Weather Radar Interferometry to Measure Cross-Beam Wind
Vector wind is important for quantifying and forecasting weather. However, weather radars
such as the WSR-88D can measure only the radial component of the wind. In contrast, the
three-dimensional wind field (including wind profiles) can be measured either by Doppler
beam swinging (DBS) or interferometric techniques
[Doviak and Zrnic, 1993;
Briggs et al., 1950].
For example, the Spaced Antenna Interferometer (SAI) technique has recently been
developed allowing the measurement of the cross-beam wind components (i.e., the component
parallel to the baseline connecting two receivers) as well as the along-beam wind component
obtained from the mean Doppler shift
[Doviak et al., 1996].
SAI can be understood as either
a radar signal received at one receiver delayed with respect to the other, or as interference
patterns formed on the antenna plane moving in correspondence to the scatterers’ motion.
Until now, wind measurements using spaced receivers have been limited to vertically pointing
wind profilers. With the availability of NSSL’s NWRT, however, implementation of SAI to
measure cross-beam wind, shear and turbulence now appears feasible for the first time with
an S-band radar.
Research in Progress
In close collaboration with NSSL scientists and engineers (Dr. Doviak, and others), we
propose to perform research and development of SAI on NWRT. The project focuses on
researching, developing and implementing the SAI and DBS techniques, and verifying results
with winds obtained from other radars (e.g., NOAA’s wind profiler at the Kessler Farm Field
Laboratory and the KTLX radar). We also plan to compare the relative performance of the
DBS and SAI techniques.
Activate the Azimuthal (Alpha) Difference Channel
Presently the difference channel
is not enabled and needs to be activated. This important task is currently being
accomplished by engineers from both NSSL and LCMO. Microwave receiver components
to down-convert the 3200 MHz RF signal to an IF frequency of 57 MHz signals will be
purchased, assembled, and tested. The sum and difference signals will be reconnected
to the in-house fabricated dual-channel microwave receiver, and its output will be
connected to an RVP-8 digital IF receiver. The two complex signals from both the sum
and difference channels (i.e., the H and V channels on the RVP-8) will be recorded.
Although this work will be primarily accomplished by NSSL and LCMO, we are willing
to assist in any capacity needed.
Reconstruction and Study of Left/Right Array Signals
A joint effort between NSSL and
OU will be made to reconstruct the signals for the left and right halves of the PAR
antenna from the sum and difference signals. We propose to study the attenuation
ratio and phase difference for the two channels. As an initial step, we will investigate
ground clutter signals to find the attenuation ratio, and the phase difference and then
synthesize a pair of balanced signals, one from the left and the other from right half of
the antenna array.
Cross-Beam Wind Estimation
The cross-beam wind is estimated from the cross-
correlation function estimates of signals from the left/right sides of the array by using
the correlation method
[Doviak et al., 1996;
Zhang et al., 2004]. The accuracy of the
resulting wind estimates will be quantified statistically, with an expected error of less
than 1 m/s with a 10 s dwell time. Verification will be accomplished by comparing
the wind measurements with profiler and/or other nearby Doppler radars.
Theoretical Formulation and Numerical Simulation
In order to fully understand and
optimize the performance of SAI for cross-beam wind measurement with the NWRT,
theoretical and numerical studies will be performed in support of the experiment.
SAI will be formulated based on wave scattering from randomly distributed scatterers
in the presence of shear and turbulence. The performance and limitation of SAI in
complex weather conditions such as shear will be studied through theoretical analysis
and numerical simulations, possibly using the radar simulator described in Section 3.1.
The auto and cross-correlation functions will be derived and calculated for various
possible configurations/conditions with both NWRT and MPAR.
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