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Volumn 272, Issue 5263, 1996, Pages 844-845

Structure of the atmosphere of Jupiter: Galileo probe measurements

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Indexed keywords


EID: 4243108527     PISSN: 00368075     EISSN: None     Source Type: Journal    
DOI: 10.1126/science.272.5263.844     Document Type: Article
Times cited : (100)

References (26)
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    • note
    • The sensor was designed to avoid problems resulting from lightning strikes, electrical discharge, and shorting by condensibles.
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    • H. B. Niemann et al., Science 272, 847 (1996).
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  • 8
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    • note
    • -1 , are an additional source of uncertainty because the sensors could not attain thermal equilibrium. Tests in progress of the engineering and flight spare sensors at temperatures and temperature rates similar to those in flight will indicate the effects of this operating environment on sensor offsets for use in correcting flight data.
  • 9
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    • note
    • For pressures between 5 and 17 bars, pressure sensor offsets were selected with guidance from sensors in the helium abundance detector (HAD). The HAD sensors, mounted in a block of nearly solid beryllium, experienced a smaller temperature range (254 to 301 K) than did the atmospheric structure instrument (ASI) sensors.
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    • The upper atmospheric data period, 240 s, was dictated by probe memory capacity and ended at the start of parachute descent. Thus, the unplanned 53-s delay in the start of descent [R. E. Young, M. A. Smith, C. K. Sobeck, Science 272, 837 (1996)] also delayed the start of entry data acquisition. With ontime deployment, the threshold would have been at the 3-μg level
    • (1996) Science , vol.272 , pp. 837
    • Young, R.E.1    Smith, M.A.2    Sobeck, C.K.3
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    • P. F. Intrieri, C. E. DeRose, D. B. Kirk, Acta Astronaut. 4, 789 (1977); P. F. Intrieri and D. B. Kirk, J. Spacecr. Rockets 24, 127 (1987).
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    • B. L. Haas and F. S. Milos, J. Spacecr. Rockets 32, 398 (1995); E. Venkatapathy, personal communication. Further computational fluid dynamics solutions have been made for the continuum flow regime and for the ablated heat shield shape.
    • (1995) J. Spacecr. Rockets , vol.32 , pp. 398
    • Haas, B.L.1    Milos, F.S.2
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    • B. L. Haas and F. S. Milos, J. Spacecr. Rockets 32, 398 (1995); E. Venkatapathy, personal communication. Further computational fluid dynamics solutions have been made for the continuum flow regime and for the ablated heat shield shape.
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    • As an initial assumption, the mean molecular mass used was a lower atmospheric value, 2.215. The upper atmosphere is believed to be dominated by molecular hydrogen [S. K. Atreya, T. M. Donahue, M. C. Festou, Astrophys. J. 247, L43 (1981)]. Temperatures at the higher altitudes in Fig. 5 may thus be up to 10% too high.
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    • note
    • We thank J. Lepetich and L. Yee, who served as ASI managers, for their contributions to this experiment. We also thank E. Tischler, C. Sobeck, and numerous other Probe Project Office personnel and those who contributed to the instrument design and development at Martin Marietta Aerospace and at Bell Aerospace.


* 이 정보는 Elsevier사의 SCOPUS DB에서 KISTI가 분석하여 추출한 것입니다.