{"id":2219,"date":"2016-05-14T23:56:57","date_gmt":"2016-05-14T23:56:57","guid":{"rendered":"http:\/\/fisicaevestibular.com.br\/novo\/?page_id=2219"},"modified":"2024-09-02T14:11:58","modified_gmt":"2024-09-02T14:11:58","slug":"laminas-de-faces-paralelas-exercicios","status":"publish","type":"page","link":"https:\/\/fisicaevestibular.com.br\/novo\/optica\/optica-geometrica\/laminas-de-faces-paralelas\/laminas-de-faces-paralelas-exercicios\/","title":{"rendered":"L\u00e2minas de faces paralelas &#8211; Exerc\u00edcios"},"content":{"rendered":"<p align=\"CENTER\"><span style=\"color: #c00000;\"><span style=\"font-family: Arial Black,serif;\"><span style=\"font-size: large;\"><b>Exerc\u00edcios de vestibulares com resolu\u00e7\u00f5es comentadas sobre <\/b><\/span><\/span><\/span><\/p>\n<p align=\"CENTER\"><span style=\"color: #0000cc;\"><span style=\"font-family: Arial Black,serif;\"><span style=\"font-size: large;\"><b>L\u00e2minas de faces paralelas<\/b><\/span><\/span><\/span><\/p>\n<p><span style=\"color: #0000cc;\"><span style=\"font-family: Arial Black,serif;\"><span style=\"font-size: medium;\"><b>01- (MACKENZIE-SP)<\/b><\/span><\/span><\/span><\/p>\n<p><img fetchpriority=\"high\" decoding=\"async\" src=\"http:\/\/fisicaevestibular.com.br\/novo\/wp-content\/uploads\/migracao\/optica\/laminas\/i_120fb32649d00c80_html_1252705c.jpg\" alt=\"\" width=\"629\" height=\"138\" name=\"graphics1\" align=\"BOTTOM\" border=\"0\" \/><\/p>\n<p><span style=\"color: #555555;\"><span style=\"font-family: Arial,serif;\"><span style=\"font-size: medium;\"><b>Sabe-se que uma onda eletromagn\u00e9tica, que se propaga em um meio homog\u00eaneo, transparente e is\u00f3tropo, ao incidir sobre a superf\u00edcie de outro meio, tamb\u00e9m transparente, homog\u00eaneo e is\u00f3tropo, continua a se propagar nele, por\u00e9m, com<\/b><\/span><\/span><\/span><\/p>\n<p><span style=\"color: #555555;\"><span style=\"font-family: Arial,serif;\"><span style=\"font-size: medium;\"><b>algumas altera\u00e7\u00f5es. Se o segundo meio citado for um corpo com a forma de paralelep\u00edpedo, pode-se ter uma situa\u00e7\u00e3o como a ilustrada ao lado, conhecida por L\u00e2mina de Faces Paralelas.<\/b><\/span><\/span><\/span><img decoding=\"async\" src=\"http:\/\/fisicaevestibular.com.br\/novo\/wp-content\/uploads\/migracao\/optica\/laminas\/i_120fb32649d00c80_html_49dac5e8.jpg\" alt=\"\" width=\"457\" height=\"275\" name=\"graphics2\" align=\"LEFT\" border=\"0\" hspace=\"12\" \/><\/p>\n<p><span style=\"color: #555555;\"><span style=\"font-family: Arial,serif;\"><span style=\"font-size: medium;\"><b>Para este exemplo, \u00e9 v\u00e1lido o modelo utilizado em \u00d3ptica Geom\u00e9trica, em que os raios incidente e emergente indicam a dire\u00e7\u00e3o orientada de certa radia\u00e7\u00e3o eletromagn\u00e9tica na faixa da luz e, nesse caso, \u00e9 v\u00e1lida a equa\u00e7\u00e3o:<\/b><\/span><\/span><\/span><\/p>\n<p><img decoding=\"async\" src=\"http:\/\/fisicaevestibular.com.br\/novo\/wp-content\/uploads\/migracao\/optica\/laminas\/i_120fb32649d00c80_html_614b50fa.jpg\" alt=\"\" width=\"140\" height=\"58\" name=\"graphics3\" align=\"BOTTOM\" border=\"0\" \/><\/p>\n<p><span style=\"color: #555555;\"><span style=\"font-family: Arial,serif;\"><span style=\"font-size: medium;\"><b>Com base nessa descri\u00e7\u00e3o, e considerando \u03b8<\/b><\/span><\/span><\/span><span style=\"color: #555555;\"><sub><span style=\"font-family: Arial,serif;\"><span style=\"font-size: medium;\"><b>1<\/b><\/span><\/span><\/sub><\/span><span style=\"color: #555555;\"><span style=\"font-family: Arial,serif;\"><span style=\"font-size: medium;\"><b>\u00a0&gt; \u03b8<\/b><\/span><\/span><\/span><span style=\"color: #555555;\"><sub><span style=\"font-family: Arial,serif;\"><span style=\"font-size: medium;\"><b>2<\/b><\/span><\/span><\/sub><\/span><span style=\"color: #555555;\"><span style=\"font-family: Arial,serif;\"><span style=\"font-size: medium;\"><b>, pode-se afirmar que<\/b><\/span><\/span><\/span><\/p>\n<p><span style=\"color: #555555;\"><span style=\"font-family: Arial,serif;\"><span style=\"font-size: medium;\"><b>a) A velocidade de propaga\u00e7\u00e3o da luz no meio A \u00e9 maior que a velocidade\u00a0\u00a0 de propaga\u00e7\u00e3o da luz no meio B.<\/b><\/span><\/span><\/span><\/p>\n<p><span style=\"color: #555555;\"><span style=\"font-family: Arial,serif;\"><span style=\"font-size: medium;\"><b>b) A velocidade de propaga\u00e7\u00e3o da luz no meio A \u00e9 menor que a velocidade de propaga\u00e7\u00e3o da luz no meio B.<\/b><\/span><\/span><\/span><\/p>\n<p><span style=\"color: #555555;\"><span style=\"font-family: Arial,serif;\"><span style=\"font-size: medium;\"><b>c) A velocidade de propaga\u00e7\u00e3o da luz no meio A \u00e9 menor que a velocidade de propaga\u00e7\u00e3o da luz no meio B, se 45\u00ba\u00a0 &lt;\u00a0 \u03b8<\/b><\/span><\/span><\/span><span style=\"color: #555555;\"><sub><span style=\"font-family: Arial,serif;\"><span style=\"font-size: medium;\"><b>1<\/b><\/span><\/span><\/sub><\/span><span style=\"color: #555555;\"><span style=\"font-family: Arial,serif;\"><span style=\"font-size: medium;\"><b>\u00a0&lt;\u00a0 90\u00ba.<\/b><\/span><\/span><\/span><\/p>\n<p><span style=\"color: #555555;\"><span style=\"font-family: Arial,serif;\"><span style=\"font-size: medium;\"><b>d) A velocidade de propaga\u00e7\u00e3o da luz no meio A \u00e9 menor que a velocidade de propaga\u00e7\u00e3o da luz no meio B, se 0\u00ba &lt; \u03b8<\/b><\/span><\/span><\/span><span style=\"color: #555555;\"><sub><span style=\"font-family: Arial,serif;\"><span style=\"font-size: medium;\"><b>1<\/b><\/span><\/span><\/sub><\/span><\/p>\n<p><span style=\"color: #555555;\">\u00a0<span style=\"font-family: Arial,serif;\"><span style=\"font-size: medium;\"><b>&lt; 45\u00ba.<\/b><\/span><\/span><\/span><\/p>\n<p><span style=\"color: #555555;\"><span style=\"font-family: Arial,serif;\"><span style=\"font-size: medium;\"><b>e) A velocidade de propaga\u00e7\u00e3o da luz no meio A \u00e9 igual \u00e0 velocidade de propaga\u00e7\u00e3o da luz no meio B.<\/b><\/span><\/span><\/span><\/p>\n<p><span style=\"color: #555555;\">\u00a0<\/span><\/p>\n<p><span style=\"color: #0000cc;\"><span style=\"font-family: Arial,serif;\"><span style=\"font-size: medium;\"><b>02-(UFG-GO)<\/b><\/span><\/span><\/span><span style=\"font-family: Arial,serif;\"><span style=\"font-size: medium;\"><b> Observe a l\u00e2mina de faces paralelas da figura abaixo,em que:<\/b><\/span><\/span><img loading=\"lazy\" decoding=\"async\" src=\"http:\/\/fisicaevestibular.com.br\/novo\/wp-content\/uploads\/migracao\/optica\/laminas\/i_120fb32649d00c80_html_dee9625e.jpg\" alt=\"\" width=\"412\" height=\"165\" name=\"Imagem 25\" align=\"LEFT\" border=\"0\" hspace=\"12\" \/><\/p>\n<p><span style=\"font-family: Arial,serif;\"><span style=\"font-size: medium;\"><b>S<\/b><\/span><\/span><sub><span style=\"font-family: Arial,serif;\"><span style=\"font-size: medium;\"><b>1<\/b><\/span><\/span><\/sub><span style=\"font-family: Arial,serif;\"><span style=\"font-size: medium;\"><b>\u00a0e\u00a0<\/b><\/span><\/span><span style=\"font-family: Arial,serif;\"><span style=\"font-size: medium;\"><span style=\"text-decoration: underline;\"><b>S<\/b><\/span><\/span><\/span><sub><span style=\"font-family: Arial,serif;\"><span style=\"font-size: medium;\"><span style=\"text-decoration: underline;\"><b>2\u00a0<\/b><\/span><\/span><\/span><\/sub><span style=\"font-family: Arial,serif;\"><span style=\"font-size: medium;\"><span style=\"text-decoration: underline;\"><b>s\u00e3o superf\u00edcies;<\/b><\/span><\/span><\/span><\/p>\n<p><span style=\"font-family: Arial,serif;\"><span style=\"font-size: medium;\"><b>e \u00e9 a espessura da l\u00e2mina;<\/b><\/span><\/span><\/p>\n<p><span style=\"font-family: Arial,serif;\"><span style=\"font-size: medium;\"><b>i \u00e9 o \u00e2ngulo de incid\u00eancia em S<\/b><\/span><\/span><sub><span style=\"font-family: Arial,serif;\"><span style=\"font-size: medium;\"><b>1<\/b><\/span><\/span><\/sub><span style=\"font-family: Arial,serif;\"><span style=\"font-size: medium;\"><b>;<\/b><\/span><\/span><\/p>\n<p><span style=\"font-family: Arial,serif;\"><span style=\"font-size: medium;\"><b>r \u00e9 o \u00e2ngulo de refra\u00e7\u00e3o em S<\/b><\/span><\/span><sub><span style=\"font-family: Arial,serif;\"><span style=\"font-size: medium;\"><b>1;<\/b><\/span><\/span><\/sub><\/p>\n<p><span style=\"font-family: Arial,serif;\"><span style=\"font-size: medium;\"><b>Sendo\u00a0<img decoding=\"async\" src=\"http:\/\/fisicaevestibular.com.br\/novo\/wp-content\/uploads\/migracao\/optica\/laminas\/i_120fb32649d00c80_html_bb472a70.gif\" alt=\"\" align=\"ABSMIDDLE\" hspace=\"8\" \/> o valor do \u00edndice de refra\u00e7\u00e3o da l\u00e2mina, i=45<\/b><\/span><\/span><sup><span style=\"font-family: Arial,serif;\"><span style=\"font-size: medium;\"><b>o<\/b><\/span><\/span><\/sup><span style=\"font-family: Arial,serif;\"><span style=\"font-size: medium;\"><b>\u00a0e 1,4cm a espessura da l\u00e2mina, e considerando que o meio 1 \u00e9 o ar (n<\/b><\/span><\/span><sub><span style=\"font-family: Arial,serif;\"><span style=\"font-size: medium;\"><b>ar<\/b><\/span><\/span><\/sub><span style=\"font-family: Arial,serif;\"><span style=\"font-size: medium;\"><b>=1), determine o valor do desvio lateral. Dados: sen 30<\/b><\/span><\/span><sup><span style=\"font-family: Arial,serif;\"><span style=\"font-size: medium;\"><b>o<\/b><\/span><\/span><\/sup><span style=\"font-family: Arial,serif;\"><span style=\"font-size: medium;\"><b>=0.5; cos 30<\/b><\/span><\/span><sup><span style=\"font-family: Arial,serif;\"><span style=\"font-size: medium;\"><b>o<\/b><\/span><\/span><\/sup><span style=\"font-family: Arial,serif;\"><span style=\"font-size: medium;\"><b>=0,87 e sen 15<\/b><\/span><\/span><sup><span style=\"font-family: Arial,serif;\"><span style=\"font-size: medium;\"><b>o<\/b><\/span><\/span><\/sup><span style=\"font-family: Arial,serif;\"><span style=\"font-size: medium;\"><b>=0,26.<\/b><\/span><\/span><\/p>\n<p>&nbsp;<\/p>\n<p><span style=\"color: #0000cc;\"><span style=\"font-family: Arial Black,serif;\"><span style=\"font-size: medium;\"><b>03-(PUCC)<\/b><\/span><\/span><\/span><b> <\/b><span style=\"font-family: Arial,serif;\"><span style=\"font-size: medium;\"><b>Quando se observa um objeto atrav\u00e9s de uma vidra\u00e7a comum, vemos:<\/b><\/span><\/span><\/p>\n<p><span style=\"font-family: Arial,serif;\"><span style=\"font-size: medium;\"><b>a) uma imagem real do objeto;\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0 <\/b><\/span><\/span><\/p>\n<p><span style=\"font-family: Arial,serif;\"><span style=\"font-size: medium;\"><b>b) uma imagem virtual do objeto\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0 <\/b><\/span><\/span><\/p>\n<p><span style=\"font-family: Arial,serif;\"><span style=\"font-size: medium;\"><b>c) o pr\u00f3prio objeto\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0 \u00a0<\/b><\/span><\/span><\/p>\n<p><span style=\"font-family: Arial,serif;\"><span style=\"font-size: medium;\"><b>d) uma imagem impr\u00f3pria do objeto;\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0 <\/b><\/span><\/span><\/p>\n<p><span style=\"font-family: Arial,serif;\"><span style=\"font-size: medium;\"><b>e) uma imagem invertida.<\/b><\/span><\/span><\/p>\n<p>&nbsp;<\/p>\n<p><span style=\"color: #0000cc;\"><span style=\"font-family: Arial Black,serif;\"><span style=\"font-size: medium;\"><b>04- (UNIRIO)<\/b><\/span><\/span><\/span><b> <\/b><span style=\"font-family: Arial,serif;\"><span style=\"font-size: medium;\"><b>Um c\u00e3o est\u00e1 diante de uma mesa, observando um peixinho dentro do aqu\u00e1rio, conforme\u00a0 representado na figura. Ao mesmo tempo, o peixinho tamb\u00e9m observa o c\u00e3o. Em rela\u00e7\u00e3o \u00e0 parede P do aqu\u00e1rio e \u00e0s dist\u00e2ncias reais, podemos afirmar que as imagens observadas por cada um dos animais obedecem \u00e0s seguintes rela\u00e7\u00f5es:<\/b><\/span><\/span><\/p>\n<p><img loading=\"lazy\" decoding=\"async\" src=\"http:\/\/fisicaevestibular.com.br\/novo\/wp-content\/uploads\/migracao\/optica\/laminas\/i_120fb32649d00c80_html_b397420d.jpg\" alt=\"\" width=\"228\" height=\"117\" name=\"Imagem 26\" align=\"BOTTOM\" border=\"0\" \/><\/p>\n<p>&nbsp;<\/p>\n<p><span style=\"font-family: Arial,serif;\"><span style=\"font-size: medium;\"><b>a) O c\u00e3o observa o olho do peixinho mais pr\u00f3ximo da parede P, enquanto o peixinho observa o olho do c\u00e3o mais distante do aqu\u00e1rio.<\/b><\/span><\/span><\/p>\n<p><span style=\"font-family: Arial,serif;\"><span style=\"font-size: medium;\"><b>b) O c\u00e3o observa o olho do peixinho mais distante da parede P, enquanto o peixinho observa o olho do c\u00e3o mais pr\u00f3ximo do aqu\u00e1rio.<\/b><\/span><\/span><\/p>\n<p><span style=\"font-family: Arial,serif;\"><span style=\"font-size: medium;\"><b>c) O c\u00e3o observa o olho do peixinho mais pr\u00f3ximo da parede P, enquanto o peixinho observa o olho do c\u00e3o mais pr\u00f3ximo do aqu\u00e1rio.<\/b><\/span><\/span><\/p>\n<p><span style=\"font-family: Arial,serif;\"><span style=\"font-size: medium;\"><b>d) O c\u00e3o observa o olho do peixinho mais distante da parede P, enquanto o peixinho observa o olho do c\u00e3o tamb\u00e9m mais distante do aqu\u00e1rio.<\/b><\/span><\/span><\/p>\n<p><span style=\"font-family: Arial,serif;\"><span style=\"font-size: medium;\"><b>e) O c\u00e3o e o peixinho observam o olho um do outro, em rela\u00e7\u00e3o \u00e0 parede P, em dist\u00e2ncias iguais \u00e0s dist\u00e2ncias reais que eles ocupam na figura.<\/b><\/span><\/span><\/p>\n<p>&nbsp;<\/p>\n<p><span style=\"color: #0000cc;\"><span style=\"font-family: Arial Black,serif;\"><span style=\"font-size: medium;\"><b>05-(UEL)<\/b><\/span><\/span><\/span><b> <\/b><span style=\"font-family: Arial,serif;\"><span style=\"font-size: medium;\"><b>Um raio de luz r atravessa uma l\u00e2mina de vidro de faces paralelas, imersa no ar, sendo parcialmente refletido nas duas faces.<\/b><\/span><\/span><\/p>\n<p align=\"CENTER\"><img loading=\"lazy\" decoding=\"async\" src=\"http:\/\/fisicaevestibular.com.br\/novo\/wp-content\/uploads\/migracao\/optica\/laminas\/i_120fb32649d00c80_html_cb464708.jpg\" alt=\"\" width=\"314\" height=\"210\" name=\"Imagem 27\" align=\"BOTTOM\" border=\"0\" \/><\/p>\n<p>&nbsp;<\/p>\n<p><span style=\"font-family: Arial,serif;\"><span style=\"font-size: medium;\"><b>Considerando os \u00e2ngulos indicados no esquema, o \u00e2ngulo q \u00e9 igual a:<\/b><\/span><\/span><\/p>\n<p><img loading=\"lazy\" decoding=\"async\" src=\"http:\/\/fisicaevestibular.com.br\/novo\/wp-content\/uploads\/migracao\/optica\/laminas\/i_120fb32649d00c80_html_a8e553c2.png\" alt=\"\" width=\"765\" height=\"20\" name=\"Imagem 24\" align=\"BOTTOM\" border=\"0\" \/><\/p>\n<p>&nbsp;<\/p>\n<p><span style=\"color: #0000cc;\"><span style=\"font-family: Arial,serif;\"><span style=\"font-size: medium;\"><b>06-(UFRS-RS) <\/b><\/span><\/span><\/span><span style=\"font-family: Arial,serif;\"><span style=\"font-size: medium;\"><b>Um raio de luz, proveniente da esquerda, incide sobre uma l\u00e2mina de vidro de faces paralelas, imersa no ar, com \u00e2ngulo de incid\u00eancia i<\/b><\/span><\/span><sub><span style=\"font-family: Arial,serif;\"><span style=\"font-size: medium;\"><b>1<\/b><\/span><\/span><\/sub><span style=\"font-family: Arial,serif;\"><span style=\"font-size: medium;\"><b>\u00a0na interface ar-vidro. Depois de atravessar a l\u00e2mina, ele emerge do vidro com \u00e2ngulo r<\/b><\/span><\/span><sub><span style=\"font-family: Arial,serif;\"><span style=\"font-size: medium;\"><b>2<\/b><\/span><\/span><\/sub><span style=\"font-family: Arial,serif;\"><span style=\"font-size: medium;\"><b>. O trajeto do raio luminoso est\u00e1 representado na figura, onde o \u00e2ngulo r<\/b><\/span><\/span><sub><span style=\"font-family: Arial,serif;\"><span style=\"font-size: medium;\"><b>1<\/b><\/span><\/span><\/sub><span style=\"font-family: Arial,serif;\"><span style=\"font-size: medium;\"><b>\u00a0designa o \u00e2ngulo de refra\u00e7\u00e3o no vidro, e i<\/b><\/span><\/span><sub><span style=\"font-family: Arial,serif;\"><span style=\"font-size: medium;\"><b>1<\/b><\/span><\/span><\/sub><span style=\"font-family: Arial,serif;\"><span style=\"font-size: medium;\"><b>, o \u00e2ngulo de incid\u00eancia na interface vidro-ar.<\/b><\/span><\/span><\/p>\n<p><img loading=\"lazy\" decoding=\"async\" src=\"http:\/\/fisicaevestibular.com.br\/novo\/wp-content\/uploads\/migracao\/optica\/laminas\/i_120fb32649d00c80_html_2eac794d.jpg\" alt=\"\" width=\"433\" height=\"159\" name=\"Imagem 28\" align=\"BOTTOM\" border=\"0\" \/><\/p>\n<p><span style=\"font-family: Arial,serif;\"><span style=\"font-size: medium;\"><b>Nessa situa\u00e7\u00e3o, pode-se afirmar que<\/b><\/span><\/span><\/p>\n<p><img loading=\"lazy\" decoding=\"async\" src=\"http:\/\/fisicaevestibular.com.br\/novo\/wp-content\/uploads\/migracao\/optica\/laminas\/i_120fb32649d00c80_html_949c2d28.png\" alt=\"\" width=\"764\" height=\"24\" name=\"Imagem 63\" align=\"BOTTOM\" border=\"0\" \/><\/p>\n<p><span style=\"color: #0000cc;\"><span style=\"font-family: Arial Black,serif;\"><span style=\"font-size: medium;\"><b>07-(UFRS-RS)<\/b><\/span><\/span><\/span><b> <\/b><span style=\"font-family: Arial,serif;\"><span style=\"font-size: medium;\"><b>Na figura a seguir, um feixe de luz monocrom\u00e1tica I, proveniente do ar, incide sobre uma placa de vidro de faces planas e paralelas, sofrendo reflex\u00f5es e refra\u00e7\u00f5es em ambas as faces da placa.<\/b><\/span><\/span><img loading=\"lazy\" decoding=\"async\" src=\"http:\/\/fisicaevestibular.com.br\/novo\/wp-content\/uploads\/migracao\/optica\/laminas\/i_120fb32649d00c80_html_3dff90d8.jpg\" alt=\"\" width=\"463\" height=\"216\" name=\"Imagem 29\" align=\"LEFT\" border=\"0\" hspace=\"12\" \/><\/p>\n<p><span style=\"font-family: Arial,serif;\"><span style=\"font-size: medium;\"><b>Na figura,\u00a0\u03b8<\/b><\/span><\/span><sub><span style=\"font-family: Arial,serif;\"><span style=\"font-size: medium;\"><b>i<\/b><\/span><\/span><\/sub><span style=\"font-family: Arial,serif;\"><span style=\"font-size: medium;\"><b> representa o \u00e2ngulo formado pela dire\u00e7\u00e3o do feixe incidente com a normal \u00e0 superf\u00edcie no ponto A, e\u00a0\u03b8<\/b><\/span><\/span><sub><span style=\"font-family: Arial,serif;\"><span style=\"font-size: medium;\"><b>r<\/b><\/span><\/span><\/sub><span style=\"font-family: Arial,serif;\"><span style=\"font-size: medium;\"><b>\u00a0representa o \u00e2ngulo formado pela dire\u00e7\u00e3o da parte refratada desse feixe com a normal no mesmo ponto A.<\/b><\/span><\/span><\/p>\n<p><span style=\"font-family: Arial,serif;\"><span style=\"font-size: medium;\"><b>Quais \u00e2ngulos s\u00e3o iguais a\u00a0a,\u00a0b\u00a0e\u00a0l?<\/b><\/span><\/span><\/p>\n<p><span style=\"color: #0000cc;\"><span style=\"font-family: Arial Black,serif;\"><span style=\"font-size: medium;\"><b>08-(UFPA)<\/b><\/span><\/span><\/span><b> <\/b><span style=\"font-family: Arial,serif;\"><span style=\"font-size: medium;\"><b>O desvio angular sofrido por um raio de luz que incide segundo o \u00e2ngulo de 60\u00b0 com a normal \u00e0\u00a0superf\u00edcie de uma l\u00e2mina de faces paralelas, ap\u00f3s atravess\u00e1-la \u00e9 de:<\/b><\/span><\/span><\/p>\n<p><img loading=\"lazy\" decoding=\"async\" src=\"http:\/\/fisicaevestibular.com.br\/novo\/wp-content\/uploads\/migracao\/optica\/laminas\/i_120fb32649d00c80_html_b2f80d77.png\" alt=\"\" width=\"765\" height=\"20\" name=\"Imagem 101\" align=\"BOTTOM\" border=\"0\" \/><\/p>\n<p><span style=\"color: #0000cc;\"><span style=\"font-family: Arial Black,serif;\"><span style=\"font-size: medium;\"><b>09-(UFBA)<\/b><\/span><\/span><\/span><b> <\/b><span style=\"font-family: Arial,serif;\"><span style=\"font-size: medium;\"><b>Um feixe de luz monocrom\u00e1tica, cuja velocidade no v\u00e1cuo tem m\u00f3dulo igual a 3,0 .10<\/b><\/span><\/span><sup><span style=\"font-family: Arial,serif;\"><span style=\"font-size: medium;\"><b>8<\/b><\/span><\/span><\/sup><span style=\"font-family: Arial,serif;\"><span style=\"font-size: medium;\"><b>m\/s, incide perpendicularmente em uma l\u00e2mina transparente e espessa de \u00edndice de refra\u00e7\u00e3o absoluto n = 1,50.\u00a0Determine a espessura da l\u00e2mina, sabendo-se que a luz gasta 1,0 .10<\/b><\/span><\/span><sup><span style=\"font-family: Arial,serif;\"><span style=\"font-size: medium;\"><b>-10<\/b><\/span><\/span><\/sup><span style=\"font-family: Arial,serif;\"><span style=\"font-size: medium;\"><b>s para atravess\u00e1-la<\/b><\/span><\/span><\/p>\n<p>&nbsp;<\/p>\n<p><span style=\"color: #0000cc;\"><span style=\"font-family: Arial Black,serif;\"><span style=\"font-size: medium;\"><b>10-(FUVEST-SP<\/b><\/span><\/span><\/span><span style=\"font-family: Arial,serif;\"><span style=\"font-size: medium;\"><b>) Um raio luminoso proveniente do ar atinge uma l\u00e2mina de vidro de faces paralelas com 8,0 cm de espessura e 1,5 de \u00edndice de refra\u00e7\u00e3o. Este raio sofre refra\u00e7\u00e3o e reflex\u00e3o ao atingir a primeira superf\u00edcie; refra\u00e7\u00e3o e reflex\u00e3o ao atingir a segunda superf\u00edcie (interna).<\/b><\/span><\/span><\/p>\n<p><span style=\"font-family: Arial,serif;\"><span style=\"font-size: medium;\"><b>a) Trace as trajet\u00f3rias dos raios: incidente, refratados e refletidos<\/b><\/span><\/span><\/p>\n<p><span style=\"font-family: Arial,serif;\"><span style=\"font-size: medium;\"><b>b) Determine o tempo para o raio refrato atravessar a l\u00e2mina, sendo o seno do \u00e2ngulo de incid\u00eancia 0,9. Considere: C=3,0.10<\/b><\/span><\/span><sup><span style=\"font-family: Arial,serif;\"><span style=\"font-size: medium;\"><b>8<\/b><\/span><\/span><\/sup><span style=\"font-family: Arial,serif;\"><span style=\"font-size: medium;\"><b>m\/s e n(ar)=1,0.<\/b><\/span><\/span><\/p>\n<p>&nbsp;<\/p>\n<p><span style=\"color: #0000cc;\"><span style=\"font-family: Arial Black,serif;\"><span style=\"font-size: medium;\"><b>11-(MED. TAUBAT\u00c9)<\/b><\/span><\/span><\/span><b> <\/b><span style=\"font-family: Arial,serif;\"><span style=\"font-size: medium;\"><b>Tem-se\u00a0 um aparelho que emite um feixe colimado, estreito, de luz verde. Mas o feixe \u00e9, na\u00a0verdade, mistura de luz amarela com azul. Pode-se descobrir tal fato, fazendo-se incidir o feixe numa\u00a0l\u00e2mina de\u00a0vidro de faces paralelas?<\/b><\/span><\/span><\/p>\n<p><span style=\"font-family: Arial,serif;\"><span style=\"font-size: medium;\"><b>a) N\u00e3o; os dois feixes emergiriam da l\u00e2mina coincidentes.<\/b><\/span><\/span><\/p>\n<p><span style=\"font-family: Arial,serif;\"><span style=\"font-size: medium;\"><b>b) Sim; aumentando-se o \u00e2ngulo de incid\u00eancia at\u00e9 o \u00e2ngulo limite de refra\u00e7\u00e3o de uma das cores; ent\u00e3o\u00a0s\u00f3 a\u00a0outra se transmitiria.<\/b><\/span><\/span><\/p>\n<p><span style=\"font-family: Arial,serif;\"><span style=\"font-size: medium;\"><b>c) Sim; uma das cores sofreria um desvio de dire\u00e7\u00e3o maior que a outra, numa incid\u00eancia obl\u00edqua.<\/b><\/span><\/span><\/p>\n<p><span style=\"font-family: Arial,serif;\"><span style=\"font-size: medium;\"><b>d) Sim; uma das cores sofreria um deslocamento paralelo maior que a outra, numa incid\u00eancia obl\u00edqua.\u00a0<\/b><\/span><\/span><\/p>\n<p><span style=\"font-family: Arial,serif;\"><span style=\"font-size: medium;\"><b>e) Sim; a cor do feixe emergente seria diferente para diferentes \u00e2ngulos de incid\u00eancia.<\/b><\/span><\/span><\/p>\n<p>&nbsp;<\/p>\n<p><span style=\"color: #0000cc;\"><span style=\"font-family: Arial Black,serif;\"><span style=\"font-size: medium;\"><b>12-(UEFS)<\/b><\/span><\/span><\/span><b> <\/b><span style=\"font-family: Arial,serif;\"><span style=\"font-size: medium;\"><b>Uma l\u00e2mina de faces paralelas, constru\u00edda de forma que uma das suas faces \u00e9 espelhada\u00a0internamente,\u00a0est\u00e1 imersa no ar. Um raio luminoso, propagando-se no ar, incide, com \u00e2ngulo i, na face n\u00e3o espelhada e \u00e9\u00a0refratado. Em seguida, o raio \u00e9 refletido na face espelhada e volta ao ar, depois de ser novamente refratado.\u00a0O \u00e2ngulo de refra\u00e7\u00e3o, no retorno do raio luminoso da l\u00e2mina para o ar, \u00e9 igual a:<\/b><\/span><\/span><\/p>\n<p><img loading=\"lazy\" decoding=\"async\" src=\"http:\/\/fisicaevestibular.com.br\/novo\/wp-content\/uploads\/migracao\/optica\/laminas\/i_120fb32649d00c80_html_a5eb80bc.png\" alt=\"\" width=\"764\" height=\"19\" name=\"Imagem 105\" align=\"BOTTOM\" border=\"0\" \/><\/p>\n<p><span style=\"color: #0000cc;\"><span style=\"font-family: Arial Black,serif;\"><span style=\"font-size: medium;\"><b>13-(UnB-DF)<\/b><\/span><\/span><\/span><b> <\/b><\/p>\n<p><img loading=\"lazy\" decoding=\"async\" src=\"http:\/\/fisicaevestibular.com.br\/novo\/wp-content\/uploads\/migracao\/optica\/laminas\/i_120fb32649d00c80_html_6ecff45.jpg\" alt=\"\" width=\"399\" height=\"234\" name=\"Imagem 30\" align=\"LEFT\" border=\"0\" hspace=\"12\" \/><\/p>\n<p><span style=\"font-family: Arial,serif;\"><span style=\"font-size: medium;\"><b>Um feixe de luz passa de um meio 1 para um meio 2 e chega novamente ao meio 1, conforme figura.<\/b><\/span><\/span><\/p>\n<p><span style=\"font-family: Arial,serif;\"><span style=\"font-size: medium;\"><b>A linha tracejada representa um prolongamento de feixe incidente. Sendo\u00a0q=30<\/b><\/span><\/span><sup><span style=\"font-family: Arial,serif;\"><span style=\"font-size: medium;\"><b>o<\/b><\/span><\/span><\/sup><span style=\"font-family: Arial,serif;\"><span style=\"font-size: medium;\"><b>, e=2\u00d63cm e X=1cm, calcule o \u00edndice de refra\u00e7\u00e3o do meio 2. Considere o meio 1 como sendo o ar o ar (n<\/b><\/span><\/span><sub><span style=\"font-family: Arial,serif;\"><span style=\"font-size: medium;\"><b>ar<\/b><\/span><\/span><\/sub><span style=\"font-family: Arial,serif;\"><span style=\"font-size: medium;\"><b>=1,0) e sen15<\/b><\/span><\/span><sup><span style=\"font-family: Arial,serif;\"><span style=\"font-size: medium;\"><b>0<\/b><\/span><\/span><\/sup><span style=\"font-family: Arial,serif;\"><span style=\"font-size: medium;\"><b>=cos75<\/b><\/span><\/span><sup><span style=\"font-family: Arial,serif;\"><span style=\"font-size: medium;\"><b>o<\/b><\/span><\/span><\/sup><span style=\"font-family: Arial,serif;\"><span style=\"font-size: medium;\"><b>=0,26<\/b><\/span><\/span><\/p>\n<p>&nbsp;<\/p>\n<p><span style=\"color: #0000cc;\"><span style=\"font-family: Arial Black,serif;\"><span style=\"font-size: medium;\"><b>14-(FUVEST)<\/b><\/span><\/span><\/span><b> <\/b><span style=\"font-family: Arial,serif;\"><span style=\"font-size: medium;\"><b>Um feixe de luz monocrom\u00e1tica incide sobre l\u00e2minas paralelas de diamante e vidro, como\u00a0representado\u00a0na figura. Sendo os \u00edndices de refra\u00e7\u00e3o absolutos 2,42 para o diamante e 1,52 para o\u00a0vidro, qual das linhas da\u00a0figura que melhor representa a trajet\u00f3ria do feixe luminoso?<\/b><\/span><\/span><\/p>\n<p><img loading=\"lazy\" decoding=\"async\" src=\"http:\/\/fisicaevestibular.com.br\/novo\/wp-content\/uploads\/migracao\/optica\/laminas\/i_120fb32649d00c80_html_4ef038b1.png\" alt=\"\" width=\"758\" height=\"172\" name=\"Imagem 107\" align=\"BOTTOM\" border=\"0\" \/><\/p>\n<p><span style=\"color: #0000cc;\"><span style=\"font-family: Arial Black,serif;\"><span style=\"font-size: medium;\"><b>15-(CESGRANRIO)<\/b><\/span><\/span><\/span><\/p>\n<p><span style=\"font-family: Arial,serif;\"><span style=\"font-size: medium;\"><b>Dois meios A e C est\u00e3o separados por uma l\u00e2mina de faces paralelas (B). Um raio luminoso I, <\/b><\/span><\/span><\/p>\n<p align=\"CENTER\"><img loading=\"lazy\" decoding=\"async\" src=\"http:\/\/fisicaevestibular.com.br\/novo\/wp-content\/uploads\/migracao\/optica\/laminas\/i_120fb32649d00c80_html_e8ce1439.jpg\" alt=\"\" width=\"370\" height=\"162\" name=\"Imagem 108\" align=\"BOTTOM\" border=\"0\" \/><\/p>\n<p><span style=\"font-family: Arial,serif;\"><span style=\"font-size: medium;\"><b>propagando-se em A, penetra em B e sofre reflex\u00e3o total na face que separa B de C, conforme indica a figura anterior.<\/b><\/span><\/span><\/p>\n<p><span style=\"font-family: Arial,serif;\"><span style=\"font-size: medium;\"><b>Sendo n<\/b><\/span><\/span><sub><span style=\"font-family: Arial,serif;\"><span style=\"font-size: medium;\"><b>A<\/b><\/span><\/span><\/sub><span style=\"font-family: Arial,serif;\"><span style=\"font-size: medium;\"><b>, n<\/b><\/span><\/span><sub><span style=\"font-family: Arial,serif;\"><span style=\"font-size: medium;\"><b>B<\/b><\/span><\/span><\/sub><span style=\"font-family: Arial,serif;\"><span style=\"font-size: medium;\"><b>\u00a0e n<\/b><\/span><\/span><sub><span style=\"font-family: Arial,serif;\"><span style=\"font-size: medium;\"><b>C<\/b><\/span><\/span><\/sub><span style=\"font-family: Arial,serif;\"><span style=\"font-size: medium;\"><b>\u00a0os \u00edndices de refra\u00e7\u00e3o dos meios A, B e C, qual a rela\u00e7\u00e3o entre eles?<\/b><\/span><\/span><\/p>\n<p>&nbsp;<\/p>\n<p><span style=\"color: #0000cc;\"><span style=\"font-family: Arial Black,serif;\"><span style=\"font-size: medium;\"><b>16-(UFMG)<\/b><\/span><\/span><\/span><b> <\/b><span style=\"font-family: Arial,serif;\"><span style=\"font-size: medium;\"><b>A figura mostra a trajet\u00f3ria de um feixe de luz que vem de um meio I, atravessa um meio II, \u00e9 totalmente refletido na interface dos meios II e III e retorna ao meio I.<\/b><\/span><\/span><\/p>\n<p align=\"CENTER\"><img loading=\"lazy\" decoding=\"async\" src=\"http:\/\/fisicaevestibular.com.br\/novo\/wp-content\/uploads\/migracao\/optica\/laminas\/i_120fb32649d00c80_html_fa374e01.jpg\" alt=\"\" width=\"316\" height=\"214\" name=\"Imagem 33\" align=\"BOTTOM\" border=\"0\" \/><\/p>\n<p><span style=\"font-family: Arial,serif;\"><span style=\"font-size: medium;\"><b>Sabe-se que o \u00edndice de refra\u00e7\u00e3o do ar \u00e9 menor que o da \u00e1gua e que o da \u00e1gua \u00e9 menor que o do vidro. Nesse caso \u00e9 correto afirmar que os meios I, II e III podem ser, respectivamente:<\/b><\/span><\/span><\/p>\n<p><span style=\"font-family: Arial,serif;\"><span style=\"font-size: medium;\"><b>a) ar, \u00e1gua e vidro\u00a0\u00a0\u00a0\u00a0\u00a0 <\/b><\/span><\/span><\/p>\n<p><span style=\"font-family: Arial,serif;\"><span style=\"font-size: medium;\"><b>b) vidro, \u00e1gua e ar\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0 <\/b><\/span><\/span><\/p>\n<p><span style=\"font-family: Arial,serif;\"><span style=\"font-size: medium;\"><b>c) \u00e1gua, ar e vidro\u00a0\u00a0\u00a0\u00a0\u00a0 <\/b><\/span><\/span><\/p>\n<p><span style=\"font-family: Arial,serif;\"><span style=\"font-size: medium;\"><b>d)\u00a0 ar, vidro e \u00e1gua<\/b><\/span><\/span><\/p>\n<p><span style=\"color: #0000cc;\">\u00a0<\/span><\/p>\n<p><span style=\"color: #0000cc;\"><span style=\"font-family: Arial Black,serif;\"><span style=\"font-size: medium;\"><b>17-(FUVEST-SP)<\/b><\/span><\/span><\/span><b> <\/b><span style=\"font-family: Arial,serif;\"><span style=\"font-size: medium;\"><b>Numa folha de papel num plano horizontal, est\u00e1 desenhado um c\u00edrculo de centro C. Sobre a folha \u00e9 colocada uma placa grossa de vidro, cobrindo metade do c\u00edrculo. A figura a seguir mostra uma pessoa olhando para o c\u00edrculo, com seu olho no eixo vertical OC.<\/b><\/span><\/span><\/p>\n<p align=\"CENTER\"><img loading=\"lazy\" decoding=\"async\" src=\"http:\/\/fisicaevestibular.com.br\/novo\/wp-content\/uploads\/migracao\/optica\/laminas\/i_120fb32649d00c80_html_2b0f4b98.jpg\" alt=\"\" width=\"451\" height=\"154\" name=\"Imagem 34\" align=\"BOTTOM\" border=\"0\" \/><\/p>\n<p><span style=\"font-family: Arial,serif;\"><span style=\"font-size: medium;\"><b>A alternativa que melhor representa o que a pessoa enxerga \u00e9:<\/b><\/span><\/span><\/p>\n<p><img loading=\"lazy\" decoding=\"async\" src=\"http:\/\/fisicaevestibular.com.br\/novo\/wp-content\/uploads\/migracao\/optica\/laminas\/i_120fb32649d00c80_html_ad211f3d.jpg\" alt=\"\" width=\"759\" height=\"198\" name=\"Imagem 35\" align=\"BOTTOM\" border=\"0\" \/><\/p>\n<p>&nbsp;<\/p>\n<p><span style=\"color: #0000cc;\"><span style=\"font-family: Arial Black,serif;\"><span style=\"font-size: medium;\"><b>18-(UFBA)<\/b><\/span><\/span><\/span><b> <\/b><span style=\"font-family: Arial,serif;\"><span style=\"font-size: medium;\"><b>A figura mostra um raio de luz \u00a0monocrom\u00e1tico que atravessa uma l\u00e2mina de faces paralelas, de \u00edndice de refra\u00e7\u00e3o igual a \u221a3 e espessura 2\u221a3cm.<\/b><\/span><\/span><img loading=\"lazy\" decoding=\"async\" src=\"http:\/\/fisicaevestibular.com.br\/novo\/wp-content\/uploads\/migracao\/optica\/laminas\/i_120fb32649d00c80_html_b6913bb1.jpg\" alt=\"\" width=\"478\" height=\"208\" name=\"Imagem 36\" align=\"LEFT\" border=\"0\" hspace=\"12\" \/><\/p>\n<p><span style=\"font-family: Arial,serif;\"><span style=\"font-size: medium;\"><b>Sendo o \u00edndice de refra\u00e7\u00e3o do ar igual a 1, sen30<\/b><\/span><\/span><sup><span style=\"font-family: Arial,serif;\"><span style=\"font-size: medium;\"><b>o<\/b><\/span><\/span><\/sup><span style=\"font-family: Arial,serif;\"><span style=\"font-size: medium;\"><b>=cos60<\/b><\/span><\/span><sup><span style=\"font-family: Arial,serif;\"><span style=\"font-size: medium;\"><b>o<\/b><\/span><\/span><\/sup><span style=\"font-family: Arial,serif;\"><span style=\"font-size: medium;\"><b>=1\/2 e sen60<\/b><\/span><\/span><sup><span style=\"font-family: Arial,serif;\"><span style=\"font-size: medium;\"><b>o<\/b><\/span><\/span><\/sup><span style=\"font-family: Arial,serif;\"><span style=\"font-size: medium;\"><b>=cos30<\/b><\/span><\/span><sup><span style=\"font-family: Arial,serif;\"><span style=\"font-size: medium;\"><b>o<\/b><\/span><\/span><\/sup><span style=\"font-family: Arial,serif;\"><span style=\"font-size: medium;\"><b>=\u221a3\/2, \u00e9 correto afirmar:<\/b><\/span><\/span><\/p>\n<p><span style=\"font-family: Arial,serif;\"><span style=\"font-size: medium;\"><b>(01) O raio incidente e o raio que emerge da l\u00e2mina possuem dire\u00e7\u00f5es diferentes.<\/b><\/span><\/span><\/p>\n<p><span style=\"font-family: Arial,serif;\"><span style=\"font-size: medium;\"><b>(02) O \u00e2ngulo de refra\u00e7\u00e3o, no interior da l\u00e2mina, mede 30<\/b><\/span><\/span><sup><span style=\"font-family: Arial,serif;\"><span style=\"font-size: medium;\"><b>o<\/b><\/span><\/span><\/sup><span style=\"font-family: Arial,serif;\"><span style=\"font-size: medium;\"><b>.<\/b><\/span><\/span><\/p>\n<p><span style=\"font-family: Arial,serif;\"><span style=\"font-size: medium;\"><b>(04) O desvio lateral, (d), sofrido pelo raio ap\u00f3s atravessar a l\u00e2mina, \u00e9 igual a 2cm.<\/b><\/span><\/span><\/p>\n<p><span style=\"font-family: Arial,serif;\"><span style=\"font-size: medium;\"><b>(08) A velocidade de propaga\u00e7\u00e3o do raio luminoso, no interior da l\u00e2mina, \u00e9 inversamente proporcional ao \u00edndice de refra\u00e7\u00e3o do material que a constitui.<\/b><\/span><\/span><\/p>\n<p><span style=\"font-family: Arial,serif;\"><span style=\"font-size: medium;\"><b>(16) O raio refratado n\u00e3o sofrer\u00e1 desvio, se o raio luminoso incidir numa dire\u00e7\u00e3o normal \u00e0 l\u00e2mina.\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0<\/b><\/span><\/span><\/p>\n<p>&nbsp;<\/p>\n<p><span style=\"color: #0000cc;\"><span style=\"font-family: Arial Black,serif;\"><span style=\"font-size: medium;\"><b>19-(UFRJ-RJ)<\/b><\/span><\/span><\/span><span style=\"color: #0000cc;\"><span style=\"font-family: Arial,serif;\"><span style=\"font-size: medium;\"><b> U<\/b><\/span><\/span><\/span><span style=\"font-family: Arial,serif;\"><span style=\"font-size: medium;\"><b>ma l\u00e2mina homog\u00eanea de faces paralelas \u00e9 constitu\u00edda de um material com \u00edndice de refra\u00e7\u00e3o n<\/b><\/span><\/span><sub><span style=\"font-family: Arial,serif;\"><span style=\"font-size: medium;\"><b>2<\/b><\/span><\/span><\/sub><span style=\"font-family: Arial,serif;\"><span style=\"font-size: medium;\"><b>=1,5. De um lado da l\u00e2mina, h\u00e1 um meio homog\u00eaneo de \u00edndice de refra\u00e7\u00e3o n<\/b><\/span><\/span><sub><span style=\"font-family: Arial,serif;\"><span style=\"font-size: medium;\"><b>1<\/b><\/span><\/span><\/sub><span style=\"font-family: Arial,serif;\"><span style=\"font-size: medium;\"><b>=2,0; do outro lado, h\u00e1 ar, cujo \u00edndice de refra\u00e7\u00e3o n<\/b><\/span><\/span><sub><span style=\"font-family: Arial,serif;\"><span style=\"font-size: medium;\"><b>3<\/b><\/span><\/span><\/sub><span style=\"font-family: Arial,serif;\"><span style=\"font-size: medium;\"><b>\u00a0consideramos igual a 1,0. Um raio luminoso proveniente do primeiro meio incide sobre a l\u00e2mina com \u00e2ngulo de incid\u00eancia \u03b8<\/b><\/span><\/span><sub><span style=\"font-family: Arial,serif;\"><span style=\"font-size: medium;\"><b>1<\/b><\/span><\/span><\/sub><span style=\"font-family: Arial,serif;\"><span style=\"font-size: medium;\"><b>, como indica a figura.<\/b><\/span><\/span><img loading=\"lazy\" decoding=\"async\" src=\"http:\/\/fisicaevestibular.com.br\/novo\/wp-content\/uploads\/migracao\/optica\/laminas\/i_120fb32649d00c80_html_82db9092.jpg\" alt=\"\" width=\"402\" height=\"173\" name=\"Imagem 37\" align=\"LEFT\" border=\"0\" hspace=\"12\" \/><\/p>\n<p><span style=\"font-family: Arial,serif;\"><span style=\"font-size: medium;\"><b>Calcule o valor de \u03b8<\/b><\/span><\/span><sub><span style=\"font-family: Arial,serif;\"><span style=\"font-size: medium;\"><b>1<\/b><\/span><\/span><\/sub><span style=\"font-family: Arial,serif;\"><span style=\"font-size: medium;\"><b>\u00a0a partir do qual o raio que atravessa a l\u00e2mina sofra reflex\u00e3o total na interface com o ar.<\/b><\/span><\/span><\/p>\n<p>&nbsp;<\/p>\n<p><span style=\"color: #0000cc;\"><span style=\"font-family: Arial Black,serif;\"><span style=\"font-size: medium;\"><b>20-(UFCE)<\/b><\/span><\/span><\/span><span style=\"color: #0000cc;\"><span style=\"font-family: Arial,serif;\"><span style=\"font-size: medium;\"><b>\u00a0 <\/b><\/span><\/span><\/span><span style=\"font-family: Arial,serif;\"><span style=\"font-size: medium;\"><b>Um raio de luz propagando-se no ar ( n<\/b><\/span><\/span><sub><span style=\"font-family: Arial,serif;\"><span style=\"font-size: medium;\"><b>ar<\/b><\/span><\/span><\/sub><span style=\"font-family: Arial,serif;\"><span style=\"font-size: medium;\"><b>=1 ) incide com um angulo de incid\u00eancia igual a 45<\/b><\/span><\/span><sup><span style=\"font-family: Arial,serif;\"><span style=\"font-size: medium;\"><b>o<\/b><\/span><\/span><\/sup><span style=\"font-family: Arial,serif;\"><span style=\"font-size: medium;\"><b>, em uma das faces de uma lamina feita com um material transparente de \u00edndice de refra\u00e7\u00e3o \u00a0n, como mostra a figura.<\/b><\/span><\/span><\/p>\n<p align=\"CENTER\"><img loading=\"lazy\" decoding=\"async\" src=\"http:\/\/fisicaevestibular.com.br\/novo\/wp-content\/uploads\/migracao\/optica\/laminas\/i_120fb32649d00c80_html_92a3b178.jpg\" alt=\"\" width=\"494\" height=\"200\" name=\"Imagem 38\" align=\"BOTTOM\" border=\"0\" \/><\/p>\n<p><span style=\"font-family: Arial,serif;\"><span style=\"font-size: medium;\"><b>Sabendo-se que a linha AC \u00e9 o prolongamento do raio incidente e que, d = 4 cm e BC = 1 cm, determine o valor de n.<\/b><\/span><\/span><\/p>\n<p>&nbsp;<\/p>\n<p><span style=\"color: #0000cc;\"><span style=\"font-family: Arial Black,serif;\"><span style=\"font-size: medium;\"><b>21-(ITA-SP)<\/b><\/span><\/span><\/span><\/p>\n<p><img loading=\"lazy\" decoding=\"async\" src=\"http:\/\/fisicaevestibular.com.br\/novo\/wp-content\/uploads\/migracao\/optica\/laminas\/i_120fb32649d00c80_html_9b28a9dd.jpg\" alt=\"\" width=\"302\" height=\"182\" name=\"Imagem 40\" align=\"LEFT\" border=\"0\" hspace=\"12\" \/><\/p>\n<p><span style=\"font-family: Arial,serif;\"><span style=\"font-size: medium;\"><b>Uma l\u00e2mina de faces paralelas de espessura 4\u221a3 cm \u00e9 constitu\u00edda de um material de \u00edndice de refra\u00e7\u00e3o \u221a3. Um raio luminoso, propagando-se no ar, encontra a l\u00e2mina, formando um \u00e2ngulo de 60<\/b><\/span><\/span><sup><span style=\"font-family: Arial,serif;\"><span style=\"font-size: medium;\"><b>o<\/b><\/span><\/span><\/sup><span style=\"font-family: Arial,serif;\"><span style=\"font-size: medium;\"><b>\u00a0com a normal. Determine o desvio sofrido pelo raio luminoso incidente.<\/b><\/span><\/span><\/p>\n<p><span style=\"color: #0000cc;\"><span style=\"font-family: Arial Black,serif;\"><span style=\"font-size: medium;\"><b>22-(CESGRANRIO-RJ)<\/b><\/span><\/span><\/span><\/p>\n<p><img loading=\"lazy\" decoding=\"async\" src=\"http:\/\/fisicaevestibular.com.br\/novo\/wp-content\/uploads\/migracao\/optica\/laminas\/i_120fb32649d00c80_html_15c3060f.jpg\" alt=\"\" width=\"244\" height=\"67\" name=\"Imagem 41\" align=\"BOTTOM\" border=\"0\" \/><\/p>\n<p><span style=\"font-family: Arial,serif;\"><span style=\"font-size: medium;\"><b>Um raio de luz monocrom\u00e1tica incide sobre a superf\u00edcie de uma l\u00e2mina delgada de vidro, com faces paralelas, fazendo com ela um \u00e2ngulo de 30\u00ba, como ilustra a figura. A l\u00e2mina est\u00e1 imersa no ar e sua espessura \u00e9\u00a0<img loading=\"lazy\" decoding=\"async\" src=\"http:\/\/fisicaevestibular.com.br\/novo\/wp-content\/uploads\/migracao\/optica\/laminas\/i_120fb32649d00c80_html_f14f35a5.gif\" alt=\"\" width=\"23\" height=\"20\" name=\"_tx_id_1_\" align=\"BOTTOM\" border=\"0\" \/>cm. <\/b><\/span><\/span><\/p>\n<p align=\"CENTER\"><img loading=\"lazy\" decoding=\"async\" src=\"http:\/\/fisicaevestibular.com.br\/novo\/wp-content\/uploads\/migracao\/optica\/laminas\/i_120fb32649d00c80_html_13d53fe5.jpg\" alt=\"\" width=\"414\" height=\"162\" name=\"Imagem 43\" align=\"BOTTOM\" border=\"0\" \/><\/p>\n<p><span style=\"font-family: Arial,serif;\"><span style=\"font-size: medium;\"><b>Sabendo-se que os \u00edndices de<\/b><\/span><\/span><\/p>\n<p><span style=\"font-family: Arial,serif;\"><span style=\"font-size: medium;\"><b>refra\u00e7\u00e3o desse vidro e do ar valem, respectivamente,\u00a0<img loading=\"lazy\" decoding=\"async\" src=\"http:\/\/fisicaevestibular.com.br\/novo\/wp-content\/uploads\/migracao\/optica\/laminas\/i_120fb32649d00c80_html_f14f35a5.gif\" alt=\"\" width=\"23\" height=\"20\" name=\"_tx_id_2_\" align=\"BOTTOM\" border=\"0\" \/>e 1, determine o desvio x, em mm, sofrido pelo raio ao sair da l\u00e2mina.<\/b><\/span><\/span><\/p>\n<p>&nbsp;<\/p>\n<p><span style=\"color: #0000cc;\"><span style=\"font-family: Arial Black,serif;\"><span style=\"font-size: medium;\"><b>23-(UDESC-SC)<\/b><\/span><\/span><\/span><\/p>\n<p><img loading=\"lazy\" decoding=\"async\" src=\"http:\/\/fisicaevestibular.com.br\/novo\/wp-content\/uploads\/migracao\/optica\/laminas\/i_120fb32649d00c80_html_fef552d6.jpg\" alt=\"\" width=\"151\" height=\"89\" name=\"Imagem 45\" align=\"BOTTOM\" border=\"0\" \/><\/p>\n<p><span style=\"font-family: Arial,serif;\"><span style=\"font-size: medium;\"><b>Considere uma l\u00e2mina de vidro de faces paralelas imersa no ar. Um raio luminoso propaga-se no ar e incide em uma das faces da l\u00e2mina, segundo um \u00e2ngulo\u00a0\u03b8\u00a0em rela\u00e7\u00e3o \u00e0 dire\u00e7\u00e3o normal ao plano da l\u00e2mina. O raio \u00e9 refratado nesta face e refletido na outra<\/b><\/span><\/span><img loading=\"lazy\" decoding=\"async\" src=\"http:\/\/fisicaevestibular.com.br\/novo\/wp-content\/uploads\/migracao\/optica\/laminas\/i_120fb32649d00c80_html_a4910e76.jpg\" alt=\"\" width=\"268\" height=\"218\" name=\"Imagem 47\" align=\"LEFT\" border=\"0\" hspace=\"12\" \/><\/p>\n<p><span style=\"font-family: Arial,serif;\"><span style=\"font-size: medium;\"><b>face, que \u00e9 espelhada. O raio refletido \u00e9 novamente refratado na face n\u00e3o espelhada, voltando a propagar-se no ar. Sendo n<\/b><\/span><\/span><sub><span style=\"font-family: Arial,serif;\"><span style=\"font-size: medium;\"><b>ar\u00a0<\/b><\/span><\/span><\/sub><span style=\"font-family: Arial,serif;\"><span style=\"font-size: medium;\"><b>e n<\/b><\/span><\/span><sub><span style=\"font-family: Arial,serif;\"><span style=\"font-size: medium;\"><b>vidro<\/b><\/span><\/span><\/sub><span style=\"font-family: Arial,serif;\"><span style=\"font-size: medium;\"><b>, respectivamente, os \u00edndices de refra\u00e7\u00e3o da luz no ar e no vidro, o \u00e2ngulo de refra\u00e7\u00e3o\u00a0\u03b1\u00a0que o raio refletido forma no vidro, com a dire\u00e7\u00e3o normal ao plano da l\u00e2mina, ao refratar-se pela segunda vez, obedece \u00e0 equa\u00e7\u00e3o:<\/b><\/span><\/span><\/p>\n<p><span style=\"font-family: Arial,serif;\"><span style=\"font-size: medium;\"><span lang=\"en-US\"><b>a)\u00a0n<\/b><\/span><\/span><\/span><sub><span style=\"font-family: Arial,serif;\"><span style=\"font-size: medium;\"><span lang=\"en-US\"><b>vidro.<\/b><\/span><\/span><\/span><\/sub><span style=\"font-family: Arial,serif;\"><span style=\"font-size: medium;\"><span lang=\"en-US\"><b>\u00a0sen<\/b><\/span><\/span><\/span><span style=\"font-family: Arial,serif;\"><span style=\"font-size: medium;\"><b> \u03b8<\/b><\/span><\/span><span style=\"font-family: Arial,serif;\"><span style=\"font-size: medium;\"><span lang=\"en-US\"><b> = n<\/b><\/span><\/span><\/span><sub><span style=\"font-family: Arial,serif;\"><span style=\"font-size: medium;\"><span lang=\"en-US\"><b>ar.<\/b><\/span><\/span><\/span><\/sub><span style=\"font-family: Arial,serif;\"><span style=\"font-size: medium;\"><span lang=\"en-US\"><b>\u00a0sen<\/b><\/span><\/span><\/span><span style=\"font-family: Arial,serif;\"><span style=\"font-size: medium;\"><b> \u03b8<\/b><\/span><\/span><span style=\"font-family: Arial,serif;\"><span style=\"font-size: medium;\"><span lang=\"en-US\"><b> \/2\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0<\/b><\/span><\/span><\/span><\/p>\n<p><span style=\"font-family: Arial,serif;\"><span style=\"font-size: medium;\"><span lang=\"en-US\"><b>b)\u00a0<\/b><\/span><\/span><\/span><span style=\"font-family: Arial,serif;\"><span style=\"font-size: medium;\"><b>\u03b1<\/b><\/span><\/span><span style=\"font-family: Arial,serif;\"><span style=\"font-size: medium;\"><span lang=\"en-US\"><b> =\u00a0<\/b><\/span><\/span><\/span><span style=\"font-family: Arial,serif;\"><span style=\"font-size: medium;\"><b>\u03b8\u00a0\u00a0<\/b><\/span><\/span><span style=\"font-family: Arial,serif;\"><span style=\"font-size: medium;\"><span lang=\"en-US\"><b>\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0<\/b><\/span><\/span><\/span><\/p>\n<p><span style=\"font-family: Arial,serif;\"><span style=\"font-size: medium;\"><span lang=\"en-US\"><b>c)\u00a0sen<\/b><\/span><\/span><\/span><span style=\"font-family: Arial,serif;\"><span style=\"font-size: medium;\"><b> \u03b1<\/b><\/span><\/span><span style=\"font-family: Arial,serif;\"><span style=\"font-size: medium;\"><span lang=\"en-US\"><b> = cos<\/b><\/span><\/span><\/span><span style=\"font-family: Arial,serif;\"><span style=\"font-size: medium;\"><b> \u03b8\u00a0\u00a0<\/b><\/span><\/span><span style=\"font-family: Arial,serif;\"><span style=\"font-size: medium;\"><span lang=\"en-US\"><b>\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0<\/b><\/span><\/span><\/span><\/p>\n<p><span style=\"font-family: Arial,serif;\"><span style=\"font-size: medium;\"><span lang=\"en-US\"><b>d)\u00a0n<\/b><\/span><\/span><\/span><sub><span style=\"font-family: Arial,serif;\"><span style=\"font-size: medium;\"><span lang=\"en-US\"><b>vidro.<\/b><\/span><\/span><\/span><\/sub><span style=\"font-family: Arial,serif;\"><span style=\"font-size: medium;\"><span lang=\"en-US\"><b>\u00a0sen<\/b><\/span><\/span><\/span><span style=\"font-family: Arial,serif;\"><span style=\"font-size: medium;\"><b> \u03b1<\/b><\/span><\/span><span style=\"font-family: Arial,serif;\"><span style=\"font-size: medium;\"><span lang=\"en-US\"><b> = n<\/b><\/span><\/span><\/span><sub><span style=\"font-family: Arial,serif;\"><span style=\"font-size: medium;\"><span lang=\"en-US\"><b>ar.<\/b><\/span><\/span><\/span><\/sub><span style=\"font-family: Arial,serif;\"><span style=\"font-size: medium;\"><span lang=\"en-US\"><b>sen<\/b><\/span><\/span><\/span><span style=\"font-family: Arial,serif;\"><span style=\"font-size: medium;\"><b> \u03b8\u00a0\u00a0<\/b><\/span><\/span><span style=\"font-family: Arial,serif;\"><span style=\"font-size: medium;\"><span lang=\"en-US\"><b>\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0<\/b><\/span><\/span><\/span><\/p>\n<p><span style=\"font-family: Arial,serif;\"><span style=\"font-size: medium;\"><span lang=\"en-US\"><b>e)\u00a0n<\/b><\/span><\/span><\/span><sub><span style=\"font-family: Arial,serif;\"><span style=\"font-size: medium;\"><span lang=\"en-US\"><b>ar.<\/b><\/span><\/span><\/span><\/sub><span style=\"font-family: Arial,serif;\"><span style=\"font-size: medium;\"><span lang=\"en-US\"><b>\u00a0sen<\/b><\/span><\/span><\/span><span style=\"font-family: Arial,serif;\"><span style=\"font-size: medium;\"><b> \u03b1<\/b><\/span><\/span><span style=\"font-family: Arial,serif;\"><span style=\"font-size: medium;\"><span lang=\"en-US\"><b> = n<\/b><\/span><\/span><\/span><sub><span style=\"font-family: Arial,serif;\"><span style=\"font-size: medium;\"><span lang=\"en-US\"><b>vidro.<\/b><\/span><\/span><\/span><\/sub><span style=\"font-family: Arial,serif;\"><span style=\"font-size: medium;\"><span lang=\"en-US\"><b>\u00a0sen<\/b><\/span><\/span><\/span><span style=\"font-family: Arial,serif;\"><span style=\"font-size: medium;\"><b> \u03b8\u00a0\u00a0<\/b><\/span><\/span><\/p>\n<p>&nbsp;<\/p>\n<p><span style=\"color: #0000cc;\"><span style=\"font-family: Arial Black,serif;\"><span style=\"font-size: medium;\"><b>24-(UEMG-MG)<\/b><\/span><\/span><\/span><\/p>\n<p><img loading=\"lazy\" decoding=\"async\" src=\"http:\/\/fisicaevestibular.com.br\/novo\/wp-content\/uploads\/migracao\/optica\/laminas\/i_120fb32649d00c80_html_67fc1ad1.jpg\" alt=\"\" width=\"588\" height=\"139\" name=\"Imagem 59\" align=\"BOTTOM\" border=\"0\" \/><\/p>\n<p><span style=\"font-family: Arial,serif;\"><span style=\"font-size: medium;\"><b>Refra\u00e7\u00e3o \u00e9 o nome dado ao fen\u00f4meno em que uma onda que se propaga num meio passa a se propagar em outro meio. Considere que voc\u00ea veja, por uma janela de vidro, uma \u00e1rvore. At\u00e9 atingir os seus olhos, a luz proveniente da \u00e1rvore veio pelo ar, passou a se propagar no vidro e, finalmente, passou do vidro para o ar novamente, at\u00e9 atingir os seus olhos.<\/b><\/span><\/span><img loading=\"lazy\" decoding=\"async\" src=\"http:\/\/fisicaevestibular.com.br\/novo\/wp-content\/uploads\/migracao\/optica\/laminas\/i_120fb32649d00c80_html_9a0cd63c.jpg\" alt=\"\" width=\"342\" height=\"247\" name=\"Imagem 60\" align=\"LEFT\" border=\"0\" hspace=\"12\" \/><\/p>\n<p><span style=\"font-family: Arial,serif;\"><span style=\"font-size: medium;\"><b>Ao sofrer essas duas refra\u00e7\u00f5es &#8211; do ar para o vidro e do vidro para o ar -, respectivamente, assinale a alternativa que apresenta CORRETAMENTE as altera\u00e7\u00f5es que ocorrem com a luz.<\/b><\/span><\/span><\/p>\n<p><span style=\"font-family: Arial,serif;\"><span style=\"font-size: medium;\"><b>A) Sua frequ\u00eancia aumenta, ao passar do ar para o vidro, e diminui, ao passar do vidro para o ar.<\/b><\/span><\/span><\/p>\n<p><span style=\"font-family: Arial,serif;\"><span style=\"font-size: medium;\"><b>B) Sua frequ\u00eancia diminui, ao passar do ar para o vidro, e aumenta, ao passar do vidro para o ar.<\/b><\/span><\/span><\/p>\n<p><span style=\"font-family: Arial,serif;\"><span style=\"font-size: medium;\"><b>C) Sua\u00a0velocidade aumenta, ao passar do ar para o vidro, e diminui, ao passar do vidro para o ar.<\/b><\/span><\/span><\/p>\n<p><span style=\"font-family: Arial,serif;\"><span style=\"font-size: medium;\"><b>D) Sua velocidade diminui, ao passar do ar para o vidro, e aumenta, ao passar do vidro para o ar.<\/b><\/span><\/span><\/p>\n<p><span style=\"color: #0000cc;\"><span style=\"font-family: Arial Black,serif;\"><span style=\"font-size: medium;\"><b>25-(PUC-RJ)<\/b><\/span><\/span><\/span><\/p>\n<p><img loading=\"lazy\" decoding=\"async\" src=\"http:\/\/fisicaevestibular.com.br\/novo\/wp-content\/uploads\/migracao\/optica\/laminas\/i_120fb32649d00c80_html_d910b28c.jpg\" alt=\"\" width=\"537\" height=\"139\" name=\"Imagem 61\" align=\"BOTTOM\" border=\"0\" \/><\/p>\n<p><span style=\"font-family: Arial,serif;\"><span style=\"font-size: medium;\"><b>Um feixe luminoso se propagando no ar incide em uma superf\u00edcie de vidro. Calcule o \u00e2ngulo que o feixe refratado faz com a normal \u00e0 superf\u00edcie sabendo que o \u00e2ngulo de incid\u00eancia \u03b8<\/b><\/span><\/span><sub><span style=\"font-family: Arial,serif;\"><span style=\"font-size: medium;\"><b>i<\/b><\/span><\/span><\/sub><span style=\"font-family: Arial,serif;\"><span style=\"font-size: medium;\"><b>\u00a0\u00e9 de 60\u00ba e que os \u00edndices de refra\u00e7\u00e3o do ar e do vidro, \u03b7<\/b><\/span><\/span><sub><span style=\"font-family: Arial,serif;\"><span style=\"font-size: medium;\"><b>ar\u00a0<\/b><\/span><\/span><\/sub><span style=\"font-family: Arial,serif;\"><span style=\"font-size: medium;\"><b>e \u03b7<\/b><\/span><\/span><sub><span style=\"font-family: Arial,serif;\"><span style=\"font-size: medium;\"><b>vidro<\/b><\/span><\/span><\/sub><span style=\"font-family: Arial,serif;\"><span style=\"font-size: medium;\"><b> vidro, s\u00e3o respectivamente 1,0 e \u221a3.<\/b><\/span><\/span><img loading=\"lazy\" decoding=\"async\" src=\"http:\/\/fisicaevestibular.com.br\/novo\/wp-content\/uploads\/migracao\/optica\/laminas\/i_120fb32649d00c80_html_a8610fc0.jpg\" alt=\"\" width=\"305\" height=\"177\" name=\"Imagem 62\" align=\"LEFT\" border=\"0\" hspace=\"12\" \/><\/p>\n<p><span style=\"font-family: Arial,serif;\"><span style=\"font-size: medium;\"><b>(A) 30\u00b0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0 <\/b><\/span><\/span><\/p>\n<p><span style=\"font-family: Arial,serif;\"><span style=\"font-size: medium;\"><b>(B) 45\u00b0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0 <\/b><\/span><\/span><\/p>\n<p><span style=\"font-family: Arial,serif;\"><span style=\"font-size: medium;\"><b>(C) 60\u00b0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0 <\/b><\/span><\/span><\/p>\n<p><span style=\"font-family: Arial,serif;\"><span style=\"font-size: medium;\"><b>(D) 73\u00b0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0 <\/b><\/span><\/span><\/p>\n<p><span style=\"font-family: Arial,serif;\"><span style=\"font-size: medium;\"><b>(E) 90\u00b0<\/b><\/span><\/span><\/p>\n<p>&nbsp;<\/p>\n<h3><a title=\"Resolu\u00e7\u00e3o comentada dos exerc\u00edcios de vestibulares sobre L\u00e2minas de faces paralelas\" href=\"http:\/\/fisicaevestibular.com.br\/novo\/optica\/optica-geometrica\/laminas-de-faces-paralelas\/resolucao-comentada-dos-exercicios-de-vestibulares-sobre-laminas-de-faces-paralelas\/\"><span style=\"color: #000080;\">Confira as resolu\u00e7\u00f5es comentadas e gabarito<\/span><\/a><\/h3>\n","protected":false},"excerpt":{"rendered":"<p>Exerc\u00edcios de vestibulares com resolu\u00e7\u00f5es comentadas sobre L\u00e2minas de faces paralelas 01- (MACKENZIE-SP) Sabe-se que uma onda eletromagn\u00e9tica, que se propaga em um meio homog\u00eaneo, transparente e is\u00f3tropo, ao incidir sobre a superf\u00edcie de outro meio, tamb\u00e9m transparente, homog\u00eaneo e is\u00f3tropo, continua a se propagar nele, por\u00e9m, com algumas altera\u00e7\u00f5es. Se o segundo meio citado for um corpo com a<\/p>\n","protected":false},"author":1,"featured_media":0,"parent":2217,"menu_order":0,"comment_status":"closed","ping_status":"closed","template":"","meta":{"om_disable_all_campaigns":false,"_monsterinsights_skip_tracking":false,"_monsterinsights_sitenote_active":false,"_monsterinsights_sitenote_note":"","_monsterinsights_sitenote_category":0,"footnotes":""},"class_list":["post-2219","page","type-page","status-publish","hentry"],"aioseo_notices":[],"_links":{"self":[{"href":"https:\/\/fisicaevestibular.com.br\/novo\/wp-json\/wp\/v2\/pages\/2219","targetHints":{"allow":["GET"]}}],"collection":[{"href":"https:\/\/fisicaevestibular.com.br\/novo\/wp-json\/wp\/v2\/pages"}],"about":[{"href":"https:\/\/fisicaevestibular.com.br\/novo\/wp-json\/wp\/v2\/types\/page"}],"author":[{"embeddable":true,"href":"https:\/\/fisicaevestibular.com.br\/novo\/wp-json\/wp\/v2\/users\/1"}],"replies":[{"embeddable":true,"href":"https:\/\/fisicaevestibular.com.br\/novo\/wp-json\/wp\/v2\/comments?post=2219"}],"version-history":[{"count":4,"href":"https:\/\/fisicaevestibular.com.br\/novo\/wp-json\/wp\/v2\/pages\/2219\/revisions"}],"predecessor-version":[{"id":10944,"href":"https:\/\/fisicaevestibular.com.br\/novo\/wp-json\/wp\/v2\/pages\/2219\/revisions\/10944"}],"up":[{"embeddable":true,"href":"https:\/\/fisicaevestibular.com.br\/novo\/wp-json\/wp\/v2\/pages\/2217"}],"wp:attachment":[{"href":"https:\/\/fisicaevestibular.com.br\/novo\/wp-json\/wp\/v2\/media?parent=2219"}],"curies":[{"name":"wp","href":"https:\/\/api.w.org\/{rel}","templated":true}]}}