Return-path: X-Andrew-Authenticated-as: 7997;andrew.cmu.edu;Ted Anderson Received: from beak.andrew.cmu.edu via trymail for +dist+/afs/andrew.cmu.edu/usr1/ota/space/space.dl@andrew.cmu.edu (->+dist+/afs/andrew.cmu.edu/usr1/ota/space/space.dl) (->ota+space.digests) ID ; Thu, 12 Oct 89 03:25:27 -0400 (EDT) Message-ID: Reply-To: space+@Andrew.CMU.EDU From: space-request+@Andrew.CMU.EDU To: space+@Andrew.CMU.EDU Date: Thu, 12 Oct 89 03:24:50 -0400 (EDT) Subject: SPACE Digest V10 #138 SPACE Digest Volume 10 : Issue 138 Today's Topics: STS-34 Press Kit [2 of 3] [Revised] (Forwarded) ---------------------------------------------------------------------- Date: 9 Oct 89 19:20:10 GMT From: trident.arc.nasa.gov!yee@ames.arc.nasa.gov (Peter E. Yee) Subject: STS-34 Press Kit [2 of 3] [Revised] (Forwarded) before reaching Jupiter, Galileo's probe must separate from the orbiter. The spacecraft turns to aim the probe precisely for its entry point in the Jupiter atmosphere, spins up to 10 revolutions per minute and releases the spin-stabilized probe. Then the Galileo orbiter maneuvers again to aim for its own Jupiter encounter and resumes its scientific measurements of the interplanetary environment underway since the launch more than 5 years before. While the probe is still approaching Jupiter, the orbiter will have its first two satellite encounters. After passing within 20,000 miles of Europa, it will fly about 600 miles above Io's volcano-torn surface, twenty times closer than the closest flyby altitude of Voyager in 1979. AT JUPITER The Probe at Jupiter The probe mission has four phases: launch, cruise, coast and entry-descent. During launch and cruise, the probe will be carried by the orbiter and serviced by a common umbilical. The probe will be dormant during cruise except for annual checkouts of spacecraft systems and instruments. During this period, the orbiter will provide the probe with electric power, commands, data transmission and some thermal control. Six hours before entering the atmosphere, the probe will be shooting through space at about 40,000 mph. At this time, its command unit signals "wake up" and instruments begin collecting data on lightning, radio emissions and energetic particles. A few hours later, the probe will slam into Jupiter's atmosphere at 115,000 mph, fast enough to jet from Los Angeles to New York in 90 seconds. Deceleration to about Mach 1 -- the speed of sound -- should take just a few minutes. At maximum deceleration as the craft slows from 115,000 mph to 100 mph, it will be hurtling against a force 350 times Earth's gravity. The incandescent shock wave ahead of the probe will be as bright as the sun and reach searing temperatures of up to 28,000 degrees Fahrenheit. After the aerodynamic braking has slowed the probe, it will drop its heat shields and deploy its parachute. This will allow the probe to float down about 125 miles through the clouds, passing from a pressure of 1/10th that on Earth's surface to about 25 Earth atmospheres. About 4 minutes after probe entry into JupiterUs atmosphere, a pilot chute deploys and explosive nuts shoot off the top section of the probe's protective shell. As the cover whips away, it pulls out and opens the main parachute attached to the inner capsule. What remains of the probe's outer shell, with its massive heat shield, falls away as the parachute slows the instrument module. From there on, suspended from the main parachute, the probe's capsule with its activated instruments floats downward toward the bright clouds below. The probe will pass through the white cirrus clouds of ammonia crystals - the highest cloud deck. Beneath this ammonia layer probably lie reddish-brown clouds of ammonium hydrosulfides. Once past this layer, the probe is expected to reach thick water clouds. This lowest cloud layer may act as a buffer between the uniformly mixed regions below and the turbulent swirl of gases above. Jupiter's atmosphere is primarily hydrogen and helium. For most of its descent through Jupiter's three main cloud layers, the probe will be immersed in gases at or below room temperature. However, it may encounter hurricane winds up to 200 mph and lightning and heavy rain at the base of the water clouds believed to exist on the planet. Eventually, the probe will sink below these clouds, where rising pressure and temperature will destroy it. The probe's active life in Jupiter's atmosphere is expected to be about 75 minutes in length. The probe batteries are not expected to last beyond this point, and the relaying orbiter will move out of reach. To understand this huge gas planet, scientists must find out about its chemical components and the dynamics of its atmosphere. So far, scientific data are limited to a two-dimensional view (pictures of the planet's cloud tops) of a three-dimensional process (Jupiter's weather). But to explore such phenomena as the planet's incredible coloring, the Great Red Spot and the swirling shapes and high-speed motion of its topmost clouds, scientists must penetrate Jupiter's visible surface and investigate the atmosphere concealed in the deep-lying layers below. A set of six scientific instruments on the probe will measure, among other things, the radiation field near Jupiter, the temperature, pressure, density and composition of the planet's atmosphere from its first faint outer traces to the hot, murky hydrogen atmosphere 100 miles below the cloud tops. All of the information will be gathered during the probe's descent on an 8-foot parachute. Probe data will be sent to the Galileo Orbiter 133,000 miles overhead then relayed across the half billion miles to Deep Space Network stations on Earth. To return its science, the probe relay radio aboard the orbiter must automatically acquire the probe signal below within 50 seconds, with a success probability of 99.5 percent. It must reacquire the signal immediately should it become lost. To survive the heat and pressure of entry, the probe spacecraft is composed of two separate units: an inner capsule containing the scientific instruments, encased in a virtually impenetrable outer shell. The probe weighs 750 pounds. The outer shell is almost all heat shield material. The Orbiter at Jupiter After releasing the probe, the orbiter will use its main engine to go into orbit around Jupiter. This orbit, the first of 10 planned, will have a period of about 8 months. A close flyby of Ganymede in July 1996 will shorten the orbit, and each time the Galileo orbiter returns to the inner zone of satellites, it will make a gravity-assist close pass over one or another of the satellites, changing Galileo's orbit while making close observations. These satellite encounters will be at altitudes as close as 125 miles above their surfaces. Throughout the 22-month orbital phase, Galileo will continue observing the planet and the satellites and continue gathering data on the magnetospheric environment. SCIENTIFIC ACTIVITIES Galileo's scientific experiments will be carried out by more than 100 scientists from six nations. Except for the radio science investigation, these are supported by dedicated instruments on the Galileo orbiter and probe. NASA has appointed 15 interdisciplinary scientists whose studies include data from more than one Galileo instrument. The instruments aboard the probe will measure the temperatures and pressure of Jupiter's atmosphere at varying altitudes and determine its chemical composition including major and minor constituents (such as hydrogen, helium, ammonia, methane, and water) and the ratio of hydrogen to helium. Jupiter is thought to have a bulk composition similar to that of the primitive solar nebula from which it was formed. Precise determination of the ratio of hydrogen to helium would provide an important factual check of the Big Bang theory of the genesis of the universe. Other probe experiments will determine the location and structure of Jupiter's clouds, the existence and nature of its lightning, and the amount of heat radiating from the planet compared to the heat absorbed from sunlight. In addition, measurements will be made of Jupiter's numerous radio emissions and of the high-energy particles trapped in the planet's innermost magnetic field. These measurements for Galileo will be made within a distance of 26,000 miles from Jupiter's cloud tops, far closer than the previous closest approach to Jupiter by Pioneer 11. The probe also will determine vertical wind shears using Doppler radio measurements made of probe motions from the radio receiver aboard the orbiter. Jupiter appears to radiate about twice as much energy as it receives from the sun and the resulting convection currents from Jupiter's internal heat source towards its cooler polar regions could explain some of the planet's unusual weather patterns. Jupiter is over 11 times the diameter of Earth and spins about two and one-half times faster -- a jovian day is only 10 hours long. A point on the equator of Jupiter's visible surface races along at 28,000 mph. This rapid spin may account for many of the bizarre circulation patterns observed on the planet. Spacecraft Scientific Activities The Galileo mission and systems were designed to investigate three broad aspects of the Jupiter system: the planet's atmosphere, the satellites and the magnetosphere. The spacecraft is in three segments to focus on these areas: the atmospheric probe; a non-spinning section of the orbiter carrying cameras and other remote sensors; and the spinning main section of the orbiter spacecraft which includes the propulsion module, the communications antennas, main computers and most support systems as well as the fields and particles instruments, which sense and measure the environment directly as the spacecraft flies through it. Probe Scientific Activities The probe will enter the atmosphere about 6 degrees north of the equator. The probe weighs just under 750 pounds and includes a deceleration module to slow and protect the descent module, which carries out the scientific mission. The deceleration module consists of an aeroshell and an aft cover designed to block the heat generated by slowing from the probe's arrival speed of about 115,000 miles per hour to subsonic speed in less than 2 minutes. After the covers are released, the descent module deploys its 8-foot parachute and its instruments, the control and data system, and the radio-relay transmitter go to work. Operating at 128 bits per second, the dual L-band transmitters send nearly identical streams of scientific data to the orbiter. The probe's relay radio aboard the orbiter will have two redundant receivers that process probe science data, plus radio science and engineering data for transmission to the orbiter communications system. Minimum received signal strength is 31 dBm. The receivers also measure signal strength and Doppler shift as part of the experiments for measuring wind speeds and atmospheric absorption of radio signals. Probe electronics are powered by long-life, high-discharge-rate 34-volt lithium batteries, which remain dormant for more than 5 years during the journey to Jupiter. The batteries have an estimated capacity of about 18 amp-hours on arrival at Jupiter. Orbiter Scientific Activities The orbiter, in addition to delivering the probe to Jupiter and relaying probe data to Earth, will support all the scientific investigations of Venus, the Earth and moon, asteroids and the interplanetary medium, Jupiter's satellites and magnetosphere, and observation of the giant planet itself. The orbiter weighs about 5,200 pounds including about 2,400 pounds of rocket propellant to be expended in some 30 relatively small maneuvers during the long gravity-assisted flight to Jupiter, the large thrust maneuver which puts the craft into its Jupiter orbit, and the 30 or so trim maneuvers planned for the satellite tour phase. The retropropulsion module consists of 12 10-newton thrusters, a single 400-newton engine, and the fuel, oxidizer, and pressurizing-gas tanks, tubing, valves and control equipment. (A thrust of 10 newtons would support a weight of about 2.2 pounds at Earth's surface). The propulsion system was developed and built by Messerschmitt-Bolkow-Blohm and provided by the Federal Republic of Germany. The orbiter's maximum communications rate is 134 kilobits per second (the equivalent of about one black-and-white image per minute); there are other data rates, down to 10 bits per second, for transmitting engineering data under poor conditions. The spacecraft transmitters operate at S-band and X-band (2295 and 8415 megahertz) frequencies between Earth and on L-band between the probe. The high-gain antenna is a 16-foot umbrella-like reflector unfurled after the first Earth flyby. Two low-gain antennas (one pointed forward and one aft, both mounted on the spinning section) are provided to support communications during the Earth-Venus-Earth leg of the flight and whenever the main antenna is not deployed and pointed at Earth. The despun section of the orbiter carries a radio relay antenna for receiving the probe's data transmissions. Electrical power is provided to Galileo's equipment by two radioisotope thermoelectric generators. Heat produced by natural radioactive decay of plutonium 238 dioxide is converted to approximately 500 watts of electricity (570 watts at launch, 480 at the end of the mission) to operate the orbiter equipment for its 8-year active period. This is the same type of power source used by the Voyager and Pioneer Jupiter spacecraft in their long outer-planet missions, by the Viking lander spacecraft on Mars and the lunar scientific packages left on the Moon. Most spacecraft are stabilized in flight either by spinning around a major axis or by maintaining a fixed orientation in space, referenced to the sun and another star. Galileo represents a hybrid of these techniques, with a spinning section rotating ordinarily at 3 rpm and a "despun" section which is counter-rotated to provide a fixed orientation for cameras and other remote sensors. Instruments that measure fields and particles, together with the main antenna, the power supply, the propulsion module, most of the computers and control electronics, are mounted on the spinning section. The instruments include magnetometer sensors mounted on a 36-foot boom to escape interference from the spacecraft; a plasma instrument detecting low-energy charged particles and a plasma-wave detector to study waves generated in planetary magnetospheres and by lightning discharges; a high-energy particle detector; and a detector of cosmic and Jovian dust. The despun section carries instruments and other equipment whose operation depends on a fixed orientation in space. The instruments include the camera system; the near-infrared mapping spectrometer to make multispectral images for atmosphere and surface chemical analysis; the ultraviolet spectrometer to study gases and ionized gases; and the photopolarimeter radiometer to measure radiant and reflected energy. The camera system is expected to obtain images of Jupiter's satellites at resolutions from 20 to 1,000 times better than Voyager's best. This section also carries a dish antenna to track the probe in Jupiter's atmosphere and pick up its signals for relay to Earth. The probe is carried on the despun section, and before it is released, the whole spacecraft is spun up briefly to 10 rpm in order to spin-stabilize the probe. The Galileo spacecraft will carry out its complex operations, including maneuvers, scientific observations and communications, in response to stored sequences which are interpreted and executed by various on-board computers. These sequences are sent up to the orbiter periodically through the Deep Space Network in the form of command loads. GROUND SYSTEMS Galileo communicates with Earth via NASA's Deep Space Network (DSN), which has a complex of large antennas with receivers and transmitters located in the California desert, another in Australia and a third in Spain, linked to a network control center at NASAUs Jet Propulsion Laboratory in Pasadena, Calif. The spacecraft receives commands, sends science and engineering data, and is tracked by Doppler and ranging measurements through this network. At JPL, about 275 scientists, engineers and technicians, will be supporting the mission at launch, increasing to nearly 400 for Jupiter operations including support from the German retropropulsion team at their control center in the FGR. Their responsibilities include spacecraft command, interpreting engineering and scientific data from Galileo to understand its performance, and analyzing navigation data from the DSN. The controllers use a set of complex computer programs to help them control the spacecraft and interpret the data. Because the time delay in radio signals from Earth to Jupiter and back is more than an hour, the Galileo spacecraft was designed to operate from programs sent to it in advance and stored in spacecraft memory. A single master sequence program can cover 4 weeks of quiet operations between planetary and satellite encounters. During busy Jupiter operations, one program covers only a few days. Actual spacecraft tasks are carried out by several subsystems and scientific instruments, many of which work from their own computers controlled by the main sequence. Designing these sequences is a complex process balancing the desire to make certain scientific observations with the need to safeguard the spacecraft and mission. The sequence design process itself is supported by software programs, for example, which display to the scientist maps of the instrument coverage on the surface of an approaching satellite for a given spacecraft orientation and trajectory. Notwithstanding these aids, a typical 3-day satellite encounter may take efforts spread over many months to design, check and recheck. The controllers also use software designed to check the command sequence further against flight rules and constraints. The spacecraft regularly reports its status and health through an extensive set of engineering measurements. Interpreting these data into trends and averting or working around equipment failures is a major task for the mission operations team. Conclusions from this activity become an important input, along with scientific plans, to the sequence design process. This too is supported by computer programs written and used in the mission support area. Navigation is the process of estimating, from radio range and Doppler measurements, the position and velocity of the spacecraft to predict its flight path and design course-correcting maneuvers. These calculations must be done with computer support. The Galileo mission, with its complex gravity-assist flight to Jupiter and 10 gravity-assist satellite encounters in the Jovian system, is extremely dependent on consistently accurate navigation. In addition to the programs that directly operate the spacecraft and are periodically transmitted to it, the mission operations team uses software amounting to 650,000 lines of programming code in the sequence design process; 1,615,000 lines in the telemetry interpretation; and 550,000 lines of code in navigation. These must all be written, checked, tested, used in mission simulations and, in many cases, revised before the mission can begin. Science investigators are located at JPL or other university laboratories and linked by computers. From any of these locations, the scientists can be involved in developing the sequences affecting their experiments and, in some cases, in helping to change preplanned sequences to follow up on unexpected discoveries with second looks and confirming observations. JUPITER'S SYSTEM Jupiter is the largest and fastest-spinning planet in the solar system. Its radius is more than 11 times Earth's, and its mass is 318 times that of our planet. Named for the chief of the Roman gods, Jupiter contains more mass than all the other planets combined. It is made mostly of light elements, principally hydrogen and helium. Its atmosphere and clouds are deep and dense, and a significant amount of energy is emitted from its interior. The earliest Earth-based telescopic observations showed bands and spots in Jupiter's atmosphere. One storm system, the Red Spot, has been seen to persist over three centuries. Atmospheric forms and dynamics were observed in increasing detail with the Pioneer and Voyager flyby spacecraft, and Earth-based infrared astronomers have recently studied the nature and vertical dynamics of deeper clouds. Sixteen satellites are known. The four largest, discovered by the Italian scientist Galileo Galilei in 1610, are the size of small planets. The innermost of these, Io, has active sulfurous volcanoes, discovered by Voyager 1 and further observed by Voyager 2 and Earth-based infrared astronomy. Io and Europa are about the size and density of Earth's moon (3 to 4 times the density of water) and probably rocky inside. Ganymede and Callisto, further out from Jupiter, are the size of Mercury but less than twice as dense as water. Their cratered surfaces look icy in Voyager images, and they may be composed partly of ice or water. Of the other satellites, eight (probably captured asteroids) orbit irregularly far from the planet, and four (three discovered by the Voyager mission in 1979) are close to the planet. Voyager also discovered a thin ring system at Jupiter in 1979. Jupiter has the strongest planetary magnetic field known. The resulting magnetosphere is a huge teardrop-shaped, plasma-filled cavity in the solar wind pointing away from the sun. JupiterUs magnetosphere is the largest single entity in our solar system, measuring more than 14 times the diameter of the sun. The inner part of the magnetic field is doughnut- shaped, but farther out it flattens into a disk. The magnetic poles are offset and tilted relative to Jupiter's axis of rotation, so the field appears to wobble with Jupiter's rotation (just under 10 hours), sweeping up and down across the inner satellites and making waves throughout the magnetosphere. WHY JUPITER INVESTIGATIONS ARE IMPORTANT With a thin skin of turbulent winds and brilliant, swift-moving clouds, the huge sphere of Jupiter is a vast sea of liquid hydrogen and helium. Jupiter's composition (about 88 percent hydrogen and 11 percent helium with small amounts of methane, ammonia and water) is thought to resemble the makeup of the solar nebula, the cloud of gas and dust from which the sun and planets formed. Scientists believe Jupiter holds important clues to conditions in the early solar system and the process of planet formation. Jupiter may also provide insights into the formation of the universe itself. Since it resembles the interstellar gas and dust that are thought to have been created in the "Big Bang," studies of Jupiter may help scientists calibrate models of the beginning of the universe. Though starlike in composition, Jupiter is too small to generate temperatures high enough to ignite nuclear fusion, the process that powers the stars. Some scientists believe that the sun and Jupiter began as unequal partners in a binary star system. (If a double star system had developed, it is unlikely life could have arisen in the solar system.) While in a sense a "failed star," Jupiter is almost as large as a planet can be. If it contained more mass, it would not have grown larger, but would have shrunk from compression by its own gravity. If it were 100 times more massive, thermonuclear reactions would ignite, and Jupiter would be a star. For a brief period after its formation, Jupiter was much hotter, more luminous, and about 10 times larger than it is now, scientists believe. Soon after accretion (the condensation of a gas and dust cloud into a planet), its brightness dropped from about one percent of the Sun's to about one billionth -- a decline of ten million times. In its present state Jupiter emits about twice as much heat as it receives from the Sun. The loss of this heat -- residual energy left over from the compressive heat of accretion -- means that Jupiter is cooling and losing energy at a tremendously rapid rate. Temperatures in Jupiter's core, which were about 90,000 degrees Fahrenheit in the planet's hot, early phase, are now about 54,000 degrees Fahrenheit, 100 times hotter than any terrestrial surface, but 500 times cooler than the temperature at the center of the sun. Temperatures on Jupiter now range from 54,000 degrees Fahrenheit at the core to minus 248 degrees Fahrenheit at the top of the cloud banks. Mainly uniform in composition, Jupiter's structure is determined by gradations in temperature and pressure. Deep in Jupiter's interior there is thought to be a small rocky core, comprising about four percent of the planet's mass. This "small" core (about the size of 10 Earths) is surrounded by a 25,000-mile-thick layer of liquid metallic hydrogen. (Metallic hydrogen is liquid, but sufficiently compressed to behave as metal.) Motions of this liquid "metal" are the source of the planet's enormous magnetic field. This field is created by the same dynamo effect found in the metallic cores of Earth and other planets. At the outer limit of the metallic hydrogen layer, pressures equal three million times that of Earth's atmosphere and the temperature has cooled to 19,000 degrees Fahrenheit. Surrounding the central metallic hydrogen region is an outer shell of "liquid" molecular hydrogen. Huge pressures compress Jupiter's gaseous hydrogen until, at this level, it behaves like a liquid. The liquid hydrogen layer extends upward for about 15,000 miles. Then it gradually becomes gaseous. This transition region between liquid and gas marks, in a sense, where the solid and liquid planet ends and its atmosphere begins. From here, Jupiter's atmosphere extends up for 600 more miles, but only in the top 50 miles are found the brilliant bands of clouds for which Jupiter is known. The tops of these bands are colored bright yellow, red and orange from traces of phosphorous and sulfur. Five or six of these bands, counterflowing east and west, encircle the planet in each hemisphere. At one point near Jupiter's equator, east winds of 220 mph blow right next to west winds of 110 mph. At boundaries of these bands, rapid changes in wind speed and direction create large areas of turbulence and shear. These are the same forces that create tornados here on Earth. On Jupiter, these "baroclinic instabilities" are major phenomena, creating chaotic, swirling winds and spiral features such as White Ovals. The brightest cloud banks, known as zones, are believed to be higher, cooler areas where gases are ascending. The darker bands, called belts, are thought to be warmer, cloudier regions of descent. The top cloud layer consists of white cirrus clouds of ammonia crystals, at a pressure six-tenths that of Earth's atmosphere at sea level (.6 bar). Beneath this layer, at a pressure of about two Earth atmospheres (2 bars) and a temperature of near minus 160 degrees Fahrenheit, a reddish-brown cloud of ammonium hydrosulfide is predicted. At a pressure of about 6 bars, there are believed to be clouds of water and ice. However, recent Earth-based spectroscopic studies suggest that there may be less water on Jupiter than expected. While scientists previously believed Jupiter and the sun would have similar proportions of water, recent work indicates there may be 100 times less water on Jupiter than if it had a solar mixture of elements. If this is the case, there may be only a thin layer of water-ice at the 6 bar level. However, Jupiter's cloud structure, except for the highest layer of ammonia crystals, remains uncertain. The height of the lower clouds is still theoretical -- clouds are predicted to lie at the temperature levels where their assumed constituents are expected to condense. The Galileo probe will make the first direct observations of Jupiter's lower atmosphere and clouds, providing crucial information. The forces driving Jupiter's fast-moving winds are not well understood yet. The classical explanation holds that strong currents are created by convection of heat from Jupiter's hot interior to the cooler polar regions, much as winds and ocean currents are driven on Earth, from equator to poles. But temperature differences do not fully explain wind velocities that can reach 265 mph. An alternative theory is that pressure differences, due to changes in the thermodynamic state of hydrogen at high and low temperatures, set up the wind jets. Jupiter's rapid rotation rate is thought to have effects on wind velocity and to produce some of Jupiter's bizarre circulation patterns, including many spiral features. These rotational effects are known as manifestations of the Coriolis force. Coriolis force is what determines the spin direction of weather systems. It basically means that on the surface of a sphere (a planet), a parcel of gas farther from the poles has a higher rotational velocity around the planet than a parcel closer to the poles. As gases then move north or south, interacting parcels with different velocities produce vortices (whirlpools). This may account for some of Jupiter's circular surface features. Jupiter spins faster than any planet in the solar system. Though 11 times Earth's diameter, Jupiter spins more than twice as fast (once in 10 hours), giving gases on the surface extremely high rates of travel -- 22,000 mph at the equator, compared with 1000 mph for air at Earth's equator. Jupiter's rapid spin also causes this gas and liquid planet to flatten markedly at the poles and bulge at the equator. Visible at the top of Jupiter's atmosphere are eye-catching features such as the famous Great Red Spot and the exotic White Ovals, Brown Barges and White Plumes. The Great Red Spot, which is 25,000 miles wide and large enough to swallow three Earths, is an enormous oval eddy of swirling gases. It is driven by two counter-flowing jet streams, which pass, one on each side of it, moving in opposite directions, each with speeds of 100-200 mph. The Great Red Spot was first discovered in 1664, by the British scientist Roger Hook, using Galileo's telescope. In the three centuries since, the huge vortex has remained constant in latitude in Jupiter's southern equatorial belt. Because of its stable position, astronomers once thought it might be a volcano. Another past theory compared the Great Red Spot to a gigantic hurricane. However, the GRS rotates anti-cyclonically while hurricanes are cyclonic features (counterclockwise in the northern hemisphere, clockwise in the southern) -- and the dynamics of the Great Red Spot appear unrelated to moisture. The Great Red Spot most closely resembles an enormous tornado, a huge vortex that sucks in smaller vortices. The Coriolis effect created by Jupiter's fast spin, appears to be the key to the dynamics that drive the spot. The source of the Great Red Spot's color remains a mystery. Many scientists now believe it to be caused by phosphorus, but its spectral line does not quite match that of phosphorus. The GRS may be the largest in a whole array of spiral phenomena with similar dynamics. About a dozen white ovals, circulation patterns resembling the GRS, exist in the southern latitudes of Jupiter and appear to be driven by the same forces. Scientists do not know why these ovals are white. Scientists believe the brown barges, which appear like dark patches on the planet, are holes in the upper clouds, through which the reddish-brown lower cloud layer may be glimpsed. The equatorial plumes, or white plumes, may be a type of wispy cirrus anvil cloud. SPACECRAFT CHARACTERISTICS Orbiter Probe Mass,lbs. 5,242 744 Propellant, lbs. 2,400 none Height (in-flight) 15 feet 34 inches Inflight span 30 feet (w/oboom) Instrument payload 10 instruments 6 instruments Payload mass, lbs. 260 66 Electric power, watts 570-480 730 (RTGs) (Lithium-sulfur battery) GALILEO MANAGEMENT The Galileo Project is managed for NASA's Office of Space Science and Applications by the NASA Jet Propulsion Laboratory, Pasadena, Calif. This responsibility includes designing, building, testing, operating and tracking Galileo. NASA's Ames Research Center, Moffett Field, Calif. is responsible for the atmosphere probe, which was built by Hughes Aircraft Company, El Segundo, Calif. The probe project and science teams will be stationed at Ames during pre-mission, mission operations, and data reduction periods. Team members will be at Jet Propulsion Laboratory for probe entry. The Federal Republic of Germany has furnished the orbiter's retropropulsion module and is participating in the scientific investigations. The radioisotope thermoelectric generators were designed and built for the U.S. Department of Energy by the General Electric Company. GALILEO ORBITER AND PROBE SCIENTIFIC INVESTIGATIONS Listed by experiment/instrument and including the Principal Investigator and scientific objectives of that investigation: PROBE Atmospheric Structure; A. Seiff, NASA's Ames Research Center; temperature, pressure, density, molecular weight profiles; Neutral Mass Spectrometer; H. Niemann, NASA's Goddard Space Flight Center; chemical composition Helium Abundance; U. von Zahn, Bonn University, FRG; helium/hydrogen ratio Nephelometer; B. Ragent, NASA's Ames Research Center; clouds, solid/liquid particles Net Flux Radiometer; L. Sromovsky, University of Wisconsin-Madison; thermal/solar energy profiles Lightning/Energetic Particles; L. Lanzerotti, Bell Laboratories; detect lightning, measuring energetic particles ORBITER (DESPUN PLATFORM) Solid-State Imaging Camera; M. Belton, National Optical Astronomy Observatories (Team Leader); Galilean satellites at 1-km resolution or better Near-Infrared Mapping Spectrometer; R. Carlson, NASA's Jet Propulsion Laboratory; surface/atmospheric composition, thermal mapping Ultraviolet Spectrometer; C. Hord, University of Colorado; atmospheric gases, aerosols Photopolarimeter Radiometer; J. Hansen, Goddard Institute for Space Studies; atmospheric particles, thermal/reflected radiation ORBITER (SPINNING SPACECRAFT SECTION) Magnetometer; M. Kivelson, University of California at Los Angeles; strength and fluctuations of magnetic fields Energetic Particles; D. Williams, Johns Hopkins Applied Physics Laboratory; electrons, protons, heavy ions in magnetosphere and interplanetary space Plasma; L. Frank, University of Iowa; composition, energy, distribution of magnetospheric ions Plasma Wave; D. Gurnett, University of Iowa; electromagnetic waves and wave-particle interactions Dust; E. Grun, Max Planck Institute; mass, velocity, charge of submicron particles Radio Science - Celestial Mechanics; J. Anderson, JPL (Team Leader); masses and motions of bodies from spacecraft tracking; Radio Science - Propagation; H. T. Howard, Stanford University; satellite radii, atmospheric structure both from radio propagation INTERDISCIPLINARY INVESTIGATORS F. P. Fanale; University of Hawaii P. Gierasch; Cornell University D. M. Hunten; University of Arizona A. P. Ingersoll; California Institute of Technology H. Masursky; U. S. Geological Survey D. Morrison; Ames Research Center M. McElroy; Harvard University G. S. Orton; NASA's Jet Propulsion Laboratory T. Owen; State University of New York, Stonybrook J. B. Pollack; NASA's Ames Research Center C. T Russell; University of California at Los Angeles C. Sagan; Cornell University G. Schubert; University of California at Los Angeles J. Van Allen; University of Iowa STS-34 INERTIAL UPPER STAGE (IUS-19) The Inertial Upper Stage (IUS) will again be used with the Space Shuttle, this time to transport NASA's Galileo spacecraft out of Earth's orbit to Jupiter, a 2.5-billion-mile journey. The IUS has been used previously to place three Tracking and Data Relay Satellites in geostationary orbit as well as to inject the Magellan spacecraft into its interplanetary trajectory to Venus. In addition, the IUS has been selected by the agency for the Ulysses solar polar orbit mission. After 2 1/2 years of competition, Boeing Aerospace Co., Seattle, was selected in August 1976 to begin preliminary design of the IUS. The IUS was developed and built under contract to the Air Force Systems Command's Space Systems Division. The Space Systems Division is executive agent for all Department of Defense activities pertaining to the Space Shuttle system. NASA, through the Marshall Space Flight Center, Huntsville, Ala., purchases the IUS through the Air Force and manages the integration activities of the upper stage to NASA spacecraft. Specifications IUS-19, to be used on mission STS-34, is a two-stage vehicle weighing approximately 32,500 lbs. Each stage has a solid rocket motor (SRM), preferred over liquid-fueled engines because of SRM's relative simplicity, high reliability, low cost and safety. The IUS is 17 ft. long and 9.25 ft. in diameter. It consists of an aft skirt, an aft stage SRM generating approximately 42,000 lbs. of thrust, an interstage, a forward-stage SRM generating approximately 18,000 lbs. of thrust, and an equipment support section. Airborne Support Equipment The IUS Airborne Support Equipment (ASE) is the mechanical, avionics and structural equipment located in the orbiter. The ASE supports the IUS and the Galileo in the orbiter payload bay and elevates the combination for final checkout and deployment from the orbiter. The IUS ASE consists of the structure, electromechanical mechanisms, batteries, electronics and cabling to support the Galileo/IUS. These ASE subsystems enable the deployment of the combined vehicle; provide, distribute and/or control electrical power to the IUS and spacecraft; provide plumbing to cool the radioisotope thermoelectric generator (RTG) aboard Galileo; and serve as communication paths between the IUS and/or spacecraft and the orbiter. IUS Structure The IUS structure is capable of supporting loads generated internally and also by the cantilevered spacecraft during orbiter operations and the IUS free flight. It is made of aluminum skin-stringer construction, with longerons and ring frames. Equipment Support Section The top of the equipment support section contains the spacecraft interface mounting ring and electrical interface connector segment for mating and integrating the spacecraft with the IUS. Thermal isolation is provided by a multilayer insulation blanket across the interface between the IUS and Galileo. The equipment support section also contains the avionics which provide guidance, navigation, control, telemetry, command and data management, reaction control and electrical power. All mission-critical components of the avionics system, along with thrust vector actuators, reaction control thrusters, motor igniter and pyrotechnic stage separation equipment are redundant to assure reliability of better than 98 percent. IUS Avionics Subsystems The avionics subsystems consist of the telemetry, tracking and command subsystems; guidance and navigation subsystem; data management; thrust vector control; and electrical power subsystems. These subsystems include all the electronic and electrical hardware used to perform all computations, signal conditioning, data processing and formatting associated with navigation, guidance, control, data and redundancy management. The IUS avionics subsystems also provide the equipment for communications between the orbiter and ground stations as well as electrical power distribution. Attitude control in response to guidance commands is provided by thrust vectoring during powered flight and by reaction control thrusters while coasting. Attitude is compared with guidance commands to generate error signals. During solid motor firing, these commands gimble the IUS's movable nozzle to provide the desired pitch and yaw control. The IUS's roll axis thrusters maintain roll control. While coasting, the error signals are processed in the computer to generate thruster commands to maintain the vehicle's altitude or to maneuver the vehicle. The IUS electrical power subsystem consists of avionics batteries, IUS power distribution units, a power transfer unit, utility batteries, a pyrotechnic switching unit, an IUS wiring harness and umbilical and staging connectors. The IUS avionics system provides 5-volt electrical power to the Galileo/IUS interface connector for use by the spacecraft telemetry system. IUS Solid Rocket Motors The IUS two-stage vehicle uses a large solid rocket motor and a small solid rocket motor. These motors employ movable nozzles for thrust vector control. The nozzles provide up to 4 degrees of steering on the large motor and 7 degrees on the small motor. The large motor is the longest-thrusting duration SRM ever developed for space, with the capability to thrust as long as 150 seconds. Mission requirements and constraints (such as weight) can be met by tailoring the amount of propellant carried. The IUS-19 first-stage motor will carry 21,488 lb. of propellant; the second stage 6,067 lb. Reaction Control System The reaction control system controls the Galileo/IUS spacecraft attitude during coasting, roll control during SRM thrustings, velocity impulses for accurate orbit injection and the final collision-avoidance maneuver after separation from the Galileo spacecraft. As a minimum, the IUS includes one reaction control fuel tank with a capacity of 120 lb. of hydrazine. Production options are available to add a second or third tank. However, IUS-19 will require only one tank. IUS To Spacecraft Interfaces Galileo is physically attached to the IUS at eight attachment points, providing substantial load-carrying capability while minimizing the transfer of heat across the connecting points. Power, command and data transmission between the two are provided by several IUS interface connectors. In addition, the IUS provides a multilayer insulation blanket of aluminized Kapton with polyester net spacers across the Galileo/IUS interface, along with an aluminized Beta cloth outer layer. All IUS thermal blankets are vented toward and into the IUS cavity, which in turn is vented to the orbiter payload bay. There is no gas flow between the spacecraft and the IUS. The thermal blankets are grounded to the IUS structure to prevent electrostatic charge buildup. Flight Sequence After the orbiter payload bay doors are opened in orbit, the orbiter will maintain a preselected attitude to keep the payload within thermal requirements and constraints. On-orbit predeployment checkout begins, followed by an IUS command link check and spacecraft communications command check. Orbiter trim maneuvers are normally performed at this time. Forward payload restraints will be released and the aft frame of the airborne-support equipment will tilt the Galileo/IUS to 29 degrees. This will extend the payload into space just outside the orbiter payload bay, allowing direct communication with Earth during systems checkout. The orbiter then will be maneuvered to the deployment attitude. If a problem has developed within the spacecraft or IUS, the IUS and its payload can be restowed. Prior to deployment, the spacecraft electrical power source will be switched from orbiter power to IUS internal power by the orbiter flight crew. After verifying that the spacecraft is on IUS internal power and that all Galileo/IUS predeployment operations have been successfully completed, a GO/NO-GO decision for deployment will be sent to the crew from ground support. When the orbiter flight crew is given a "Go" decision, they will activate the ordnance that separates the spacecraft's umbilical cables. The crew then will command the electromechanical tilt actuator to raise the tilt table to a 58-degree deployment position. The orbiter's RCS thrusters will be inhibited and an ordnance-separation device initiated to physically separate the IUS/spacecraft combination from the tilt table. Six hours, 20 minutes into the mission, compressed springs provide the force to jettison the IUS/Galileo from the orbiter payload bay at approximately 6 inches per second. The deployment is normally performed in the shadow of the orbiter or in Earth eclipse. The tilt table then will be lowered to minus 6 degrees after IUS and its spacecraft are deployed. A small orbiter maneuver is made to back away from IUS/Galileo. Approximately 15 minutes after deployment, the orbiter's OMS engines will be ignited to move the orbiter away from its released payload. After deployment, the IUS/Galileo is controlled by the IUS onboard computers. Approximately 10 minutes after IUS/Galileo deployment from the orbiter, the IUS onboard computer will send out signals used by the IUS and/or Galileo to begin mission sequence events. This signal will also enable the IUS reaction control system. All subsequent operations will be sequenced by the IUS computer, from transfer orbit injection through spacecraft separation and IUS deactivation. After the RCS has been activated, the IUS will maneuver to the required thermal attitude and perform any required spacecraft thermal control maneuvers. At approximately 45 minutes after deployment from the orbiter, the ------------------------------ End of SPACE Digest V10 #138 *******************