Giotto
The mission
Giotto was the European Space Agency's first interplanetary mission, and was part of the international
armada of spacecraft which made flybys of Comet P/Halley in 1986. Following its encounter with Halley,
the spacecraft was put into hibernation. It was reawoken to make a close approach of Earth in 1990,
which enabled it to make a flyby of Comet Grigg-Skjellerup in July 1992.
The Johnstone Plasma Analyser
The Johnstone Plasma Analyser (JPA) aboard the Giotto spacecraft consisted of an Implanted Ion Sensor
(IIS), Fast Ion Sensor (FIS) and Common Digital Processing Unit (DPU). They were designed to cover the
solar wind and cometary ions during the Halley encounter. The FIS was damaged during that encounter,
and was thus not operating when the spacecraft flew by Grigg-Skjellerup. The instrument development
was headed by the Space Plasma Physics Group of the Mullard Space Science Laboratory. Collaborators
on the project were from The Max-Planck-Institut fuer Aeronomie (Germany), Istituto di Fisica dello
Spazio Interplanetario (Italy), Kiruna Geophysical Institute (Sweden), Southwest Research Intitute (USA)
and the Rutherford-Appleton Laboratory (UK).
The Fast Ion Sensor provided 3D positive ion distribution every 4 seconds in
the energy range 10eV to 20 keV. This instrument was damaged during the Halley
flyby, and was not operational during the Grigg-Skjellerup encounter.
The Implanted Ion Sensor covered cometary pickup ions in 32 energy levels from
86 eV to 86 keV, with a time resolution of 128 seconds (at Grigg-Skjellerup
this provided a 1790km along-track resolution). The instrument had a very high
sensitivity, to detect the low fluxes of cometary ions.
As its name suggests, the IIS is an ion spectrometer whose primary function was
to investigate cometary ions implanted in the solar wind flow. Five sensors in
the IIS covered the angular range of 15degrees to 165degrees in five
equally-spaced 10degree sectors in a plane including the spacecraft spin axis.
As the spacecraft rotated, three-dimensional coverage was provided of the ion
populations. Each of the five sensors consisted of a spherical-section
electrostatic segment analyser (ESA), and a time-of-flight (TOF) analyser.
The mean radius of the ESA sectors is 50mm, their plate spacing is 3mm,
and the energy bandwidth deltaE/E = 10%. The outer plate was held at 0V,
and up to -11kV could be applied to the inner plate. Positive ions were
selected in the ESA according to their E/q. Following selection, the ions were
accelerated by 10kV to pass through a thin carbon foil at the entrance of the
TOF analyser. While passing through the foil, a small amount of energy was
tranferred to secondary electrons that were deflected from the foil onto an MCP
to record the `start' signal. The `stop' detector was an aluminium absorber
which released secondary electrons from its surface layer. The error in
flight-path length caused by coulomb angular scattering of the ions with atoms
in the `start' foil was limited to ~5% by using a spherical concave shape
for the `stop' detector.
The response of the incident ions to a given accelerating potential depends on
q/mass and therefore the selected E/q and the measured time of flight (after
acceleration) over a known path length are combined to give m/q. Counts are
sorted into 5 mass bins using an on-board look-up table. Further pulses cannot
be processed during the 25 microseconds required to process the signals for each
event. The maximum time interval allowed between start and stop signals in 80ns
(after which the event is discounted). Using this coincidence technique, a high
rejection of background signals was given, allowing the relibale measurement of
low densities.
During each spacecraft spin, an entire angular distribution was obtained by the
instrument in one of the 32 logarithmically-spaced energy levels, from 86 eV/q
to 86 keV/q. As the spacecraft rotated every 8 seconds, the entire energy range
was covered by the IIS in 128 seconds.
For more detailed descriptions, see :
The Giotto three-dimensional positive ion analyser, A.D.Johnstone,
J.A.Bowles,
A.J.Coates, A.J.Coker, S.J.Kellock, J.Raymont, B.Wilken, W.Studemann, W.Weiss,
R Cerulli Irelli, V.Formisano,
E.de Giorgi, P.Perani, M. de Bernardi, H.Borg, S.Olsen, J.D.Winningham and
D.A.Bryant , ESA SP-1077, 15-32, 1985.
The Giotto three-dimensional positive ion analyser, A.D.Johnstone,
A.J.Coates, B.Wilken, W.Studemann, W.Weiss, R Cerulli Irelli, V.Formisano,
H.Borg, S.Olsen, J.D.Winningham,D.A.Bryant and S.J.Kellock, J. Phys. E:
Sci. Instrum., 20, pp.795 - 805, 1987.
Overview of Results
Descriptions of the Halley
and Grigg-Skjellerup
encounters are available.
Publications
Click here
for a list of Giotto-related publications by MSSL personnel.
Further Information
The Giotto Mission
Two Giotto pages are located at the NSSDC - an
overview and a
detailed page, containing more information about the mission and other instruments.
An image of Giotto
prior to launch may also be viewed.
Comets
For more information on cometary science, see the
Small Bodies Page and
the Cometary Observations Page at
JPL, the Comet Page at
the Los Alamos National Laboratory, and the
Small Bodies Page
in the Tour of the Nine Planets, which all include images and descriptions
of various comets, including Halley. There is also a
Comet Information Page
at the Royal Greenwich Observatory.
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