Balloon satellite


A balloon satellite is inflated with gas after it has been put into orbit.

List of balloon satellites

SatelliteLaunch date DecayMassDiameterNSSDC IDNationUsage
Beacon 11958-10-24 03:211958-10-24 4.23.66USado
Beacon 21959-08-15 00:31:001959-08-15 4.23.66USado
Echo 11960-08-12 09:36:001968-05-2418030.48USpcr, ado, spc, tri
Explorer 91961-02-16 13:12:001964-04-09363.66USado
Explorer 19 1963-12-19 18:43:001981-10-057.73.66USado
Echo 21964-01-25 13:55:001969-06-0725641USpcr, tri
Explorer 24 1964-11-21 17:17:001968-10-188.63.6USado
PAGEOS 11966-06-24 00:14:001975-07-1256.730.48UStri
PasComSat 1966-07-14 02:10:021978-01-043.29.1USpcr
Explorer 39 1968-08-08 20:12:001981-06-229.43.6USado
Mylar Balloon1971-08-07 00:11:001981-09-010.82.13USado
Qi Qiu Weixing 11990-09-03 00:53:001991-03-1143PRCado
Qi Qiu Weixing 21990-09-03 00:53:001991-07-2442.5PRCado
Naduvaniy gazovoy balloon1991-03-30 1986-017FJRU
Orbital Reflector2018-12-03USsculpture

abbreviations:
The first flying body of this type was Echo 1, which was launched into a high orbit on August 12, 1960, by the United States. It originally had a spherical shape measuring, with a thin metal-coated plastic shell made of Mylar. It served for testing as a "passive" communication and geodetic satellite. Its international COSPAR number was 6000901.
One of the first radio contacts using the satellite was successful at a distance of nearly . By the time Echo 1 burned up in 1968, the measurements of its orbit by several dozen earth stations had improved our knowledge of the precise shape of the planet by nearly a factor of ten.
Its successor was the similarly built Echo 2. This satellite circled the Earth about lower, not at an angle of 47° like that of Echo 1, but in a polar orbit with an average angle of 81°. This enabled radio contact and measurements to be made at higher latitudes. Taking part in the Echo orbit checks to analyze disturbances in its orbit and in the Earth's gravitational field were thirty to fifty professional earth stations, as well as around two hundred amateur astronomers across the planet in "Moonwatch" stations; these contributed around half of all sightings.

Range of radio waves, visibility

The Pythagorean theorem allows us to calculate easily how far a satellite is visible at such a great height. It can be determined that a satellite in a orbit rises and sets when the horizontal distance is. However, the atmosphere causes this figure to vary slightly. Thus if two radio stations are apart and the satellite's orbit goes between them, they may be able to receive each other's reflected radio signals if the signals are strong enough.
Optical visibility is, however, lower than that of radio waves, because
Despite this there is no problem observing a flying body such as Echo 1 for precise purposes of satellite geodesy, down to a 20° elevation, which corresponds to a distance of. In theory this means that distances of up to between measuring points can be "bridged", and in practice this can be accomplished at up to.
For visual and photographic observation of bright satellites and balloons, and regarding their geodetic use, see Echo 1 and Pageos for further information.

Other balloon satellites

For special testing purposes two or three satellites of the Explorer series were constructed as balloons.
Echo 1 was an acknowledged success of radio engineering, but the passive principle of telecommunications was soon replaced by active systems. Telstar 1 and Early Bird were able to transmit several hundred audio channels simultaneously in addition to a television program exchanged between continents.
Satellite geodesy with Echo 1 and 2 was able to fulfill all expectations not only for the planned 2–3 years, but for nearly 10 years. For this reason NASA soon planned the launch of the even larger balloon Pageos. The name is from "passive geodesic satellite", and sounds similar to "Geos", a successful active electronic satellite from 1965.

Pageos and the global network

was specially launched for the "global network of satellite geodesy", which occupied about 20 full-time observing teams all over the world until 1973. All together they recorded 3000 usable photographic plates from 46 tracking stations with calibrated all-electronic BC-4 cameras. From these images they were able to calculate the stations' position three-dimensionally with a precision of about. The coordinator of this project was Professor Hellmut Schmid, from the ETH Zurich.
Three stations of the global network were situated in Europe: Catania in Sicily, Hohenpeißenberg in Bavaria and Tromsø in northern Norway. For the completion of the navigational network exact distance measurements were needed; these were taken on four continents and across Europe with a precision of per kilometer.
The global network enabled the calculation of a "geodetic date" on different continents, within a few meters. By the early 1970s reliable values for nearly 100 coefficients of the Earth's gravity field could be calculated.

1965-1975: Success with flashing light beacons

Bright balloon satellites are well visible and were measurable on fine-grained photographic plates, even at the beginning of space travel, but there were problems with the exact chronometry of a satellite's track. In those days it could only be determined within a few milliseconds.
Since satellites circle the earth at about, a time error of 0.002 second translates into a deviation of about. In order to meet a new goal of measuring the tracking stations precisely within a couple of years, a method of flashing light beacons was adopted around 1960.
To build a three-dimensional measuring network, geodesy needs exactly defined target points, more so than a precise time. This precision is easily reached by having two tracking stations record the same series of flashes from one satellite.
Flash technology was already mature in 1965 when the small electronic satellite Geos was launched; along with its companion Geos 2, it brought about a remarkable increase in precision.
From about 1975 on, almost all optical measurement methods lost their importance, as they were overtaken by speedy progress in electronic distance measurement. Only newly developed methods of observation using CCD and the highly precise star positions of the astrometry satellite Hipparcos made further improvement possible in the measurement of distance.