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@MastersThesis{Roballo:2007:EsEsAt,
               author = "Roballo, Suelen Trindade",
                title = "Estudo do escoamento atmosf{\'e}rico no Centro de 
                         Lan{\c{c}}amento de Alc{\^a}ntara (CLA) atrav{\'e}s de medidas 
                         de torre anemom{\'e}trica e em t{\'u}nel de vento",
               school = "Instituto Nacional de Pesquisas Espaciais (INPE)",
                 year = "2007",
              address = "S{\~a}o Jos{\'e} dos Campos",
                month = "2007-04-02",
             keywords = "meteorologia, penhasco, n{\'u}mero de Reynolds, anem{\^o}metro 
                         de fio quente, rugosidade superficial, t{\'u}nel de vento, 
                         atmosfera neutra, meteorology, cliff, Reynolds number, hot wire 
                         ane.",
             abstract = "Estudou-se o escoamento atmosf{\'e}rico no Centro de 
                         Lan{\c{c}}amento de Alc{\^a}ntara(CLA), localizado junto a uma 
                         fal{\'e}sia de 50 m de altura, (i) analisando dados de vento 
                         coletados, nos per{\'{\i}}odos 1995 - 1999 (anos base) e 2004 - 
                         2005 (para valida{\c{c}}{\~a}o), em seis n{\'{\i}}veis de 
                         torre anemom{\'e}trica (TA) de 70 m, situada 200 m a jusante da 
                         fal{\'e}sia, pr{\'o}ximo {\`a} rampa de lan{\c{c}}amento de 
                         foguetes e (ii) simula{\c{c}}{\~o}es em t{\'u}nel de vento 
                         (TV), na escala geom{\'e}trica 1:1000, com a 
                         realiza{\c{c}}{\~a}o de quatro s{\'e}ries de ensaios, incluindo 
                         configura{\c{c}}{\~o}es do piso, representando a fal{\'e}sia. 
                         As observa{\c{c}}{\~o}es na TA, mostraram que a velocidade de 
                         atrito u* foi igual a 0,32 ± 0,13 m/s (per{\'{\i}}odo chuvoso) e 
                         0,46 ± 0,11 m/s (seco); o comprimento de rugosidade z0 foi igual a 
                         0,19 ± 0,32 (chuvoso) e 0,06 ± 0,05 m (seco), demonstrando a 
                         sazonalidade do perfil do vento. O expoente \α da lei de 
                         pot{\^e}ncia para a velocidade variou de 0,19 a 0,27, ao longo 
                         dos meses do ano, com R2s entre 0,88 e 0,99, e a decrescendo com a 
                         altura zn. A valida{\c{c}}{\~a}o de \α com dados de vento 
                         de 2004 a 2005 mostrou, em m{\^e}s chuvoso, velocidades locais 
                         estimadas maiores que as observadas, talvez devido a neutralidade 
                         atmosf{\'e}rica menos forte; entretanto, em m{\^e}s seco, elas 
                         foram equivalentes, demonstrando condi{\c{c}}{\~o}es neutras da 
                         atmosfera. Finalmente, a dire{\c{c}}{\~a}o do vento predominante 
                         foi de Nordeste, seguida das de Norte e de Leste. Os ensaios no 
                         TV, com degraus de 90° e de 70°, correspondentes {\`a} 
                         fal{\'e}sia, ambos sem e com emula{\c{c}}{\~a}o de rugosidade 
                         adicional a jusante deles, mostraram: (i) a perfeita 
                         emula{\c{c}}{\~a}o do perfil de vento oce{\^a}nico (\α = 
                         0,15) sobre a posi{\c{c}}{\~a}o do degrau representativo da 
                         fal{\'e}sia, utilizando pista de tapete, a montante, para prover 
                         a rugosidade necess{\'a}ria; (ii) que o n{\'u}mero de Reynolds 
                         m{\'a}ximo poss{\'{\i}}vel com comprimento 
                         caracter{\'{\i}}stico igual {\`a} altura do degrau neste TV foi 
                         6,52.104, enquanto no CLA foi da ordem de 3.107, raz{\~a}o pela 
                         qual {\'e} necess{\'a}rio um t{\'u}nel mais potente para emular 
                         esta; (iii) que os \α mais pr{\'o}ximos dos observados 
                         foram obtidos com um degrau reto, sem nenhum revestimento especial 
                         no piso normal do t{\'u}nel, exceto o tapete a montante do 
                         degrau; (iv) que a fixa{\c{c}}{\~a}o de cubos a jusante do 
                         degrau resulta em rugosidades bem maiores que as observadas sobre 
                         a vegeta{\c{c}}{\~a}o do CLA, possivelmente emulando 
                         situa{\c{c}}{\~o}es urbanas ou industriais; (v) que 
                         caracter{\'{\i}}sticas t{\'{\i}}picas do escoamento ap{\'o}s 
                         o degrau, tais como o descolamento, a forma{\c{c}}{\~a}o de 
                         bolha de circula{\c{c}}{\~a}o e nova ader{\^e}ncia foram 
                         emuladas; (vi) que o uso de TVs mais potentes certamente 
                         permitir{\'a} a emula{\c{c}}{\~a}o da situa{\c{c}}{\~a}o 
                         atmosf{\'e}rica do CLA. Finalmente, com a utiliza{\c{c}}{\~a}o 
                         de um TV mais potente, al{\'e}m da replica{\c{c}}{\~a}o dos 
                         ensaios deste trabalho, testes com ventos incidindo em 
                         {\^a}ngulos n{\~a}o retos no degrau s{\~a}o recomendados. 
                         ABSTRACT: The atmospheric flow at the Alcantara Launching Center 
                         (CLA), which is localized near a 50 m cliff, was studied through 
                         (i) the analysis of wind data that were measured during the 
                         periods from 1995 to 1999 (base years) and from 2004 to 2005 (for 
                         validation), at six levels of a 70 m anemometric tower (TA), which 
                         is placed 200 m downwind of the cliff, near a rocket launching 
                         pad, and (ii) wind tunnel (TV) experiments, using a 1:1000 
                         geometric scale and floor level configurations to represent the 
                         cliff and its downwind roughness. The data at the TA determined 
                         that the roughness velocity u* was equal to 0.32 ± 0.13 m/s (0.46 
                         ± 0.11 m/s) during the rainy (dry) period, while the roughness 
                         length z0 equalled 0.19 ± 0.32 m (0.06 ± 0.05 m) for the rainy 
                         (dry) period, thus showing the seasonality of the wind profiles. 
                         The exponent \α of the velocity power law varied along the 
                         yearly months from 0.19 to 0.27, with R2s between 0.88 and 0.99; 
                         \α decreased with the altitude zn. For a rainy month, the 
                         validation of \α with 2004 2005 wind data showed estimated 
                         velocities greater than the ones observed at the TA, which was 
                         possibly due a weaker atmospheric neutrality; however, for a dry 
                         month, these velocities were equivalent, thus implying a neutral 
                         atmosphere. Finally, the predominant wind direction was from the 
                         Northeast, followed by the ones from the North and the East. The 
                         TV experiments, with 90° and 70° steps representing the cliff, 
                         both with and without additional downwind roughness, did show: (i) 
                         a perfect emulation of the ocean wind profile (\α = 0.15) 
                         above the position of the step representing the cliff, through the 
                         use of a upwind carpeted fetch to provide the necessary roughness; 
                         (ii) that the highest Reynolds number possible, based on the 
                         height of the cliff, was 6.52 x 104 inside this TV, while it 
                         reached 3 x107 at the CLA thus, a more powerfull tunnel is needed 
                         to emulate this last situation; (iii) that the values of \α 
                         nearest to the ones obtained at the CLA resulted from the 90° step 
                         experiment without any extra covering over the floor, except the 
                         upwind carpet; (iv) that the fixing of cubes downwind of the step 
                         resulted roughnesses much greater than the ones observed over the 
                         CLA vegetation, so possibly emulating urban or industrial 
                         situations; (v) that typical characteristics which occur downwind 
                         a step were emulated, such as the dettachment and the posterior 
                         reattachment of the flow, plus the formation of circulation 
                         bubbles; (vi) that the use of more powerfull TVs would certainly 
                         permit the emulation of the atmospheric behavior of the CLA. 
                         Finally, with the use of a more powerfull TV, besides the 
                         replication of the experiments of the present work, experiments 
                         with wind incidences on the step with angles other than 90° should 
                         be recommended.",
            committee = "Alval{\'a}, Regina C{\'e}lia dos Santos (presidente) and Fisch, 
                         Gilberto Fernando (orientador) and Girardi, Roberto da Mota 
                         (orientador) and Gielow, Ralf and Acevedo, Ot{\'a}vio Costa",
           copyholder = "SID/SCD",
         englishtitle = "Atmospheric flow study in the Alcantara Launching Center, using 
                         anemometric tower and wind tunnel measurements",
             language = "pt",
                pages = "137",
                  ibi = "6qtX3pFwXQZGivnK2Y/Qr5M8",
                  url = "http://urlib.net/ibi/6qtX3pFwXQZGivnK2Y/Qr5M8",
           targetfile = "publicacao.pdf",
        urlaccessdate = "15 jun. 2024"
}


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