Camera tubes for recording Stratoscope II TELESCOPE images.
Camera tubes for recording Stratoscope II TELESCOPE, noting photometric fidelity
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Camera tubes for recording Stratoscope II TELESCOPE, noting photometric fidelity
Stratoscope II unmanned balloon-borne telescope design, detailing pointing, focusing and thermal characteristics
IR spectroscopic observations with balloon-borne telescope, Stratoscope II
IR spectroscopic observations with balloon-borne telescope, Stratoscope II
Composition of mars atmosphere, observed in first flight of stratoscope ii telescope
The nucleus of M31 was photographed at a resolution of 0.2 sec with the 91-cm balloon-borne Stratoscope II telescope. At the half-intensity level, the nucleus was observed to be elliptical with its major axis lying in position angle of 63 (plus or minus 5) deg. The peak surface brightness was 12.7 plus or minus 0.3 V mag per square second of arc assuming B - V = 1.0. The nucleus appears to be a separate feature from the bulge with a scale height of approximately 0.5 pc. The mass of the nucleus is of the order of 100 million solar masses, and the apparent visual mass-to-light ratio is of the order of 20.
Signal-generating astronomical sensors, describing Stratoscope Ii balloon-borne telescope
Infrared spectroscopy and high resolution photography of planets using the stratoscope ii balloon-borne telescope
Ultraviolet astronomy researches dealing with UV NEBULOSITIES, deficiency, and interstellar extinction - Balloon-borne telescopes to measure infrared spectrum
Moon IR spectrum scanning during second flight of Stratoscope II at balloon altitude of 83500 ft
IR reflection spectrum of Jupiter from second flight of Stratoscope II, discussing deep absorption features
Programmable integrating image-orthicon TV chain for application to Stratoscope II balloon-borne astronomical telescope
A number of general characteristics of a diffraction limited telescope are examined, giving attention to the optical system of the Stratoscope II instrument. The optical resolution of a telescope can be described in at least three different ways, involving the wavefront error, the optical transfer function, and the point spread function. The Stratoscope II tolerance budget and the performance of the instrument are discussed together with a goal for the resolution of the large space telescope (LST) which is to be designed. The very high resolving power of the LST will be utilized in many ways. The imagery of extended objects with low surface contrast is considered along with the photometry of very faint stars.
The paper considers photographs of Uranus obtained by the Stratoscope II balloon-borne telescope in 1970. These data have been redigitized and reanalyzed, and the geometric oblateness of Uranus was determined from the isophotes near the limb using an expression in terms of the equatorial and polar radii.
Stratoscope 2 balloon-borne IR telescope, discussing launch, operation and planetary and stellar IR spectra
Princeton Observatory has been working for several years under NASA sponsorship to develop television type sensors to use in place of photographic film for space astronomy. This paper discusses the performance of an SEC-vidicon with a 25 mm x 25 mm active area, MgF2 window, and bi-alkali photocathode. Results from ground based use on the Coude spectrograph of the 200-inch Hale telescope are included. The intended use of this tube in an echelle spectrograph sounding rocket payload and on Stratoscope II for direct high resolution imagery is also discussed. The paper also discusses the Large Space Telescope image sensor requirements and the development of a larger television tube for this mission.
Radio controlled balloon-borne astronomical tele- scope - stratoscope ii
The oblateness of a planet is closely related to its rotation rate and internal mass distribution, and is therefore an important indicator of gross planetary structure. Analysis of Stratoscope II images of Uranus yields epsilon = 0.022 + or - 0.001, and stellar occultation observations yield epsilon = 0.024 + or - 0.003. Because of the current pole on aspect of Uranus, it is unlikely that a significantly more accurate value can be determined by stellar occultations before Voyager 2 encounters Uranus in January, 1986. Neptune's oblateness has been determined from stellar occultation observations made in 1968 and 1983. The 1968 observations yield an oblateness of 0.021 + or - 0.004. A recent determination of Neptune's oblateness using both the 1968 and 1983 observations is consistent with this value. Space Telescope observations of several stellar occultations by Neptune could provide a significantly more accurate determination of the oblateness before the Voyager 2 encounter in 1990.