DATA_SET_DESCRIPTION |
Data Set Overview
=================
This data set includes all data from the High Rate Detector (HRD)
through the end of 2006. All data products in this data set are in
tabular format. Since HRD is mounted on the same platform as the
Dust Analyzer, the pointing is the same for both instruments.
Data file types and contents
============================
Data files in the 'raw' subdirectory contain all recorded events,
including impacts, noise events, and calibration events. The first
column of each file is a unique event number of the format
Xnnnnnnnnn where X is a code for the year (A = 2000, B = 2001, etc,)
and nnnnnnnnn is a sequential number within the year. The raw
filenames are of the form hrd_yyyy_doy_doy.tab and include data
within the date range specified.
Data files in the 'calibrate' subdirectory contain calibration
events extracted from the raw files. Note that the sample rate is
changed periodically, resulting to changes in the time increments in
the calibration files. Calibration files are grouped by year, and
since in-flight calibrations were not done in all years,
subdirectories do not exist for all years of the mission. The event
number corresponds to that in the raw file. The filenames are of
the form hrd_yyyy_doy_doy_cal.tab and include data within the date
range specified.
Data files in the 'processed' subdirectory have had calibration
events and noisy events removed. On 2005-248 there occurred an M4
event in the large detector which resulted in a noisy M1 threshold.
Since then, all M1 events are considered to be noise and have been
removed from the processed data unless the M2 threshold is triggered
or the small detector m1 threshold is triggered or the large
detector High Mass is set. The processed files have filenames of
the form hrd_yyyy_doy_doy_prc.tab and include data within the date
range specified.
The calibration and processed files include a quality code flag.
The QC flag indicates a discrepancy in the data line and is set if
any one of the following obtain:
1. Missing latch data.
2. Counters change with no latch data.
3. Higher threshold triggered and lower threshold did not.
The data directory 'onoff' contains files with the on-off times of
the HRD, divided by year. These have filenames of the form
hrd_yyyy_on_off.tab. Note that if the instrument was not powered on
or off during the covered time period, there will not be an on-off
file for that time period.
The data directory 'pointing' contains hourly instrument pointing
and spacecraft positions generated from the SPICE kernels. The
pointing data pertains to both the CDA and HRD instruments, which
are mounted on the same platform. Gaps in the pointing and position
data are due to the fact kernels are not available for those time
periods. The metakernel listing the kernels used to generate the
pointing and position files is included in the document directory.
Calibration of the HRD Detectors
================================
The HRD calibrations are similar to those for the Dust Flux Monitor
Instrument(DFMI) on the STARDUST misssion to comet Wild 2. The
calibrations of HRD detectors for the Cassini mission as well as for
those for the DFMI have done with dust particle accellerators in
Heidelgerg and Munich. During the calibration at Heidelberg iron
particles in the velocity range of 1-12 km/sec were used while at
Munich accelerator glass particles at similar range were used.
Please refer to Simpson and Tuzzolino (1985), Simpson and Tuzzolino
(1989), and Tuzzolino et al. (2000) for more details and description
of how these calibrations were performed.
Besides laboratory calibration, in-flight pulser calibrations were
performed periodically to ascertain the performance of the
electronic system of the HRD instrument.
References
==========
Srama, R., T.J. Ahrens, N. Altobelli, S. Auer, J.G. Bradley, and 35
others, The Cassini Dust Analyzer, Space Science Reviews 114,
465-518, 2004.
Simpson, J.A. and Tuzzolino, A.J., Polarized Polymer Films as
Electronic Pulse Detectors of Cosmic Dust Particles, Nucl. Instrum.
Methods A236, 187-202, 1985.
Simpson, J.A., D. Rabinowitz, and Tuzzolino, A.J., Cosmic Dust
Investigations, I: PVDF Detector Signal Dependence on Mass and
Velocity for Penetrating Particles, Nucl. Instrum. Methods A279,
611, 1989.
Simpson, J.A. and Tuzzolino, A.J., Cosmic Dust Investigations, II:
Instruments for measurement of particle trajectory, velocity, and
mass, Nucl. Instrum. Methods A279, 625, 1989.
Tuzzolino, A.J., R.B. McKibben, J.A. Simpson, J.A.M. McDonnell, M.J.
Burchell, and 8 others, Calibration of the Dust Flux Monitor
Instrument (DFMI) for the Stardust Mission to Comet Wild 2, in the
Stardust Docushare, Jet Propulsion Laboratory, 2000.
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CONFIDENCE_LEVEL_NOTE |
Confidence Level Overview
=========================
Large impact during Ring Plane Crossing
=======================================
The HRD performed well throughout the entire mission. However,
after crossing the Saturn G ring on DOY 2005_248, the #1 large HRD
sensor was hit by a large size dust particle that exceeded all
mass thresholds of the HRD instrument (the size was greater than
several hundred microns). This event probably changed the
capacitance of the sensor and the HRD instrument started to show
some noise in the lowest threshold M1 of the #1 sensor in the
range of several counts per mimute. It was decided not to change
the threshold level by a factor of 10 (the only possible response)
in order not to lose the data from the other three thresholds (M2,
M3, M4). So, the M1 data are not trustworthy for low count rates,
but they could be useful when the counting rate is high during the
ring crossing, or satellite flybys.
Both detectors triggered
========================
In some events in the 'raw' data, both detectors are triggered.
This implies simultaneous impacts in the two detectors. In the
'processed' files, such events have been split into two lines, one
for each impact. Both lines have the same event number since they
come from the same entry in the corresponding events file.
Note that within a single detector, the triggering of a higher
threshold will ordinarily be accompanied by the lower thresholds
being set also. If not, the impact is suspect and the quality code
is set.
Cumulative count discrepancy
============================
In some instances the cumulative counts don't agree with the
individual counts numerically. This is due to the processing time
the CPU takes to reset the latch for the next discrete event. If
an event occurs during the latch reset cycle the event will not be
saved by the latch and the CPU will read a zero value. However,
the missing latched event will still be recorded by the eight
16-bit counters.
HRD instrument reset
====================
On instrument power-on, the HRD performs a power-on reset. The
reset sets the HRD clock and all the counters to zero. Since the
counters are set to zero on reset, the counts appear to go down
with time on reset. Missing data can be determined by looking at
the on-off files (described above) which contain a list of the
power on and off times.
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