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Published byArchibald Hunter Modified over 9 years ago
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TEMPERATURE LAPSE RATE ESTIMATION BY DOPPLER SODAR Jean-Michel FAGE, PRESIDENT, REMTECH INC, 2 Red Oak Road, St James NY 11780, USA Tel: (303) 772 68 25, Fax: (303) 772 6827, sales@remtechinc.com
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OBJECTIVE The goal of the study is to determine if it is possible to use the data from a Doppler SODAR to determine the lapse rate under stable conditions. Compare data from SODAR with tall tower to develop empirical coefficients for further use and algorithm development.
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DATA SOURCE FOR INITIAL ALGORITHM DEVELOPMENT Kernforschungszentrum (Nuclear Research Center), Karlsruhe, Germany) 200 meter measurement tower
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The PA2 SODAR, similar to the system at Kernforschungszentrum (Nuclear Research Center) in Karlsruhe (West Germany)
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The following approach corresponds to the so-called “Level 2” of Mellor & Yamda where advection and diffusion terms are neglected in the Fluid Mechanics equations, which leads to (in the PBL approximation): q 3 / 1 = – uw ( U / z) – vw ( V/ z) + g w ’ q ²/ 2 = – w ’ ( / z) where: - characteristics lengths - u, w horizontal and vertical speed fluctuations - ’ potential temperature fluctuation - q kinetic energy - sigma of the potential temperature fluctuations THEORY
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The derivation resolves down to: / z E 3/2 w -1 The empirical formula, which is applied to the SODAR data reads: / z = A + B E 3/2 w -1 A and B are empirical coefficients which have been estimated using previous data. THEORY
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A and B coefficients of the lapse rate formula vary They are constantly recalibrated using two techniques: - if the RASS is not present we infer that the atmosphere is adiabatic at least for a few hundred meters above the surface layer during the afternoon - if the RASS is present we use the RASS data themselves by a least square optimization between the RASS data derived lapse rate and the lapse rate obtained from the Sodar only. THEORY
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6.0°C/100m 3.0°C/100m 0.0°C/100m -3.0°C/100m -___ TOWER ----- SODAR
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STATISTICS Correlation Between SODAR and Tower: 0.78 Standard Deviation of the difference between the SODAR and tower, by level (in °C/100 m): 180 m0.63 160 m0.54 140 m0.60 120 m0.64 100 m0.78 80 m0.98 60 m1.13
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PA0 SODAR Antenna
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WIND SPEED DATA FROM PA0 ON ROOF
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LAPSE RATE DATA FROM PA0 ON ROOF
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PA5 Antenna RASS Antennas Solar Power Array Radio Acoustic Sounding System (RASS)
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CONCLUSIONS 1.Possible to measure lapse rate with SODAR 2.Can be included with all versions of the SODAR 3.Empirical nature of system requires it to learn at each site for a period of time 4.System improves with RASS as part of the system
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