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dbo:MilitaryUnit . @prefix owl: . rdf:type owl:Thing ; rdfs:label "Resistencia (fluidos)"@es , "Luftmotst\u00E5nd"@sv , "\u963B\u529B"@zh , "Arrasto"@pt , "Tra\u00EEn\u00E9e"@fr , "Gaya hambat"@in , "\u041B\u043E\u0431\u043E\u0432\u043E\u0435 \u0441\u043E\u043F\u0440\u043E\u0442\u0438\u0432\u043B\u0435\u043D\u0438\u0435"@ru , "Str\u00F6mungswiderstand"@de , "\u6297\u529B"@ja , "Drag (physics)"@en , "\u0391\u03BD\u03C4\u03AF\u03C3\u03C4\u03B1\u03C3\u03B7 (\u03BC\u03B7\u03C7\u03B1\u03BD\u03B9\u03BA\u03AE \u03C1\u03B5\u03C5\u03C3\u03C4\u03CE\u03BD)"@el , "Arrossegament"@ca , "\uD56D\uB825"@ko , "Odpor prost\u0159ed\u00ED"@cs , "Stromingsweerstand"@nl , "\u0645\u0642\u0627\u0648\u0645\u0629 \u0645\u0627\u0626\u0639"@ar , "Op\u00F3r aero(hydro)dynamiczny"@pl , "\u0410\u0435\u0440\u043E\u0433\u0456\u0434\u0440\u043E\u0434\u0438\u043D\u0430\u043C\u0456\u0447\u043D\u0438\u0439 \u043E\u043F\u0456\u0440"@uk , "C\u00FAltarraingt"@ga , "Resistenza fluidodinamica"@it ; rdfs:comment "In fluid dynamics, drag (sometimes called air resistance, a type of friction, or fluid resistance, another type of friction or fluid friction) is a force acting opposite to the relative motion of any object moving with respect to a surrounding fluid. This can exist between two fluid layers (or surfaces) or between a fluid and a solid surface. Unlike other resistive forces, such as dry friction, which are nearly independent of velocity, the drag force depends on velocity. Drag forces always tend to decrease fluid velocity relative to the solid object in the fluid's path."@en , "La resistenza fluidodinamica \u00E8 quella forza che si oppone al movimento di un corpo in un fluido, in particolare in un liquido o un aeriforme. In riferimento al moto nei liquidi \u00E8 anche indicata come resistenza idrodinamica, nel caso degli aeriformi come resistenza aerodinamica."@it , "En din\u00E0mica de fluids, l'arrossegament \u00E9s la for\u00E7a que actua en el sentit contrari del moviment relatiu d'un objecte que es mou respecte al fluid que l'envolta. Pot haver-hi arrossegament entre dues capes (o superf\u00EDcies) de fluids o una superf\u00EDcie fluida i una de s\u00F2lida. A difer\u00E8ncia d'altres forces de resist\u00E8ncia, com ara la fricci\u00F3, que pr\u00E0cticament no depenen de la velocitat, les forces d'arrossegament hi tenen una relaci\u00F3 directa. La for\u00E7a d'arrossegament \u00E9s proporcional a la velocitat en un flux laminar i proporcional a la velocitat elevada al quadrat en un flux turbulent. Tot i que, en \u00FAltima inst\u00E0ncia, la causa de l'arrossegament \u00E9s el fregament visc\u00F3s, l'arrossegament turbulent \u00E9s independent de la viscositat."@ca , "\u0391\u03BD\u03C4\u03AF\u03C3\u03C4\u03B1\u03C3\u03B7 \u03AE \u03BF\u03C0\u03B9\u03C3\u03B8\u03AD\u03BB\u03BA\u03BF\u03C5\u03C3\u03B1 (drag) \u03BF\u03BD\u03BF\u03BC\u03AC\u03B6\u03B5\u03C4\u03B1\u03B9 \u03B7 \u03B4\u03CD\u03BD\u03B1\u03BC\u03B7 \u03B7 \u03BF\u03C0\u03BF\u03AF\u03B1 \u03AD\u03C7\u03B5\u03B9 \u03C4\u03BF\u03BD \u03AF\u03B4\u03B9\u03BF \u03C6\u03BF\u03C1\u03AD\u03B1 \u03BC\u03B5 \u03B1\u03C5\u03C4\u03CC\u03BD \u03C4\u03B7\u03C2 \u03C4\u03B1\u03C7\u03CD\u03C4\u03B7\u03C4\u03B1\u03C2, \u03B1\u03BB\u03BB\u03AC \u03B1\u03BD\u03C4\u03AF\u03B8\u03B5\u03C4\u03B7 \u03C6\u03BF\u03C1\u03AC, \u03BA\u03B1\u03B9 \u03B5\u03BC\u03C6\u03B1\u03BD\u03AF\u03B6\u03B5\u03C4\u03B1\u03B9 \u03BA\u03B1\u03C4\u03AC \u03C4\u03B7\u03BD \u03BA\u03AF\u03BD\u03B7\u03C3\u03B7 \u03B1\u03BD\u03C4\u03B9\u03BA\u03B5\u03B9\u03BC\u03AD\u03BD\u03C9\u03BD \u03B5\u03BD\u03C4\u03CC\u03C2 \u03C1\u03B5\u03C5\u03C3\u03C4\u03BF\u03CD. \u0397 \u03C0\u03B1\u03C1\u03BF\u03C5\u03C3\u03AF\u03B1 \u03C4\u03B7\u03C2 \u03B4\u03CD\u03BD\u03B1\u03BC\u03B7\u03C2 \u03BF\u03C6\u03B5\u03AF\u03BB\u03B5\u03C4\u03B1\u03B9 \u03C3\u03C4\u03B7 \u03B4\u03B9\u03B1\u03C6\u03BF\u03C1\u03B5\u03C4\u03B9\u03BA\u03AE \u03C0\u03AF\u03B5\u03C3\u03B7 \u03B7 \u03BF\u03C0\u03BF\u03AF\u03B1 \u03B5\u03C0\u03B9\u03BA\u03C1\u03B1\u03C4\u03B5\u03AF \u03C3\u03C4\u03B9\u03C2 \u03B4\u03CD\u03BF \u03C0\u03BB\u03B5\u03C5\u03C1\u03AD\u03C2 \u03B5\u03BD\u03CC\u03C2 \u03C3\u03CE\u03BC\u03B1\u03C4\u03BF\u03C2."@el , "\uC720\uCCB4\uB3D9\uC5ED\uD559\uC5D0\uC11C \uD56D\uB825(\u6297\u529B, drag)\uC740 \u2018\uBB3C\uCCB4\uAC00 \uC720\uCCB4 \uB0B4\uB97C \uC6C0\uC9C1\uC77C \uB54C \uC774 \uC6C0\uC9C1\uC784\uC5D0 \uC800\uD56D\uD558\uB294 \uD798\u2019\uC774\uB2E4. \uD56D\uB825\uC740 \uB9C8\uCC30\uB825\uACFC \uC555\uB825\uC73C\uB85C \uAD6C\uBD84\uB41C\uB2E4. \uB9C8\uCC30\uB825\uC740 \uBB3C\uCCB4\uC758 \uD45C\uBA74\uC5D0 \uD3C9\uD589\uD55C \uBC29\uD5A5\uC73C\uB85C \uC791\uC6A9\uD558\uBA70, \uC555\uB825\uC740 \uBB3C\uCCB4\uC758 \uD45C\uBA74\uC5D0 \uC218\uC9C1\uD55C \uBC29\uD5A5\uC73C\uB85C \uC791\uC6A9\uD55C\uB2E4. \uC720\uCCB4 \uB0B4\uC5D0\uC11C \uC6C0\uC9C1\uC774\uB294 \uACE0\uCCB4 \uBB3C\uCCB4\uC758 \uACBD\uC6B0, \uD56D\uB825\uC740 \u2018\uC720\uCCB4\uC758 \uC720\uB3D9\uACFC \uB3D9\uC77C\uD55C \uBC29\uD5A5\uC73C\uB85C \uC791\uC6A9\uD558\uB294 \uBAA8\uB4E0 \uC720\uCCB4\uC5ED\uD559\uC801 \uD798\uC758 \uD569\u2019\uC774\uB2E4. \uB530\uB77C\uC11C \uD56D\uB825\uC740 \uBB3C\uCCB4\uC758 \uC6C0\uC9C1\uC784\uC744 \uBC29\uD574\uD558\uB294 \uD798\uC774\uB2E4. \uD56D\uACF5\uAE30\uC5D0\uC11C \uCD94\uB825\uC774 \uD544\uC694\uD55C \uAC83\uC740 \uBC14\uB85C \uC774 \uD56D\uB825\uC774\uB77C\uB294 \uD798\uC744 \uADF9\uBCF5\uD558\uACE0 \uB098\uC544\uAC00\uAE30 \uC704\uD574\uC11C\uC774\uB2E4. \uC720\uCCB4 \uC720\uB3D9\uC758 \uBC29\uD5A5\uC5D0 \uC218\uC9C1\uC73C\uB85C \uC791\uC6A9\uD558\uB294 \uD798\uC740 \uC591\uB825(lift)\uC774\uB77C\uACE0 \uD55C\uB2E4. \uBB3C\uCCB4\uC5D0 \uB300\uD55C \uD56D\uB825\uC740 \uBB34\uCC28\uC6D0 \uC218\uC778 \uD56D\uB825 \uACC4\uC218(Cd, drag coefficient, coefficient of drag)\uB85C \uB098\uD0C0\uB0BC \uC218 \uC788\uC73C\uBA70, \uD56D\uB825 \uBC29\uC815\uC2DD\uC744 \uC0AC\uC6A9\uD574 \uACC4\uC0B0\uD560 \uC218 \uC788\uB2E4. \uD56D\uB825 \uACC4\uC218\uB97C \uC0C1\uC218\uB77C\uACE0 \uAC00\uC815\uD55C\uB2E4\uBA74, \uC77C\uBC18\uC801\uC73C\uB85C \uD56D\uB825\uC740 \uC18D\uB3C4\uC758 \uC81C\uACF1\uC5D0 \uBE44\uB840\uD55C\uB2E4."@ko , "F\u00F3rsa a chuireann bac ar ghluaiseacht r\u00E9ada tr\u00ED shreabh\u00E1n. Tarla\u00EDonn s\u00ED de bharr frithchuimilte idir an r\u00E9ad is an sreabh\u00E1n ag sreabhadh thar dhromchla an r\u00E9ada (c\u00FAltarraingt shlaodach n\u00F3 fhrithchuimilteach) agus na difr\u00EDochta\u00ED br\u00FA de bharr an tsreafa m\u00F3rthimpeall an r\u00E9ada (c\u00FAltarraingt foirme n\u00F3 phr\u00F3if\u00EDle). Tugtar friota\u00EDocht aeir ar an gc\u00FAltarraingt ar r\u00E9ad i sruth aeir."@ga , "Dalam dinamika fluida, gaya hambat (yang kadang-kadang disebut hambatan fluida atau seretan) adalah gaya yang menghambat pergerakan sebuah benda padat melalui sebuah fluida ( cairan atau gas). Bentuk gaya hambat yang paling umum tersusun dari sejumlah gaya gesek, yang bertindak sejajar dengan permukaan benda, plus gaya tekanan, yang bertindak dalam arah tegak lurus dengan permukaan benda. Bagi sebuah benda padat yang bergerak melalui sebuah fluida, gaya hambat merupakan komponen dari aerodinamika atau gaya dinamika fluida yang bekerja dalam arahnya pergerakan. Komponen tegak lurus terhadap arah pergerakan ini dianggap sebagai gaya angkat. Dengan begitu gaya hambat berlawanan dengan arah pergerakan benda, dan dalam sebuah kendaraan yang digerakkan mesin diatasi dengan gaya dorong."@in , "\u0410\u0435\u0440\u043E\u0433\u0456\u0434\u0440\u043E\u0434\u0438\u043D\u0430\u043C\u0456\u0447\u043D\u0438\u0439 (\u043B\u043E\u0431\u043E\u0432\u0438\u0439) \u043E\u043F\u0456\u0440 \u2014 \u043E\u043F\u0456\u0440 \u0440\u0443\u0445\u043E\u0432\u0456 \u0442\u0456\u043B\u0430 \u0432 \u0433\u0430\u0437\u0456 \u0430\u0431\u043E \u0440\u0456\u0434\u0438\u043D\u0456."@uk , "\u0645\u0642\u0627\u0648\u0645\u0629 \u0627\u0644\u0645\u0627\u0626\u0639 (\u0628\u0627\u0644\u0625\u0646\u062C\u0644\u064A\u0632\u064A\u0629: Drag)\u200F \u0623\u0648 \u0627\u0644\u0625\u0639\u0627\u0642\u0629 \u0647\u064A \u0645\u0635\u0637\u0644\u062D \u064A\u0633\u062A\u062E\u062F\u0645 \u0641\u064A \u0639\u0644\u0645 \u062F\u064A\u0646\u0627\u0645\u064A\u0643\u0627 \u0627\u0644\u0645\u0648\u0627\u0626\u0639 \u064A\u0634\u064A\u0631 \u0625\u0644\u0649 \u0627\u0644\u0642\u0648\u0649 \u0627\u0644\u062A\u064A \u062A\u0639\u064A\u0642 \u0645\u0646 \u0645\u0631\u0648\u0631 \u062C\u0633\u0645 \u062E\u0644\u0627\u0644 \u0645\u0627\u062F\u0629 \u0645\u0627\u0626\u0639\u0629 (\u063A\u0627\u0632 \u0623\u0648 \u0633\u0627\u0626\u0644) \u0645\u062B\u0644 \u0627\u0644\u0645\u0627\u0621 \u0623\u0648 \u0627\u0644\u0647\u0648\u0627\u0621. \u062A\u062A\u0646\u0627\u0633\u0628 \u0647\u0630\u0647 \u0627\u0644\u0625\u0639\u0627\u0642\u0629 \u0637\u0631\u062F\u064A\u0627 \u0645\u0639 \u0633\u0631\u0639\u0629 \u0627\u0644\u062C\u0633\u0645 \u0641\u064A \u0627\u0644\u0633\u0627\u0626\u0644\u060C \u0639\u0644\u0649 \u0639\u0643\u0633 \u0627\u0644\u0627\u062D\u062A\u0643\u0627\u0643 \u0627\u0644\u0630\u064A \u0644\u0627\u064A\u062A\u0623\u062B\u0631 \u0628\u0627\u0644\u0633\u0631\u0639\u0629 (\u0642\u0627\u0631\u0646 \u0627\u0644\u062D\u0627\u0644\u0627\u062A \u0641\u064A \u0627\u0644\u0634\u0643\u0644 \u0628\u064A\u0646 \u0627\u0644\u0625\u0639\u0627\u0642\u0629 \u0648\u0627\u0644\u0627\u062D\u062A\u0643\u0627\u0643 friction)."@ar , "\u041B\u043E\u0431\u043E\u0432\u043E\u0435 \u0441\u043E\u043F\u0440\u043E\u0442\u0438\u0432\u043B\u0435\u043D\u0438\u0435 \u2014 \u0441\u0438\u043B\u0430, \u043F\u0440\u0435\u043F\u044F\u0442\u0441\u0442\u0432\u0443\u044E\u0449\u0430\u044F \u0434\u0432\u0438\u0436\u0435\u043D\u0438\u044E \u0442\u0435\u043B \u0432 \u0436\u0438\u0434\u043A\u043E\u0441\u0442\u044F\u0445 \u0438 \u0433\u0430\u0437\u0430\u0445. \u041B\u043E\u0431\u043E\u0432\u043E\u0435 \u0441\u043E\u043F\u0440\u043E\u0442\u0438\u0432\u043B\u0435\u043D\u0438\u0435 \u0441\u043A\u043B\u0430\u0434\u044B\u0432\u0430\u0435\u0442\u0441\u044F \u0438\u0437 \u0434\u0432\u0443\u0445 \u0442\u0438\u043F\u043E\u0432 \u0441\u0438\u043B: \u0441\u0438\u043B \u043A\u0430\u0441\u0430\u0442\u0435\u043B\u044C\u043D\u043E\u0433\u043E (\u0442\u0430\u043D\u0433\u0435\u043D\u0446\u0438\u0430\u043B\u044C\u043D\u043E\u0433\u043E) \u0442\u0440\u0435\u043D\u0438\u044F, \u043D\u0430\u043F\u0440\u0430\u0432\u043B\u0435\u043D\u043D\u044B\u0445 \u0432\u0434\u043E\u043B\u044C \u043F\u043E\u0432\u0435\u0440\u0445\u043D\u043E\u0441\u0442\u0438 \u0442\u0435\u043B\u0430, \u0438 \u0441\u0438\u043B \u0434\u0430\u0432\u043B\u0435\u043D\u0438\u044F, \u043D\u0430\u043F\u0440\u0430\u0432\u043B\u0435\u043D\u043D\u044B\u0445 \u043F\u043E \u043D\u043E\u0440\u043C\u0430\u043B\u0438 \u043A \u043F\u043E\u0432\u0435\u0440\u0445\u043D\u043E\u0441\u0442\u0438. \u0421\u0438\u043B\u0430 \u0441\u043E\u043F\u0440\u043E\u0442\u0438\u0432\u043B\u0435\u043D\u0438\u044F \u044F\u0432\u043B\u044F\u0435\u0442\u0441\u044F \u0434\u0438\u0441\u0441\u0438\u043F\u0430\u0442\u0438\u0432\u043D\u043E\u0439 \u0441\u0438\u043B\u043E\u0439 \u0438 \u0432\u0441\u0435\u0433\u0434\u0430 \u043D\u0430\u043F\u0440\u0430\u0432\u043B\u0435\u043D\u0430 \u043F\u0440\u043E\u0442\u0438\u0432 \u0432\u0435\u043A\u0442\u043E\u0440\u0430 \u0441\u043A\u043E\u0440\u043E\u0441\u0442\u0438 \u0442\u0435\u043B\u0430 \u0432 \u0441\u0440\u0435\u0434\u0435. \u041D\u0430\u0440\u044F\u0434\u0443 \u0441 \u043F\u043E\u0434\u044A\u0451\u043C\u043D\u043E\u0439 \u0441\u0438\u043B\u043E\u0439 \u044F\u0432\u043B\u044F\u0435\u0442\u0441\u044F \u0441\u043E\u0441\u0442\u0430\u0432\u043B\u044F\u044E\u0449\u0435\u0439 \u043F\u043E\u043B\u043D\u043E\u0439 \u0430\u044D\u0440\u043E\u0434\u0438\u043D\u0430\u043C\u0438\u0447\u0435\u0441\u043A\u043E\u0439 \u0441\u0438\u043B\u044B."@ru , "Na din\u00E2mica dos fluidos, arrasto \u00E9 a for\u00E7a que faz resist\u00EAncia ao movimento de um objeto s\u00F3lido atrav\u00E9s de um fluido (um l\u00EDquido ou g\u00E1s). O arrasto \u00E9 feito de for\u00E7as de fric\u00E7\u00E3o (atrito), que agem em dire\u00E7\u00E3o paralela \u00E0 superf\u00EDcie do objeto (primariamente pelos seus lados, j\u00E1 que as for\u00E7as de fric\u00E7\u00E3o da frente e de tr\u00E1s se anulam), e de for\u00E7as de press\u00E3o, que atuam em uma dire\u00E7\u00E3o perpendicular \u00E0 superf\u00EDcie do objeto (primariamente na frente e atr\u00E1s, j\u00E1 que as for\u00E7as de press\u00E3o se cancelam nas laterais do objeto). Ao contr\u00E1rio de outras for\u00E7as resistivas, como o atrito, que \u00E9 quase independente da velocidade, for\u00E7as de arrasto dependem da velocidade. Um exemplo de for\u00E7as dependentes da velocidade \u00E9 o arrasto aerodin\u00E2mico, como o usado para explicar o desempenho de Usain Bolt."@pt , "En m\u00E9canique des fluides, la tra\u00EEn\u00E9e ou train\u00E9e est la force qui s'oppose au mouvement d'un corps dans un liquide ou un gaz et agit comme un frottement. Math\u00E9matiquement, c'est la composante des efforts exerc\u00E9s sur le corps, dans le sens oppos\u00E9 \u00E0 la v\u00E9locit\u00E9 relative du corps par rapport au fluide. En a\u00E9rodynamique, c'est, avec la portance, l'une des deux grandeurs fondamentales. Le rapport entre portance et tra\u00EEn\u00E9e s'appelle la finesse."@fr , "Luftmotst\u00E5nd \u00E4r en kraft som beror p\u00E5 det mekaniska motst\u00E5nd som str\u00F6mmande luft orsakar. Det finns p\u00E5 grund av luftens molekyler. Till exempel n\u00E4r man cyklar studsar dessa mot en och man f\u00F6rlorar r\u00F6relseenergi som molekylerna tar upp. Luftmotst\u00E5ndet \u00E4r proportionellt mot tv\u00E4rsnittsytan och mot kvadraten p\u00E5 hastigheten. Detta beror p\u00E5 att molekylernas r\u00F6relseenergi \u00E4r en kvadrat p\u00E5 hastigheten och sedan p\u00E5 att antalet luftmolekyler som kolliderar med f\u00F6rem\u00E5let \u00E4r proportionellt mot tv\u00E4rsnittsytan. Luftmotst\u00E5ndet ber\u00E4knas som d\u00E4r"@sv , "Stromingsweerstand (in het Engels drag) is de weerstandskracht op een bewegend object in een stationair flu\u00EFdum of een bewegend flu\u00EFdum langs een stationair object. Die kracht zal dus altijd in de tegenovergestelde richting van de beweging werken. Het object kan in sommige gevallen ook een flu\u00EFdum (of het contactoppervlak van de twee) zijn, wanneer twee flu\u00EFdum-lagen apart van elkaar bewegen en in contact zijn. Echter is het in de bekende gevallen een object van een vaste stof langs een flu\u00EFdum. Het is een primair begrip in de stromingsleer, fysische transportverschijnselen, aerodynamica en hydrauliek."@nl , "Op\u00F3r aero(hydro)dynamiczny \u2013 sk\u0142adowa wektora si\u0142y aerodynamicznej lub , r\u00F3wnoleg\u0142a do kierunku ruchu cia\u0142a wzgl\u0119dem p\u0142ynu i skierowana zawsze przeciwnie do kierunku ruchu cia\u0142a. Si\u0142a aerodynamiczna powstaje podczas ruchu cia\u0142a w p\u0142ynie; gdy ruch cia\u0142a ustaje, si\u0142a oporu zanika. Op\u00F3r aero(hydro)dynamiczny traktowa\u0107 mo\u017Cna jako rodzaj si\u0142y biernej, przy\u0142o\u017Conej do poruszaj\u0105cego si\u0119 cia\u0142a."@pl , "Odpor prost\u0159ed\u00ED je soubor v\u0161ech sil, kter\u00FDmi plyn nebo kapalina p\u016Fsob\u00ED proti pohybu t\u011Bles v n\u011Bm. Odpor je zp\u016Fsoben t\u0159en\u00EDm, kter\u00E9 vznik\u00E1 p\u0159i kontaktu t\u011Blesa a prost\u0159ed\u00ED. Proto\u017Ee pohyb je relativn\u00ED, je jedno, jestli se t\u011Bleso pohybuje v nehybn\u00E9m plynu nebo kapalin\u011B, nebo jestli je t\u011Bleso v klidu a kolem n\u011Bj proud\u00ED plyn nebo kapalina (v takov\u00E9m p\u0159\u00EDpad\u011B se \u010Dasto hovo\u0159\u00ED o obt\u00E9k\u00E1n\u00ED t\u011Bles). Rozhoduj\u00EDc\u00ED je relativn\u00ED rychlost mezi t\u011Blesem a tekutinou."@cs , "\u6297\u529B\uFF08\u3053\u3046\u308A\u3087\u304F\u3001\u82F1: drag\uFF09\u3068\u306F\u3001\u6D41\u4F53\uFF08\u6DB2\u4F53\u3084\u6C17\u4F53\uFF09\u4E2D\u3092\u79FB\u52D5\u3059\u308B\u3001\u3042\u308B\u3044\u306F\u6D41\u308C\u4E2D\u306B\u304A\u304B\u308C\u305F\u7269\u4F53\u306B\u306F\u305F\u3089\u304F\u529B\u306E\u3001\u6D41\u308C\u306E\u901F\u5EA6\u306B\u5E73\u884C\u306A\u65B9\u5411\u3067\u540C\u3058\u5411\u304D\u306E\u6210\u5206\uFF08\u5206\u529B\uFF09\u3067\u3042\u308B\u3002\u6D41\u308C\u306E\u901F\u5EA6\u65B9\u5411\u306B\u5782\u76F4\u306A\u6210\u5206\u306F\u63DA\u529B\u3068\u3044\u3046\u3002 \u8FFD\u3044\u98A8\u3067\u6C34\u9762\u3092\u304B\u304D\u5206\u3051\u3066\u9032\u3093\u3067\u3044\u308B\u5E06\u8239\u306F\u3001\u7A7A\u6C17\u304B\u3089\u9032\u884C\u65B9\u5411\u306E\u6297\u529B\u3092\u3001\u305D\u308C\u3088\u308A\u5F31\u3044\u9006\u65B9\u5411\u306E\u6297\u529B\u3092\u6C34\u304B\u3089\u53D7\u3051\u3066\u3044\u308B\u3002\u307E\u305F\u3001\u30EC\u30FC\u30B7\u30F3\u30B0\u30AB\u30FC\u7B49\u3067\u306F\u30DE\u30A4\u30CA\u30B9\u306E\u63DA\u529B\u3067\u30C0\u30A6\u30F3\u30D5\u30A9\u30FC\u30B9\u3092\u767A\u751F\u3055\u305B\u3066\u3044\u308B\u3002\u6297\u529B\u3082\u63DA\u529B\u3082\u30B1\u30FC\u30B9\u30D0\u30A4\u30B1\u30FC\u30B9\u3067\u3001\u305D\u306E\u65B9\u5411\u304C\u5B57\u7FA9\u901A\u308A\u3067\u306F\u306A\u3044\u5834\u5408\u304C\u3042\u308B\u3002"@ja , "En din\u00E1mica de fluidos, la resistencia o fricci\u00F3n de fluido, incorrectamente denominada en ocasiones como arrastre, es la fricci\u00F3n entre un objeto s\u00F3lido y el fluido (un l\u00EDquido o gas) por el que se mueve. En el caso particular de que el fluido sea l\u00EDquido (por ejemplo, el agua), se denomina resistencia hidrodin\u00E1mica, mientras que en el caso de que el fluido sea gaseoso (por ejemplo, el aire atmosf\u00E9rico), se denomina resistencia aerodin\u00E1mica. En la f\u00EDsica del deporte, tiene muchas aplicaciones como por ejemplo, explicar el alto rendimiento del corredor Usain Bolt.\u200B"@es , "\u963B\u529B\uFF08\u53C8\u79F0\u5F8C\u66F3\u529B\u6216\u6D41\u9AD4\u963B\u529B\uFF09\u662F\u7269\u9AD4\u5728\u6D41\u9AD4\u4E2D\u76F8\u5C0D\u904B\u52D5\u6240\u7522\u751F\u8207\u904B\u52D5\u65B9\u5411\u76F8\u53CD\u7684\u529B\u3002\u5C0D\u65BC\u4E00\u500B\u5728\u6D41\u9AD4\u4E2D\u79FB\u52D5\u7684\u7269\u9AD4\uFF0C\u963B\u529B\u70BA\u5468\u570D\u6D41\u9AD4\u5C0D\u7269\u9AD4\u65BD\u529B\uFF0C\u5728\u79FB\u52D5\u65B9\u5411\u7684\u53CD\u65B9\u5411\u4E0A\u5206\u91CF\u7684\u7E3D\u548C\u3002\u800C\u65BD\u529B\u548C\u79FB\u52D5\u65B9\u5411\u5782\u76F4\u7684\u5206\u91CF\u4E00\u822C\u5247\u8996\u70BA\u5347\u529B\u3002\u56E0\u6B64\u963B\u529B\u548C\u7269\u9AD4\u79FB\u52D5\u65B9\u5411\u6070\u597D\u76F8\u53CD\uFF0C\u50CF\u98DB\u6A5F\u524D\u9032\u6642\u6703\u7522\u751F\u63A8\u529B\u4F86\u514B\u670D\u963B\u529B\u7684\u5F71\u97FF\u3002 \u5728\u822A\u5929\u52A8\u529B\u5B66\u4E2D\uFF0C\u5927\u6C23\u963B\u529B\u53EF\u4EE5\u8996\u70BA\u592A\u7A7A\u98DB\u884C\u5668\u5728\u767C\u5C04\u6642\u7684\u4F4E\u6548\u7387\uFF0C\u5176\u5F71\u97FF\u5247\u662F\u5728\u767C\u5C04\u6642\u9700\u8981\u984D\u5916\u7684\u80FD\u91CF\uFF0C\u4E0D\u904E\u5728\u8FD4\u56DE\u8ECC\u9053\u6642\u5927\u6C23\u963B\u529B\u6709\u52A9\u65BC\u592A\u7A7A\u98DB\u884C\u5668\u6E1B\u901F\uFF0C\u53EF\u6E1B\u5C11\u6E1B\u901F\u984D\u5916\u9700\u8981\u7684\u80FD\u91CF\uFF0C\u4E0D\u904E\u5927\u6C23\u963B\u529B\u7522\u751F\u7684\u71B1\u91CF\u751A\u81F3\u53EF\u4EE5\u5C07\u7269\u9AD4\u7194\u5316\u3002"@zh , "Der Str\u00F6mungswiderstand ist eine physikalische Gr\u00F6\u00DFe, die in der Fluiddynamik die Kraft bezeichnet, die das Fluid als Medium einer Bewegung entgegensetzt.Ein K\u00F6rper, der sich relativ zu einem gasf\u00F6rmigen oder fl\u00FCssigen Medium bewegt, erf\u00E4hrt einen Str\u00F6mungswiderstand, eine der Relativgeschwindigkeit entgegengesetzt wirkende Kraft.Bewegt sich ein Objekt wie ein Flugzeug durch die Luft, so spricht man auch vom Luftwiderstand oder von der Luftreibung, siehe auch Aerodynamik. Bei Bewegungen im Wasser spricht man von Wasserwiderstand, siehe auch Hydrodynamik."@de ; foaf:depiction , , , , , , , , , , , . @prefix dcterms: . @prefix dbc: . dcterms:subject dbc:Articles_containing_video_clips , dbc:Force , ; dbo:abstract "Stromingsweerstand (in het Engels drag) is de weerstandskracht op een bewegend object in een stationair flu\u00EFdum of een bewegend flu\u00EFdum langs een stationair object. Die kracht zal dus altijd in de tegenovergestelde richting van de beweging werken. Het object kan in sommige gevallen ook een flu\u00EFdum (of het contactoppervlak van de twee) zijn, wanneer twee flu\u00EFdum-lagen apart van elkaar bewegen en in contact zijn. Echter is het in de bekende gevallen een object van een vaste stof langs een flu\u00EFdum. Het is een primair begrip in de stromingsleer, fysische transportverschijnselen, aerodynamica en hydrauliek."@nl , "F\u00F3rsa a chuireann bac ar ghluaiseacht r\u00E9ada tr\u00ED shreabh\u00E1n. Tarla\u00EDonn s\u00ED de bharr frithchuimilte idir an r\u00E9ad is an sreabh\u00E1n ag sreabhadh thar dhromchla an r\u00E9ada (c\u00FAltarraingt shlaodach n\u00F3 fhrithchuimilteach) agus na difr\u00EDochta\u00ED br\u00FA de bharr an tsreafa m\u00F3rthimpeall an r\u00E9ada (c\u00FAltarraingt foirme n\u00F3 phr\u00F3if\u00EDle). Tugtar friota\u00EDocht aeir ar an gc\u00FAltarraingt ar r\u00E9ad i sruth aeir."@ga , "La resistenza fluidodinamica \u00E8 quella forza che si oppone al movimento di un corpo in un fluido, in particolare in un liquido o un aeriforme. In riferimento al moto nei liquidi \u00E8 anche indicata come resistenza idrodinamica, nel caso degli aeriformi come resistenza aerodinamica."@it , "Odpor prost\u0159ed\u00ED je soubor v\u0161ech sil, kter\u00FDmi plyn nebo kapalina p\u016Fsob\u00ED proti pohybu t\u011Bles v n\u011Bm. Odpor je zp\u016Fsoben t\u0159en\u00EDm, kter\u00E9 vznik\u00E1 p\u0159i kontaktu t\u011Blesa a prost\u0159ed\u00ED. Proto\u017Ee pohyb je relativn\u00ED, je jedno, jestli se t\u011Bleso pohybuje v nehybn\u00E9m plynu nebo kapalin\u011B, nebo jestli je t\u011Bleso v klidu a kolem n\u011Bj proud\u00ED plyn nebo kapalina (v takov\u00E9m p\u0159\u00EDpad\u011B se \u010Dasto hovo\u0159\u00ED o obt\u00E9k\u00E1n\u00ED t\u011Bles). Rozhoduj\u00EDc\u00ED je relativn\u00ED rychlost mezi t\u011Blesem a tekutinou. S\u00EDly, kter\u00E9 v d\u016Fsledku t\u0159en\u00ED p\u016Fsob\u00ED proti pohybu t\u011Blesa, se ozna\u010Duj\u00ED jako odporov\u00E9 s\u00EDly. Odporov\u00E1 s\u00EDla p\u016Fsob\u00ED v\u017Edy proti sm\u011Bru relativn\u00EDho pohybu, tzn. t\u011Bleso pohybuj\u00EDc\u00ED se v nehybn\u00E9 tekutin\u011B je zpomalov\u00E1no, zat\u00EDmco nehybn\u00E9 t\u011Bleso v pohybuj\u00EDc\u00ED se tekutin\u011B je tekutinou urychlov\u00E1no. Nap\u0159. odpor prost\u0159ed\u00ED (odpor vzduchu) na Zemi zp\u016Fsobuje \"rychlej\u0161\u00ED p\u00E1d\" t\u011B\u017E\u0161\u00EDch p\u0159edm\u011Bt\u016F. Pokud v\u0161ak na t\u011Blesa p\u016Fsob\u00ED pouze gravitace a \u017E\u00E1dn\u00FD odpor prost\u0159ed\u00ED, padaj\u00ED v\u0161echna stejnou rychlost\u00ED, co\u017E m\u016F\u017Eeme dok\u00E1zat situac\u00ED v prost\u0159ed\u00ED bez odporu prost\u0159ed\u00ED (nap\u0159. vakuov\u00E1 komora nebo n\u00E1\u0161 M\u011Bs\u00EDc), kde t\u011B\u017E\u0161\u00ED i leh\u010D\u00ED t\u011Bleso dopadnou na vodorovn\u00FD povrch ve stejnou chv\u00EDli, jsou-li upu\u0161t\u011Bna ze stejn\u00E9 v\u00FD\u0161ky a ve stejnou dobu."@cs , "En din\u00E1mica de fluidos, la resistencia o fricci\u00F3n de fluido, incorrectamente denominada en ocasiones como arrastre, es la fricci\u00F3n entre un objeto s\u00F3lido y el fluido (un l\u00EDquido o gas) por el que se mueve. En el caso particular de que el fluido sea l\u00EDquido (por ejemplo, el agua), se denomina resistencia hidrodin\u00E1mica, mientras que en el caso de que el fluido sea gaseoso (por ejemplo, el aire atmosf\u00E9rico), se denomina resistencia aerodin\u00E1mica. Para un s\u00F3lido que se mueve por un fluido, la resistencia es la suma de todas las fuerzas aerodin\u00E1micas o hidrodin\u00E1micas en la direcci\u00F3n del flujo del fluido externo. Por lo tanto, act\u00FAa opuestamente al movimiento del objeto, y en un veh\u00EDculo motorizado esto se resuelve con el empuje. Generalmente al estudiar el movimiento bi o tridimensional de un objeto, casi siempre se ignora la resistencia del aire. En muchos problemas esta es una excelente aproximaci\u00F3n; en otros, la resistencia del aire es importante, y se necesita saber c\u00F3mo cuantificarla. Si bien se habla generalmente de resistencia \"del aire\", porque el aire es el medio a trav\u00E9s del cual se mueven los cuerpos, se pueden aplicar las mismas consideraciones para otros gases e incluso l\u00EDquidos. Sin embargo en el presente art\u00EDculo se asume que la fuerza de resistencia f y la velocidad v tienen la misma direcci\u00F3n pero sentidos opuestos. Esto es, se consideran solamente objetos en los que la fuerza lateral es cero o despreciable. La situaci\u00F3n es ilustrada en la figura adjunta. En la astrodin\u00E1mica, dependiendo de la situaci\u00F3n, la resistencia atmosf\u00E9rica se puede considerar como una ineficiencia que requiere energ\u00EDa adicional durante el lanzamiento de un objeto al espacio o como una ventaja que simplifica el regreso desde la \u00F3rbita. En la f\u00EDsica del deporte, tiene muchas aplicaciones como por ejemplo, explicar el alto rendimiento del corredor Usain Bolt.\u200B"@es , "Der Str\u00F6mungswiderstand ist eine physikalische Gr\u00F6\u00DFe, die in der Fluiddynamik die Kraft bezeichnet, die das Fluid als Medium einer Bewegung entgegensetzt.Ein K\u00F6rper, der sich relativ zu einem gasf\u00F6rmigen oder fl\u00FCssigen Medium bewegt, erf\u00E4hrt einen Str\u00F6mungswiderstand, eine der Relativgeschwindigkeit entgegengesetzt wirkende Kraft.Bewegt sich ein Objekt wie ein Flugzeug durch die Luft, so spricht man auch vom Luftwiderstand oder von der Luftreibung, siehe auch Aerodynamik. Bei Bewegungen im Wasser spricht man von Wasserwiderstand, siehe auch Hydrodynamik. Wenn ein Fluid hingegen durch eine Rohrleitung str\u00F6mt, so erf\u00E4hrt es aufgrund der Rohrreibung entlang der zur\u00FCckgelegten Strecke einen Druckverlust. Siehe: Str\u00F6mungen in Rohrleitungen"@de , "Na din\u00E2mica dos fluidos, arrasto \u00E9 a for\u00E7a que faz resist\u00EAncia ao movimento de um objeto s\u00F3lido atrav\u00E9s de um fluido (um l\u00EDquido ou g\u00E1s). O arrasto \u00E9 feito de for\u00E7as de fric\u00E7\u00E3o (atrito), que agem em dire\u00E7\u00E3o paralela \u00E0 superf\u00EDcie do objeto (primariamente pelos seus lados, j\u00E1 que as for\u00E7as de fric\u00E7\u00E3o da frente e de tr\u00E1s se anulam), e de for\u00E7as de press\u00E3o, que atuam em uma dire\u00E7\u00E3o perpendicular \u00E0 superf\u00EDcie do objeto (primariamente na frente e atr\u00E1s, j\u00E1 que as for\u00E7as de press\u00E3o se cancelam nas laterais do objeto). Ao contr\u00E1rio de outras for\u00E7as resistivas, como o atrito, que \u00E9 quase independente da velocidade, for\u00E7as de arrasto dependem da velocidade. Um exemplo de for\u00E7as dependentes da velocidade \u00E9 o arrasto aerodin\u00E2mico, como o usado para explicar o desempenho de Usain Bolt."@pt , "In fluid dynamics, drag (sometimes called air resistance, a type of friction, or fluid resistance, another type of friction or fluid friction) is a force acting opposite to the relative motion of any object moving with respect to a surrounding fluid. This can exist between two fluid layers (or surfaces) or between a fluid and a solid surface. Unlike other resistive forces, such as dry friction, which are nearly independent of velocity, the drag force depends on velocity. Drag force is proportional to the velocity for low-speed flow and the squared velocity for high speed flow, where the distinction between low and high speed is measured by the Reynolds number. Even though the ultimate cause of drag is viscous friction, turbulent drag is independent of viscosity. Drag forces always tend to decrease fluid velocity relative to the solid object in the fluid's path."@en , "Op\u00F3r aero(hydro)dynamiczny \u2013 sk\u0142adowa wektora si\u0142y aerodynamicznej lub , r\u00F3wnoleg\u0142a do kierunku ruchu cia\u0142a wzgl\u0119dem p\u0142ynu i skierowana zawsze przeciwnie do kierunku ruchu cia\u0142a. Si\u0142a aerodynamiczna powstaje podczas ruchu cia\u0142a w p\u0142ynie; gdy ruch cia\u0142a ustaje, si\u0142a oporu zanika. Op\u00F3r aero(hydro)dynamiczny traktowa\u0107 mo\u017Cna jako rodzaj si\u0142y biernej, przy\u0142o\u017Conej do poruszaj\u0105cego si\u0119 cia\u0142a."@pl , "\u0391\u03BD\u03C4\u03AF\u03C3\u03C4\u03B1\u03C3\u03B7 \u03AE \u03BF\u03C0\u03B9\u03C3\u03B8\u03AD\u03BB\u03BA\u03BF\u03C5\u03C3\u03B1 (drag) \u03BF\u03BD\u03BF\u03BC\u03AC\u03B6\u03B5\u03C4\u03B1\u03B9 \u03B7 \u03B4\u03CD\u03BD\u03B1\u03BC\u03B7 \u03B7 \u03BF\u03C0\u03BF\u03AF\u03B1 \u03AD\u03C7\u03B5\u03B9 \u03C4\u03BF\u03BD \u03AF\u03B4\u03B9\u03BF \u03C6\u03BF\u03C1\u03AD\u03B1 \u03BC\u03B5 \u03B1\u03C5\u03C4\u03CC\u03BD \u03C4\u03B7\u03C2 \u03C4\u03B1\u03C7\u03CD\u03C4\u03B7\u03C4\u03B1\u03C2, \u03B1\u03BB\u03BB\u03AC \u03B1\u03BD\u03C4\u03AF\u03B8\u03B5\u03C4\u03B7 \u03C6\u03BF\u03C1\u03AC, \u03BA\u03B1\u03B9 \u03B5\u03BC\u03C6\u03B1\u03BD\u03AF\u03B6\u03B5\u03C4\u03B1\u03B9 \u03BA\u03B1\u03C4\u03AC \u03C4\u03B7\u03BD \u03BA\u03AF\u03BD\u03B7\u03C3\u03B7 \u03B1\u03BD\u03C4\u03B9\u03BA\u03B5\u03B9\u03BC\u03AD\u03BD\u03C9\u03BD \u03B5\u03BD\u03C4\u03CC\u03C2 \u03C1\u03B5\u03C5\u03C3\u03C4\u03BF\u03CD. \u0397 \u03C0\u03B1\u03C1\u03BF\u03C5\u03C3\u03AF\u03B1 \u03C4\u03B7\u03C2 \u03B4\u03CD\u03BD\u03B1\u03BC\u03B7\u03C2 \u03BF\u03C6\u03B5\u03AF\u03BB\u03B5\u03C4\u03B1\u03B9 \u03C3\u03C4\u03B7 \u03B4\u03B9\u03B1\u03C6\u03BF\u03C1\u03B5\u03C4\u03B9\u03BA\u03AE \u03C0\u03AF\u03B5\u03C3\u03B7 \u03B7 \u03BF\u03C0\u03BF\u03AF\u03B1 \u03B5\u03C0\u03B9\u03BA\u03C1\u03B1\u03C4\u03B5\u03AF \u03C3\u03C4\u03B9\u03C2 \u03B4\u03CD\u03BF \u03C0\u03BB\u03B5\u03C5\u03C1\u03AD\u03C2 \u03B5\u03BD\u03CC\u03C2 \u03C3\u03CE\u03BC\u03B1\u03C4\u03BF\u03C2."@el , "\u0645\u0642\u0627\u0648\u0645\u0629 \u0627\u0644\u0645\u0627\u0626\u0639 (\u0628\u0627\u0644\u0625\u0646\u062C\u0644\u064A\u0632\u064A\u0629: Drag)\u200F \u0623\u0648 \u0627\u0644\u0625\u0639\u0627\u0642\u0629 \u0647\u064A \u0645\u0635\u0637\u0644\u062D \u064A\u0633\u062A\u062E\u062F\u0645 \u0641\u064A \u0639\u0644\u0645 \u062F\u064A\u0646\u0627\u0645\u064A\u0643\u0627 \u0627\u0644\u0645\u0648\u0627\u0626\u0639 \u064A\u0634\u064A\u0631 \u0625\u0644\u0649 \u0627\u0644\u0642\u0648\u0649 \u0627\u0644\u062A\u064A \u062A\u0639\u064A\u0642 \u0645\u0646 \u0645\u0631\u0648\u0631 \u062C\u0633\u0645 \u062E\u0644\u0627\u0644 \u0645\u0627\u062F\u0629 \u0645\u0627\u0626\u0639\u0629 (\u063A\u0627\u0632 \u0623\u0648 \u0633\u0627\u0626\u0644) \u0645\u062B\u0644 \u0627\u0644\u0645\u0627\u0621 \u0623\u0648 \u0627\u0644\u0647\u0648\u0627\u0621. \u062A\u062A\u0646\u0627\u0633\u0628 \u0647\u0630\u0647 \u0627\u0644\u0625\u0639\u0627\u0642\u0629 \u0637\u0631\u062F\u064A\u0627 \u0645\u0639 \u0633\u0631\u0639\u0629 \u0627\u0644\u062C\u0633\u0645 \u0641\u064A \u0627\u0644\u0633\u0627\u0626\u0644\u060C \u0639\u0644\u0649 \u0639\u0643\u0633 \u0627\u0644\u0627\u062D\u062A\u0643\u0627\u0643 \u0627\u0644\u0630\u064A \u0644\u0627\u064A\u062A\u0623\u062B\u0631 \u0628\u0627\u0644\u0633\u0631\u0639\u0629 (\u0642\u0627\u0631\u0646 \u0627\u0644\u062D\u0627\u0644\u0627\u062A \u0641\u064A \u0627\u0644\u0634\u0643\u0644 \u0628\u064A\u0646 \u0627\u0644\u0625\u0639\u0627\u0642\u0629 \u0648\u0627\u0644\u0627\u062D\u062A\u0643\u0627\u0643 friction)."@ar , "\u6297\u529B\uFF08\u3053\u3046\u308A\u3087\u304F\u3001\u82F1: drag\uFF09\u3068\u306F\u3001\u6D41\u4F53\uFF08\u6DB2\u4F53\u3084\u6C17\u4F53\uFF09\u4E2D\u3092\u79FB\u52D5\u3059\u308B\u3001\u3042\u308B\u3044\u306F\u6D41\u308C\u4E2D\u306B\u304A\u304B\u308C\u305F\u7269\u4F53\u306B\u306F\u305F\u3089\u304F\u529B\u306E\u3001\u6D41\u308C\u306E\u901F\u5EA6\u306B\u5E73\u884C\u306A\u65B9\u5411\u3067\u540C\u3058\u5411\u304D\u306E\u6210\u5206\uFF08\u5206\u529B\uFF09\u3067\u3042\u308B\u3002\u6D41\u308C\u306E\u901F\u5EA6\u65B9\u5411\u306B\u5782\u76F4\u306A\u6210\u5206\u306F\u63DA\u529B\u3068\u3044\u3046\u3002 \u8FFD\u3044\u98A8\u3067\u6C34\u9762\u3092\u304B\u304D\u5206\u3051\u3066\u9032\u3093\u3067\u3044\u308B\u5E06\u8239\u306F\u3001\u7A7A\u6C17\u304B\u3089\u9032\u884C\u65B9\u5411\u306E\u6297\u529B\u3092\u3001\u305D\u308C\u3088\u308A\u5F31\u3044\u9006\u65B9\u5411\u306E\u6297\u529B\u3092\u6C34\u304B\u3089\u53D7\u3051\u3066\u3044\u308B\u3002\u307E\u305F\u3001\u30EC\u30FC\u30B7\u30F3\u30B0\u30AB\u30FC\u7B49\u3067\u306F\u30DE\u30A4\u30CA\u30B9\u306E\u63DA\u529B\u3067\u30C0\u30A6\u30F3\u30D5\u30A9\u30FC\u30B9\u3092\u767A\u751F\u3055\u305B\u3066\u3044\u308B\u3002\u6297\u529B\u3082\u63DA\u529B\u3082\u30B1\u30FC\u30B9\u30D0\u30A4\u30B1\u30FC\u30B9\u3067\u3001\u305D\u306E\u65B9\u5411\u304C\u5B57\u7FA9\u901A\u308A\u3067\u306F\u306A\u3044\u5834\u5408\u304C\u3042\u308B\u3002"@ja , "Luftmotst\u00E5nd \u00E4r en kraft som beror p\u00E5 det mekaniska motst\u00E5nd som str\u00F6mmande luft orsakar. Det finns p\u00E5 grund av luftens molekyler. Till exempel n\u00E4r man cyklar studsar dessa mot en och man f\u00F6rlorar r\u00F6relseenergi som molekylerna tar upp. Luftmotst\u00E5ndet \u00E4r proportionellt mot tv\u00E4rsnittsytan och mot kvadraten p\u00E5 hastigheten. Detta beror p\u00E5 att molekylernas r\u00F6relseenergi \u00E4r en kvadrat p\u00E5 hastigheten och sedan p\u00E5 att antalet luftmolekyler som kolliderar med f\u00F6rem\u00E5let \u00E4r proportionellt mot tv\u00E4rsnittsytan. Om ett f\u00F6rem\u00E5l r\u00F6r sig med h\u00F6g hastighet \u00E4r luftmotst\u00E5ndet stort. N\u00E4r en tung kropp med liten tv\u00E4rsnittsarea faller en kortare str\u00E4cka \u00E4r luftmotst\u00E5ndet i praktiken s\u00E5 litet att man kan bortse ifr\u00E5n det. D\u00E5 \u00E4r f\u00F6rem\u00E5let i fritt fall. Ett fallande f\u00F6rem\u00E5l n\u00E5r till slut en konstant hastighet, den s\u00E5 kallade gr\u00E4nshastigheten. Detta beror p\u00E5 att med hastigheten \u00F6kar \u00E4ven luftmotst\u00E5ndet, till den punkt d\u00E5 luftmotst\u00E5ndet blir lika stor som tyngdkraften som f\u00E5r f\u00F6rem\u00E5let att falla och f\u00F6rem\u00E5let d\u00E4rf\u00F6r slutar accelerera. Luftmotst\u00E5ndet ber\u00E4knas som d\u00E4r Fd \u00E4r luftmotst\u00E5ndetC \u00E4r luftmotst\u00E5ndskoefficienten, beroende p\u00E5 f\u00F6rem\u00E5lets str\u00F6mlinjeform, till exempel 0,25 till 0,45 f\u00F6r en personbil\u03C1 \u00E4r luftens densitetA \u00E4r f\u00F6rem\u00E5lets tv\u00E4rsnittsareav \u00E4r f\u00F6rem\u00E5lets relativa hastighet genom luften"@sv , "\u963B\u529B\uFF08\u53C8\u79F0\u5F8C\u66F3\u529B\u6216\u6D41\u9AD4\u963B\u529B\uFF09\u662F\u7269\u9AD4\u5728\u6D41\u9AD4\u4E2D\u76F8\u5C0D\u904B\u52D5\u6240\u7522\u751F\u8207\u904B\u52D5\u65B9\u5411\u76F8\u53CD\u7684\u529B\u3002\u5C0D\u65BC\u4E00\u500B\u5728\u6D41\u9AD4\u4E2D\u79FB\u52D5\u7684\u7269\u9AD4\uFF0C\u963B\u529B\u70BA\u5468\u570D\u6D41\u9AD4\u5C0D\u7269\u9AD4\u65BD\u529B\uFF0C\u5728\u79FB\u52D5\u65B9\u5411\u7684\u53CD\u65B9\u5411\u4E0A\u5206\u91CF\u7684\u7E3D\u548C\u3002\u800C\u65BD\u529B\u548C\u79FB\u52D5\u65B9\u5411\u5782\u76F4\u7684\u5206\u91CF\u4E00\u822C\u5247\u8996\u70BA\u5347\u529B\u3002\u56E0\u6B64\u963B\u529B\u548C\u7269\u9AD4\u79FB\u52D5\u65B9\u5411\u6070\u597D\u76F8\u53CD\uFF0C\u50CF\u98DB\u6A5F\u524D\u9032\u6642\u6703\u7522\u751F\u63A8\u529B\u4F86\u514B\u670D\u963B\u529B\u7684\u5F71\u97FF\u3002 \u5728\u822A\u5929\u52A8\u529B\u5B66\u4E2D\uFF0C\u5927\u6C23\u963B\u529B\u53EF\u4EE5\u8996\u70BA\u592A\u7A7A\u98DB\u884C\u5668\u5728\u767C\u5C04\u6642\u7684\u4F4E\u6548\u7387\uFF0C\u5176\u5F71\u97FF\u5247\u662F\u5728\u767C\u5C04\u6642\u9700\u8981\u984D\u5916\u7684\u80FD\u91CF\uFF0C\u4E0D\u904E\u5728\u8FD4\u56DE\u8ECC\u9053\u6642\u5927\u6C23\u963B\u529B\u6709\u52A9\u65BC\u592A\u7A7A\u98DB\u884C\u5668\u6E1B\u901F\uFF0C\u53EF\u6E1B\u5C11\u6E1B\u901F\u984D\u5916\u9700\u8981\u7684\u80FD\u91CF\uFF0C\u4E0D\u904E\u5927\u6C23\u963B\u529B\u7522\u751F\u7684\u71B1\u91CF\u751A\u81F3\u53EF\u4EE5\u5C07\u7269\u9AD4\u7194\u5316\u3002"@zh , "\u041B\u043E\u0431\u043E\u0432\u043E\u0435 \u0441\u043E\u043F\u0440\u043E\u0442\u0438\u0432\u043B\u0435\u043D\u0438\u0435 \u2014 \u0441\u0438\u043B\u0430, \u043F\u0440\u0435\u043F\u044F\u0442\u0441\u0442\u0432\u0443\u044E\u0449\u0430\u044F \u0434\u0432\u0438\u0436\u0435\u043D\u0438\u044E \u0442\u0435\u043B \u0432 \u0436\u0438\u0434\u043A\u043E\u0441\u0442\u044F\u0445 \u0438 \u0433\u0430\u0437\u0430\u0445. \u041B\u043E\u0431\u043E\u0432\u043E\u0435 \u0441\u043E\u043F\u0440\u043E\u0442\u0438\u0432\u043B\u0435\u043D\u0438\u0435 \u0441\u043A\u043B\u0430\u0434\u044B\u0432\u0430\u0435\u0442\u0441\u044F \u0438\u0437 \u0434\u0432\u0443\u0445 \u0442\u0438\u043F\u043E\u0432 \u0441\u0438\u043B: \u0441\u0438\u043B \u043A\u0430\u0441\u0430\u0442\u0435\u043B\u044C\u043D\u043E\u0433\u043E (\u0442\u0430\u043D\u0433\u0435\u043D\u0446\u0438\u0430\u043B\u044C\u043D\u043E\u0433\u043E) \u0442\u0440\u0435\u043D\u0438\u044F, \u043D\u0430\u043F\u0440\u0430\u0432\u043B\u0435\u043D\u043D\u044B\u0445 \u0432\u0434\u043E\u043B\u044C \u043F\u043E\u0432\u0435\u0440\u0445\u043D\u043E\u0441\u0442\u0438 \u0442\u0435\u043B\u0430, \u0438 \u0441\u0438\u043B \u0434\u0430\u0432\u043B\u0435\u043D\u0438\u044F, \u043D\u0430\u043F\u0440\u0430\u0432\u043B\u0435\u043D\u043D\u044B\u0445 \u043F\u043E \u043D\u043E\u0440\u043C\u0430\u043B\u0438 \u043A \u043F\u043E\u0432\u0435\u0440\u0445\u043D\u043E\u0441\u0442\u0438. \u0421\u0438\u043B\u0430 \u0441\u043E\u043F\u0440\u043E\u0442\u0438\u0432\u043B\u0435\u043D\u0438\u044F \u044F\u0432\u043B\u044F\u0435\u0442\u0441\u044F \u0434\u0438\u0441\u0441\u0438\u043F\u0430\u0442\u0438\u0432\u043D\u043E\u0439 \u0441\u0438\u043B\u043E\u0439 \u0438 \u0432\u0441\u0435\u0433\u0434\u0430 \u043D\u0430\u043F\u0440\u0430\u0432\u043B\u0435\u043D\u0430 \u043F\u0440\u043E\u0442\u0438\u0432 \u0432\u0435\u043A\u0442\u043E\u0440\u0430 \u0441\u043A\u043E\u0440\u043E\u0441\u0442\u0438 \u0442\u0435\u043B\u0430 \u0432 \u0441\u0440\u0435\u0434\u0435. \u041D\u0430\u0440\u044F\u0434\u0443 \u0441 \u043F\u043E\u0434\u044A\u0451\u043C\u043D\u043E\u0439 \u0441\u0438\u043B\u043E\u0439 \u044F\u0432\u043B\u044F\u0435\u0442\u0441\u044F \u0441\u043E\u0441\u0442\u0430\u0432\u043B\u044F\u044E\u0449\u0435\u0439 \u043F\u043E\u043B\u043D\u043E\u0439 \u0430\u044D\u0440\u043E\u0434\u0438\u043D\u0430\u043C\u0438\u0447\u0435\u0441\u043A\u043E\u0439 \u0441\u0438\u043B\u044B. \u0421\u0438\u043B\u0430 \u043B\u043E\u0431\u043E\u0432\u043E\u0433\u043E \u0441\u043E\u043F\u0440\u043E\u0442\u0438\u0432\u043B\u0435\u043D\u0438\u044F \u043E\u0431\u044B\u0447\u043D\u043E \u043F\u0440\u0435\u0434\u0441\u0442\u0430\u0432\u043B\u044F\u0435\u0442\u0441\u044F \u0432 \u0432\u0438\u0434\u0435 \u0441\u0443\u043C\u043C\u044B \u0434\u0432\u0443\u0445 \u0441\u043E\u0441\u0442\u0430\u0432\u043B\u044F\u044E\u0449\u0438\u0445: \u0441\u043E\u043F\u0440\u043E\u0442\u0438\u0432\u043B\u0435\u043D\u0438\u044F \u043F\u0440\u0438 \u043D\u0443\u043B\u0435\u0432\u043E\u0439 \u043F\u043E\u0434\u044A\u0451\u043C\u043D\u043E\u0439 \u0441\u0438\u043B\u0435 \u0438 \u0438\u043D\u0434\u0443\u043A\u0442\u0438\u0432\u043D\u043E\u0433\u043E \u0441\u043E\u043F\u0440\u043E\u0442\u0438\u0432\u043B\u0435\u043D\u0438\u044F. \u041A\u0430\u0436\u0434\u0430\u044F \u0441\u043E\u0441\u0442\u0430\u0432\u043B\u044F\u044E\u0449\u0430\u044F \u0445\u0430\u0440\u0430\u043A\u0442\u0435\u0440\u0438\u0437\u0443\u0435\u0442\u0441\u044F \u0441\u0432\u043E\u0438\u043C \u0441\u043E\u0431\u0441\u0442\u0432\u0435\u043D\u043D\u044B\u043C \u0431\u0435\u0437\u0440\u0430\u0437\u043C\u0435\u0440\u043D\u044B\u043C \u043A\u043E\u044D\u0444\u0444\u0438\u0446\u0438\u0435\u043D\u0442\u043E\u043C \u0441\u043E\u043F\u0440\u043E\u0442\u0438\u0432\u043B\u0435\u043D\u0438\u044F \u0438 \u043E\u043F\u0440\u0435\u0434\u0435\u043B\u0451\u043D\u043D\u043E\u0439 \u0437\u0430\u0432\u0438\u0441\u0438\u043C\u043E\u0441\u0442\u044C\u044E \u043E\u0442 \u0441\u043A\u043E\u0440\u043E\u0441\u0442\u0438 \u0434\u0432\u0438\u0436\u0435\u043D\u0438\u044F. \u041B\u043E\u0431\u043E\u0432\u043E\u0435 \u0441\u043E\u043F\u0440\u043E\u0442\u0438\u0432\u043B\u0435\u043D\u0438\u0435 \u043C\u043E\u0436\u0435\u0442 \u0441\u043F\u043E\u0441\u043E\u0431\u0441\u0442\u0432\u043E\u0432\u0430\u0442\u044C \u043A\u0430\u043A \u043E\u0431\u043B\u0435\u0434\u0435\u043D\u0435\u043D\u0438\u044E \u043B\u0435\u0442\u0430\u0442\u0435\u043B\u044C\u043D\u044B\u0445 \u0430\u043F\u043F\u0430\u0440\u0430\u0442\u043E\u0432 (\u043F\u0440\u0438 \u043D\u0438\u0437\u043A\u0438\u0445 \u0442\u0435\u043C\u043F\u0435\u0440\u0430\u0442\u0443\u0440\u0430\u0445 \u0432\u043E\u0437\u0434\u0443\u0445\u0430), \u0442\u0430\u043A \u0438 \u0432\u044B\u0437\u044B\u0432\u0430\u0442\u044C \u043D\u0430\u0433\u0440\u0435\u0432\u0430\u043D\u0438\u0435 \u043B\u043E\u0431\u043E\u0432\u044B\u0445 \u043F\u043E\u0432\u0435\u0440\u0445\u043D\u043E\u0441\u0442\u0435\u0439 \u041B\u0410 \u043F\u0440\u0438 \u0441\u0432\u0435\u0440\u0445\u0437\u0432\u0443\u043A\u043E\u0432\u044B\u0445 \u0441\u043A\u043E\u0440\u043E\u0441\u0442\u044F\u0445 \u0443\u0434\u0430\u0440\u043D\u043E\u0439 \u0438\u043E\u043D\u0438\u0437\u0430\u0446\u0438\u0435\u0439."@ru , "En din\u00E0mica de fluids, l'arrossegament \u00E9s la for\u00E7a que actua en el sentit contrari del moviment relatiu d'un objecte que es mou respecte al fluid que l'envolta. Pot haver-hi arrossegament entre dues capes (o superf\u00EDcies) de fluids o una superf\u00EDcie fluida i una de s\u00F2lida. A difer\u00E8ncia d'altres forces de resist\u00E8ncia, com ara la fricci\u00F3, que pr\u00E0cticament no depenen de la velocitat, les forces d'arrossegament hi tenen una relaci\u00F3 directa. La for\u00E7a d'arrossegament \u00E9s proporcional a la velocitat en un flux laminar i proporcional a la velocitat elevada al quadrat en un flux turbulent. Tot i que, en \u00FAltima inst\u00E0ncia, la causa de l'arrossegament \u00E9s el fregament visc\u00F3s, l'arrossegament turbulent \u00E9s independent de la viscositat."@ca , "\uC720\uCCB4\uB3D9\uC5ED\uD559\uC5D0\uC11C \uD56D\uB825(\u6297\u529B, drag)\uC740 \u2018\uBB3C\uCCB4\uAC00 \uC720\uCCB4 \uB0B4\uB97C \uC6C0\uC9C1\uC77C \uB54C \uC774 \uC6C0\uC9C1\uC784\uC5D0 \uC800\uD56D\uD558\uB294 \uD798\u2019\uC774\uB2E4. \uD56D\uB825\uC740 \uB9C8\uCC30\uB825\uACFC \uC555\uB825\uC73C\uB85C \uAD6C\uBD84\uB41C\uB2E4. \uB9C8\uCC30\uB825\uC740 \uBB3C\uCCB4\uC758 \uD45C\uBA74\uC5D0 \uD3C9\uD589\uD55C \uBC29\uD5A5\uC73C\uB85C \uC791\uC6A9\uD558\uBA70, \uC555\uB825\uC740 \uBB3C\uCCB4\uC758 \uD45C\uBA74\uC5D0 \uC218\uC9C1\uD55C \uBC29\uD5A5\uC73C\uB85C \uC791\uC6A9\uD55C\uB2E4. \uC720\uCCB4 \uB0B4\uC5D0\uC11C \uC6C0\uC9C1\uC774\uB294 \uACE0\uCCB4 \uBB3C\uCCB4\uC758 \uACBD\uC6B0, \uD56D\uB825\uC740 \u2018\uC720\uCCB4\uC758 \uC720\uB3D9\uACFC \uB3D9\uC77C\uD55C \uBC29\uD5A5\uC73C\uB85C \uC791\uC6A9\uD558\uB294 \uBAA8\uB4E0 \uC720\uCCB4\uC5ED\uD559\uC801 \uD798\uC758 \uD569\u2019\uC774\uB2E4. \uB530\uB77C\uC11C \uD56D\uB825\uC740 \uBB3C\uCCB4\uC758 \uC6C0\uC9C1\uC784\uC744 \uBC29\uD574\uD558\uB294 \uD798\uC774\uB2E4. \uD56D\uACF5\uAE30\uC5D0\uC11C \uCD94\uB825\uC774 \uD544\uC694\uD55C \uAC83\uC740 \uBC14\uB85C \uC774 \uD56D\uB825\uC774\uB77C\uB294 \uD798\uC744 \uADF9\uBCF5\uD558\uACE0 \uB098\uC544\uAC00\uAE30 \uC704\uD574\uC11C\uC774\uB2E4. \uC720\uCCB4 \uC720\uB3D9\uC758 \uBC29\uD5A5\uC5D0 \uC218\uC9C1\uC73C\uB85C \uC791\uC6A9\uD558\uB294 \uD798\uC740 \uC591\uB825(lift)\uC774\uB77C\uACE0 \uD55C\uB2E4. \uBB3C\uCCB4\uC5D0 \uB300\uD55C \uD56D\uB825\uC740 \uBB34\uCC28\uC6D0 \uC218\uC778 \uD56D\uB825 \uACC4\uC218(Cd, drag coefficient, coefficient of drag)\uB85C \uB098\uD0C0\uB0BC \uC218 \uC788\uC73C\uBA70, \uD56D\uB825 \uBC29\uC815\uC2DD\uC744 \uC0AC\uC6A9\uD574 \uACC4\uC0B0\uD560 \uC218 \uC788\uB2E4. \uD56D\uB825 \uACC4\uC218\uB97C \uC0C1\uC218\uB77C\uACE0 \uAC00\uC815\uD55C\uB2E4\uBA74, \uC77C\uBC18\uC801\uC73C\uB85C \uD56D\uB825\uC740 \uC18D\uB3C4\uC758 \uC81C\uACF1\uC5D0 \uBE44\uB840\uD55C\uB2E4."@ko , "En m\u00E9canique des fluides, la tra\u00EEn\u00E9e ou train\u00E9e est la force qui s'oppose au mouvement d'un corps dans un liquide ou un gaz et agit comme un frottement. Math\u00E9matiquement, c'est la composante des efforts exerc\u00E9s sur le corps, dans le sens oppos\u00E9 \u00E0 la v\u00E9locit\u00E9 relative du corps par rapport au fluide. En a\u00E9rodynamique, c'est, avec la portance, l'une des deux grandeurs fondamentales. Le rapport entre portance et tra\u00EEn\u00E9e s'appelle la finesse. En ce qui concerne les transports terrestres, la tra\u00EEn\u00E9e a\u00E9rodynamique est toujours accompagn\u00E9e d'une tra\u00EEn\u00E9e de roulement (s'agissant de transport routiers, par exemple c'est la r\u00E9sistance au roulement des pneumatiques sur la chauss\u00E9e). Diff\u00E9rents types de ph\u00E9nom\u00E8nes concourent \u00E0 la tra\u00EEn\u00E9e a\u00E9rodynamique totale, et on distingue la , la (la plus importante pour les corps profil\u00E9s) et en r\u00E9gimes transsonique et supersonique, la . La tra\u00EEn\u00E9e induite par la portance est \u00E9galement tr\u00E8s importante s'agissant des ailes, mais on la retrouve (avec un ordre de grandeur plus faible) pour tous les corps d\u00E9veloppant une portance ou d\u00E9portance (donc, par exemple, pour les automobiles ou les dirigeables). Dans le cas d'un mouvement acc\u00E9l\u00E9r\u00E9, il faut \u00E9galement prendre en compte la masse ajout\u00E9e."@fr , "\u0410\u0435\u0440\u043E\u0433\u0456\u0434\u0440\u043E\u0434\u0438\u043D\u0430\u043C\u0456\u0447\u043D\u0438\u0439 (\u043B\u043E\u0431\u043E\u0432\u0438\u0439) \u043E\u043F\u0456\u0440 \u2014 \u043E\u043F\u0456\u0440 \u0440\u0443\u0445\u043E\u0432\u0456 \u0442\u0456\u043B\u0430 \u0432 \u0433\u0430\u0437\u0456 \u0430\u0431\u043E \u0440\u0456\u0434\u0438\u043D\u0456."@uk , "Dalam dinamika fluida, gaya hambat (yang kadang-kadang disebut hambatan fluida atau seretan) adalah gaya yang menghambat pergerakan sebuah benda padat melalui sebuah fluida ( cairan atau gas). Bentuk gaya hambat yang paling umum tersusun dari sejumlah gaya gesek, yang bertindak sejajar dengan permukaan benda, plus gaya tekanan, yang bertindak dalam arah tegak lurus dengan permukaan benda. Bagi sebuah benda padat yang bergerak melalui sebuah fluida, gaya hambat merupakan komponen dari aerodinamika atau gaya dinamika fluida yang bekerja dalam arahnya pergerakan. Komponen tegak lurus terhadap arah pergerakan ini dianggap sebagai gaya angkat. Dengan begitu gaya hambat berlawanan dengan arah pergerakan benda, dan dalam sebuah kendaraan yang digerakkan mesin diatasi dengan gaya dorong. Dalam , tergantung pada situasi, hambatan atmosfer bisa dianggap sebagai ketidak efesiensian yang membutuhkan pengeluaran energi tambahan dalam peluncuran objek angkasa luar. Tipe-tipe gaya hambat pada umumnya terbagi menjadi kategori berikut ini: \n* , terdiri dari \n* seretan bentuk, \n* gesekan permukaan, \n* seretan interferensi, \n* , dan \n* (aerodinamika) atau hambatan gelombang (hidrodinamika kapal). Frasa gaya hambat parasit sering digunakan dalam aerodinmika, gaya hambat sayap angkat pada umumnya lebih kecil dari gaya angkat. Aliran fluida di sekeliling bagian benda yang curam pada umumnya mendominasi, dan lalu menciptakan gaya hambat. Lebih jauh lagi, gaya hambat imbas baru relevan ketika ada sayap atau , dan dengan begitu biasanya didiskusikan baik dalam perspektif aviasinya gaya hambat, atau dalam desainnya semi-planing atau badan kapal. Gaya hambat gelombang berlangsung saat sebuah benda padat bergerak melalui sebuah fluida atau mendekati kecepatan suara dalam fluida itu \u2014 atau dalam kasus di mana sebuah permukaan fluida yang bergerak bebas bergelombang permukaan menyebar dari objek, misalnya saja dari sebuah kapal. Untuk kecepatan yang tinggi \u2014 atau lebih tepatnya, pada bilangan Reynolds yang tinggi \u2014 gaya hambat keseluruhannya sebuah benda dikarakterisasikan oleh sebuah bilangan tak berdimensi yang disebut koefisien hambatan. Mengumpamakan sebuah koefisien hambatan yang lebih-atau-kurang konstan, seretan akan bervariasi sebagai kuadratnya kecepatan. Dengan begitu, tenaga resultan yang dibutuhkan untuk mengatasi gaya hambat ini akan bervariasi sebagai pangkat tiganya kecepatan. Persamaan standar untuk gaya hambat adalah satu setengah koefisiennya seretan dikali dengan massa jenis fluida, luas dari item tertentu, dan kuadratnya kecepatan. Hambatan angin merupakan istilah orang awam yang digunakan untuk mendeskripsikan gaya hambat. Penggunaannya sering kali tak jelas, dan biasanya digunakan dalam sebuah makna perbandingan (sebagai misal, kok bulu tangkis memiliki hambatan angin yang lebih tinggi dari bola squash)."@in ; dbo:wikiPageWikiLink dbr:Dynamic_viscosity , dbr:Velocity , dbr:Fluid , dbr:Archibald_Reith_Low , dbr:Nose_cone_design , , dbr:Melvill_Jones , , dbr:Angle_of_attack , dbr:Automobile_drag_coefficient , dbr:Windage , , dbr:Solid , dbr:Shock_wave , dbr:Cambridge_University_Press , dbr:Drag_coefficient , dbr:Concorde , dbr:Skin_friction_drag , dbr:Aircraft , , dbr:Aerodynamic_force , dbr:Limit_of_a_function , , , dbr:Ludwig_Prandtl , , dbr:Aristotle , dbr:Diameter , dbr:Order_of_magnitude , dbr:Wave_drag , dbr:Fluid_dynamics , dbr:Steady_flow , dbr:Boundary_layer , dbr:Morison_equation , dbr:Bejan_number , dbr:Lift-induced_drag , dbr:Force , dbr:Flow_separation , dbr:Lifting_body , dbr:Ocean_surface_wave , dbr:Landing_gear , dbr:Pressure , dbr:Carnot_cycle , dbr:Differential_equation , dbr:McDonnell_Douglas_DC-9 , dbr:Laminar_flow , dbr:Inviscid_flow , , dbr:Terminal_velocity , dbr:Friction , dbr:Dimension , dbr:Claude-Louis_Navier , dbr:Busemann_biplane , dbr:Kinematic_viscosity , dbr:Royal_Aeronautical_Society , dbr:Pressure_drag , dbr:Dimensionless_number , dbr:Ram_pressure , , , , dbr:Viscous_drag , , dbr:Glide_ratio , dbr:Atmospheric_density , , , dbr:Symmetry , dbr:Planing_hull , , dbr:Freestream , dbr:Wave-making_resistance , , dbr:Stokes_Law , , , , , , dbr:Aerodynamics , dbr:Area_rule , dbr:Stokes_radius , dbr:Form_drag , dbr:Louis_Charles_Breguet , dbr:Potential_flow , , dbr:Projectile_motion , , dbr:Coefficient , dbr:Reynolds_number , dbr:Hyperbolic_tangent , dbr:Mechanical_work , dbr:Wing , dbr:Hyperbolic_cotangent , dbr:Hydrodynamics , dbr:Lift_coefficient , dbr:Parasitic_drag , dbr:Net_force , dbr:Drag_crisis , dbc:Force , dbr:Asymptotically , dbr:Orthographic_projection , , dbr:Transonic , dbr:Watercraft , , , dbc:Articles_containing_video_clips , dbr:Douglas_DC-3 , , , dbr:Lord_Rayleigh , dbr:Drag_force , dbr:Gravity_drag , dbr:George_Gabriel_Stokes , dbr:Density , dbr:Added_mass , dbr:Drag_equation , , dbr:Viscosity . @prefix dbp: . @prefix dbt: . dbp:wikiPageUsesTemplate dbt:ISBN , dbt:Authority_control , , dbt:Reflist , dbt:Cite_book , dbt:Div_col , dbt:Div_col_end , dbt:Rp , dbt:Main , dbt:Convert , dbt:Short_description , dbt:Other_uses ; 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