[Contents]
[Index]
[Search]
[Home]
1999 Incoherent Scatter Coordinated Observation Days
URSI-ISWG
[Note: If your browser does not support tables, try this
version.]
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 1400UT
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.
1999 Incoherent Scatter Coordinated Observation Days |
| Month |
Dates |
Day |
Length |
NewMoon |
Notes |
| January |
12-13 |
Tuesday |
1 |
17 |
- Hi-TRAC (note 1)/DataBase (note 2)
|
| February |
09-12 |
Tuesday |
3 |
16 |
- Global Ionosphere-Thermosphere
Coupling Study (note 3)
|
| March |
02-12 |
(Monday default) |
4, floating default 08-12 |
17 |
- Joint Observations of
Effects of Storms in Lower Thermosphere
Project (note 4)
- 4 day observations within 10-day 'alert' interval
- Final date selection by
Foster
|
| April |
20-22 |
Tuesday |
2 |
16 |
- WLS (note 5)/UARC/TERRIERS
|
| May |
|
|
|
15 |
|
| June |
|
|
|
13 |
|
| July |
06-08 |
Tuesday |
3 |
13 |
- Global ionospheric convection (note 6)
- Mid-July Baseline (note 7)
|
| August |
|
|
|
11 |
|
| September |
06-24 |
(Tuesday default) |
3, floating default 7-9 |
09 |
- 3 day floating WLS (note 5) and First
S-RAMP Space Weather Campaign (note 8)
observations within month-long 'alert' interval
- Final date selection by
Foster
- Note changed month!
|
| October |
12-14 |
Tuesday |
3 |
09 |
- LTCS (note 7)
- Note changed month!
|
| October |
08-09 |
Friday |
1 |
09 |
|
| November |
|
|
|
08 |
|
| December |
14-15 |
Tuesday |
1 |
07 |
|
| Total |
|
|
21 |
|
|
| Last updated: Friday, 12-Mar-99 14:15:51 GMT |
Notes
- 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.
(John Holt)
- Database: The emphasis should be on broad latitudinal coverage of the
F region.
(Tony van Eyken)
- 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. Adititional, optical, thermospheric
and neutral wind and temperature measurements would be an advantage.
(Mike Kosch and
Chantal Lathuillere)
- Joint Observations of Effects of Storms in the lower thermosphere
Measurements of E- and F-region plasma temperatures, densities and
ion drifts, with emphasis on derived neutral temperatures and winds in the
lower thermosphere (90-150 km), during an intense geomagnetic disturbance.
A time window for the
observations will be identified (March 1999 preferred), and will be
narrowed down to a four or five day period of ISR measurements upon alert
of a major magnetic storm (Kp>7). ISRs are to be run in a local coverage
mode with high resolution in altitude and time similar to recent LTCS
campaigns. Supporting data from optical, MF/MW radar and lidar available
at each ISR site are to be obtained to investigate coupling effects in
various altitude regions. The requested experiment is planned as a pilot
project for CEDAR-TIMED investigations of the effects of geomagnetic
storms on the lower thermosphere structure and dynamics. We envisage
a coordinated effort to alert ISR multi-instrument sites regarding the
occurrence of the storm and the need to initiate observations.
(Joe Salah)
- 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.
(John Foster)
- Global ionospheric convection
All radars concentrate on ionospheric electric field measurements,
preferably in the magnetic field aligned position. 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. Initial
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.
(Kosch and Levitin)
- 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.
(Michael Buonsanto,
Cassendra Fessen)
- First S-RAMP Space Weather Campaign
The objective of this campaign is to study the effects of space weather
disturbances on the coupled magnetosphere-ionosphere-thermosphere system on
a global scale including the impacts on technological systems such as
electric power grids, satellites, and ground or space based communication
and navigation systems. In order to better understand the physical
processes, as well as to provide a quantitative assessment of the effects on
technological systems, the campaign will also include observations from
other global arrays of radio, optical and magnetic instruments.
(Sunanda Basu)
- 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.
(Phil Erickson)
Updated 25 January 1999.