Table of Contents
This document is a standard product of
NCAR/ATD/RTF
which gives an overview of the measurements taken by PAM and ASTER
and conditions during the CASES97 field experiment.
This document can be obtained either in hard copy from RTF or in electronic
form from the NCAR/ATD WWW site.
Dataset Status
The first 10 days or so of data are often missing and have errors
as the stations were being set up. Please ignore these values unless you
specifically need data before 20 April.
***** NEW: The data values were reprocessed 5 June 2000 to fix krypton
hygrometer values (see below). Note that a lot of sensible heat flux values
(H) are now missing, since the conversion from sonic temperature to actual
temperature depends on humidity. For approximate values of H during these
periods, use: rho*Cp*w'tc', where rho~1.16 g/m3 and
Cp~(1006 + 1857*Q*0.001) J/kgK. *****
The 5-minute and 30-minute datasets have been corrected for:
- Tilt corrections applied to all sonic anemometer statistics (see below).
(NOTE: Values involving u and v are still in boom-oriented coordinates.)
- The empirical calibration applied to the soil moisture data (see below).
- Removal of calibration events in the rain gauge data.
- Rlw.up recomputed without Tdome correction, since Tdome.up was bad.
Also, some early bad pyrgeometer values removed.
- Removal of values when the krypton hygrometers were covered with plastic
bags.
A lower resolution dataset contains statistics averaged over 30-min periods for
the entire project. These have been generated with all corrections
applied to the data, though outlier values may still be present. In
addition, some quantities have been derived, such as the sensible heat
flux (H), latent heat flux (LE.dry), and soil heat flux evaluted at the
surface (Gsfc).
In addition to the corrections mentioned above, the 30-minute dataset contains:
- Specific humidity (Q) has been computed from T and RH.
- Include boom azimuth for the sonic, so all values involving u and v are
now in geographic coordinates.
- The momentum, sensible and latent heat fluxes (u*, H, LE) have been
computed from the sonic data using all known corrections (Webb, recover T from
Tc, etc.). Note that u* is from the magnitude of u'w' and v'w', not the
projection of the stress vector on the mean wind vector (which would be
correct).
- The surface heat flux (Gsfc) has been computed from the soil heat flux
(Gsoil) plus heat storage determined from soil temperature and moisture.
- The "oxygen correction" has been applied to LE calculated from the
krypton values.
Table of Variables
A complete table of variables
is available for the 5-min. statistics and
the 30-min. statistics.
Data Access
Data for CASES97 are available in several forms:
- 5-minute averages of first and second-order moments of calibrated data,
including data from all eight PAM and ASTER sites.
We recommend combining these to obtain more statistically-significant
averages over longer time periods (note that 30-minute averages are also
available).
These are available at NetCDF data files.
- 30-minute averages of first and second-order moments of selected
calibrated data. Note that the second-order moments include the "variance
of the means" and thus are the true 30-minute average.
These 30-minute statistics are available at cases97_30min.nc.
- 1, 10, or 20 sample/second uncalibrated values from the ASTER sites.
Software is maintained at RTF to generate calibrated time series
on demand using the most current calibration routines, in either
ASCII or floating point binary format.
For access to the ASTER time series, please contact RTF.
Also available is a computer-readable
logbook of comments noted by RTF
personnel.
Location
There are 6 PAM sites and 2 ASTER sites throughout the lower
Walnut River watershed south and east of Wichita, Kansas.
The sites were selected to have terrain and land cover typical of
the watershed, with good exposure to the predominate winds (SE-S-SW
and NW-N). The fetch for these winds generally is at least 200m.
The positions of various sites were:
- PAM (map): rangeland, 37deg 35.44' N, 96deg 39.10' W
- PAM (map): rangeland, 37deg 33.11' N, 96deg 33.31' W
- PAM (map): new corn/beans, 37deg 29' 40" N, 97deg 01.90' W
- PAM (map): milo stubble/rangeland, 37deg 35.59' N, 96deg 57.12' W
- PAM (map): new milo, 37deg 30.21' N, 97deg 08.38' W
- PAM (map): winter wheat (floodplain), 37deg 16.30' N, 97deg 00.56' W
- ASTER (map): winter wheat, 37deg 26.65' N, 96deg 59.97' W
- ASTER (map): rangeland, 37deg 24.04' N, 96deg 56.80' W
Sensors
Most of this section will be completed later.
The PAM
sites were instrumented with standard sensors and the
ASTER
sites were instrumented to function similar to the PAM stations. In addition,
other sensors were added to the ASTER sites (see below). Generally, chemistry
and spectral-resolving radiation sensors were added at site #7 and site #8 was
used for testing sensors.
Since NCAR/ATD did not have enough
flux sensors to instrument 8 stations, it was necessary to obtain sensors
from several sources, and thus a mix of sensors was used for CASES.
These were:
- Gill sonic; krypton hygrometer
- Gill sonic; krypton hygrometer
- ATI sonic; krypton hygrometer
- ATI sonic; krypton hygrometer
- ATI sonic; krypton hygrometer
- Gill sonic; krypton hygrometer
- ATI sonic; OPHIR hygrometer
- ATI sonic; OPHIR hygrometer
We are especially grateful to Chris Fairall of NOAA/ETL for the use
of 4 of these sonic anemometers and 2 hygrometers.
Soil measurements were made to characterize the first 10 cm depth.
The temperature probe was inserted on a slant to average from 1-9cm.
The (automatic) soil moisture probe was inserted horizontally at 5cm and its
radiation pattern roughly integrates from 3-7cm. Soil moisture comparison
measurements were made manually using (TRIME) probes inserted on a slant to
integrate between 0-10cm and using core samples taken from 1-7cm (note that
this is weighted higher than the other measurements).
Several non-standard sensors were used for this program:
- ETI rain gauges were deployed at stations #2 and #6 for comparison
to the MRI rain gauges used at all other sites.
- A 4-component
(visible and infrared radiation, upward and downward
looking) set of radiation sensors at station #7.
- Two PAR sensors were mounted facing up and down to get a "PAR
albedo" at station #7.
- A Licor carbon dioxide sensor with an inlet colocated with the
sonic anemometer at station #7 for measuring CO2 fluxes.
- A fast-response surface effect chemiluminescent ozone detector
with an inlet at the sonic anemometer at station #7 for measuring ozone
fluxes.
- A prototype low-power surface effect chemiluminescent ozone
sensor (SECLOD)near the sonic anemometer
at station #7.
- A Campbell Scientific sonic anemometer at station #8 which was
being evaluated as a future sensor for PAMIII.
- A prototype low-power infrared humidity sensor at station #8.
- An aspirated temperature and humidity sensor at station #8
to test our bandpass covariance method for measuring fluxes.
-
A Skye Instruments "veggie" meter (possibly their
SKR 110)
measured radiation at 630 and 780 nm to estimate NDVI.
Initially, this was deployed at station #7 to measure wheat growth.
It was moved 22 Aug to station #8 and was mounted at 7m pointing about SSE,
to capture the green-up of the grassland. WARNING: The variables
"Rveg.660" and "Rveg.730" have from this instrument at both locations.
ALSO, the data from this instrument are suspect (sometimes negative values)
until further notice.
Known Instrument Problems
IN PROGRESS.
Rain Gauges
The rain gauge field calibration checks are summarized in a
table.
Most gauges read within 5% of the nominal reading, which is considered
acceptable. The gauge at site 5 was moved when this site was finally
deployed at which time the calibration shifted by 10%. We will do a post-
calibration to determine if this was due to mis-leveling or an actual
change in the calibration. In any case, the data probably should be
corrected by 8% (the average of the two calibrations). This has not
been applied to the NetCDF files, but may in the future. Similarly,
it may be desirable to adjust the calibration at site 6.
I will remove the jumps in the data caused by these calibrations from the
final data set.
A plot of the accumulation time
series for the period 18 April - 26 May is available (without any
adjustments). The total accumulations (both with and without adjustments
for the above calibrations) at the end of this period are shown in another
table. Note that both ETI gauges read
less than the MRI gauges by about 30%. (Although Ed Brandes has
noted that the ETI is sometimes higher than the MRI for an individual rain
event.)
Soil Moisture
The soil moisture field calibration checks are summarized in a
table.
These have been used to create new calibrations, which is described in a
report.
Pyrgeometers
Pyrgeometers were deployed at site #7 to measure long-wave (infrared)
radiation. The sensor has a thermopile to measure the difference in
temperature between an exposed black plate and the metal housing. The
temperature of the housing, along with the dome and the case of the instrument,
are measured seperately with thermistors. The equation normally used to
compute the radiation from these measurements is:
Rlw = Rpile + sigma Tcomp^4 - [1.11 sigma (Tdome^4 - Tcase^4) + 0.036 Rsw]
However, the Tdome signal from the downward-looking radiometer (measuring
pyg.out) was bad, with an offset of about -8 C and noise. Since the sensor
operated normally in the lab, and the A/D channel passed its check-out, the
problem presumably was an electrical connection. This isn't a serious
problem, since we expect Tdome to be nearly equal to Tcase for the
downward-looking sensor. Thus, the Tdome^4 - Tcase^4 term above should be
neglected for pyg.out.
Chronology
Day: Action
- 3 April: Base installed.
- 16 April: All sites reporting data.
- 22 April: Official start of operations.
- 21 May: Official end of operations.
- 28 May: Estimated end of tear-down.
Data Processing Notes
STILL UNDER PROGRESS.
Sonic Anemometer Tilt Correction
Tilt corrections will be applied to the final data set (they have not been
done in the preliminary data sets). This correction compensates for any
misalignment of the sonic anemometers with respect to a plane parallel to
the surface of the ground. Generally, the anemometers are set up so that
the vertical velocity is reasonably well aligned (within 1 degree) to gravity.
However, our alignment of these sensors may not be perfect, the mount may
sag with time, and the surface usually is not perfectly horizontal.
We generate this correction by fitting to the equation: W = Wo + a*U + b*V,
where U, V, W are 5-minute averages of the measured wind components and the
fit is done over the entire period that the instrument was not moved. The
fit is reported as an offset in W, a "lean angle" (where 0 is vertical), and
a "lean direction" (where 0 is along the azimuth of the anemometer
u-component). An example of this fit is given here for the
CSAT anemometer.
We use one fit for the entire data set, unless we know of a discontinuity.
There were only 2 such events during CASES; the u-component was readjusted
(and bias might have changed) at site 3 on 21 April and the entire anemometer
was raised at site 6 on 7 May. However, neither event appeared to affect
the fit significantly (based on examining the time series of the fit
coefficients when a separate fit was generated for each day), so only
one fit was used. For a few other sites, the fit differed as a function of
time, however this probably was due to limited wind directions, and data
composited over the entire period had a reasonably low amount of scatter.
The resulting coefficients from this process are given in a
table. Note that many of the biases
were rather large (about 5 cm/s), which may have been the result of
preferentially locating the towers at the top of ridges.
Daily Weather Plots
THE PLOTS IN THIS SECTION ARE NOT FINAL.
The following plots summarize conditions at each station during each
day of the project.
Each plot covers one and a half days (0100-1300+1 CDT) and is labeled with time
in GMT at the bottom and local time (CDT) at the top. The top panel
displays temperature and specific humidity measured at 2m, pressure,
and precipitation rates (if present). Below that is a plot of wind speed
and direction measured at 10m, with dotted lines showing the
directions in which flow distortion by the towers should not be a problem
(there may be more). The next panel shows net radiation, and sensible
and latent heat flux. The bottom panel shows the Monin-Obukhov
stability parameter, z/L, the friction velocity, u*, and the Bowen
ratio calculated from the flux data.
Since these fluxes and derived parameters are based on smoothed, 5-minute
average statistics, they should not be used quantitatively and are only
shown for guidance in selecting periods to analyze further.
- Date: Station
- 17 April: #1,
#2,
#3,
#4,
#5,
#6,
#7,
#8
- 18 April: #1,
#2,
#3,
#4,
#5,
#6,
#7,
#8
- 19 April: #1,
#2,
#3,
#4,
#5,
#6,
#7,
#8
- 20 April: #1,
#2,
#3,
#4,
#5,
#6,
#7,
#8
- 21 April: #1,
#2,
#3,
#4,
#5,
#6,
#7,
#8
- 22 April: #1,
#2,
#3,
#4,
#5,
#6,
#7,
#8
- 23 April: #1,
#2,
#3,
#4,
#5,
#6,
#7,
#8
- 24 April: #1,
#2,
#3,
#4,
#5,
#6,
#7,
#8
- 25 April: #1,
#2,
#3,
#4,
#5,
#6,
#7,
#8
- 26 April: #1,
#2,
#3,
#4,
#5,
#6,
#7,
#8
- 27 April: #1,
#2,
#3,
#4,
#5,
#6,
#7,
#8
- 28 April: #1,
#2,
#3,
#4,
#5,
#6,
#7,
#8
- 29 April: #1,
#2,
#3,
#4,
#5,
#6,
#7,
#8
- 30 April: #1,
#2,
#3,
#4,
#5,
#6,
#7,
#8
- 1 May: #1,
#2,
#3,
#4,
#5,
#6,
#7,
#8
- 2 May: #1,
#2,
#3,
#4,
#5,
#6,
#7,
#8
- 3 May: #1,
#2,
#3,
#4,
#5,
#6,
#7,
#8
- 4 May: #1,
#2,
#3,
#4,
#5,
#6,
#7,
#8
- 5 May: #1,
#2,
#3,
#4,
#5,
#6,
#7,
#8
- 6 May: #1,
#2,
#3,
#4,
#5,
#6,
#7,
#8
- 7 May: #1,
#2,
#3,
#4,
#5,
#6,
#7,
#8,
- 8 May: #1,
#2,
#3,
#4,
#5,
#6,
#7,
#8,
- 9 May: #1,
#2,
#3,
#4,
#5,
#6,
#7,
#8,
- 10 May: #1,
#2,
#3,
#4,
#5,
#6,
#7,
#8,
- 11 May: #1,
#2,
#3,
#4,
#5,
#6,
#7,
#8,
- 12 May: #1,
#2,
#3,
#4,
#5,
#6,
#7,
#8,
- 13 May: #1,
#2,
#3,
#4,
#5,
#6,
#7,
#8,
- 14 May: #1,
#2,
#3,
#4,
#5,
#6,
#7,
#8,
- 15 May: #1,
#2,
#3,
#4,
#5,
#6,
#7,
#8,
- 16 May: #1,
#2,
#3,
#4,
#5,
#6,
#7,
#8,
- 17 May: #1,
#2,
#3,
#4,
#5,
#6,
#7,
#8,
- 18 May: #1,
#2,
#3,
#4,
#5,
#6,
#7,
#8,
- 19 May: #1,
#2,
#3,
#4,
#5,
#6,
#7,
#8,
- 20 May: #1,
#2,
#3,
#4,
#5,
#6,
#7,
#8,
- 21 May: #1,
#2,
#3,
#4,
#5,
#6,
#7,
#8,
- 22 May: #1,
#2,
#3,
#4,
#5,
#6,
#7,
#8,
- 23 May: #1,
#2,
#3,
#4,
#5,
#6,
#7,
#8,
Other plots
Rain
Soil Moisture
Downwelling radiation
These are plots of downwelling shortwave radiation measured by the Li-Cor
sensors at each site versus that from the Epply at site 7 for mostly clear
cases. If there were no clouds, we expect these to be nearly the same.
A second-order fit was applied to these data, which shows some systematic
differences, though all within the +/-5% specification for these radiometers
by Li-Cor. It is possible to correct these data using these fits, but
be cautioned that we don't know the reason for these differences.
All of this analyses were contributed by Peggy Lemone.
Site 1,
Site 2,
Site 3,
Site 4,
Site 5 (first part),
Site 5 (entire period),
Site 6,
Site 7,
Site 8
Roughness length
This is a plot of histograms of the log10 of
zo for each site, computed from the near-neutral 30-min average
statistics by:
zo <- 10*exp(-0.4*dat("Spd")/dat("u*"))
zo[zo<1e-6] <- NA
ineut <- abs(dat("w't'")<.01
par(mfrow=c(3,3))
for (i in 1:8) {
hist(log10(zo[ineut[,i],i]),n=30)
title(paste("#",i,"; ",round(10^median(log10(zo[ineut[,i],i]),na.rm=T),
dig=4),sep="")) }
The title is the site number and the median roughness length (in meters).
The values are (in cm):
Site: 1 2 3 4 5 6 7 8
Cover: range range crn/bns dirt wheat wheat wheat range
zo (cm) median 0.6 0.2 0.7 1.3 0.8 5.3 1.4 0.8
zo (cm) maxhist 1.0 0.4 0.7 2.2 4.5 7.1 7.1 2.5
I don't quite believe these results, which says that wheat had a roughness
of about 5cm, dirt about 2cm, rangeland and planted crops about 1cm. Three
weaknesses with this analysis are that all wind directions have been lumped
together, only heat flux is used to characterize near-neutral, and z was set
to 10m, ignoring displacement height (this last should be a relatively minor
problem).
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This page was prepared by
Steven Oncley,
NCAR Research Technology Facility