2000 Incoherent Scatter Coordinated Observation Days
URSI-ISWG
In the following table, column 2
gives the start and end date of the experiment, column 3 gives
the day of the week of the start of the experiment, column 4
is the length of the experiment and column 5 shows the date of the new moon.
Incoherent Scatter Coordinated Observation Days should start at 1300UT
on the first day indicated (to ensure that all radars are operating correctly
by 1600UT) and end at 1600UT on the last day indicated. However,
radars are encouraged to start as early as possible on the first day where operational considerations allow.
2000 Incoherent Scatter Coordinated Observation Days |
| Month |
Dates |
Day |
Length |
NewMoon |
Notes |
| January |
06-07 |
Thursday |
1 |
06 |
|
| February |
|
|
|
05 |
|
| March |
14-17 |
Tuesday |
3 |
06 |
- Global convection (note 2)
- Hi-TRAC (note 3)
|
| April |
04-26 |
(Tuesday default) |
2, floating default 11-13 |
4 |
- WLS(E) (note 5)
observations within month-long 'alert' interval
- Final date selection by
Foster
- SPARC (note 6)
|
| May |
|
|
|
04 |
|
| June |
13-14 |
Tuesday |
1 |
02 |
|
| July |
05-07 |
Wednesday |
2 |
01, 31 |
- Mid-July Baseline (note 7)
|
| August |
|
|
|
29 |
|
| September |
04-29 |
(Thursday default) |
6, floating default 21-27 |
27 |
- 6 day floating LTCS (note 8)
observations within month-long 'alert' interval
- Final date selection depends on
TIMED
operations (note 9); to be co-ordinated by
Salah
|
| October |
24-27 |
Tuesday |
2 |
27 |
- Global ionosphere-themosphere coupling (note 10)
- WLS(E) (note 5)
- SPARC (note 6)
|
| November |
|
|
|
25 |
|
| December |
04-22 |
(Monday default) |
4, floating default 11-15 |
25 |
- 4 day floating LTCS (note 8)
observations within month-long 'alert' interval
- Final date selection depends on
TIMED
operations (note 9); to be co-ordinated by
Salah
|
| Total |
|
|
21 |
|
|
| Last updated: Thursday, 05-Aug-99 09:41:00 GMT |
Notes
- POLITE
POLITE aims to advance our understanding of topside light ion morphology
and dynamics through a combination of modeling efforts and coordinated
observations by the ISR chain and by DMSP satellite overflights. The use
of the full latitudinal and longitudinal extent of the ISR chain is
critical to the campaign, as one key objective is the study of the
latitudinal and longitudinal variations of hydrogen, oxygen, and
helium ions. Simultaneous measurements of neutral oxygen, hydrogen, and
helium are also important, in order to explore the coupling between
ionic and neutral species in the lower topside. The helium ion layer
descends in altitude and increases in strength during the wintertime,
making observation easier for the ISR chain. Significant asymmetries
in field-aligned flows are also at their maximums during summer and
winter solstices. IMF support is not very important, but new moon
periods are critical since optical support is required for simultaneous
neutral species measurements.
Contact: Phil Erickson
- Global ionospheric convection - time-dependent model fitting
It is important that all radars concentrate on ionospheric
electric field measurements, preferably in the magnetic field aligned position
where possible.
The IZMIRAN Electrodynamic Model (IZMEM) has been developed from magnetometer
data to reproduce the global electric potential patterns for all seasons. The
model is time dependent on the magnitude and sign of the interplanetary magnetic
field (IMF) components. Qualtitative tests of the model using data from the
STARE and SABRE coherent radar systems, as well as SUPERDARN, have been very
encouraging. For quantitative comparisons, which will allow fine adjustment of
the model, it is necessary to get an accurate measurement of the ionospheric
electric field at several points on the globe simultaneously. Initial
quantitative comparisons with EISCAT are good but lack global coverage. For this
purpose, a world day campaign of all available incoherent-backscatter radars
would be ideal.
A long run of several days (at least 3-5) is best to cover as many IMF
conditions as possible. An existing world day run is scheduled for the summer of
1999. As there is a need to cover all seasons, the next choice would be equinox
for 2000. The exact date is not important, although the predicted position of
satellites used for IMF measurements could be taken into consideration in-so-far
as this is practical.
Contact: Kosch and Levitin
- Hi-TRAC: High Time Resolution Auroral Radar Convection. Combines
incoherent and coherent scatter radars to provide optimum high latitude
convection measurements. High latitude radars should endevour to
record high-time resolution line-of-sight velocities over as wide a
latitude interval as possible. Low latitude radars should use
database (q.v.) modes.
Contact: John Holt
- Database: The emphasis should be on broad latitudinal coverage of the
F region.
Contact: Tony van Eyken
- Wide-Latitude Substorm Dynamics
These are 'floating' days, the exact operation dates to be selected about
one month before based on available predictions.
Radars which cannot accommodate this flexibility should run on the default
dates. Modes with temporal resolutions better than 5 minutes
should be used. In 1999, we should address substorm phenomena with
better time resolution.
Contact: John Foster
- SPARC
SPARC brings together researchers in upper atmospheric and space physics
from around the world, providing them a set of online collaboration tools
and workspaces that link together scientific instruments, data, and models.
The collaboratory is itself a subject of study by computer and behavioral
scientists who are developing and refining the tools and organizational
structures that will make such real-time, online collaborative research
commonplace.
Contact: Tim Killeen
- Mid-July Baseline
The purpose of this experiment is to help improve our statistics of all
the parameters measured by the ISRs. These are deficient in summer.
In particular seasonal effects on magnetospheric convection are not well
established for the differing levels of geomagnetic activity.
Another 2-day experiment at any time during July, 2000 would
satisfy this objective. The widest latitude coverage possible
should be obtained, as good time-resolution is not required for
building up our statistics.
Contact: Mike Buonsanto
- LTCS
Combined local E and F region measurements, including vector
velocities, with 15 minute time resolution. Latitudinal coverage may
be sacrificed to meet this goal.
Contact: Cassendra Fessen
- CEDAR-TIMED
Joint Observations of the Effects of Storms on the Lower Thermosphere
The goal of this project is to gather observations on the temperature and
winds in the lower thermosphere during geomagnetic storms. Data from
ISRs and supporting instrumentation available at the upper atmosphere
facilities are needed in the primary altitude range of 90-150 km with fine
altitude and time resolution (similar to LTCS modes). Data at altitudes
in the middle and upper atmosphere will also be useful to study coupling
with the lower thermosphere. The observations will be made in response
to an alert of a major sustained geomagnetic storm (Kp>5 or 6), and will
be studied in coordination with TIMED satellite observations using
general circulation and tidal models. A one-month period will be identified
one year in advance, and then narrowed to a 10-day stand-by period 6 weeks
before the start of the month. The observations will last 4 full days.
We request two such periods in year 2000 following the launch of the
TIMED satellite (May 2000) and initial validation of its data. The
requested periods are for Fall (Sep or Oct) and Winter 2000 (Nov, Dec or
Jan 2001).
Contact: Joe Salah
- Global Ionosphere-Thermosphere Coupling Study
All radars should measure electron density, ion and electron temperature
and ion velocities parallel to the magnetic field direction.
Electric field measurements are not essential for monostatic radars.
Objectives:
- Fit and constrain global models of the thermosphere (eg. UCL 3D
thermospheric model) and ionosphere (eg. Grenoble TRANSCAR model)
using simultaneous measurements at F-region altitudes.
- Compute ion-neutral collision frequencies (O-O+) using neutral
meridional winds from interferometer and radar measurements. This
will include the O-density from the adjusted neutral atmosphere
model (from above) and direct neutral temperature measurements
where available.
Both objectives are best studied during quiet geomagnetic conditions.
In the case of substorms, however, a study of the global thermospheric
response will be possible. All available interferometers near
radar
sites suitable for thermospheric measurements should be
operated. Neutral wind measurements at OID 630 nm are essential.
Neutral temperature measurements at OID 630 nm should be done if
possible.
All radars should measure in the magnetic field parallel direction.
Electron density, ion and electron temperature and ion velocities
parallel to the magnetic field direction are required. Ionospheric
electric field measurements are not essential for monostatic radars.
A long coordinated run is preferred (3-5 days) in order to (1) cover
a variety of geomagnetic conditions, (2) measure for extended periods
during quiet times to improve the collision frequency estimate and
(3) maximise the chance of success due to cloud cover problems for
ground-based optical observations. Moon free periods are essential
to reduce any optical scattering which can severely affect optical
interferometry.
This experiment was run in February 1999, however, it would be
greatly advantageous to increase the data base. This would help
confirm any results and provide for better consistency.
Contact: Mike Kosch and
Chantal Lathuillere
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Updated by Tony,
Thursday, 05-Aug-99 09:41:00 GMT
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