"\u30DE\u30AF\u30B9\u30A6\u30A7\u30EB\u306E\u5FDC\u529B\u30C6\u30F3\u30BD\u30EB"@ja . . . . . . . . . . . "V elektrodynamice se pojmem Maxwell\u016Fv tenzor ozna\u010Duje tenzor nap\u011Bt\u00ED vyjad\u0159uj\u00EDc\u00ED tok hybnosti elektromagnetick\u00E9ho pole zvolenou plochou. V jednotk\u00E1ch SI je pro izotropn\u00ED prost\u0159ed\u00ED d\u00E1n vztahem kde \u03B4 zna\u010D\u00ED druh\u00E9ho \u0159\u00E1du, resp. analogicky ve slo\u017Ek\u00E1ch jako S pomoc\u00ED Maxwellova tenzoru lze formulovat z\u00E1kon zachov\u00E1n\u00ED hybnosti pro elektromagnetick\u00E9 pole jako rovnici kontinuity kde je hustota s\u00EDly p\u016Fsob\u00EDc\u00ED na dan\u00FD objem a je . Analogicky ve slo\u017Ek\u00E1ch"@cs . "\uC804\uC790\uAE30\uD559\uC5D0\uC11C \uB9E5\uC2A4\uC6F0 \uBCC0\uD615\uB825 \uD150\uC11C(Maxwell stress Tensor)\uB294 \uC804\uC790\uAE30\uC7A5\uC73C\uB85C \uC778\uD574 \uBC1C\uC0DD\uD558\uB294 \uBCC0\uD615\uB825\uC744 \uB098\uD0C0\uB0B4\uB294 3\u00D73 \uD150\uC11C\uB2E4. \uC989, \uC804\uC790\uAE30\uC7A5\uC5D0 \uC758\uD55C \uC6B4\uB3D9\uB7C9\uC758 \uC218\uC1A1\uC744 \uAE30\uC220\uD55C\uB2E4. \uC81C\uC784\uC2A4 \uD074\uB7EC\uD06C \uB9E5\uC2A4\uC6F0\uC758 \uC774\uB984\uC744 \uB544\uB2E4."@ko . . "El tensor de Maxwell o tensor de tensiones de Maxwell (llamado as\u00ED en honor de James Clerk Maxwell) es un tensor de segundo rango utilizado en electromagnetismo cl\u00E1sico para representar la interacci\u00F3n entre las fuerzas el\u00E9ctrica/magn\u00E9tica y el impulso mec\u00E1nico. En situaciones simples, tales como una carga el\u00E9ctrica movi\u00E9ndose libremente en un campo magn\u00E9tico homog\u00E9neo, es f\u00E1cil calcular las fuerzas sobre la carga a partir de la ley de la fuerza de Lorentz. Cuando la situaci\u00F3n se vuelve m\u00E1s complicada, este procedimiento ordinario puede convertirse en incre\u00EDblemente dif\u00EDcil, con ecuaciones que abarcan varias l\u00EDneas. Por tanto, es conveniente recoger muchos de estos t\u00E9rminos en el tensor de tensiones de Maxwell, y utilizar la aritm\u00E9tica de tensores para encontrar la respuesta al problema que nos ocupa. Se define como: Donde es la componente k-\u00E9sima y es la delta de Kronecker."@es . "In elettrodinamica, il tensore degli sforzi di Maxwell \u00E8 un tensore il cui flusso rappresenta la variazione di quantit\u00E0 di moto di un campo elettromagnetico per unit\u00E0 di tempo. In relativit\u00E0 ristretta il tensore degli sforzi di Maxwell viene generalizzato dal tensore degli sforzi elettromagnetico, che \u00E8 il tensore energia impulso associato al campo elettromagnetico."@it . . . "El tensor de Maxwell o tensor de tensiones de Maxwell (llamado as\u00ED en honor de James Clerk Maxwell) es un tensor de segundo rango utilizado en electromagnetismo cl\u00E1sico para representar la interacci\u00F3n entre las fuerzas el\u00E9ctrica/magn\u00E9tica y el impulso mec\u00E1nico. En situaciones simples, tales como una carga el\u00E9ctrica movi\u00E9ndose libremente en un campo magn\u00E9tico homog\u00E9neo, es f\u00E1cil calcular las fuerzas sobre la carga a partir de la ley de la fuerza de Lorentz. Cuando la situaci\u00F3n se vuelve m\u00E1s complicada, este procedimiento ordinario puede convertirse en incre\u00EDblemente dif\u00EDcil, con ecuaciones que abarcan varias l\u00EDneas. Por tanto, es conveniente recoger muchos de estos t\u00E9rminos en el tensor de tensiones de Maxwell, y utilizar la aritm\u00E9tica de tensores para encontrar la respuesta al problema que"@es . . . . "Der Maxwellsche Spannungstensor (benannt nach James Clerk Maxwell) ist ein symmetrischer Tensor zweiter Stufe, der in der klassischen Elektrodynamik verwendet wird, um die Wechselwirkung zwischen elektromagnetischen Kr\u00E4ften und mechanischem Impuls darzustellen. In einfachen Situationen, beispielsweise eine elektrische Punktladung, die sich in einem homogenen Magnetfeld frei bewegt, lassen sich die Kr\u00E4fte auf die Ladung durch die Lorentzkraft berechnen. F\u00FCr komplexere Probleme wird das Verfahren \u00FCber die Lorentzkraft sehr lang. Es ist daher zweckm\u00E4\u00DFig, verschiedene Gr\u00F6\u00DFen der Elektrodynamik im Maxwellschen Spannungstensor zu sammeln. In der relativistischen Formulierung des Elektromagnetismus erscheint der Maxwell-Tensor als Teil des elektromagnetischen Energie-Impuls-Tensors."@de . "Le tenseur des contraintes de Maxwell (nomm\u00E9 en l'honneur de James Clerk Maxwell) est un tenseur de rang 2 utilis\u00E9 en \u00E9lectromagn\u00E9tisme classique pour exprimer dans le cas g\u00E9n\u00E9ral les forces \u00E9lectromagn\u00E9tiques. Dans la situation physique la plus simple, constitu\u00E9e d'une charge ponctuelle se d\u00E9pla\u00E7ant librement dans un champ magn\u00E9tique uniforme, on peut calculer ais\u00E9ment la force exerc\u00E9e sur la particule en utilisant la loi de la force de Lorentz. Dans le cas le plus g\u00E9n\u00E9ral, o\u00F9 le syst\u00E8me est caract\u00E9ris\u00E9 par une distribution volumique de charge , une densit\u00E9 volumique de courant , un champ \u00E9lectrique et un champ magn\u00E9tique , on peut exprimer une densit\u00E9 volumique de force de Lorentz, . En utilisant les \u00E9quations de Maxwell, on montre qu'on peut \u00E9liminer la densit\u00E9 de courant , et ainsi r\u00E9\u00E9crire cette densit\u00E9 volumique de force uniquement en fonction des champs \u00E9lectrique et magn\u00E9tique . Cette nouvelle expression permet alors de d\u00E9finir le tenseur des contraintes de Maxwell, ce que nous allons voir ci-dessous. Dans la formulation relativiste de l'\u00E9lectromagn\u00E9tisme, le tenseur de Maxwell appara\u00EEt comme la composante \u00E9lectromagn\u00E9tique du tenseur \u00E9nergie-impulsion. Ce dernier d\u00E9crit les densit\u00E9s et flux respectivement de l'\u00E9nergie et de l'impulsion dans l'espace-temps."@fr . . . "Tensore degli sforzi di Maxwell"@it . "\u0422\u0435\u043D\u0437\u043E\u0440 \u043D\u0430\u043F\u0440\u044F\u0436\u0435\u043D\u0438\u0439 \u041C\u0430\u043A\u0441\u0432\u0435\u043B\u043B\u0430 (\u043D\u0430\u0437\u0432\u0430\u043D \u0432 \u0447\u0435\u0441\u0442\u044C \u0414\u0436\u0435\u0439\u043C\u0441\u0430 \u041A\u043B\u0435\u0440\u043A\u0430 \u041C\u0430\u043A\u0441\u0432\u0435\u043B\u043B\u0430) \u043F\u0440\u0435\u0434\u0441\u0442\u0430\u0432\u043B\u044F\u0435\u0442 \u0441\u043E\u0431\u043E\u0439 \u0441\u0438\u043C\u043C\u0435\u0442\u0440\u0438\u0447\u043D\u044B\u0439 \u0442\u0435\u043D\u0437\u043E\u0440 \u0432\u0442\u043E\u0440\u043E\u0433\u043E \u043F\u043E\u0440\u044F\u0434\u043A\u0430, \u0438\u0441\u043F\u043E\u043B\u044C\u0437\u0443\u0435\u043C\u044B\u0439 \u0432 \u043A\u043B\u0430\u0441\u0441\u0438\u0447\u0435\u0441\u043A\u043E\u043C \u044D\u043B\u0435\u043A\u0442\u0440\u043E\u043C\u0430\u0433\u043D\u0435\u0442\u0438\u0437\u043C\u0435 \u0434\u043B\u044F \u043F\u0440\u0435\u0434\u0441\u0442\u0430\u0432\u043B\u0435\u043D\u0438\u044F \u0432\u0437\u0430\u0438\u043C\u043E\u0434\u0435\u0439\u0441\u0442\u0432\u0438\u044F \u043C\u0435\u0436\u0434\u0443 \u044D\u043B\u0435\u043A\u0442\u0440\u043E\u043C\u0430\u0433\u043D\u0438\u0442\u043D\u044B\u043C\u0438 \u0441\u0438\u043B\u0430\u043C\u0438 \u0438 \u043C\u0435\u0445\u0430\u043D\u0438\u0447\u0435\u0441\u043A\u0438\u043C \u0438\u043C\u043F\u0443\u043B\u044C\u0441\u043E\u043C. \u0412 \u043F\u0440\u043E\u0441\u0442\u044B\u0445 \u0441\u043B\u0443\u0447\u0430\u044F\u0445, \u0442\u0430\u043A\u0438\u0445 \u043A\u0430\u043A \u0442\u043E\u0447\u0435\u0447\u043D\u044B\u0439 \u0437\u0430\u0440\u044F\u0434, \u0441\u0432\u043E\u0431\u043E\u0434\u043D\u043E \u0434\u0432\u0438\u0436\u0443\u0449\u0438\u0439\u0441\u044F \u0432 \u043E\u0434\u043D\u043E\u0440\u043E\u0434\u043D\u043E\u043C \u043C\u0430\u0433\u043D\u0438\u0442\u043D\u043E\u043C \u043F\u043E\u043B\u0435, \u043B\u0435\u0433\u043A\u043E \u0440\u0430\u0441\u0441\u0447\u0438\u0442\u0430\u0442\u044C \u0441\u0438\u043B\u044B, \u0434\u0435\u0439\u0441\u0442\u0432\u0443\u044E\u0449\u0438\u0435 \u043D\u0430 \u0437\u0430\u0440\u044F\u0434, \u0441\u043E\u0433\u043B\u0430\u0441\u043D\u043E \u0441\u0438\u043B\u0435 \u041B\u043E\u0440\u0435\u043D\u0446\u0430. \u0412 \u0431\u043E\u043B\u0435\u0435 \u0441\u043B\u043E\u0436\u043D\u044B\u0445 \u0441\u043B\u0443\u0447\u0430\u044F\u0445 \u0442\u0430\u043A\u0430\u044F \u043E\u0431\u044B\u0447\u043D\u0430\u044F \u043F\u0440\u043E\u0446\u0435\u0434\u0443\u0440\u0430 \u043C\u043E\u0436\u0435\u0442 \u0441\u0442\u0430\u0442\u044C \u043D\u0435\u043F\u0440\u0430\u043A\u0442\u0438\u0447\u043D\u043E \u0441\u043B\u043E\u0436\u043D\u043E\u0439 \u0441 \u0443\u0440\u0430\u0432\u043D\u0435\u043D\u0438\u044F\u043C\u0438, \u043E\u0445\u0432\u0430\u0442\u044B\u0432\u0430\u044E\u0449\u0438\u043C\u0438 \u043D\u0435\u0441\u043A\u043E\u043B\u044C\u043A\u043E \u0441\u0442\u0440\u043E\u043A. \u041F\u043E\u044D\u0442\u043E\u043C\u0443 \u0443\u0434\u043E\u0431\u043D\u043E \u0441\u043E\u0431\u0440\u0430\u0442\u044C \u043C\u043D\u043E\u0433\u0438\u0435 \u0438\u0437 \u044D\u0442\u0438\u0445 \u0447\u043B\u0435\u043D\u043E\u0432 \u0432 \u0442\u0435\u043D\u0437\u043E\u0440\u0435 \u043D\u0430\u043F\u0440\u044F\u0436\u0435\u043D\u0438\u0439 \u041C\u0430\u043A\u0441\u0432\u0435\u043B\u043B\u0430 \u0438 \u0438\u0441\u043F\u043E\u043B\u044C\u0437\u043E\u0432\u0430\u0442\u044C \u0442\u0435\u043D\u0437\u043E\u0440\u043D\u0443\u044E \u0430\u0440\u0438\u0444\u043C\u0435\u0442\u0438\u043A\u0443, \u0447\u0442\u043E\u0431\u044B \u043D\u0430\u0439\u0442\u0438 \u043E\u0442\u0432\u0435\u0442 \u043D\u0430 \u043F\u043E\u0441\u0442\u0430\u0432\u043B\u0435\u043D\u043D\u0443\u044E \u0437\u0430\u0434\u0430\u0447\u0443. \u0412 \u0440\u0435\u043B\u044F\u0442\u0438\u0432\u0438\u0441\u0442\u0441\u043A\u043E\u0439 \u0444\u043E\u0440\u043C\u0443\u043B\u0438\u0440\u043E\u0432\u043A\u0435 \u044D\u043B\u0435\u043A\u0442\u0440\u043E\u043C\u0430\u0433\u043D\u0435\u0442\u0438\u0437\u043C\u0430 \u0442\u0435\u043D\u0437\u043E\u0440 \u041C\u0430\u043A\u0441\u0432\u0435\u043B\u043B\u0430 \u043F\u043E\u044F\u0432\u043B\u044F\u0435\u0442\u0441\u044F \u043A\u0430\u043A \u0447\u0430\u0441\u0442\u044C \u044D\u043B\u0435\u043A\u0442\u0440\u043E\u043C\u0430\u0433\u043D\u0438\u0442\u043D\u043E\u0433\u043E \u0442\u0435\u043D\u0437\u043E\u0440\u0430 \u044D\u043D\u0435\u0440\u0433\u0438\u0438-\u0438\u043C\u043F\u0443\u043B\u044C\u0441\u0430, \u043A\u043E\u0442\u043E\u0440\u044B\u0439 \u044F\u0432\u043B\u044F\u0435\u0442\u0441\u044F \u044D\u043B\u0435\u043A\u0442\u0440\u043E\u043C\u0430\u0433\u043D\u0438\u0442\u043D\u043E\u0439 \u0441\u043E\u0441\u0442\u0430\u0432\u043B\u044F\u044E\u0449\u0435\u0439 \u043F\u043E\u043B\u043D\u043E\u0433\u043E \u0442\u0435\u043D\u0437\u043E\u0440\u0430 \u044D\u043D\u0435\u0440\u0433\u0438\u0438-\u0438\u043C\u043F\u0443\u043B\u044C\u0441\u0430. \u041F\u043E\u0441\u043B\u0435\u0434\u043D\u0438\u0439 \u043E\u043F\u0438\u0441\u044B\u0432\u0430\u0435\u0442 \u043F\u043B\u043E\u0442\u043D\u043E\u0441\u0442\u044C \u0438 \u043F\u043E\u0442\u043E\u043A \u044D\u043D\u0435\u0440\u0433\u0438\u0438 \u0438 \u0438\u043C\u043F\u0443\u043B\u044C\u0441\u0430 \u0432 \u043F\u0440\u043E\u0441\u0442\u0440\u0430\u043D\u0441\u0442\u0432\u0435-\u0432\u0440\u0435\u043C\u0435\u043D\u0438."@ru . . . "The Maxwell stress tensor (named after James Clerk Maxwell) is a symmetric second-order tensor used in classical electromagnetism to represent the interaction between electromagnetic forces and mechanical momentum. In simple situations, such as a point charge moving freely in a homogeneous magnetic field, it is easy to calculate the forces on the charge from the Lorentz force law. When the situation becomes more complicated, this ordinary procedure can become impractically difficult, with equations spanning multiple lines. It is therefore convenient to collect many of these terms in the Maxwell stress tensor, and to use tensor arithmetic to find the answer to the problem at hand."@en . "1122673410"^^ . . . . . . . . . . . . . "3170723"^^ . . . . "Le tenseur des contraintes de Maxwell (nomm\u00E9 en l'honneur de James Clerk Maxwell) est un tenseur de rang 2 utilis\u00E9 en \u00E9lectromagn\u00E9tisme classique pour exprimer dans le cas g\u00E9n\u00E9ral les forces \u00E9lectromagn\u00E9tiques. Dans la situation physique la plus simple, constitu\u00E9e d'une charge ponctuelle se d\u00E9pla\u00E7ant librement dans un champ magn\u00E9tique uniforme, on peut calculer ais\u00E9ment la force exerc\u00E9e sur la particule en utilisant la loi de la force de Lorentz. Dans le cas le plus g\u00E9n\u00E9ral, o\u00F9 le syst\u00E8me est caract\u00E9ris\u00E9 par une distribution volumique de charge , une densit\u00E9 volumique de courant , un champ \u00E9lectrique et un champ magn\u00E9tique , on peut exprimer une densit\u00E9 volumique de force de Lorentz, . En utilisant les \u00E9quations de Maxwell, on montre qu'on peut \u00E9liminer la densit\u00E9 de courant , et ainsi r\u00E9"@fr . . . "Tensor de Maxwell"@ca . . "\u0422\u0435\u043D\u0437\u043E\u0440 \u043D\u0430\u043F\u0440\u044F\u0436\u0435\u043D\u0438\u0439 \u041C\u0430\u043A\u0441\u0432\u0435\u043B\u043B\u0430"@ru . . . "Tensor de Maxwell"@es . . . . . . . "El tensor de tensions de Maxwell o Tensor de Maxwell (en honor de James Clerk Maxwell) \u00E9s un objecte matem\u00E0tic en la f\u00EDsica, m\u00E9s concretament es tracta d'un tensor de segon rang utilitzat en electromagnetisme cl\u00E0ssic per representar la interacci\u00F3 entre les forces electromagn\u00E8tiques i l'impuls mec\u00E0nic. En situacions simples, com ara una c\u00E0rrega puntual que es mou lliurement en un camp magn\u00E8tic homogeni, \u00E9s f\u00E0cil de calcular les forces de les c\u00E0rregues segons la llei de la for\u00E7a de Lorentz. Quan la situaci\u00F3 es torna m\u00E9s complexa, aquest procediment ordinari pot arribar a ser incre\u00EFblement dif\u00EDcil, amb equacions que abasten diverses l\u00EDnies. Per tant, \u00E9s convenient recollir molts d'aquests termes en el tensor de tensions de Maxwell i utilitzar l'aritm\u00E8tica tensor per trobar la resposta al problema en q\u00FCesti\u00F3."@ca . "\u0422\u0435\u043D\u0437\u043E\u0440 \u043D\u0430\u043F\u0440\u044F\u0436\u0435\u043D\u0438\u0439 \u041C\u0430\u043A\u0441\u0432\u0435\u043B\u043B\u0430 (\u043D\u0430\u0437\u0432\u0430\u043D \u0432 \u0447\u0435\u0441\u0442\u044C \u0414\u0436\u0435\u0439\u043C\u0441\u0430 \u041A\u043B\u0435\u0440\u043A\u0430 \u041C\u0430\u043A\u0441\u0432\u0435\u043B\u043B\u0430) \u043F\u0440\u0435\u0434\u0441\u0442\u0430\u0432\u043B\u044F\u0435\u0442 \u0441\u043E\u0431\u043E\u0439 \u0441\u0438\u043C\u043C\u0435\u0442\u0440\u0438\u0447\u043D\u044B\u0439 \u0442\u0435\u043D\u0437\u043E\u0440 \u0432\u0442\u043E\u0440\u043E\u0433\u043E \u043F\u043E\u0440\u044F\u0434\u043A\u0430, \u0438\u0441\u043F\u043E\u043B\u044C\u0437\u0443\u0435\u043C\u044B\u0439 \u0432 \u043A\u043B\u0430\u0441\u0441\u0438\u0447\u0435\u0441\u043A\u043E\u043C \u044D\u043B\u0435\u043A\u0442\u0440\u043E\u043C\u0430\u0433\u043D\u0435\u0442\u0438\u0437\u043C\u0435 \u0434\u043B\u044F \u043F\u0440\u0435\u0434\u0441\u0442\u0430\u0432\u043B\u0435\u043D\u0438\u044F \u0432\u0437\u0430\u0438\u043C\u043E\u0434\u0435\u0439\u0441\u0442\u0432\u0438\u044F \u043C\u0435\u0436\u0434\u0443 \u044D\u043B\u0435\u043A\u0442\u0440\u043E\u043C\u0430\u0433\u043D\u0438\u0442\u043D\u044B\u043C\u0438 \u0441\u0438\u043B\u0430\u043C\u0438 \u0438 \u043C\u0435\u0445\u0430\u043D\u0438\u0447\u0435\u0441\u043A\u0438\u043C \u0438\u043C\u043F\u0443\u043B\u044C\u0441\u043E\u043C. \u0412 \u043F\u0440\u043E\u0441\u0442\u044B\u0445 \u0441\u043B\u0443\u0447\u0430\u044F\u0445, \u0442\u0430\u043A\u0438\u0445 \u043A\u0430\u043A \u0442\u043E\u0447\u0435\u0447\u043D\u044B\u0439 \u0437\u0430\u0440\u044F\u0434, \u0441\u0432\u043E\u0431\u043E\u0434\u043D\u043E \u0434\u0432\u0438\u0436\u0443\u0449\u0438\u0439\u0441\u044F \u0432 \u043E\u0434\u043D\u043E\u0440\u043E\u0434\u043D\u043E\u043C \u043C\u0430\u0433\u043D\u0438\u0442\u043D\u043E\u043C \u043F\u043E\u043B\u0435, \u043B\u0435\u0433\u043A\u043E \u0440\u0430\u0441\u0441\u0447\u0438\u0442\u0430\u0442\u044C \u0441\u0438\u043B\u044B, \u0434\u0435\u0439\u0441\u0442\u0432\u0443\u044E\u0449\u0438\u0435 \u043D\u0430 \u0437\u0430\u0440\u044F\u0434, \u0441\u043E\u0433\u043B\u0430\u0441\u043D\u043E \u0441\u0438\u043B\u0435 \u041B\u043E\u0440\u0435\u043D\u0446\u0430. \u0412 \u0431\u043E\u043B\u0435\u0435 \u0441\u043B\u043E\u0436\u043D\u044B\u0445 \u0441\u043B\u0443\u0447\u0430\u044F\u0445 \u0442\u0430\u043A\u0430\u044F \u043E\u0431\u044B\u0447\u043D\u0430\u044F \u043F\u0440\u043E\u0446\u0435\u0434\u0443\u0440\u0430 \u043C\u043E\u0436\u0435\u0442 \u0441\u0442\u0430\u0442\u044C \u043D\u0435\u043F\u0440\u0430\u043A\u0442\u0438\u0447\u043D\u043E \u0441\u043B\u043E\u0436\u043D\u043E\u0439 \u0441 \u0443\u0440\u0430\u0432\u043D\u0435\u043D\u0438\u044F\u043C\u0438, \u043E\u0445\u0432\u0430\u0442\u044B\u0432\u0430\u044E\u0449\u0438\u043C\u0438 \u043D\u0435\u0441\u043A\u043E\u043B\u044C\u043A\u043E \u0441\u0442\u0440\u043E\u043A. \u041F\u043E\u044D\u0442\u043E\u043C\u0443 \u0443\u0434\u043E\u0431\u043D\u043E \u0441\u043E\u0431\u0440\u0430\u0442\u044C \u043C\u043D\u043E\u0433\u0438\u0435 \u0438\u0437 \u044D\u0442\u0438\u0445 \u0447\u043B\u0435\u043D\u043E\u0432 \u0432 \u0442\u0435\u043D\u0437\u043E\u0440\u0435 \u043D\u0430\u043F\u0440\u044F\u0436\u0435\u043D\u0438\u0439 \u041C\u0430\u043A\u0441\u0432\u0435\u043B\u043B\u0430 \u0438 \u0438\u0441\u043F\u043E\u043B\u044C\u0437\u043E\u0432\u0430\u0442\u044C \u0442\u0435\u043D\u0437\u043E\u0440\u043D\u0443\u044E \u0430\u0440\u0438\u0444\u043C\u0435\u0442\u0438\u043A\u0443, \u0447\u0442\u043E\u0431\u044B \u043D\u0430\u0439\u0442\u0438 \u043E\u0442\u0432\u0435\u0442 \u043D\u0430 \u043F\u043E\u0441\u0442\u0430\u0432\u043B\u0435\u043D\u043D\u0443\u044E \u0437\u0430\u0434\u0430\u0447\u0443."@ru . . "\u99AC\u514B\u58EB\u5A01\u61C9\u529B\u5F35\u91CF"@zh . . "Tenseur des contraintes de Maxwell"@fr . . . "\uB9E5\uC2A4\uC6F0 \uBCC0\uD615\uB825 \uD150\uC11C"@ko . . "\uC804\uC790\uAE30\uD559\uC5D0\uC11C \uB9E5\uC2A4\uC6F0 \uBCC0\uD615\uB825 \uD150\uC11C(Maxwell stress Tensor)\uB294 \uC804\uC790\uAE30\uC7A5\uC73C\uB85C \uC778\uD574 \uBC1C\uC0DD\uD558\uB294 \uBCC0\uD615\uB825\uC744 \uB098\uD0C0\uB0B4\uB294 3\u00D73 \uD150\uC11C\uB2E4. \uC989, \uC804\uC790\uAE30\uC7A5\uC5D0 \uC758\uD55C \uC6B4\uB3D9\uB7C9\uC758 \uC218\uC1A1\uC744 \uAE30\uC220\uD55C\uB2E4. \uC81C\uC784\uC2A4 \uD074\uB7EC\uD06C \uB9E5\uC2A4\uC6F0\uC758 \uC774\uB984\uC744 \uB544\uB2E4."@ko . . "Maxwell stress tensor"@en . . . . "\u5728\u96FB\u78C1\u5B78\u88CF\uFF0C\u99AC\u514B\u58EB\u5A01\u61C9\u529B\u5F35\u91CF(Maxwell stress tensor)\u662F\u63CF\u8FF0\u96FB\u78C1\u5834\u5E36\u6709\u4E4B\u61C9\u529B\u7684\u4E8C\u968E\u5F35\u91CF\u3002\u99AC\u514B\u58EB\u5A01\u61C9\u529B\u5F35\u91CF\u53EF\u4EE5\u8868\u73FE\u51FA\u96FB\u5834\u529B\u3001\u78C1\u5834\u529B\u548C\u6A5F\u68B0\u52D5\u91CF\u4E4B\u9593\u7684\u76F8\u4E92\u4F5C\u7528\u3002\u5C0D\u65BC\u7C21\u55AE\u7684\u72C0\u6CC1\uFF0C\u4F8B\u5982\u4E00\u500B\u9EDE\u96FB\u8377\u81EA\u7531\u5730\u79FB\u52D5\u65BC\u5747\u52FB\u78C1\u5834\uFF0C\u61C9\u7528\u52DE\u4F96\u8332\u529B\u5B9A\u5F8B\uFF0C\u5C31\u53EF\u4EE5\u5F88\u5BB9\u6613\u5730\u8A08\u7B97\u51FA\u9EDE\u96FB\u8377\u6240\u611F\u53D7\u7684\u4F5C\u7528\u529B\u3002\u4F46\u662F\uFF0C\u7576\u9047\u5230\u7A0D\u5FAE\u8907\u96DC\u4E00\u9EDE\u7684\u72C0\u6CC1\u6642\uFF0C\u9019\u5F88\u666E\u901A\u7684\u7A0B\u5E8F\u6703\u8B8A\u5F97\u975E\u5E38\u56F0\u96E3\uFF0C\u65B9\u7A0B\u5F0F\u6D0B\u6D0B\u7051\u7051\u5730\u4E00\u884C\u53C8\u4E00\u884C\u7684\u5EF6\u7E8C\u3002\u56E0\u6B64\uFF0C\u7269\u7406\u5B78\u5BB6\u901A\u5E38\u6703\u805A\u96C6\u5F88\u591A\u9805\u76EE\u65BC\u99AC\u514B\u58EB\u5A01\u61C9\u529B\u5F35\u91CF\u5167\uFF0C\u7136\u5F8C\u4F7F\u7528\u5F35\u91CF\u6578\u5B78\u4F86\u89E3\u6790\u554F\u984C\u3002"@zh . . . "In elettrodinamica, il tensore degli sforzi di Maxwell \u00E8 un tensore il cui flusso rappresenta la variazione di quantit\u00E0 di moto di un campo elettromagnetico per unit\u00E0 di tempo. In relativit\u00E0 ristretta il tensore degli sforzi di Maxwell viene generalizzato dal tensore degli sforzi elettromagnetico, che \u00E8 il tensore energia impulso associato al campo elettromagnetico."@it . . "The Maxwell stress tensor (named after James Clerk Maxwell) is a symmetric second-order tensor used in classical electromagnetism to represent the interaction between electromagnetic forces and mechanical momentum. In simple situations, such as a point charge moving freely in a homogeneous magnetic field, it is easy to calculate the forces on the charge from the Lorentz force law. When the situation becomes more complicated, this ordinary procedure can become impractically difficult, with equations spanning multiple lines. It is therefore convenient to collect many of these terms in the Maxwell stress tensor, and to use tensor arithmetic to find the answer to the problem at hand. In the relativistic formulation of electromagnetism, the Maxwell's tensor appears as a part of the electromagnetic stress\u2013energy tensor which is the electromagnetic component of the total stress\u2013energy tensor. The latter describes the density and flux of energy and momentum in spacetime."@en . "Der Maxwellsche Spannungstensor (benannt nach James Clerk Maxwell) ist ein symmetrischer Tensor zweiter Stufe, der in der klassischen Elektrodynamik verwendet wird, um die Wechselwirkung zwischen elektromagnetischen Kr\u00E4ften und mechanischem Impuls darzustellen. In der relativistischen Formulierung des Elektromagnetismus erscheint der Maxwell-Tensor als Teil des elektromagnetischen Energie-Impuls-Tensors."@de . . "\u30DE\u30AF\u30B9\u30A6\u30A7\u30EB\u306E\u5FDC\u529B\u30C6\u30F3\u30BD\u30EB\uFF08\u30DE\u30AF\u30B9\u30A6\u30A7\u30EB\u306E\u304A\u3046\u308A\u3087\u304F\u30C6\u30F3\u30BD\u30EB\u3001\u82F1: Maxwell stress tensor\uFF09\u3068\u306F\u3001\u96FB\u78C1\u5834\u306E\u5FDC\u529B\u30C6\u30F3\u30BD\u30EB\u3067\u3042\u308B\u3002\u30DE\u30AF\u30B9\u30A6\u30A7\u30EB\u5FDC\u529B\u306F\u96FB\u78C1\u5834\u306E\u904B\u52D5\u91CF\u306E\u6D41\u308C\u306E\u5BC6\u5EA6\u3092\u8868\u3059\u3002 \u30DE\u30AF\u30B9\u30A6\u30A7\u30EB\u5FDC\u529B T \u306F \u3067\u5B9A\u7FA9\u3055\u308C\u308B\u3002\u771F\u7A7A\u4E2D\u306B\u304A\u3044\u3066\u306F \u3068\u306A\u308B\u3002"@ja . . . . . . . "15470"^^ . . . "\u30DE\u30AF\u30B9\u30A6\u30A7\u30EB\u306E\u5FDC\u529B\u30C6\u30F3\u30BD\u30EB\uFF08\u30DE\u30AF\u30B9\u30A6\u30A7\u30EB\u306E\u304A\u3046\u308A\u3087\u304F\u30C6\u30F3\u30BD\u30EB\u3001\u82F1: Maxwell stress tensor\uFF09\u3068\u306F\u3001\u96FB\u78C1\u5834\u306E\u5FDC\u529B\u30C6\u30F3\u30BD\u30EB\u3067\u3042\u308B\u3002\u30DE\u30AF\u30B9\u30A6\u30A7\u30EB\u5FDC\u529B\u306F\u96FB\u78C1\u5834\u306E\u904B\u52D5\u91CF\u306E\u6D41\u308C\u306E\u5BC6\u5EA6\u3092\u8868\u3059\u3002 \u30DE\u30AF\u30B9\u30A6\u30A7\u30EB\u5FDC\u529B T \u306F \u3067\u5B9A\u7FA9\u3055\u308C\u308B\u3002\u771F\u7A7A\u4E2D\u306B\u304A\u3044\u3066\u306F \u3068\u306A\u308B\u3002"@ja . . . "\u5728\u96FB\u78C1\u5B78\u88CF\uFF0C\u99AC\u514B\u58EB\u5A01\u61C9\u529B\u5F35\u91CF(Maxwell stress tensor)\u662F\u63CF\u8FF0\u96FB\u78C1\u5834\u5E36\u6709\u4E4B\u61C9\u529B\u7684\u4E8C\u968E\u5F35\u91CF\u3002\u99AC\u514B\u58EB\u5A01\u61C9\u529B\u5F35\u91CF\u53EF\u4EE5\u8868\u73FE\u51FA\u96FB\u5834\u529B\u3001\u78C1\u5834\u529B\u548C\u6A5F\u68B0\u52D5\u91CF\u4E4B\u9593\u7684\u76F8\u4E92\u4F5C\u7528\u3002\u5C0D\u65BC\u7C21\u55AE\u7684\u72C0\u6CC1\uFF0C\u4F8B\u5982\u4E00\u500B\u9EDE\u96FB\u8377\u81EA\u7531\u5730\u79FB\u52D5\u65BC\u5747\u52FB\u78C1\u5834\uFF0C\u61C9\u7528\u52DE\u4F96\u8332\u529B\u5B9A\u5F8B\uFF0C\u5C31\u53EF\u4EE5\u5F88\u5BB9\u6613\u5730\u8A08\u7B97\u51FA\u9EDE\u96FB\u8377\u6240\u611F\u53D7\u7684\u4F5C\u7528\u529B\u3002\u4F46\u662F\uFF0C\u7576\u9047\u5230\u7A0D\u5FAE\u8907\u96DC\u4E00\u9EDE\u7684\u72C0\u6CC1\u6642\uFF0C\u9019\u5F88\u666E\u901A\u7684\u7A0B\u5E8F\u6703\u8B8A\u5F97\u975E\u5E38\u56F0\u96E3\uFF0C\u65B9\u7A0B\u5F0F\u6D0B\u6D0B\u7051\u7051\u5730\u4E00\u884C\u53C8\u4E00\u884C\u7684\u5EF6\u7E8C\u3002\u56E0\u6B64\uFF0C\u7269\u7406\u5B78\u5BB6\u901A\u5E38\u6703\u805A\u96C6\u5F88\u591A\u9805\u76EE\u65BC\u99AC\u514B\u58EB\u5A01\u61C9\u529B\u5F35\u91CF\u5167\uFF0C\u7136\u5F8C\u4F7F\u7528\u5F35\u91CF\u6578\u5B78\u4F86\u89E3\u6790\u554F\u984C\u3002"@zh . . . . . . . . "V elektrodynamice se pojmem Maxwell\u016Fv tenzor ozna\u010Duje tenzor nap\u011Bt\u00ED vyjad\u0159uj\u00EDc\u00ED tok hybnosti elektromagnetick\u00E9ho pole zvolenou plochou. V jednotk\u00E1ch SI je pro izotropn\u00ED prost\u0159ed\u00ED d\u00E1n vztahem kde \u03B4 zna\u010D\u00ED druh\u00E9ho \u0159\u00E1du, resp. analogicky ve slo\u017Ek\u00E1ch jako S pomoc\u00ED Maxwellova tenzoru lze formulovat z\u00E1kon zachov\u00E1n\u00ED hybnosti pro elektromagnetick\u00E9 pole jako rovnici kontinuity kde je hustota s\u00EDly p\u016Fsob\u00EDc\u00ED na dan\u00FD objem a je . Analogicky ve slo\u017Ek\u00E1ch"@cs . . . . "Maxwell\u016Fv tenzor"@cs . . "El tensor de tensions de Maxwell o Tensor de Maxwell (en honor de James Clerk Maxwell) \u00E9s un objecte matem\u00E0tic en la f\u00EDsica, m\u00E9s concretament es tracta d'un tensor de segon rang utilitzat en electromagnetisme cl\u00E0ssic per representar la interacci\u00F3 entre les forces electromagn\u00E8tiques i l'impuls mec\u00E0nic. En situacions simples, com ara una c\u00E0rrega puntual que es mou lliurement en un camp magn\u00E8tic homogeni, \u00E9s f\u00E0cil de calcular les forces de les c\u00E0rregues segons la llei de la for\u00E7a de Lorentz. Quan la situaci\u00F3 es torna m\u00E9s complexa, aquest procediment ordinari pot arribar a ser incre\u00EFblement dif\u00EDcil, amb equacions que abasten diverses l\u00EDnies. Per tant, \u00E9s convenient recollir molts d'aquests termes en el tensor de tensions de Maxwell i utilitzar l'aritm\u00E8tica tensor per trobar la resposta al prob"@ca . . . "Maxwellscher Spannungstensor"@de .