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Cloud
Radar System(CRS)
The CRS is
a 94 GHz (W-band; 3 mm wavelength) Doppler radar developed for autonomous
operation in the NASA ER-2 high-altitude aircraft and for ground-based
operation. It will provide high-resolution profiles of reflectivity
and Doppler velocity in clouds and it has important applications
to atmospheric remote sensing studies. The CRS was designed to fly
with the Cloud Lidar System (CLS), in the tail cone of an ER-2 superpod.
There are two basic modes of operation of the CRS: 1) ER-2 with
reflectivity, Doppler, and linear-depolarization measurements, and
2) ground-based with full polarimetric capability. The overall radar
system parameters are listed in the attached table.
The CRS consists
of subsystems including the transmitter/receiver, antenna, processor/radar
controller, and disk data storage. The transmitter/receiver subsystem
utilizes an Extended Interaction Amplifier (EIA) Varian transmitter
tube that transmits 1.7 kW peak power. This subsystem has a custom
modulator, power supply, and timing and control designed for ER-2
autonomous operation and with flexibility to transmit a wide variety
of modulation schemes with range pulse widths between 0.25 and 3.0
ms at pulse repetition frequencies (PRF) up to 42 kHz (limited to
£ 1% duty cycle), and with capability to perform multiple
PRFs. For Doppler measurements on the ER-2, the range-Doppler
ambiguity at 94 GHz necessitates using a dual-PRF (5 kHz and 10
kHz) approach to extend the unambiguous range and Nyquist interval.
The two channel receiver downconverts signals to a 60 MHz IF which
is then processed by the digital-IF/processor subsystem. The data
system is similar to that of the 9.6 GHz EDOP system; it has a high
degree of flexibility and performs all the signal processing from
bandpass filtering to calculation of the Doppler velocities through
the autocovariance method. Switching of the transmit polarization
by the radar controller provides measurement of the linear depolarization
ratio, LDR, differential reflectivity, ZDR, and differential phase
measurements. The radar has two antennas; one antenna is used for
ground-based operation and has 55 dBi gain. The other antenna designed
for the ER-2 installation is an offset parabolic reflector antenna
with 47 dBi gain. Both antennas are novel designs utilizing Flat
Parabolic Surface (FLAPS) technology developed under an SBIR contract.
Absolute calibration
of the transmitter and receiver is performed externally using standard
methodologies. Internal calibration of the CRS receiver is performed
continuously through consecutive looks at a single noise source.
IF calibration is performed by injecting the IF phase-locked oscillator
signal at the output of the mixer/preamplifier stages. Digitally-stepped
attenuators are used to step the calibration signal over the receiver
full dynamic range during flight. Phase calibration of the coherent
detector is achieved by varying the phase of the reference signal.
Transmitter power is monitored continuously through a detector.
So far the radar has not participated in any field experiments but
has operated successfully from the rooftop laboratory at NASA Goddard.
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