Introduction
High-quality data collection depends upon preparation and
proper field procedures. Never-the-less, there follows a
post-field evalution process that may result in modifications
to the data set, or potential improvements to increase data
utility. Changes made to the in-field S-PolKa data set are
detailed, here.
Changes/Improvements to S-PolKa Data
Considerable energy has been invested in making the
S-PolKa/DYNAMO data set one of the most accurate and usable
S-Pol date sets, ever. Specific changes include:
- Noise power for all S-band and Ka-band power quantities
has been re-estimated on a beam-by-beam basis; this impacts
all noise-power corrections and mostly impacts reflectivity
values and censoring/thresholding at low measured powers.
- Advanced techniques for data censoring have been
developed, resulting in a more reliable elimination of bad
data. See a complete description
in
Dixon and Hubbert, 2012.
- A merged data set has been created, incorporating
S-band, PID, rain rates, and several of the most useful
Ka-band fields within single cfRadial files. During
creation, it was necessary to degrade Ka gate resolution
from 75 m to 150m, to match the S-band gates. The merged
data set was created for user convenience, and the
original-resolution, quality-controlled, full-parameter, Ka
data are avaialble in a separate data set. The merged data
set should be considered the recommended, complete data
set, except when the full-resolution Ka is required.
- Multiple S-band velocity fields have been created,
reprocessed from the original phase data. The traditional
velocity field is maintained, with two additional fields
that provide less noisy data in low SNR regions and for
non-meteorological echoes.
- PID uses local soundings to develop information on
freezing levels. Reprocessing has allowed use of better
time-aligned soundings for the entire data set.
- PID has been significantly altered to remove/mitigate
erroneous classifications of graupel, make use of the
noise-corrected RHOHV, and flag regions of likely receiver
saturation (which led to errors in particle
classification). Membership functions for the fuzzy logic
algorithms have been changed; Scott Ellis has prepared a
summary
document.
- Some small tuning of the precipitation rate algorithms
was performed
(see
this). Precip estimates were also improved by changes
to censoring and recalculation of RHOHV.
- The test pulse was eliminated from the final data set.
The test pulse had existed at extreme radar range. It was
removed to avoid problems with any automated user
processing and analysis of the data. (note that, at high
elevation angles, the test pulse had already been eliminated
as part of S-Pol's standard data reduction through
truncation procedures)
- The S-band atmospheric attenuation was re-estimated
using a technique detailed in Doviak and Zrnic (Doppler
Radar and Weather Observations, 2nd ed., 1993, pp44-45).
The attenuation-corrected reflectivity is included as the
primary reflectivity field, while the
non-attenuation-corrected field is also included in the
merged data set.
- The original RHOHV field has been renamed to
RHOHV_NNC_S, for NO_NOISE_CORRECTION. And the RHOHV_S
field now has noise correction applied.
- The Ka reflectivity was corrected to account for the
change-out of the Ka-band magnetron and to correct an
ambiguity in the in-field calibration information.
- There were no changes to either the S-band power
calibrations or the value of the Zdr-bias used during the
field phase.
What Has Not Changed
EOL maintains a complete set of the original S-PolKa data.
Should any problems be found in derivations or
re-calculations, data can be reprocessed.
The original COVAR data set has not been changed. Derived
power quantities (DBMHC, DBMHX, etc.) remain unchanged,
except where censoring has flagged these values as "bad".
Implications for Data Users
Obviously, if you are using a data set derived from the
real-time, in-field data stream, you should update your data
set. While many parameters have not been changed, the
censoring algorithm has been greatly improved, and use of the
(version-1) final data set will ease any tasks associated
with further data editing or censoring.
It is particularly important that you update any in-field
data sets using the PID or precipitation rate variables.
Both have been re-computed using the new censoring and the
attenuation-corrected S-band reflectivity. The updated
noise-power correction combined with a recalculated RHOHV,
has resulted in better PID on the edges of echoes.