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1
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33847635908
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This well-known fact is statistically documented at 29
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This well-known fact is statistically documented at (29).
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3
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0022213335
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H. E. Willoughby, D. P. Jorgensen, R. A. Black, S. L. Rosenthal, Bull. Am. Meteorol. Soc. 66, 505 (1985).
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(1985)
Bull. Am. Meteorol. Soc
, vol.66
, pp. 505
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Willoughby, H.E.1
Jorgensen, D.P.2
Black, R.A.3
Rosenthal, S.L.4
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4
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1442285284
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R. Simpson, Ed, American Geophysical Union, Washington, DC, chap. 3
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R. C. Sheets, in Hurricane! Coping With Disaster, R. Simpson, Ed. (American Geophysical Union, Washington, DC, 2003), chap. 3.
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(2003)
Hurricane! Coping With Disaster
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Sheets, R.C.1
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11
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33847655443
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D. Ortt, S. S. Chen, 27th Conference on Hurricanes and Tropical Meteorology, American Meteorological Society, 24 to 28 April 2006, Monterey, CA, preprint 12A.S (2006) (available at http://ams.confex.com/ams/pdfpapers/108643. pdf).
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D. Ortt, S. S. Chen, 27th Conference on Hurricanes and Tropical Meteorology, American Meteorological Society, 24 to 28 April 2006, Monterey, CA, preprint 12A.S (2006) (available at http://ams.confex.com/ams/pdfpapers/108643. pdf).
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12
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33847635473
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Precipitation particles are liquid drops or ice particles heavy enough to be falling relative to Earth's surface. Most meteorological radars, including those deployed on the aircraft in RAINEX, detect precipitation but do not see smaller, non-falling cloud particles. Therefore, the intensity of the radar signal is related to precipitation intensity. The radar also detects the Doppler shift between emitted and received signals, which indicates the speed of movement of the precipitation particles along the beam of the radar. The wind speed and direction can be inferred from the Doppler velocities when the same precipitation particles are observed in more than one radar beam
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Precipitation particles are liquid drops or ice particles heavy enough to be falling relative to Earth's surface. Most meteorological radars, including those deployed on the aircraft in RAINEX, detect precipitation but do not see smaller, non-falling cloud particles. Therefore, the intensity of the radar signal is related to precipitation intensity. The radar also detects the Doppler shift between emitted and received signals, which indicates the speed of movement of the precipitation particles along the beam of the radar. The wind speed and direction can be inferred from the Doppler velocities when the same precipitation particles are observed in more than one radar beam.
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15
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0033927655
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P. D. Reasor, M. T. Montgomery, F. D. Marks Jr., J. F. Gamache, Mon. Weather Rev. 128, 1653 (2000).
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(2000)
Mon. Weather Rev
, vol.128
, pp. 1653
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Reasor, P.D.1
Montgomery, M.T.2
Marks Jr., F.D.3
Gamache, J.F.4
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17
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1442285284
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R. Simpson, Ed, Amerian Geophysical Union, Washington, DC, chap. 12
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E. A. Ritchie et al., in Hurricane! Coping With Disaster, R. Simpson, Ed. (Amerian Geophysical Union, Washington, DC, 2003), chap. 12.
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(2003)
Hurricane! Coping With Disaster
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Ritchie, E.A.1
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19
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33847667150
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When air subsides, its relative humidity decreases because the air temperature increases adiabatically. Consequently, saturation vapor pressure rises while the water vapor content remains constant
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When air subsides, its relative humidity decreases because the air temperature increases adiabatically. Consequently, saturation vapor pressure rises while the water vapor content remains constant.
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20
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33847612674
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A dropsonde is a package of pressure, temperature, and humidity sensors that is dropped from an aircraft and tracked with a Global Positioning System receiver. The data obtained provide vertical profiles of temperature, humidity, and wind below the aircraft. For further information, see 30
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A dropsonde is a package of pressure, temperature, and humidity sensors that is dropped from an aircraft and tracked with a Global Positioning System receiver. The data obtained provide vertical profiles of temperature, humidity, and wind below the aircraft. For further information, see (30).
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22
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33847659040
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A temperature inversion is not required for a layer of air to be stable, i.e., resistant to vertical mixing. Stability exists in unsaturated air as long as the temperature decrease with height is >10°C/km.
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A temperature inversion is not required for a layer of air to be stable, i.e., resistant to vertical mixing. Stability exists in unsaturated air as long as the temperature decrease with height is >10°C/km.
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24
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33748355559
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M. T. Montgomery, M. M. Bell, S. D. Aberson, M. L. Black, Bull. Am. Meteorol. Soc. 87, 1335 (2006).
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(2006)
Bull. Am. Meteorol. Soc
, vol.87
, pp. 1335
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Montgomery, M.T.1
Bell, M.M.2
Aberson, S.D.3
Black, M.L.4
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26
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33847687552
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The hurricane-strength categories 1 to 5 represent, in ascending order, the degree of damage that can be done by the storm. For further details, see (27, 31).
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The hurricane-strength categories 1 to 5 represent, in ascending order, the degree of damage that can be done by the storm. For further details, see (27, 31).
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27
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1442285284
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R. Simpson, Ed, American Geophysical Union, Washington, DC, chap. 7
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H. S. Saffir, in Hurricane! Coping With Disaster, R. Simpson, Ed. (American Geophysical Union, Washington, DC, 2003), chap. 7.
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(2003)
Hurricane! Coping With Disaster
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Saffir, H.S.1
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28
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33847670775
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The range of the observed winds can be found at 32
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The range of the observed winds can be found at (32).
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29
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33847616387
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National Hurricane Center NHC
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National Hurricane Center (NHC), www.nhc.noaa.gov/verification.
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31
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33847610931
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NHC
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NHC, www.nhc.noaa.gov/aboutsshs.shtml.
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32
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33847663616
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NHC
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NHC, www.nhc.noaa.gov/pdf/TCR-AL18200S_Rita.pdf.
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34
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33748071081
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in press; available at
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S. S. Chen, J. F. Price, W. Zhao, M. A. Donelan, E. J. Walsh, Bull. Am. Meteorol. Soc., in press; available at http://orca.rsmas.miami.edu/ ~schen/publications/Chen.etal_InBox_CBLAST_final_8Sept06.pdf.
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Bull. Am. Meteorol. Soc
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Chen, S.S.1
Price, J.F.2
Zhao, W.3
Donelan, M.A.4
Walsh, E.J.5
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35
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33847621471
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In RAINEX, the high-resolution MM5 was run with input from four different global models. The input from NOGAPS (33) gave the best result for Hurricane Rita. Also see (7).
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In RAINEX, the high-resolution MM5 was run with input from four different global models. The input from NOGAPS (33) gave the best result for Hurricane Rita. Also see (7).
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36
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0020969818
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G. M. Barnes, E. J. Zipser, D. Jorgensen, F. D. Marks Jr., J. Atmos. Sci. 40, 2125 (1983).
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(1983)
J. Atmos. Sci
, vol.40
, pp. 2125
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Barnes, G.M.1
Zipser, E.J.2
Jorgensen, D.3
Marks Jr., F.D.4
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37
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33847685057
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Aircraft operations in RAINEX were under the direction of C. Newman (NRL aircraft) and J. MacFadden (NOAA aircraft, Lead airborne missions scientists for RAINEX included R. Rogers, M. Black (NOAA Hurricane Research Division, and D. Jorgensen (NOAA National Severe Storms Laboratory, Daily aircraft mission planning was led by J. Moore and G. Stossmeister (University Corporation for Atmospheric Research, and D. Nolan (University of Miami) contributed scientific guidance to the planning. Engineering support for ground control of flights was provided by C. Burghart and J. Scannel (NCAR, P. Chang (NOAA National Environmental Satellite, Data, and Information Service, J. Carswell (Remote Sensing Solutions, Inc, and S. Brodzik (University of Washington, Engineering support for the radar and dropsonde measurements was directed by E. Loew, M. Strong, H.-Q. Cai, and E. Korn (NCAR, Real-time high-resolution model runs were carried out by W. Zhao University of Miami, Forecasting for flig
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Aircraft operations in RAINEX were under the direction of C. Newman (NRL aircraft) and J. MacFadden (NOAA aircraft). Lead airborne missions scientists for RAINEX included R. Rogers, M. Black (NOAA Hurricane Research Division), and D. Jorgensen (NOAA National Severe Storms Laboratory). Daily aircraft mission planning was led by J. Moore and G. Stossmeister (University Corporation for Atmospheric Research), and D. Nolan (University of Miami) contributed scientific guidance to the planning. Engineering support for ground control of flights was provided by C. Burghart and J. Scannel (NCAR), P. Chang (NOAA National Environmental Satellite, Data, and Information Service), J. Carswell (Remote Sensing Solutions, Inc.), and S. Brodzik (University of Washington). Engineering support for the radar and dropsonde measurements was directed by E. Loew, M. Strong, H.-Q. Cai, and E. Korn (NCAR). Real-time high-resolution model runs were carried out by W. Zhao (University of Miami). Forecasting for flight operations was done by J. Cangialosi and D. Ortt (University of Miami). G. Stossmeister and J. Meitín (University Corporation for Atmospheric Research) provided web support and data management for the project. B. Tully (University of Washington) coordinated the graphics. This research was supported by NSF grants ATM-0432623 and ATM-0432717.
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