Helios (spacecraft)
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![]() Prototype of theHeliosspacecraft | |
Mission type | Solar observation |
---|---|
Operator | |
COSPAR ID | Helios-A:1974-097A Helios-B:1976-003A |
SATCATno. | Helios-A:7567 Helios-B:8582 |
Website | Helios-A:[1] Helios-B:[2] |
Mission duration | Helios-A:10 years, 1 month, 2 days Helios-B:3 years, 5 months, 2 days |
Spacecraft properties | |
Manufacturer | MBB |
Launch mass | Helios-A:371.2 kg (818 lb) Helios-B:374 kg (825 lb) |
Power | 270 watts (solar array) |
Start of mission | |
Launch date | Helios-A:December 10, 1974, 07:11:01[1] Helios-B:January 15, 1976, 05:34:00 UTC[2] | UTC
Rocket | Titan IIIE/Centaur |
Launch site | Cape CanaveralSLC-41 |
Entered service | Helios-A:January 16, 1975 Helios-B:July 21, 1976 |
End of mission | |
Deactivated | Helios-A:February 18, 1985 Helios-B:December 23, 1979 |
Last contact | Helios-A:February 10, 1986 Helios-B:March 3, 1980 |
Orbital parameters | |
Reference system | Heliocentric |
Eccentricity | Helios-A:0.5218 Helios-B:0.5456 |
Perihelion altitude | Helios-A:0.31 AU Helios-B:0.29 AU |
Aphelion altitude | Helios-A:0.99 AU Helios-B:0.98 AU |
Inclination | Helios-A:0.02° Helios-B:0° |
Period | Helios-A:190.15 days Helios-B:185.6 days |
Epoch | Helios-A:January 15, 1975, 19:00 UTC[1] Helios-B:July 20, 1976, 20:00 UTC[2] |
Helios-AandHelios-B(after launch renamedHelios 1andHelios 2) are a pair ofprobesthat were launched intoheliocentric orbitto studysolarprocesses. As a joint venture betweenGerman Aerospace Center(DLR) andNASA,the probes were launched fromCape Canaveral Air Force Station,Florida,on December10, 1974, and January15, 1976, respectively.
The Helios project set a maximum speed record for spacecraft of 252,792 km/h (157,078 mph; 70,220 m/s).[3]Helios-Bperformed the closest flyby of theSunof any spacecraft until that time. The probes are no longer functional, but as of 2024 remain inelliptical orbitsaround the Sun.
Construction
[edit]The Helios project was a joint venture ofWest Germany's space agency DLR (70 percent share) and NASA (30 percent share). As built by the main contractor,Messerschmitt-Bölkow-Blohm,they were the first space probes built outside the United States and theSoviet Unionto leave Earth orbit.[citation needed]
Structure
[edit]The twoHeliosprobes look similar.Helios-Ahas a mass of 370 kilograms (820 lb), andHelios-Bhas a mass of 376.5 kilograms (830 lb). Their scientific payloads have a mass of 73.2 kilograms (161 lb) onHelios-Aand 76.5 kilograms (169 lb) onHelios-B.The central bodies are sixteen-sided prisms 1.75 metres (5 ft 9 in) in diameter and 0.55 metres (1 ft 10 in) high. Most of the equipment and instrumentation is mounted in this central body. The exceptions are the masts and antennae used during experiments and small telescopes that measure thezodiacal lightand emerge from the central body. Two conical solar panels extend above and below the central body, giving the assembly the appearance of adiaboloor spool of thread.
At launch, each probe was 2.12 metres (6 ft 11 in) tall with a maximum diameter of 2.77 metres (9 ft 1 in). Once in orbit, the telecommunications antennae unfolded on top of the probes and increased the heights to 4.2 metres (14 ft). Also deployed were two rigid booms carrying sensors and magnetometers, attached on both sides of the central bodies, and two flexible antennae used for the detection of radio waves, which extended perpendicular to the axes of the spacecraft for a design length of 16 metres (52 ft) each.[4]
The spacecraft spin around their axes, which are perpendicular to theecliptic,at 60rpm.
Systems
[edit]Power
[edit]Electrical poweris provided bysolar cellsattached to the two truncated cones. To keep the solar panels at a temperature below 165 °C (329 °F) when in proximity to the Sun, the solar cells are interspersed with mirrors, covering 50% of the surface and reflecting part of the incident sunlight while dissipating the excess heat. The power supplied by the solar panels is a minimum of 240wattswhen the probe is ataphelion.Its voltage is regulated to 28voltsDC.Silver-zinc batteries were used only during launch.
Thermal control
[edit]![](https://upload.wikimedia.org/wikipedia/commons/thumb/6/6f/Helios_-_launch_configuration_diagram.png/180px-Helios_-_launch_configuration_diagram.png)
The biggest technical challenge was to avoid heating during orbit while close to the Sun. At 0.3 astronomical units (45,000,000 km; 28,000,000 mi) from the Sun, approximate heat flow is 11solar constants,(11 times the amount ofsolar irradiancereceived while in Earth orbit), or 22.4kWper exposed square meter. At that distance, the probe could reach 370 °C (698 °F).
Thesolar cells,and the central compartment of instruments had to be maintained at much lower temperatures. The solar cells could not exceed 165 °C (329 °F), while the central compartment had to be maintained between −10 and 20 °C (14 and 68 °F). These restrictions required the rejection of 96 percent of the energy received from the Sun. The conical shape of the solar panels was decided on to reduce heating. Tilting the solar panels with respect to sunlight arriving perpendicularly to the axis of the probe, reflects a greater proportion of thesolar radiation."Second surface mirrors" specially developed byNASAcover the entire central body and 50 percent of the solar generators. These are made of fused quartz, with a silver film on the inner face, which is itself covered with a dielectric material. For additional protection,multi-layer insulation– consisting of 18 layers of 0.25 millimetres (0.0098 in)MylarorKapton(depending on location), held apart from each other by small plastic pins intended to prevent the formation ofthermal bridges– was used to partially cover the core compartment. In addition to these passive devices, the probes used an active system of movable louvers arranged in a shutter-like pattern along the bottom and top side of the compartment. The opening thereof is controlled separately by a bimetal spring whose length varies with temperature and causes the opening or closing of the shutter. Resistors were also used to help maintain a temperature sufficient for certain equipment.[5]
Telecommunications system
[edit]The telecommunication system uses a radio transceiver, whose power could be adjusted to between 0.5 and 20 watts. Three antennas are mounted on top of each probe. A high-gain antenna (23dB) of 11° beam width, a medium-gain antenna (3 dB for transmission and 6.3 dB for reception) emits a signal in all directions of the ecliptic plane at the height of 15°, and a low-gain dipole antenna (0.3 dB transmission and 0.8 dB for reception). To be directed continuously towardEarth,the high-gain antenna is rotated by a motor at a speed that counterbalances the spin of the probe. Synchronizing the rotation speed is performed using data supplied by aSun sensor.The maximum data rate obtained with the large antenna gain was 4096 bits per second upstream. The reception and transmission of signals were supported by theDeep Space Networkantennas on Earth.
Altitude control
[edit]![](https://upload.wikimedia.org/wikipedia/commons/thumb/6/67/Helios_-_testing.png/170px-Helios_-_testing.png)
To maintain orientation during the mission, the spacecraftrotated continuously at 60 RPM around its main axis.The orientation control system manages the speed and orientation of the probe's shafts. To determine its orientation, Helios used a crudeSun sensor.Guidance corrections were performed using cold gas thrusters (7.7 kgnitrogen) with a boost of 1Newton.The axis of the probe was permanently maintained keeping it both perpendicular to the direction of the Sun and to the ecliptic plane.
On-board computer and data storage
[edit]The onboard controllers were capable of handling 256 commands. The mass memory could store 500kb,(this was a very large memory for space probes of the time), and was mainly used when the probes were insuperior conjunctionrelative to theEarth(i.e. the Sun comes between the Earth and the spacecraft). A conjunction could last up to 65 days.
Mission profile
[edit]Helios-AandHelios-Bwere launched on December 10, 1974, and January 15, 1976, respectively.Helios-Bflew 3,000,000 kilometres (1,900,000 mi) closer to the Sun thanHelios-A,achievingperihelionon April17, 1976, at a record distance of 43.432 million km (26,987,000 mi; 0.29032 AU),[6]closer than the orbit ofMercury.Helios-Bwas sent into orbit 13 months after the launch ofHelios-A.Helios-Bperformed the closest flyby of theSunof any spacecraft untilParker Solar Probein 2018, 0.29 AU (43.432 million km) from the Sun.[6]
The Helios space probes completed their primary missions by the early 1980s, but continued to send data until 1985.
Scientific instruments and investigations
[edit]BothHeliosprobes had ten scientific instruments[7]and two passive science investigations using the spacecraft telecommuniction system and the spacecraft orbit.
Plasma experiment investigation
[edit]Measures the velocity and distribution ofsolar windplasma. Developed by theMax Planck Institute for Aeronomyfor the study of low-energy particles. Data collected included the density, speed, and temperature of the solar wind. Measurements were taken every minute, with the exception of flux density, which occurred every 0.1 seconds to highlight irregularities in plasma waves. Instruments used included:[8]
- Electron detector
- Detector for protons and heavy particles
- An analyzer for protons and alpha particles with energies between 231eV and 16,000eV
![](https://upload.wikimedia.org/wikipedia/commons/thumb/6/6a/Helios_-_helios2.gif/170px-Helios_-_helios2.gif)
Flux-gate magnetometer
[edit]Theflux-gate magnetometermeasures the field strength and direction of low frequency magnetic fields in the Sun's environment. It was developed by theUniversity of Braunschweig,Germany. It measures three-vector components of solar wind and its magnetic field with high precision. The intensity is measured with an accuracy to within 0.4nTwhen below 102.4nT, and within 1.2nT at intensities below 409.6nT. Two sample rates are available: search every two seconds or eight readings per second.[9]
Flux-gate magnetometer 2
[edit]Measures variations of the field strength and direction of low frequency magnetic fields in the Sol environment. Developed by theGoddard Space Flight Centerof NASA; measures variations of the three-vector components of solar wind and its magnetic field with an accuracy to within 0.1nT at about 25nT, within 0.3nT at about 75nT, and within 0.9nT at an intensity of 225nT.[10]
Search coil magnetometer
[edit]Thesearch coil magnetometercomplements the flux-gate magnetometer by measuring the magnetic fields between 0 and 3 kHz. Also developed by the University of Braunschweig, it detects fluctuations in themagnetic fieldin the 5Hz to 3000Hz range. Thespectral resolutionis performed on the probe's rotation axis.[11]
Plasma wave investigation
[edit]The Plasma Wave Investigation developed by theUniversity of Iowauses two 15 m antennas forming an electric dipole for the study of electrostatic and electromagnetic waves in the solar wind plasma in frequencies between 10 Hz and 3 MHz.[12][13][14]
Cosmic radiation investigation
[edit]The Cosmic Radiation Investigation developed by theUniversity of Kielsought to determine the intensity, direction, and energy of the protons and heavy constituent particles in radiation to determine the distribution of cosmic rays. The three detectors (semiconductor detector,scintillation counter,andCherenkov detector) were encapsulated in an anti-coincidence detector.[15]
Cosmic ray instrument
[edit]The Cosmic Ray Instrument developed at theGoddard Space Flight Centermeasures the characteristics of protons with energies between 0.1 and 800MeVand electrons with energies between 0.05 and 5MeV. It uses three telescopes, which cover the ecliptic plane. A proportional counter studies theX-raysfrom the Sun.[16]
Low energy electron and proton spectrometer
[edit]Developed by theMax Planck Institute for Aeronomy,the low energy electron and proton spectrometer uses spectrometers to measure particle characteristics (protons) with energies between 20 keV and 2 MeV and electrons and positrons with an energy between 80 keV and 1 MeV.[17]
Zodiacal light photometer
[edit]TheZodiacal light instrumentincludes threephotometersdeveloped by theMax Planck Institute for Astronomyto measure the intensity and polarization of the zodiac light in white light and in the 550nm and 400 nm wavelength bands, using three telescopes whose optical axes form angles of 15, 30, and 90° to the ecliptic. From these observations, information is obtained about the spatial distribution of interplanetary dust and the size and nature of the dust particles.[18]
![](https://upload.wikimedia.org/wikipedia/commons/thumb/a/a1/Helios_spacecraft_2.jpg/170px-Helios_spacecraft_2.jpg)
Micrometeoroid analyzer
[edit]TheMicrometeoroid analyzerdeveloped by theMax Planck Institute for Nuclear Physicsis capable of detectingcosmic dustparticles if their mass is greater than 10−15g. It can determine the mass and energy of a micro-meteorite greater than 10−14g. These measurements are made by exploiting the fact that micrometeorites vaporize and ionize when they hit a target. The instrument separates the ions and electrons in the plasma generated by the impacts, and measures the mass and energy of the incident particle. A low-resolutionmass spectrometerdetermines the composition of impacting cosmic dust particles with a mass greater than 10−13g.[19][20]
Celestial mechanic experiment
[edit]The Celestial Mechanic Experiment developed by theUniversity of Hamburguses theHeliosorbit specifics to clarify astronomical measurements: flattening of the Sun; verification of predictedgeneral relativityeffects; determining the mass of the planetMercury;the Earth–Moon mass ratio; and the integrated electron density between the Helios spacecraft and the data receivig station on Earth.[21]
Coronal sounding experiment
[edit]The Coronal Sounding Experiment developed by theUniversity of Bonnmeasures the rotation (Faraday effect) of the linear polarized radio beam from the spacecraft when it passes during opposition through the corona of the Sun. This rotation is a measure of the density of electrons and the intensity of the magnetic field in the traversed region.[22]
Mission specifications
[edit]Helios-A
[edit]Helios-Awas launched on December 10, 1974, fromCape Canaveral Air Force Station Launch Complex 41inCape Canaveral, Florida.[23]This was the first operational flight of theTitan IIIErocket. The rocket'stest flighthad failed when the engine on the upperCentaur stagedid not light, but the launch ofHelios-Awas uneventful.
The probe was placed in a heliocentric orbit of 192 days with a perihelion of 46,500,000 km (28,900,000 mi; 0.311 AU) from the Sun. Several problems affected operations. One of the two antennas did not deploy correctly, reducing the sensitivity of the radio plasma apparatus to low-frequency waves. When the high-gain antenna was connected, the mission team realized that their emissions interfered with the analyzer particles and the radio receiver. To reduce the interference, communications were carried out using reduced power, but this required using the large diameter terrestrial receivers already in place thanks to other space missions in progress.[24]
During the firstperihelionin late February 1975, the spacecraft came closer to the Sun than any previous spacecraft. The temperature of some components reached more than 100 °C (212 °F), while the solar panels reached 127 °C (261 °F), without affecting probe operations. During the second pass on September 21, however, temperatures reached 132 °C (270 °F), which affected the operation of certain instruments.
Helios-B
[edit]![A Titan 3E rocket sitting on its launch pad at Cape Canaveral Air Force Station.](https://upload.wikimedia.org/wikipedia/commons/thumb/b/bf/Titan_3E_Centaur_with_Helios_1.jpg/170px-Titan_3E_Centaur_with_Helios_1.jpg)
BeforeHelios-Bwas launched, some modifications were made to the spacecraft based on lessons learned from the operations ofHelios-A.The small engines used for attitude control were improved. Changes were made to the implementation mechanism of the flexible antenna and high gain antenna emissions. TheX-raydetectors were improved so that they could detectgamma ray bursts,allowing them to be used in conjunction with Earth-orbiting satellites to triangulate the location of the bursts. As temperatures onHelios-Awere always greater than 20 °C (36 °F) below the design maximum at perihelion, it was decided thatHelios-Bwould orbit even closer to the Sun, and the thermal insulation was enhanced to allow the satellite to resist 15 percent higher temperatures.
Tight schedule constraints pressed on theHelios-Blaunch in early 1976. Facilities damaged during the launch of theViking 2spacecraft in September 1975 had to be repaired, while theVikinglanding onMarsin summer 1976 made the Deep Space Network antennas thatHelios-Bneeded to conduct its science while at perihelion unavailable.
Helios-Bwas launched on January 10, 1976, using a Titan IIIE rocket. The probe was placed in an orbit with a 187-day period and a perihelion of 43,500,000 km (27,000,000 mi; 0.291 AU). The orientation ofHelios-Bwith respect to the ecliptic was reversed 180 degrees compared toHelios-Aso that the micrometeorite detectors could have 360 degree coverage. On April 17, 1976,Helios-Bmade its closest pass of the Sun at a record heliocentric speed of 70 kilometres per second (250,000 km/h; 160,000 mph). The maximum recorded temperature was 20 °C (36 °F) higher than measured byHelios-A.
End of operations
[edit]The primary mission of each probe spanned 18 months, but they operated much longer. On March3, 1980, four years after its launch, the radio transceiver onHelios-Bfailed. On January7, 1981, a stop command was sent to prevent possible radio interference during future missions.Helios-Acontinued to function normally, but with the large-diameter DSN antennae not available, data was collected by small diameter antennae at a lower rate. By its 14th orbit,Helios-A's degraded solar cells could no longer provide enough power for the simultaneous collection and transmission of data unless the probe was close to its perihelion. In 1984, the main and backup radio receivers failed, indicating that the high-gain antenna was no longer pointed towards Earth. The lasttelemetrydata was received on February10, 1986.[25]
Mission results
[edit]![](https://upload.wikimedia.org/wikipedia/commons/thumb/1/1c/Helios_-_Trajectory.png/280px-Helios_-_Trajectory.png)
Both probes collected important data about solar wind processes and the particles that make up the interplanetary medium andcosmic rays.These observations were made over a period fromsolar minimumin 1976 to asolar maximumin the early 1980s.
The observation of the zodiacal light established some of the properties ofinterplanetary dustpresent between 0.1 and 1 AU from the Sun, such as their spatial distribution, color andpolarization.The amount of dust was observed to be 10 times that around the Earth.Heterogeneousdistribution was generally expected due to the passage of comets, but observations have not confirmed this.[citation needed]
Helioscollected data about comets, observing the passage ofC/1975 V1 (West)in 1976,C/1978 H1(Meir) in November 1978 andC/1979 Y1(Bradfield) in February 1980. During the last event, probe detected disturbances in solar wind later explained by a break in the comet's tail. The plasma analyzer showed that the acceleration phenomena of the high-speed solar wind were associated with the presence of coronal holes. This instrument also detected, for the first time, helium ions isolated in the solar wind. In 1981, during the peak of solar activity, the data collected byHelios-Aat a short distance from the Sun helped to complete visual observations of coronal mass ejections performed from the Earth's orbit. Data collected byHeliosmagnetometers supplemented data collected byPioneerandVoyagerand were used to determine the direction of the magnetic field at staggered distances from the Sun.
The radio and plasma wave detectors were used to detect radio explosions and shock waves associated with solar flares, usually during solar maximum. The cosmic ray detectors studied how the Sun and interplanetary medium influenced the spread of the same rays, of solar or galactic origin. The cosmic ray gradient, as a function of distance from the Sun, was measured. These observations, combined with those made byPioneer11between 1977 and 1980 in a distance of 12–23AU from the Sun produced a good model of thisgradient.Some features of the inner solar corona were measured during occultations. For this purpose, either a radio signal was sent from the spacecraft to Earth or the ground station sent a signal that was returned by the probe. Changes in signal propagation resulting from the solar corona crossing provided information on density fluctuations.
As of 2020, the probes are no longer functional, but remain in orbit around the Sun.[26][27][1][28]
See also
[edit]References
[edit]- ^abcNASA Space Science Data Coordinated Archive.Note that there is no "Epoch end" date given, which is NASA's way of saying it is still in orbit.
- ^ab"Helios-B – Trajectory Details".National Space Science Data Center.NASA.RetrievedJuly 12,2017.
- ^Wilkinson, John (2012),New Eyes on the Sun: A Guide to Satellite Images and Amateur Observation,Astronomers' Universe Series, Springer, p. 37,Bibcode:2012nesg.book.....W,ISBN978-3-642-22838-4
- ^Helios.Bernd Leitenberger. Retrieved May 20, 2016.
- ^Sandscheper, Günter (December 26, 1974)."The trip to hot space".New Scientist.64(929): 918.[permanent dead link]
- ^ab"Solar System Exploration: Missions: By Target: Our Solar System: Past: Helios 2".Archived fromthe originalon October 5, 2008.RetrievedNovember 1,2009.
- ^"Tracking and Data Systems Support for the Helios Project"(PDF).NASA Jet Propulsion Laboratory.RetrievedMay 20,2016.
- ^Schwenn, R.; Rosenbauer, H.; Miggenrieder, H (October 1975)."Das Plasmaexperiment auf Helios (E1)".Raumfahrtforschung.19:226.Bibcode:1975RF.....19..226S.RetrievedMay 2,2022.
- ^G liem, F.; Dehmel, G.; Tuerke, C.; Krupstedt, U.; Kugel, R.P. (February 1976)."The onboard computers of the Helios magnetometer experiments E 2 and E 4".Raumfahrtforschung.19:16.Bibcode:1976RF.....20...16G.RetrievedMay 3,2022.
- ^Scearce, C.; Cantarano, S.; Ness, N.; Mariani, F.; Terenzi, R; Burlage, I. (October 1975)."The Rome-GSFC magnetic field experiment for Helios A and B (E3)".Raumfahrtforschung.19:237.Bibcode:1975RF.....19..237S.RetrievedMay 2,2022.
- ^Dehmel, G.; Neubauer, F.M.; Lukoschus, D; Wawretzko, J.; Lammers, E. (October 1975)."Das Induktionsspulen-Magnetometer-Experiment (E4)".Raumfahrtforschung.19:241.Bibcode:1975RF.....19..241D.RetrievedMay 2,2022.
- ^Gurnett, D.A.; Anderson, R.R; Odem, D.L. (October 1975)."The University of Iowa Helios solar wind plasma wave experiment (E5a)".Raumfahrtforschung.19:245.Bibcode:1975RF.....19..245G.RetrievedMay 2,2022.
- ^Kellog, P.J.; Person, G.A.; Lacabanne, L. (October 1975)."The electric field experiment for Helios /E 5b/".Raumfahrtforschung.19:248.Bibcode:1975RF.....19..248K.RetrievedMay 2,2022.
- ^Weber, R:R. (October 1975)."The radio astronomy experiment on Helios A and B /E 5c".Raumfahrtforschung.19:250.Bibcode:1975RF.....19..250W.RetrievedMay 2,2022.
- ^Kunow, H.; Wibberenz, G.; Green, G.; Mueller-Mellin, R.; Witte, M.; Hempe, H. (October 1975)."The Kiel University experiment for measuring cosmic radiation between 1.0 and 0.3 AE /E 6/".Raumfahrtforschung.9:253.Bibcode:1975RF.....19..253K.RetrievedMay 2,2022.
- ^Trainor, J.H.; Stilwell, D.E.; Joyce, R.M.; Teegarden, B.J.; White, H.O. (October 1975)."The Helios A/B cosmic ray instrument /E 7/".Raumfahrtforschung.19:258.Bibcode:1975RF.....19..258T.RetrievedMay 2,2022.
- ^Keppler, E.; Wilken, B.; Umlauft, G.; Richter, K. (October 1975)."Instrument for detecting low-energy electrons and protons on board the solar probe Helios /E 8/".Raumfahrtforschung.19:261.Bibcode:1976RF.....20...16G.RetrievedMay 3,2022.
- ^Leinert, Ch.; Link, H.; Salm, N.; Knueppelberg, D. (October 1975)."The Helios zodiacal light experiment (E9)".Raumfahrtforschung.19:264.Bibcode:1975RF.....19..264L.RetrievedMay 2,2022.
- ^Helios B – Micrometeoroid Detector and Analyzer.NASANSSDC Master Catalog.Retrieved May 20, 2016.
- ^Grün, E.; Fechtig, H.; Gammelin, P.; Kissel, J (October 1975)."Das Staubexperiment auf Helios (E10)".Raumfahrtforschung.19:268.Bibcode:1975RF.....19..268G.RetrievedMay 2,2022.
- ^Kundt, W. (October 1974)."The Helios experiment on theories of gravitation".In Arbeitsgemeinschaft für Weltraumforsch. Helios Satellite Sci. Data Evaluation:15.Bibcode:1974hsde.rept...15K.RetrievedMay 3,2022.
- ^Edenhofer, P. (October 1974)."Determination of the coronal electron density distribution from range and range rate data during solar occultations of the HELIOS spacecraft".In Arbeitsgemeinschaft für Weltraumforsch. Helios Satellite Sci. Data Evaluation:12.Bibcode:1974hsde.rept...12E.RetrievedMay 3,2022.
- ^Administrator, NASA Content (April 17, 2015)."Helios-A Solar Probe At Launch Complex".NASA.RetrievedMay 1,2020.
- ^"NASA - NSSDCA - Spacecraft - Details".nssdc.gsfc.nasa.gov.RetrievedMay 1,2020.
- ^"Helios".www.honeysucklecreek.net.RetrievedMay 1,2020.
- ^"Search Satellite Database: HELIOS 1".www.n2yo.com.
- ^"Search Satellite Database: HELIOS 2".www.n2yo.com.
- ^NASA Space Science Data Coordinated Archive.
External links
[edit]![](https://upload.wikimedia.org/wikipedia/en/thumb/4/4a/Commons-logo.svg/30px-Commons-logo.svg.png)
- Helios-Aat NSSDC Master Catalog
- Helios-Bat NSSDC Master Catalog
- Helios-AMission ProfilebyNASA's Solar System Exploration
- Helios-BMission ProfilebyNASA's Solar System Exploration
- Titan/Centaur D-1T TC-2,Helios-A,Flight Data Report
- Titan/Centaur D-1T TC-5,Helios-B,Flight Data Report
- Helios-Aand-Bby Honeysuckle Creek Tracking Station
- Helios webpageby Max-Planck-Institut für Sonnensystemforschung