The Ulysses Cosmic Ray and Solar Particle
Investigations (COSPIN)
(Adapted from Simpson et al., Astron. & Astrophys., 92, 365-399,
1992)
Summary
The Ulysses spacecraft, launched on 6 October 1990, is the first to undertake
measurements in the heliosphere far from the ecliptic plane and over the polar regions of the
Sun. The instrumentation carried by the spacecraft includes the COSPIN Consortium
Experiment, a group of six charged particle telescopes to measure the energy, composition,
intensity and anisotropy of nucleons in the energy range from ~0.5 MeV/nucleon to ~600
MeV/nucleon for elements in the range H to Ni. Isotopic abundances for nuclei H to Ni are
obtained over a more limited energy range. Electron measurements extend from 4 to
several hundred MeV. One set of telescopes will measure the three-dimensional
anisotropies of protons and helium at low energies. A special high flux telescope provides
measurements of protons and heavier particles ~ 0.2 to ~ 10 MeV/n with high azimuthal
resolution. These instruments were prepared by the international COSPIN consortium to
address a wide range of scientific objectives made possible by a mission to investigate the
Sun and the heliosphere in three dimensions. Their program is called "Cosmic Ray and
Solar Particle Investigation" or COSPIN.
Examples of the COSPIN scientific goals include:
- For energetic charged particles of solar origin, to determine the role of coronal
magnetic fields for their acceleration and propagation and to search for the
origin of 3He- and Fe-rich nuclei;
- Using galactic cosmic radiation measurements, to explore the likely reduction or
elimination of solar modulation in polar regions relative to the equator, to search
for the origin of the anomalous nuclear component and to determine the
nucleosynthetic origins of nuclei at lowest measurable energies;
- For energetic nuclei and electrons of interplanetary origin, to study the three-
dimensional character of traveling shocks, CIRs and their associated charged
particle acceleration, and;
- As a secondary scientific objective at Jupiter encounter (closest approach 8 Feb.
1992), to characterize the energetic charged particle populations during the first
traversal of the dusk side of the Jovian magnetosphere and to search for the
mechanism producing the ~ 10 hour "clock" variation of Jovian electrons in the
interplanetary medium.
Scientific Objectives
Investigations over the past 35 years have shown that the heliosphere is the largest structure
so far directly accessible for spacecraft investigations of the electrodynamical interactions of
plasmas, magnetic fields, and energetic charged particles on astrophysical scales. Studies
made with the Pioneer 10 and 11, and Voyager 1 and 2 spacecraft out to > 50 A.U. have
yielded discoveries vital for understanding phenomena such as collisionless shocks,
charged particle acceleration mechanisms, galactic cosmic ray propagation and the
interactions of the Sun with its environment mediated by the plasmas and magnetic fields in
the solar wind. These phenomena, while studied locally in the heliosphere, are important
in a wide variety of astrophysical settings. A limitation on heliospheric investigations to
date is that observations have so far been available only from ground-based and spacecraft
investigations restricted to the low solar latitudes in and near the ecliptic. Very little has
been established regarding phenomena in the high latitude regions of the heliosphere or
indeed, in the polar regions of the Sun itself, except through remote sensing techniques
such as radio scintillations and the limited observations that can be made of the polar
regions of the sun as a result of the seven degree tilt of the Sun's rotation axis with respect
to the ecliptic.
The Ulysses Mission is the first mission, and the only mission in the foreseeable
future, that will undertake measurements in regions of the heliosphere far from the ecliptic
plane and over the polar regions of the sun. The instrumentation which it carries must be
capable of being both exploratory, with the wide dynamic range of instrument response
required to encompass unexpected phenomena and, simultaneously, definitive, with the
sophistication and resolution necessary to completely characterize whatever phenomena are
discovered.
For these investigations the galactic cosmic radiation, the anomalous nuclear
component, the galactic and jovian electron components, and the solar flare accelerated high
energy particles are important charged particle test "probes" of large scale heliospheric
phenomena and their changes with time. The measurement of a wide range of charged
particle properties, including energies, anisotropies, spectra, and the chemical and isotopic
composition of nucleons reveals specific acceleration mechanisms, propagation modes,
and small scale transient phenomena, and provides information important for astrophysics
beyond the solar system as well. These measurements, provided by the Cosmic Ray and
Solar Particle Investigation (COSPIN), have a central role in achieving the scientific goals
of the Ulysses Mission. For example, the COSPIN will measure at low energies (e.g., ~ 1
MeV) the acceleration of charged particles from solar flares, radial and corotating
interplanetary shocks and, at higher energies (e.g., ~1 GeV), the modulation of the galactic
cosmic ray spectrum resulting from large scale interplanetary dynamical phenomena. Thus,
the primary experimental goals of the COSPIN are to address fundamental astrophysical
questions concerning solar, heliospheric and galactic phenomena in the hitherto unexplored
high latitude regions of the Sun and heliosphere.
With Ulysses plasma and magnetic field measurements, and in collaborative
investigations with Pioneer-10, Voyager-1, and Voyager-2 in the distant heliosphere, we
expect to be able to deduce the large scale, three-dimensional structure of the heliosphere
and to investigate its changes with solar cycle activity.
Since Ulysses will reach its maximum latitude when the ~ 11 year solar cycle
approaches a minimum, the modulation of cosmic rays will also be near a minimum. Thus,
depending upon the topology of the heliospheric magnetic fields over the solar polar
regions, we may have access to a lower energy portion of the interstellar spectrum than
would be possible at low latitudes.
The following are some of the specific scientific goals of the COSPIN investigators
for the Ulysses Mission during 1990-1996.
From the measurement of charged particles of solar origin we shall study their energy
spectra, elemental and isotopic composition and anisotropy during propagation to high
heliospheric latitudes to determine:
- The role of coronal magnetic fields for the storage and propagation of
solar flare accelerated nuclei and electrons;
- The origin of the enrichment of 3He and Fe-rich nuclei in solar flares;
- The importance of emission of energetic particles from regions other than
solar flares.
For the galactic cosmic ray investigations we shall:
- Explore the likely reduction in solar modulation near solar minimum over
the solar polar regions to deduce the interstellar galactic cosmic ray spectra
at low energies both for nucleons and electrons, and to determine the
abundances of electron-capture isotopes.
- Investigate the propagation of positively charged nuclei and the electrons
over polar and equatorial regions during the period when nucleons are
predicted to gradient drift from over the polar regions to the inner
heliosphere. This would provide a test of the importance of the 22 year
solar polar magnetic field reversal cycle for cosmic ray modulation.
- Based on latitudinal variations in the anomalous nuclear component fluxes and spectra, search for evidence that these components may be accelerated at a terminal shock over the heliospheric
polar regions;
- Measure the elemental and isotopic abundances of the galactic cosmic rays
from H to Ni down to the lowest energies determined by either:
- i) residual modulation if significant transverse magnetic field
irregularities exist at polar latitudes, or;
- ii) instrumental response thresholds if the field lines are open to the
interstellar medium so that residual modulation is unimportant;
- e) From the results on the cosmic ray abundances attempt to derive the nucleosynthetic origin of the low
energy interstellar cosmic radiation.
With regard to the acceleration or modulation of charged particles in the interplanetary
medium, we intend to:
- Study the latitudinal extent and three-dimensional character of
interplanetary shocks which accelerate charged particles and modulate
(e.g., by Forbush decreases) the galactic cosmic rays and the anomalous
nuclear component;
- Establish the latitudinal gradients of nucleons and electrons during the
solar magnetic cycle prevailing in 1992-1996;
- Measure the distribution of Jovian electrons as probes of heliospheric
magnetic fields at high solar latitudes.
During the Ulysses encounter with Jupiter (closest approach, 8 February 1992) our
magnetospheric studies will include:
- The first traversal of the dusk side of the Jovian magnetosphere;
- A search for the mechanism producing the ~10 hour "clock" variation of
the Jovian relativistic electron spectra both in the magnetosphere and in
interplanetary space.
- Measurements of the intensities, spectra, anisotropies, and composition of
the trapped radiation.
The COSPIN Measurements
To achieve the scientific goals discussed above, a degree of flexibility is needed from the
instrumentation which can only be realized by employing a variety of sensor designs. A set
of five telescope subsystems are combined within the COSPIN experiment to cover the
charged-particle flux wide energy and nuclear charge intervals.
Each COSPIN sensor is designed to address a different range of the measurements
required to characterize the cosmic rays and other energetic charged particles in the high
latitude regions of the heliosphere.
- The High-Energy Telescope (HET) will make spectral
and chemical-abundance measurements of all elements from H to Ni over an energy range
of ~ 14-600 MeV/nucleon depending on nuclear charge, and isotopic measurements from H
to Ni over a more limited energy range.
- The Low-Energy Telescope (LET) will provide
spectral and chemical-abundance measurements over the charge range Z = 1-26, to carry
the chemical composition downward in energy to 1.8 MeV for protons and ~3
MeV/nucleon for particles with Z > 5.
- The twin Anisotropy Telescopes (ATs) will measure
the three-dimensional anisotropies of protons and alpha particles in the energy range 0.8 to
6 MeV/nucleon.
- The High-Flux Telescope (HFT) will provide measurements of protons
and heavier particles with high immunity to electron contamination under high flux
conditions and with high azimuthal resolution.
- The Kiel Electron Telescope (KET) is designed
to measure electron fluxes between 4 and 2000 MeV and to determine energy spectra in the
range 12-150 MeV. It will also provide proton and alpha-particle measurements over a
wide energy range.
- A Digital Processing Unit (DPU) combines the data from all sensor
subsystems into a COSPIN data format and transmits them after suitable processing into
the spacecraft telemetry stream.
- Two power converters, each capable of supporting the full COSPIN instrumentation, complete the COSPIN package.
The development of the instrumentation concepts extended from 1975 to 1978 The
instrumentation was designed, built and tested for space flight for the initially-planned STS
launch by NASA in 1983. Because of the long duration of the Ulysses Mission, care has
gone into the design of COSPIN to assure reliability and the ability to survive, to the
maximum extent possible, failures in individual subsystems. A basic ground rule is that no
single failure in any subsystem should result in complete loss of useful data from COSPIN.
Thus, certain critical subsystems, such as the low voltage power converter and the central
DPU, have been made completely redundant. The other subsystems have been designed to
be isolated from each other so that a failure in one would cause a loss of data only from that
subsystem.
The complete COSPIN instrumentation is packaged in five units mounted separately on the
spacecraft platform and interconnected with one interface to the spacecraft. Within the
Ulysses ESA and NASA Project nomenclature the five units are referred to as SIM-1, SIM-
2, etc.
A tungsten shield protects the HET telescope from the intense gamma-radiation of the spacecraft
Radio-isotope Thermal Generator (RTG) to minimize background in key data channels.
Many of the studies to be undertaken by the Ulysses mission in general and the
COSPIN investigation in particular are greatly strengthened by the availability of
comparable measurements from a stationary point in the heliosphere to permit separation of
spatial from temporal variations, and to provide a baseline against which spatial variations
may be measured. A 1 A.U. baseline for the Ulysses measurements is provided by
instruments on the IMP-8 satellite which provide measurements of interplanetary
charged particles, the solar wind, and magnetic fields .