velocities. Because the radar is an operational radar, the scanning strategies for this radar are not controllable by the research team and limited to three Volume Coverage Patterns (VCPs). See Fig. 5.1 for a graphical representation of scanning levels for the three main VCPs. A data recorder will be installed at this facility during the field campaign.

VCP-11 is a precipitation mode that uses a short radar pulse giving a nominal 250 m range resolution. This mode has two surveillance scans for reflectivity and Doppler velocities. The slow rate of pulsing gives a 460 km unambiguous range and the fast rate of pulsing for a 150 km unambiguous range and high Nyquist or folding velocity exceeding 25 m/s. The fast pulse rate is used only in the low scan angles. The precipitation mode consists of 360-deg-in-azimuth scans at 14 elevation angles to obtain 5 minute updates of full volume scans. The lowest seven elevation angles are contiguous and the remaining steps between elevation angles exceed the nominal radar beamwidth of 0.95 deg, leaving some gaps in the vertical coverage.

VCP-21 is a very similar precipitation mode to the VCP-11 mode. This mode uses a short radar pulse giving a nominal 250 m range resolution. This mode has two surveillance scans for reflectivity and Doppler velocities. The slow rate of pulsing gives a 460 km unambiguous range and the fast rate of pulsing for a 150 km unambiguous range and high Nyquist or folding velocity exceeding 25 m/s. The fast pulse rate is used only in the low scan angles. The precipitation mode consists of 360-deg-in-azimuth scans at 9 elevation angles to obtain 6 minute updates of full volume scans. The lowest five elevation angles are contiguous and the remaining steps between elevation angles exceed the nominal radar beamwidth of 0.95 deg, leaving some gaps in the vertical coverage.

VCP-31 is a clear air mode and is used to detect early formation of convective precipitation, air mass discontinuities, and to obtain wind profiles. It uses a long pulse transmission at 5 elevation angles to obtain a 10 minute update rate. The long pulse is used to provide a greater sensitivity. There are separate surveillance and Doppler scans at the lowest three elevation angles.  

Fig. 5.1. Graphs depicting elevation versus distance from radar for different scan angles of the three different VCPs.

5.1.4 Radar Scanning Strategies  [Table of Contents]

The main priority is for the two research radars to conduct dual polarimetric, dual Doppler radar sampling. Both radars will be performing similar scans and integration times to obtain high quality polarimetric and Doppler measurements. The scanning strategy used by the radars needs to have both broad scale and fine scale measurements of the storm dynamics and microphysics. To achieve this goal a PPI-RHI scanning strategy, which toggles between PPI and RHI mode, will be used. This strategy consists of a ~5 minute storm volume scan across azimuthal sectors at a sequence of constant elevation angles (PPI). Following this, a ~2 min storm volume scan in the elevation angle direction at a sequence of constant azimuth angles (RHI) will be conducted. This will give a repeat cycle of ~7 min for a complete PPI-RHI scan sequence. This scan sequence will be repeated continuously except during aircraft penetrations.

The RHI scan will be focused on the storm section that is of primary interest. In this case, the primary interests would be updrafts and electrically active regions. This can be determined from radar, aircraft, electrical measurements, and field reports. Specific placement of the PPIs and RHIs will be determined with the help of scan optimizers and some "canned" scans determined before the start of the field study.

The NWS Doppler radar (KHGX) will be used for surveillance scans to keep track of the larger scale development of storms in the region. The data from KHGX will also be incorporated into the data set to allow triple Doppler analysis in certain areas of the study region. Additional near real time data from nearby NWS radars will also be available in the operations center for planning purposes.

5.2 Surface Mesonet Systems  [Table of Contents]

5.2.1 TNRCC Measurement Stations

The Texas Natural Resource Conservation Commission (TNRCC) maintains a set of surface air monitoring stations in southeast Texas. These stations are mainly for atmospheric pollution monitoring. There are approximately 40 stations with a majority of them in the Houston metro region. Figure 5.2 shows the location of most of the sites in southeast Texas. Figure 5.3 is the zoomed map of Houston showing the location of the various TNRCC monitoring stations. Each monitoring station does not measure the same atmospheric variables, but many measure trace gas concentrations or aerosol concentrations. The three variables that each station does measure include temperature, moisture, and horizontal wind. To obtain information on the variables monitored at each station, please refer to the following web address: http://www.tnrcc.state.tx.us/cgi-bin/monops/select_month?region12.gif.

TNRCC performs regular maintenance of all monitoring stations and performs thorough quality checks on all data. The data from the stations will be available from TNRCC as an archived set after the finish of the HEAT field campaign. The operations center can obtain access to rough data through TNRCC’s website if needed.  

Fig. 5.2. Map of southeast Texas showing the location of TNRCC air monitoring stations. Houston area denoted in yellow.  

 

Fig. 5.3. Close up map of Houston depicting the location of air monitoring stations. Houston urban area denoted in yellow.

5.3 Aircraft  [Table of Contents]
 
5.3.1 University of Wyoming King Air
  [Table of Contents]

The University of Wyoming King Air aircraft is a research craft with several meteorological instrument packages for boundary-layer, turbulence/flux, cloud physics, and atmospheric chemistry studies. This craft is not armored like the T-28, thus is not capable of penetrating strong convective regions with hail. This craft is still capable of penetrating storms and taking microphysical measurements of various cloud and precipitation particles. The main measurements that will be taken are: pollution concentrations near sea breeze and over Houston and supercooled liquid water content. Table 5.4 is a listing of the instruments that will be included on the aircraft.

Table 5.4. Wyoming King Air instrument packages with instrument measurement range, accuracy, and resolution.

VARIABLE

INSTRUMENT

RANGE

ACCURACY

RESOLUTION

Air temperature Rosemount 102 -50 - +50°C 0.5°C 0.006°C
Air temperature Reverse flow (Minco element) -50 - +50°C 0.5°C 0.006°C
Dew point temp. Cambridge Model 137C3 -50 - +50°C 1.0°C if > 0°C 0.006°C
2.0°C if < 0°C
Static pressure Rosemount 1501 0 - 1080 mb 0.5 mb 0.003 mb
Static pressure Rosemount 1201FA1B1A 0 - 1034 mb 0.5 mb 0.06 mb
Geometric alt. Stewart Warner APN159 radar altimeter 60,000 ft (18,288 m) 1% 0.24 ft (0.07 m)
Geometric alt. King KRA 405 2000 ft (610 m) 3% if < 500 ft 0.48 ft (0.15 m)
5% if > 500 ft
(152 m)
Total pressure Rosemount 831CPX 0 - 85 mb 0.2 mb 0.005 mb
Lat./long. Trimble 2000 GPS ± 90° lat. 100 m 0.000172°
± 180° long.
Ground velocity Honeywell Laseref SM 0 - 4095 kts 13.5 ft/s 0.0039 kts
Vertical velocity Honeywell Laseref SM ± 32,768 ft/min 0.5 ft/s 0.03125 ft/min
Pitch/roll angle Honeywell Laseref SM ± 90° pitch 0.05° 0.000172°
± 180° roll
True heading Honeywell Laseref SM ± 180° 0.2° 0.000172°
Flow angle Rosemount 858AJ/831CPX ± 15° 0.2° 0.00015°
Cloud droplet spectra Particle Measuring Systems, FSSP scattering probe 0.5 - 45 µm

---

0.5 - 3 µm
Cloud particle spectra Particle Measuring Systems 200X (1D-C) optical array 12.5 - 185.5 µm

---

12.5 µm
Cloud particle spectra Particle Measuring Systems, 2D-C optical array

---

---

25 µm
Precipitation particle spectra Particle Measuring Systems, 2D-C optical array

---

---

200 µm
Liquid water content DMT LWC-100 0 - 3 g/m3 0.2 g/m3 0.00015 g/m3
Liquid water content Gerber PVM-100 0.002 - 10 g/m3 5% 0.000015 g/m3
Droplet surface area Gerber PVM-100 5 - 20,000 cm2/m3 5% 0.03 cm2/m3
Droplet effective radius Gerber PVM-100 2 - 70 mm 10% 0.00015 g/m3
Icing rate Rosemount 871FA 0.5 mm/trip n/a 0.0004 cm
CCN Concentrations UWyo CCNC-100A 0 - 1000 cm-3 ± 30% ± 1 cm-3
CN Concentration TSI 3010 0 - 10,000 cm-3 ± 10% 30 cm-3

5.3.2 WMI LearJet  [Table of Contents]

WMI's (Weather Modification Inc.) Learjet is a high performance aircraft used for weather modification and atmospheric research. The craft's maximum altitude of 45,000 ft and speed of Mach 0.83 allow the craft to operate near thunderstorm tops and respond quickly to targeted storms. Fitted with strengthened engine nacelle inlets to minimize damage due to severe weather, the aircraft is capable of storm penetration. Below is a list of sensors that are currently on (regular font) and need to be added (bold font) to the aircraft. 

  • Passive Cavity Aerosol Spectrometer Probe (PCASP)
  • Forward Scatter Spectrometer Probe (FSSP)
  • 2D-C Cloud Droplet Probe
  • 2D-P Precipitation Probe
  • Liquid Water Content Hot Wire Probe
  • Total Temperature Sensor
  • Dew Point Temperature Sensor
  • Pressure Transducer · Differential Pressure Transducer
  • Instantaneous Vertical Speed Indicator
  • Angle of Attack Sensor · Pitch Rate Gyro
  • CCN Counter
  • Droplet Surface Area - Gerber PVM-100
  • Icing Rate - Rosemount 871FA 

5.3.3 Airborne Chemistry Instrumentation

Chemistry instrumentation will be placed on board the University of Wyoming's King Air Research Aircraft (UWKA) and the Weather Modification, Inc. (WMI) Lear jet. Below is a table of the proposed instrumentation used to measure the particular chemical species. 

Table 5.5. Chemical instrumentation to be placed on board the UWKA and WMI Lear jet.

Species

Technique

Detection Limit

Sampling Rate

Accuracy

NO

Chemiluminescence (CL)

3 ppt

1 s

5% (for 0.2 ppb)

NO2

photolytic converter + CL

15 ppt

5 s

10% (for 0.2 ppb)

NOy

Au-Converter + CL

50 ppt

1 s

15% (for 0.2 ppb)

O3

UV-Absorption

1 ppb

5 s

5%

CO

VUV-Flourescence

2 ppb

3 s

10%

CO2

NDIR

1 ppm

1 s

5%


5.4 Balloon Sounding Unit
s
  [Table of Contents]

5.4.1 MGLASS Units (2)

The NCAR Mobile GLASS (MGLASS) facility is a completely self-contained unit that can be carried by any full-size pickup truck. The basic system contains all the hardware required to make up to four simultaneous atmospheric soundings, including equipment to make supporting surface meteorological observations. The mobility gives the project planner the option to deploy to a specific site, make a sounding, and if required move to another site for the next sounding. The first sounding can be active and in the air while the truck is mobile, although this does affect sounding quality. Sounding site station elevation values are typically taken from a topographic map. If that is not available or if the location is not absolutely certain, a calibrated aircraft pressure altimeter can be used.

The sondes used by the MGLASS units are Vaisala brand rawinsondes. The rawinsonde package includes a 403 MHz band transmitter, GPS receiver, and pressure, temperature, and relative humidity sensors. Table 5.6 lists the specifications for the devices in the rawinsonde package. Both the thermodynamic and navigation signals are transmitted roughly every 1.5 seconds to the MGLASS data system to be processed and archived.

In addition to the standard rawinsonde package, a CCN concentration-measuring package will be added to obtain CCN concentration profiles in storm environments. The instrument was developed at the University of Wyoming Laramie to obtain improved vertical profiles of CCN. The CCN counter is similar to other static thermal-gradient diffusion chamber instruments, except that it utilizes a lightweight photodetector, instead of a charged coupled device (CCD). The instrument uses voltage measurements from the photodetector to relate the amount of scattered light to the CCN concentration approximately every 30 seconds. The actual value of CCN concentration is determined during post processing. From calibration studies, the estimated accuracy is estimated to be +/- 15% for a supersaturation of 1%.

The standard GLASS data system consists of a power supply, an RS-232 Multiplexer (MUX), a rack controller, a 403 MHz receiver, a MWG201 GPS navigation data processor, a NCAR RS-80 meteorological data processor, and a personal computer. Information is transferred to and from the GLASS personal computer through RS-232 connections using the MUX, which switches between the navigator, the Met processor and the Campbell data logger to gather the data required to process and display the atmospheric soundings.

Table 5.6. Instrument specifications for the MGLASS rawinsonde package.  

Rawinsonde Specifications
Manufacturer - type Vaisala RS 80-15 GH
Mass                   525 grams with activated wet battery
Dimensions             6cm X 14cm X 20cm
Ascent Rate 4 m/s avg
Transmitter Frequency 403.5 MHz
Transmitter Power 300 mW
Pressure Measurement
Sensor                  BAROCAP Capacitive aneroid
Range                   3 to 1060 mb
Accuracy                0.5 mb
Data System Resolution 0.1 mb
Sensor Resolution 0.1 mb
Temperature Measurement
Sensor                  THERMOCAP Capacitive bead
Range                   -90°C to 60°C
Accuracy                0.2 C
Data System Resolution 0.1 C
Sensor Resolution 0.1 C
Time Constant 2.5 seconds @ 6m/s flow and 1000 mb
Relative Humidity Measurement
Sensor                  HUMICAP thin film capacitor
Range                   0 - 100% Relative Humidity
Accuracy                2.0% Relative Humidity
Data System Resolution 0.1% Relative Humidity
Time Constant 1.0 second @ 6m/s flow, 1000mb, 20°C
Wind and Position Measurement
Model # MWG201
Wind Accuracy 0.5 m/s
Averaging Time 0.5 seconds
Data System Resolution 0.1 meter; 0.1 m/s

 
5.4.2 Mobile Electrical Sounding Units (2)
[Table of Contents]

Mobile electrical balloon units will be modeled after the MGLASS units. The mobile facilities will consist of a mobile balloon facility housed in a standard conversion van and a minivan for additional crew members. The balloon facility will contain all the necessary equipment to conduct atmospheric soundings and an electric field mill to measure the static electric field. If possible, sequential soundings will be made from a fixed location as the storm moves, in part because data reception is best when the mobile laboratory remains stationary. However, data can be acquired as the vehicle moves, if necessary either for safety or for targeting another part of the storm.

The crew will have nine members, one to remain available for communication with the operations center during launch, one to monitor balloon data reception, five to launch the balloon and instruments, and two to begin inflating the next balloon. Balloons will be launched from a portable launch tube, which has been used for launches in wind with speeds up to 75 mph (65 knots).

Each flight will carry one electric field meter and a rawinsonde. Forty electric field meters will be available for flights to measure the electric field inside storms. The mobile laboratory will house receivers to acquire data from up to four electric field meters simultaneously. Balloon tracking and standard thermodynamic measurements will be similar to the NCAR MGLASS system, which can process data from up to four sondes simultaneously. The data produced from each flight are the electric field, pressure, temperature, dew point, horizontal wind speed and direction, ascent rate, time, latitude, longitude, and altitude at approximately 1-s intervals along the balloon track. In addition, the electric field will be measured at the ground during periods of interest.

5.4.3 TAOS Units  [Table of Contents]

The NCAR Tethered Atmospheric Observing System (TAOS) is a balloon born, lower atmospheric sounding system. This setup allows a balloon to be deployed up to height of 1 km and brought back down to ground when observations are finished. This permits the sensor packages to be used repeatedly, unlike normal rawinsonde setups. The basic instrument package, Vaisala rawinsonde, installed on the tether measures temperature, relative humidity, wind speed, and wind direction (See Table 5.6 for more information). Each sensor reports at a one second sampling rate. The sensor package is powered by a common cell phone battery, which typically last for five hours. With a two balloon / winch system, operations in wind speed up to 45 mph are possible.

5.4.4 Upper-Air Sounding Station  [Table of Contents]

Due to the lack of an Upper Air sounding station near Houston, a temporary station will be established for the field campaign. The tentative location for the balloon launch facility will be the NWS office in League City, TX (~15 miles southeast of downtown Houston). The instrument package will be the Vaisala GPS rawinsonde that is also used in the mobile balloon units. See Table 5.6 for a detailed list of rawinsonde specifications. The facility will conduct soundings at the standard twelve-hour intervals (00Z and 12Z). During intensive operations periods, the Operations Director may request soundings to be conducted at three or six hour intervals. The data will be immediately accessible to both the League City Weather Forecast Office and the HEAT Operations Center. The data will be useful for both real-time forecasting and post analysis.

5.5 Wind Profiler System [Table of Contents]

Doppler Sodar systems, built by Remtech, Inc., will be deployed around the Houston area to obtain lower tropospheric wind profiles. These profilers are capable of reliably measuring horizontal wind speed and direction and vertical motions. In ideal atmospheric conditions, the sodars can obtain measurements up to 1.5 km, but the normal range is approximately 1 km. These measurements are accomplished by emitting a strong acoustic pulse vertically. The system then detects the Doppler frequency shifts in the backscattered echo, due to thermal turbulence in the atmosphere. These frequency shifts and relative return strengths are then processed to obtain a vertical wind profile. A list of the systems specifications can be found in Table 5.7 below.

The system only requires one phased array antenna to operate. A total of three electronically steered beams are used to achieve a three dimensional wind. Two of the beams are tilted 30 degrees from vertical and turned 90 degrees from each other to provide the horizontal component of wind velocity. The third beam is pointed vertically and provides that component of the wind. The system software controls the sequence and rate of operation for each beam.  

 Table 5.7. Technical Specifications of the Remtech Sodar.

SODAR Technical Specifications  
Receiver gain 100 dB
Minimum Altitude sampled 20 meters
Number of range gates 1 to 20 (30 optional)
Thickness of each gate 10 to 200 meters in 1 meter layer increments
Averaging period 2 min to 1 hour
Receiver filter type Sixth order Cauer
Initial processing 1024 frequency point FFT by software
Background noise correction Signal/noise ratio continuously measured and used for validation of data vs. background noise.
Horizontal wind speed range 0 to 30 m/sec
Horizontal speed accuracy Better than 0.2 m/sec or 3% for wind speed over 6 m/sec
Vertical speed range - 4 - + 4 m/sec
Vertical speed accuracy 5 cm/sec or better
Horizontal direction accuracy 3 deg or better for winds faster than 2 m/s.
Acoustic Power 10 W
Average Range in typical conditions 1050 m
Maximum Range 1500 m
Antenna size (meters) 1.3 x 1.3
Antenna weight 100 kg

 
5.6 Lightning Detection
[Table of Contents]

5.6.1 Lightning Detection and Ranging (LDAR II) Network

The LDAR II network will be deployed over a 100-km diameter area both within and around Houston, Texas and will consist of twelve time-of-arrival Lightning Detection and Ranging (LDAR-II) stations. The network, manufactured by Vaisala-Global Atmospherics, Inc., will be capable of mapping the lightning in three spatial dimensions and time. Figure 5.5 displays the approximate locations of the LDAR II stations relative to the area under investigation. The electric field instruments will measure the overall charge structure of storms and the amount and sign of the charge transferred from lightning. For detecting and locating ground strokes and intracloud discharges, the 'fast' electric field change waveform recording stations, CSU three-station flat plate antenna network, will be used.

The LDAR II network operates by detecting RF radiation in the VHF electromagnetic field signature of lightning events in a bandwidth of 5 MHz in the 50 to 150 MHz frequency range. Discharges from initial breakdown processes to subsequent charge transfer are measured with an accuracy of 110 nanoseconds relative to the other sensors in the network using a clock that is synchronized via a Global Positioning System (GPS) receiver. To provide redundancy and provide a larger area of measurements, twelve stations will be used in the LDAR II network.

The LDAR network will be capable of producing large amounts of data in a short period of time due to extremely fast electronics. High-resolution systems provide the position of all possible events in real time and require a maximum data rate of 300 kbps. All time-related information is sent to the Location Processor in real time and the solutions are displayed. Detailed position and density maps of lighting channels will be generated, resulting in up to 10,000 source locations per second. If we choose to require amplitude and diagnostic information then the maximum data rate required will be 600 kbps.

Fig. 5.5. Approximate location of LDAR II stations (green circles) in the HEAT campaign area. Purple box denotes the area of the study considered as the 'urban area'

5.6.2 National Lightning Detection Network  [Table of Contents]

The National Lightning Detection Network (NLDN) managed by Vaisala-Global Atmospherics, Incorporated will be utilized to detect and record cloud-to-ground (CG) lightning activity. The network consists of 106 Time-Of-Arrival (TOA) sensors with approximately half containing Direction Finder (DF) sensors. This nationwide network monitors location, polarity, current, and multiplicity of each flash. The NLDN detection efficiency for SE Texas is typically 80-90% of all CG flashes, with a location error of less than 500 m. Fig. 5.6 is a map of the NLDN sensor type and locations. Real time NLDN information will be available at the Operations Center to assist in identifying and tracking electrical activity within storms. Additionally, an archive of lightning data for the region will be obtained from Global Atmospherics, Inc. for research purposes.

Fig 5.6. Map of NLDN sensor locations and type (IMPACT - Improved Performance from Combined Technology; TOA - Time Of Arrival) for the continental United States.

5.7 Additional Instrument Information [Table of Contents]

Below is a list of web addresses for further information on the various instruments used in the HEAT field campaign.

NCAR S-Pol Research Radar:  http://www.atd.ucar.edu/rsf/spol/spol.html

CSU-CHILL Research Radar:  http://chill.colostate.edu/

TNRCC Measurement Stations:  http://www.tnrcc.state.tx.us/air/monops/index.html

CCN Concentration Instrument:  http://www-das.uwyo.edu/ccp/documents/ccn_instrument.pdf

SDSMT Armored T-28:  http://www.ias.sdsmt.edu/institute/t28/

University of Wyoming King Air:  http://flights.uwyo.edu/  

WMI Lear Jet 35A: http://www.weathermod.com/aircraft_lear.htm

MGLASS Units:  http://www.atd.ucar.edu/sssf/facilities/class/class.html

TAOS Units:  http://www.atd.ucar.edu/sssf/facilities/taos/taos.pdf

Wind Profiler System:  http://www.remtechinc.com/sodidx.htm

Lightning Mapping Array:  http://www.glatmos.com

NLDN:  http://www.glatmos.com/nldn/nldn.html