The purpose of the high altitude solar cell calibration program was to produce air mass zero (AM0) standard solar cells that could be used for accurately setting solar simulator intensities. The program was started in 1962 by the Jet Propulsion Laboratory of the California Institute of Technology in Pasadena and endured for more than 40 years.
Since the output of solar cells is spectrally selective, the electrical power derived from solar cells depends on the total intensity and the spectral distribution of the light source: the Sun. Attempts were made to procure a laboratory light source which has the same spectral character and intensity as the Sun. However, such attempts have been complicated as different types of radiation sensing devices, such as pyrheliometers and thermopiles, have been used which can not be accurately calibrated on either a total intensity or spectral intensity basis. To overcome this was introduced the concept of flying cells on a balloon, to measure their output at altitudes, to recover the cells and to use them as reference standards. The calibrated standard solar cell is placed in the solar simulator beam, and the beam intensity is adjusted until the standard solar cell reads the same as it reads on the balloon.
Althought some modifications were introduced over time, the main components of the balloon flight system were maintained along the entire program: a sun tracker, a helium-filled balloon, a telemetry system, and a battery power supply, as shown in the scheme at left (click for more detail). The sun tracker was mounted on the balloon apex, which is the most stable position of the balloon system. The telemetry transmitter and battery power supply, along with several instruments for measuring altitude, were suspended in a second gondola beneath the balloon. An electrical cable, incorporated into the balloon during manufacture, connected the top and bottom payloads.
The solar tracker was used to position the solar cell payload toward the sun, independent of balloon movements. The tracker was capable of movement in both elevation and azimuth to maintain an "on-sun" condition within +2 deg. A reflection shield attached to the solar tracker was used to prevent unwanted reflected light from reaching the solar cell payload. The tracker and associated electronics boxes were mounted on a plywood disk 6 ft in diameter, which, in turn, was bolted to the balloon top end fitting. The plywood disk permited the tracker to "float" on top of the helium bubble.
Balloon launched on: 8/13/1965 at 7:56 cdt
Launch site: University of Minnesota Airport, New Brighton, US
Balloon launched by: Litton Industries Inc.
Balloon manufacturer/size/composition: Zero Pressure Balloon 77-1-2 4DRS771 (1.5 mil)
Flight identification number: LITTON 3029
End of flight (L for landing time, W for last contact, otherwise termination time): 8/13/1965
Balloon flight duration (F: time at float only, otherwise total flight time in d:days / h:hours or m:minutes - ): 9 h 50 m
Landing site: 2 miles of Belle Plain, Winsconsin, US
Payload weight: 249 lbs
The balloon was launched by dynamic method from the Litton Flight Facility located near New Brighton, Minnesota at 8:56 CDT on 13 August 1965 as Flight No. 3029. The balloon moved N after launch until it, reached 60,000 feet where it turned SE until it reached float above a point two miles NE of Pine Bend, Minnesota. The track was SW during the extended float period to a point two miles east of Gaylord, Minnesota at an altitude of 65.000 ft on descent. Descent course was varied but generally eastward to an impact point located 2 miles N of Belle Plaine, Minnesota. As the system neared the surface it appeared to be moving toward a water impact in the Minnesota River but the actual touchdown was about one mile north of the river in an open field.
The balloon was ripped open imediately, but as it deflated the system was dragged a few hundred feet into a deep weed patch where it came gently to a rest. Battery acid spillage and a sheared elevation drive pin were the only damages to the equipment.
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