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2
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4243050346
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note
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The sensor was designed to avoid problems resulting from lightning strikes, electrical discharge, and shorting by condensibles.
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5
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4243066123
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H. B. Niemann et al., Science 272, 847 (1996).
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Niemann, H.B.1
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7
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4243084218
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B. Ragent, D. S. Colburn, P. Avrin, K. A. Rages, Science 272, 855 (1996).
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Avrin, P.3
Rages, K.A.4
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8
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4243195746
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note
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-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.
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9
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4243052561
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note
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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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11
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0000417011
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T. Guillot, D. Gautier, G. Chabrier, B. Mosser, Icarus 112, 337 (1994).
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Guillot, T.1
Gautier, D.2
Chabrier, G.3
Mosser, B.4
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4243173523
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personal communication
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R. Preston, personal communication.
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Preston, R.1
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13
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4243098194
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personal communication
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R. Woo, personal communication.
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Woo, R.1
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15
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0029664462
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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
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Science
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Young, R.E.1
Smith, M.A.2
Sobeck, C.K.3
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16
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4243200257
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personal communication
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J. Neff, personal communication.
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Neff, J.1
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17
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0017508910
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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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Intrieri, P.F.1
DeRose, C.E.2
Kirk, D.B.3
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0023310565
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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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Intrieri, P.F.1
Kirk, D.B.2
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19
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0029310284
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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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Haas, B.L.1
Milos, F.S.2
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20
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0029310284
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personal communication
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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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Venkatapathy, E.1
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0002050810
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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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(1981)
Astrophys. J.
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Atreya, S.K.1
Donahue, T.M.2
Festou, M.C.3
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0013464219
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S. K. Atreya, T. M. Donahue, B. R. Sandel, A. L. Broadfoot, G. R. Smith, Geophys. Res. Lett. 6, 795 (1979).
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Atreya, S.K.1
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Broadfoot, A.L.4
Smith, G.R.5
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note
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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.
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