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<Text-field style="Heading 1" layout="Normal"><Font encoding="UTF-8">Equa\303\247\303\265es de Maxwell (do eletromagnetismo), </Font></Text-field>
<Text-field style="Text" layout="Normal"><Font italic="true">s.</Font><Font encoding="UTF-8"> um conjunto de quatro equa\303\247\303\265es que resumem as leis da eletricidade e magnetismo. Estas equa\303\247\303\265es relacionam os </Font>vetores <Font bold="true">E</Font> e <Font bold="true">B </Font>do  <Hyperlink linktarget="Dictionary:Definition/electricfield" hyperlink="true"><Font style="Dictionary Hyperlink" family="Times New Roman" encoding="UTF-8">campo el\303\251trico</Font></Hyperlink> e <Hyperlink linktarget="Dictionary:Definition/magneticfield" hyperlink="true"><Font style="Dictionary Hyperlink" family="Times New Roman" encoding="UTF-8">campo magn\303\251tico</Font></Hyperlink><Font encoding="UTF-8">  a suas fontes, carga el\303\251trica, </Font><Hyperlink linktarget="Dictionary:Definition/current" hyperlink="true"><Font style="Dictionary Hyperlink" family="Times New Roman">corrente</Font></Hyperlink> <Font encoding="UTF-8">e mudan\303\247a de campos. As equa\303\247\303\265es de Maxwell s\303\243o, na forma diferencial: </Font></Text-field><Table alignment="left" showinput="true" interior="none" order="row" exterior="none" width="100.0%" randomized="false" showlabel="true" postexecute="insert" pagebreak="cell" showgroup="true"><Table-Column weight="100" separator="true"></Table-Column><Table-Column weight="100" separator="true"></Table-Column><Table-Row align="center" separator="true"><Table-Cell columnspan="1" backgroundstyle="0" rowspan="1" fillcolor="[255,255,255]">
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<Text-field style="Text" layout="Normal">onde <Equation executable="false" style="2D Math" input-equation="" display="LUklbXJvd0c2Iy9JK21vZHVsZW5hbWVHNiJJLFR5cGVzZXR0aW5nR0koX3N5c2xpYkdGJzYkLUkjbWlHRiQ2JVEmJnJobztGJy8lJ2l0YWxpY0dRJmZhbHNlRicvJSxtYXRodmFyaWFudEdRJ25vcm1hbEYnRjI=">LUklbXJvd0c2Iy9JK21vZHVsZW5hbWVHNiJJLFR5cGVzZXR0aW5nR0koX3N5c2xpYkdGJzYkLUkjbWlHRiQ2JVEmJnJobztGJy8lJ2l0YWxpY0dRJmZhbHNlRicvJSxtYXRodmFyaWFudEdRJ25vcm1hbEYnRjI=</Equation><Font encoding="UTF-8"> \303\251 a densidade da carga, </Font><Equation executable="false" style="2D Math" input-equation="" display="LUklbXJvd0c2Iy9JK21vZHVsZW5hbWVHNiJJLFR5cGVzZXR0aW5nR0koX3N5c2xpYkdGJzYmLUkjbWlHRiQ2I1EhRictSSVtc3ViR0YkNiUtRiw2JVEtJnZhcmVwc2lsb247RicvJSdpdGFsaWNHUSZmYWxzZUYnLyUsbWF0aHZhcmlhbnRHUSdub3JtYWxGJy1JI21uR0YkNiRRIjBGJ0Y4LyUvc3Vic2NyaXB0c2hpZnRHUSIwRidGK0Y4">LUklbXJvd0c2Iy9JK21vZHVsZW5hbWVHNiJJLFR5cGVzZXR0aW5nR0koX3N5c2xpYkdGJzYmLUkjbWlHRiQ2I1EhRictSSVtc3ViR0YkNiUtRiw2JVEtJnZhcmVwc2lsb247RicvJSdpdGFsaWNHUSZmYWxzZUYnLyUsbWF0aHZhcmlhbnRHUSdub3JtYWxGJy1JI21uR0YkNiRRIjBGJ0Y4LyUvc3Vic2NyaXB0c2hpZnRHUSIwRidGK0Y4</Equation> e <Equation executable="false" style="2D Math" input-equation="" display="LUklbXJvd0c2Iy9JK21vZHVsZW5hbWVHNiJJLFR5cGVzZXR0aW5nR0koX3N5c2xpYkdGJzYmLUkjbWlHRiQ2I1EhRictSSVtc3ViR0YkNiUtRiw2JVElJm11O0YnLyUnaXRhbGljR1EmZmFsc2VGJy8lLG1hdGh2YXJpYW50R1Enbm9ybWFsRictSSNtbkdGJDYkUSIwRidGOC8lL3N1YnNjcmlwdHNoaWZ0R1EiMEYnRitGOA==">LUklbXJvd0c2Iy9JK21vZHVsZW5hbWVHNiJJLFR5cGVzZXR0aW5nR0koX3N5c2xpYkdGJzYmLUkjbWlHRiQ2I1EhRictSSVtc3ViR0YkNiUtRiw2JVElJm11O0YnLyUnaXRhbGljR1EmZmFsc2VGJy8lLG1hdGh2YXJpYW50R1Enbm9ybWFsRictSSNtbkdGJDYkUSIwRidGOC8lL3N1YnNjcmlwdHNoaWZ0R1EiMEYnRitGOA==</Equation><Font encoding="UTF-8"> s\303\243o constantes fundamentais (chamadas, respectivamente, a </Font><Font italic="true">permissividade</Font> e a <Font encoding="UTF-8" italic="true">permeabilidade do espa\303\247o livre</Font>) e <Equation executable="false" style="2D Math" input-equation="" display="LUklbXJvd0c2Iy9JK21vZHVsZW5hbWVHNiJJLFR5cGVzZXR0aW5nR0koX3N5c2xpYkdGJzYkLUkjbWlHRiQ2J1EiakYnLyUlYm9sZEdRJXRydWVGJy8lJ2l0YWxpY0dGMS8lLG1hdGh2YXJpYW50R1EsYm9sZC1pdGFsaWNGJy8lK2ZvbnR3ZWlnaHRHUSVib2xkRicvRjVRJ25vcm1hbEYn">LUklbXJvd0c2Iy9JK21vZHVsZW5hbWVHNiJJLFR5cGVzZXR0aW5nR0koX3N5c2xpYkdGJzYkLUkjbWlHRiQ2J1EiakYnLyUlYm9sZEdRJXRydWVGJy8lJ2l0YWxpY0dGMS8lLG1hdGh2YXJpYW50R1EsYm9sZC1pdGFsaWNGJy8lK2ZvbnR3ZWlnaHRHUSVib2xkRicvRjVRJ25vcm1hbEYn</Equation><Font encoding="UTF-8"> \303\251 a densidade de </Font><Hyperlink linktarget="Dictionary:Definition/current" hyperlink="true"><Font style="Dictionary Hyperlink" family="Times New Roman">corrente</Font></Hyperlink><Font encoding="UTF-8">. Em princ\303\255pio, todos os problemas em eletromagnetismo podem ser resolvidos usando as equa\303\247\303\265es de Maxwell. Pode ser facilmente demonstrado, que as equa\303\247\303\265es de Maxwell implicam que os vetores do campo magn\303\251tico e el\303\251trico, obedecem a uma </Font><Hyperlink linktarget="Dictionary:Definition/waveequation" hyperlink="true"><Font style="Dictionary Hyperlink" family="Times New Roman" encoding="UTF-8">equa\303\247\303\243o de onda</Font></Hyperlink> que descreve a <Hyperlink linktarget="Dictionary:Definition/electromagneticradiation" hyperlink="true"><Font style="Dictionary Hyperlink" family="Times New Roman" encoding="UTF-8">radia\303\247\303\243o eletromagn\303\251tica</Font></Hyperlink><Font encoding="UTF-8">  se propagando atrav\303\251s de um v\303\241cuo com a velocidade da luz. Embora um resultado cl\303\241ssico, essencialmente, as equa\303\247\303\265es de Maxwell ficam inalteradas na forma quando reformuladas na relatividade especial. (Estas leis foram apresentados pela primeira vez em sua forma completa, pelo f\303\255sico escoc\303\252s </Font><Font italic="true">James Clerk Maxwell</Font> (1831-79), cujo primeiro trabalho foi publicado pela Royal Society of Edinburgh, enquanto ele ainda estava na escola. Ele se tornou o primeiro Professor &quot;Cavendish&quot;<Font encoding="UTF-8"> de F\303\255sica em Cambridge e escreveu uma vasta gama de aspectos da radia\303\247\303\243o eletromagn\303\251tica, assim como mec\303\242nica, a teoria cin\303\251tica dos gases e astronomia.) Veja tamb\303\251m </Font><Hyperlink linktarget="Dictionary:Definition/electromagneticpotentials" hyperlink="true"><Font style="Dictionary Hyperlink" family="Times New Roman" encoding="UTF-8">potenciais eletromagn\303\251ticos</Font></Hyperlink>.</Text-field>
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