{"id":2175,"date":"2016-05-02T03:47:38","date_gmt":"2016-05-02T03:47:38","guid":{"rendered":"http:\/\/fisicaevestibular.com.br\/novo\/?page_id=2175"},"modified":"2024-09-02T14:02:16","modified_gmt":"2024-09-02T14:02:16","slug":"resolucao-comentada-dos-exercicios-de-vestibulares-sobre-espelhos-esfericos-construcao-geometrica-de-imagens","status":"publish","type":"page","link":"https:\/\/fisicaevestibular.com.br\/novo\/optica\/optica-geometrica\/espelhos-esfericos-construcao-geometrica-de-imagens\/resolucao-comentada-dos-exercicios-de-vestibulares-sobre-espelhos-esfericos-construcao-geometrica-de-imagens\/","title":{"rendered":"Espelhos esf\u00e9ricos \u2013 Constru\u00e7\u00e3o geom\u00e9trica de imagens &#8211; Resolu\u00e7\u00e3o"},"content":{"rendered":"<p align=\"CENTER\"><span style=\"color: #c00000;\"><span style=\"font-family: Arial Black,serif;\"><span style=\"font-size: large;\"><b>Resolu\u00e7\u00e3o comentada dos exerc\u00edcios de vestibulares 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>Espelhos esf\u00e9ricos \u2013 Constru\u00e7\u00e3o geom\u00e9trica de imagens<\/b><\/span><\/span><\/span><\/p>\n<p><span style=\"color: #c00000;\">\u00a0<span style=\"font-family: Arial Black,serif;\"><span style=\"font-size: medium;\"><b>01-<\/b><\/span><\/span><\/span><b> <\/b><span style=\"font-family: Arial,serif;\"><span style=\"font-size: medium;\"><b>Trata-se de um espelho convexo e nele a imagem \u00e9 sempre virtual, direita,\u00a0 menor que o objeto e est\u00e1 sempre atr\u00e1s do espelho e entre\u00a0 o v\u00e9rtice V e o foco F, para qualquer posi\u00e7\u00e3o do objeto<\/b><\/span><\/span><span style=\"font-family: Arial,serif;\"><span style=\"font-size: medium;\"><b>. R- D<\/b><\/span><\/span><\/p>\n<p><span style=\"color: #c00000;\"><span style=\"font-family: Arial Black,serif;\"><span style=\"font-size: medium;\"><b>02-<\/b><\/span><\/span><\/span><b> <\/b><span style=\"font-family: Arial,serif;\"><span style=\"font-size: medium;\"><b>R- A\u00a0 (veja esquema abaixo)<\/b><\/span><\/span><\/p>\n<p align=\"CENTER\"><img fetchpriority=\"high\" decoding=\"async\" src=\"http:\/\/fisicaevestibular.com.br\/novo\/wp-content\/uploads\/migracao\/optica\/espelhos-efericos\/i_5cc0b4c3c9fe01ca_html_590d35d3.jpg\" alt=\"\" width=\"533\" height=\"210\" name=\"Imagem 125\" align=\"BOTTOM\" border=\"0\" \/><\/p>\n<p><span style=\"color: #c00000;\"><span style=\"font-family: Arial Black,serif;\"><span style=\"font-size: medium;\"><b>03-<\/b><\/span><\/span><\/span><b> <\/b><span style=\"font-family: Arial,serif;\"><span style=\"font-size: medium;\"><b>R- C\u00a0 (veja figura abaixo)<\/b><\/span><\/span><\/p>\n<p align=\"CENTER\"><img decoding=\"async\" src=\"http:\/\/fisicaevestibular.com.br\/novo\/wp-content\/uploads\/migracao\/optica\/espelhos-efericos\/i_5cc0b4c3c9fe01ca_html_8e924f33.jpg\" alt=\"\" width=\"422\" height=\"200\" name=\"Imagem 126\" align=\"BOTTOM\" border=\"0\" \/><\/p>\n<p><span style=\"color: #c00000;\"><span style=\"font-family: Arial Black,serif;\"><span style=\"font-size: medium;\"><b>04-<\/b><\/span><\/span><\/span><b> <\/b><span style=\"font-family: Arial,serif;\"><span style=\"font-size: medium;\"><b>R- E\u00a0 (veja teoria)<\/b><\/span><\/span><\/p>\n<p><span style=\"color: #c00000;\"><span style=\"font-family: Arial Black,serif;\"><span style=\"font-size: medium;\"><b>05-<\/b><\/span><\/span><\/span><b> <\/b><span style=\"font-family: Arial,serif;\"><span style=\"font-size: medium;\"><b>R- A\u00a0 (veja esquema abaixo)<\/b><\/span><\/span><\/p>\n<p align=\"CENTER\"><img decoding=\"async\" src=\"http:\/\/fisicaevestibular.com.br\/novo\/wp-content\/uploads\/migracao\/optica\/espelhos-efericos\/i_5cc0b4c3c9fe01ca_html_ea02208c.jpg\" alt=\"\" width=\"611\" height=\"166\" name=\"Imagem 129\" align=\"BOTTOM\" border=\"0\" \/><\/p>\n<p><span style=\"color: #c00000;\"><span style=\"font-family: Arial Black,serif;\"><span style=\"font-size: medium;\"><b>06-<\/b><\/span><\/span><\/span><b> <\/b><span style=\"font-family: Arial,serif;\"><span style=\"font-size: medium;\"><b>R- B<\/b><\/span><\/span><\/p>\n<p><span style=\"font-family: Arial,serif;\"><span style=\"font-size: medium;\"><b>Todo raio de luz que incide no espelho c\u00f4ncavo passando pelo foco (ou sendo emitido nele) atinge o espelho e retorna paralelamente ao eixo principal.<\/b><\/span><\/span><\/p>\n<p align=\"CENTER\"><img loading=\"lazy\" decoding=\"async\" src=\"http:\/\/fisicaevestibular.com.br\/novo\/wp-content\/uploads\/migracao\/optica\/espelhos-efericos\/i_5cc0b4c3c9fe01ca_html_e6f04a5b.jpg\" alt=\"\" width=\"411\" height=\"183\" name=\"Imagem 131\" align=\"BOTTOM\" border=\"0\" \/><\/p>\n<p><span style=\"color: #c00000;\"><span style=\"font-family: Arial Black,serif;\"><span style=\"font-size: medium;\"><b>07-<\/b><\/span><\/span><\/span><\/p>\n<p align=\"CENTER\"><img loading=\"lazy\" decoding=\"async\" src=\"http:\/\/fisicaevestibular.com.br\/novo\/wp-content\/uploads\/migracao\/optica\/espelhos-efericos\/i_5cc0b4c3c9fe01ca_html_60eb5327.jpg\" alt=\"\" width=\"469\" height=\"206\" name=\"Imagem 136\" align=\"BOTTOM\" border=\"0\" \/><\/p>\n<p><span style=\"color: #c00000;\"><span style=\"font-family: Arial Black,serif;\"><span style=\"font-size: medium;\"><b>08-<\/b><\/span><\/span><\/span><b> <\/b><span style=\"font-family: Arial,serif;\"><span style=\"font-size: medium;\"><b>O objeto (l\u00e2mpada) est\u00e1 sob a caixa e sobre o foco do espelho e nessas condi\u00e7\u00f5es a imagem ser\u00e1 real, do mesmo tamanho que o objeto e estar\u00e1 sobre ele.Objeto e imagem s\u00e3o id\u00eanticos e ter\u00e3o o mesmo brilho (mesma pot\u00eancia de 40W).\u00a0<\/b><\/span><\/span><span style=\"font-family: Arial,serif;\"><span style=\"font-size: medium;\"><b>R- A<\/b><\/span><\/span><\/p>\n<p><span style=\"color: #c00000;\"><span style=\"font-family: Arial Black,serif;\"><span style=\"font-size: medium;\"><b>09-<\/b><\/span><\/span><\/span><b> <\/b><span style=\"font-family: Arial,serif;\"><span style=\"font-size: medium;\"><b>Em todo espelho esf\u00e9rico convexo a imagem est\u00e1 atr\u00e1s do espelho e entre C (O) e F e a \u00fanica alternativa que satisfaz \u00e9 a\u00a0<\/b><\/span><\/span><span style=\"font-family: Arial,serif;\"><span style=\"font-size: medium;\"><b>B<\/b><\/span><\/span><span style=\"font-family: Arial,serif;\"><span style=\"font-size: medium;\"><b>.<\/b><\/span><\/span><\/p>\n<p><span style=\"color: #c00000;\"><span style=\"font-family: Arial Black,serif;\"><span style=\"font-size: medium;\"><b>10-<\/b><\/span><\/span><\/span><\/p>\n<p align=\"CENTER\"><img loading=\"lazy\" decoding=\"async\" src=\"http:\/\/fisicaevestibular.com.br\/novo\/wp-content\/uploads\/migracao\/optica\/espelhos-efericos\/i_5cc0b4c3c9fe01ca_html_7e8001e.jpg\" alt=\"\" width=\"591\" height=\"229\" name=\"Imagem 138\" align=\"BOTTOM\" border=\"0\" \/><\/p>\n<p><span style=\"color: #c00000;\"><span style=\"font-family: Arial Black,serif;\"><span style=\"font-size: medium;\"><b>11-<\/b><\/span><\/span><\/span><b> <\/b><span style=\"font-family: Arial,serif;\"><span style=\"font-size: medium;\"><b>a) Convexo. A imagem \u00e9 direita e menor<\/b><\/span><\/span><\/p>\n<p>&nbsp;<\/p>\n<p><span style=\"font-family: Arial,serif;\"><span style=\"font-size: medium;\"><b>b) e c)<\/b><\/span><\/span><\/p>\n<p align=\"CENTER\"><img loading=\"lazy\" decoding=\"async\" src=\"http:\/\/fisicaevestibular.com.br\/novo\/wp-content\/uploads\/migracao\/optica\/espelhos-efericos\/i_5cc0b4c3c9fe01ca_html_3d797d30.jpg\" alt=\"\" width=\"524\" height=\"198\" name=\"Imagem 139\" align=\"BOTTOM\" border=\"0\" \/><\/p>\n<p><span style=\"color: #c00000;\"><span style=\"font-family: Arial Black,serif;\"><span style=\"font-size: medium;\"><b>12-<\/b><\/span><\/span><\/span><b> <\/b><span style=\"font-family: Arial,serif;\"><span style=\"font-size: medium;\"><b>R- 17cm\u00a0 (veja figura abaixo)<\/b><\/span><\/span><\/p>\n<p align=\"CENTER\"><img loading=\"lazy\" decoding=\"async\" src=\"http:\/\/fisicaevestibular.com.br\/novo\/wp-content\/uploads\/migracao\/optica\/espelhos-efericos\/i_5cc0b4c3c9fe01ca_html_ece9f4a.jpg\" alt=\"\" width=\"501\" height=\"221\" name=\"Imagem 140\" align=\"BOTTOM\" border=\"0\" \/><\/p>\n<p>&nbsp;<\/p>\n<p><span style=\"color: #c00000;\"><span style=\"font-family: Arial Black,serif;\"><span style=\"font-size: medium;\"><b>13-<\/b><\/span><\/span><\/span><b> <\/b><span style=\"font-family: Arial,serif;\"><span style=\"font-size: medium;\"><b>Observe na figura abaixo que P\u2019 est\u00e1 exatamente abaixo de P e com o mesmo tamanho (sob e sobre C) e usando os dois raios not\u00e1veis foi localizado Q\u2019.\u00a0 R- D<\/b><\/span><\/span><\/p>\n<p align=\"CENTER\"><img loading=\"lazy\" decoding=\"async\" src=\"http:\/\/fisicaevestibular.com.br\/novo\/wp-content\/uploads\/migracao\/optica\/espelhos-efericos\/i_5cc0b4c3c9fe01ca_html_e01af7b8.jpg\" alt=\"\" width=\"553\" height=\"211\" name=\"Imagem 141\" align=\"BOTTOM\" border=\"0\" \/><\/p>\n<p><span style=\"color: #c00000;\"><span style=\"font-family: Arial Black,serif;\"><span style=\"font-size: medium;\"><b>14-<\/b><\/span><\/span><\/span><b> <\/b><span style=\"font-family: Arial,serif;\"><span style=\"font-size: medium;\"><b>a)<\/b><\/span><\/span><\/p>\n<p align=\"CENTER\"><img loading=\"lazy\" decoding=\"async\" src=\"http:\/\/fisicaevestibular.com.br\/novo\/wp-content\/uploads\/migracao\/optica\/espelhos-efericos\/i_5cc0b4c3c9fe01ca_html_c18da961.jpg\" alt=\"\" width=\"446\" height=\"241\" name=\"Imagem 142\" align=\"BOTTOM\" border=\"0\" \/><\/p>\n<p><span style=\"font-family: Arial,serif;\"><span style=\"font-size: medium;\"><b>b) real<\/b><\/span><\/span><\/p>\n<p><span style=\"color: #c00000;\"><span style=\"font-family: Arial Black,serif;\"><span style=\"font-size: medium;\"><b>15-<\/b><\/span><\/span><\/span><b> <\/b><span style=\"font-family: Arial,serif;\"><span style=\"font-size: medium;\"><b>Basta achar R\u2019 sim\u00e9trico a R e unir P a R\u2019. Onde esta reta cruzar o eixo principal, est\u00e1 o espelho\u00a0<\/b><\/span><\/span><span style=\"font-family: Arial,serif;\"><span style=\"font-size: medium;\"><b>R- D<\/b><\/span><\/span><\/p>\n<p align=\"CENTER\"><img loading=\"lazy\" decoding=\"async\" src=\"http:\/\/fisicaevestibular.com.br\/novo\/wp-content\/uploads\/migracao\/optica\/espelhos-efericos\/i_5cc0b4c3c9fe01ca_html_12d68378.jpg\" alt=\"\" width=\"499\" height=\"223\" name=\"Imagem 143\" align=\"BOTTOM\" border=\"0\" \/><\/p>\n<p>&nbsp;<\/p>\n<p><span style=\"color: #c00000;\"><span style=\"font-family: Arial Black,serif;\"><span style=\"font-size: medium;\"><b>16-<\/b><\/span><\/span><\/span><b> <\/b><span style=\"font-family: Arial,serif;\"><span style=\"font-size: medium;\"><b>O espelho deve ser c\u00f4ncavo e o rosto deve estar entre o foco e o espelho, ou seja, a dist\u00e2ncia focal deve ser superior a 15cm\u00a0<\/b><\/span><\/span><span style=\"font-family: Arial,serif;\"><span style=\"font-size: medium;\"><b>\u2013 R- E<\/b><\/span><\/span><\/p>\n<p><span style=\"color: #c00000;\"><span style=\"font-family: Arial Black,serif;\"><span style=\"font-size: medium;\"><b>17-<\/b><\/span><\/span><\/span><span style=\"color: #c00000;\"><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>R- A<\/b><\/span><\/span><span style=\"font-family: Arial,serif;\"><span style=\"font-size: medium;\"><b>\u00a0 (veja teoria)<\/b><\/span><\/span><\/p>\n<p><span style=\"color: #c00000;\"><span style=\"font-family: Arial Black,serif;\"><span style=\"font-size: medium;\"><b>18-<\/b><\/span><\/span><\/span><b> <\/b><span style=\"font-family: Arial,serif;\"><span style=\"font-size: medium;\"><b>R:<\/b><\/span><\/span><\/p>\n<p align=\"CENTER\"><img loading=\"lazy\" decoding=\"async\" src=\"http:\/\/fisicaevestibular.com.br\/novo\/wp-content\/uploads\/migracao\/optica\/espelhos-efericos\/i_5cc0b4c3c9fe01ca_html_87402ec1.jpg\" alt=\"\" width=\"488\" height=\"220\" name=\"Imagem 144\" align=\"BOTTOM\" border=\"0\" \/><\/p>\n<p><span style=\"color: #c00000;\"><span style=\"font-family: Arial Black,serif;\"><span style=\"font-size: medium;\"><b>19-<\/b><\/span><\/span><\/span><b> <\/b><span style=\"font-family: Arial,serif;\"><span style=\"font-size: medium;\"><b>S\u00f3 imagem virtual n\u00e3o\u00a0 pode ser projetada o que, nos espelhos c\u00f4ncavos, s\u00f3 acontece quando o objeto estiver a uma dist\u00e2ncia inferior \u00e0 distancia focal f (40cm) \u2013\u00a0<\/b><\/span><\/span><span style=\"font-family: Arial,serif;\"><span style=\"font-size: medium;\"><b>R- A<\/b><\/span><\/span><\/p>\n<p><span style=\"color: #c00000;\"><span style=\"font-family: Arial Black,serif;\"><span style=\"font-size: medium;\"><b>20-<\/b><\/span><\/span><\/span><b> <\/b><span style=\"font-family: Arial,serif;\"><span style=\"font-size: medium;\"><b>I e II s\u00e3o virtuais, pois as imagens s\u00e3o direitas e III \u00e9 real, pois qualquer imagem<\/b><\/span><\/span><span style=\"font-family: Arial,serif;\"><span style=\"font-size: medium;\"><b>projetada<\/b><\/span><\/span><span style=\"font-family: Arial,serif;\"><span style=\"font-size: medium;\"><b>\u00a0\u00e9 real\u00a0 &#8212;\u00a0\u00a0<\/b><\/span><\/span><span style=\"font-family: Arial,serif;\"><span style=\"font-size: medium;\"><b>R- B<\/b><\/span><\/span><\/p>\n<p><span style=\"color: #c00000;\"><span style=\"font-family: Arial Black,serif;\"><span style=\"font-size: medium;\"><b>21-<\/b><\/span><\/span><\/span><b> <\/b><span style=\"font-family: Arial,serif;\"><span style=\"font-size: medium;\"><b>R=2m\u00a0 &#8212;\u00a0 f=1m\u00a0 &#8212;\u00a0 o caminh\u00e3ozinho est\u00e1 entre o foco e o espelho c\u00f4ncavo (0,5m do espelho) e assim, a imagem \u00e9 virtual, direita e maior\u00a0 &#8212;\u00a0\u00a0<\/b><\/span><\/span><span style=\"font-family: Arial,serif;\"><span style=\"font-size: medium;\"><b>R- C<\/b><\/span><\/span><\/p>\n<p><span style=\"color: #c00000;\"><span style=\"font-family: Arial Black,serif;\"><span style=\"font-size: medium;\"><b>22-<\/b><\/span><\/span><\/span><span style=\"color: #c00000;\"><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>R- C<\/b><\/span><\/span><span style=\"font-family: Arial,serif;\"><span style=\"font-size: medium;\"><b>\u00a0 (veja teoria)<\/b><\/span><\/span><\/p>\n<p><span style=\"color: #c00000;\"><span style=\"font-family: Arial Black,serif;\"><span style=\"font-size: medium;\"><b>23-<\/b><\/span><\/span><\/span><b> <\/b><span style=\"font-family: Arial,serif;\"><span style=\"font-size: medium;\"><b>a) C\u00e1lculo da dist\u00e2ncia Terra-Lua\u00a0 &#8212;\u00a0 V=d<\/b><\/span><\/span><sub><span style=\"font-family: Arial,serif;\"><span style=\"font-size: medium;\"><b>L<\/b><\/span><\/span><\/sub><span style=\"font-family: Arial,serif;\"><span style=\"font-size: medium;\"><b>\u0394t\u00a0 &#8212;\u00a0 3.10<\/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>=d<\/b><\/span><\/span><sub><span style=\"font-family: Arial,serif;\"><span style=\"font-size: medium;\"><b>L<\/b><\/span><\/span><\/sub><span style=\"font-family: Arial,serif;\"><span style=\"font-size: medium;\"><b>\/1,3\u00a0 &#8212;\u00a0 d<\/b><\/span><\/span><sub><span style=\"font-family: Arial,serif;\"><span style=\"font-size: medium;\"><b>L<\/b><\/span><\/span><\/sub><span style=\"font-family: Arial,serif;\"><span style=\"font-size: medium;\"><b>=3,9.10<\/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\u00a0 &#8212;\u00a0 no tri\u00e2ngulo da figura 1\u00a0 &#8212;\u00a0 cos\u03b1=cateto adjacente\/hipotenusa\u00a0 &#8212;\u00a0 2,6.10<\/b><\/span><\/span><sup><span style=\"font-family: Arial,serif;\"><span style=\"font-size: medium;\"><b>-3<\/b><\/span><\/span><\/sup><span style=\"font-family: Arial,serif;\"><span style=\"font-size: medium;\"><b>=3,9.10<\/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>\/d<\/b><\/span><\/span><sub><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>\u00a0\u00a0<\/b><\/span><\/span><span style=\"font-family: Arial,serif;\"><span style=\"font-size: medium;\"><b>&#8212;\u00a0 d<\/b><\/span><\/span><sub><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>=1,5.10<\/b><\/span><\/span><sup><span style=\"font-family: Arial,serif;\"><span style=\"font-size: medium;\"><b>11<\/b><\/span><\/span><\/sup><span style=\"font-family: Arial,serif;\"><span style=\"font-size: medium;\"><b>m<\/b><\/span><\/span><\/p>\n<p><span style=\"font-family: Arial,serif;\"><span style=\"font-size: medium;\"><b>b) Observe a figura a seguir.<\/b><\/span><\/span><\/p>\n<p align=\"CENTER\"><img loading=\"lazy\" decoding=\"async\" src=\"http:\/\/fisicaevestibular.com.br\/novo\/wp-content\/uploads\/migracao\/optica\/espelhos-efericos\/i_5cc0b4c3c9fe01ca_html_c7661637.jpg\" alt=\"\" width=\"425\" height=\"209\" name=\"Imagem 145\" align=\"BOTTOM\" border=\"0\" \/><\/p>\n<p>&nbsp;<\/p>\n<p><span style=\"color: #c00000;\"><span style=\"font-family: Arial Black,serif;\"><span style=\"font-size: medium;\"><b>24-<\/b><\/span><\/span><\/span><b> <\/b><span style=\"font-family: Arial,serif;\"><span style=\"font-size: medium;\"><b>Quanto mais pr\u00f3ximo do foco maior ser\u00e1 a concentra\u00e7\u00e3o de raios luminosos e maior ser\u00e1 o aquecimento. Maior temperatura P<\/b><\/span><\/span><sub><span style=\"font-family: Arial,serif;\"><span style=\"font-size: medium;\"><b>4<\/b><\/span><\/span><\/sub><span style=\"font-family: Arial,serif;\"><span style=\"font-size: medium;\"><b>\u00a0(no foco). P<\/b><\/span><\/span><sub><span style=\"font-family: Arial,serif;\"><span style=\"font-size: medium;\"><b>5<\/b><\/span><\/span><\/sub><span style=\"font-family: Arial,serif;\"><span style=\"font-size: medium;\"><b>\u00a0e P<\/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>\u00a0est\u00e3o eq\u00fcidistantes e ter\u00e3o mesma temperatura e a menor temperatura \u00e9 P<\/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>\u00a0(mais afastada do foco).\u00a0 &#8212;\u00a0\u00a0<\/b><\/span><\/span><span style=\"font-family: Arial,serif;\"><span style=\"font-size: medium;\"><b>R &#8211; B<\/b><\/span><\/span><\/p>\n<p><span style=\"color: #c00000;\"><span style=\"font-family: Arial Black,serif;\"><span style=\"font-size: medium;\"><b>25-<\/b><\/span><\/span><\/span><b> <\/b><span style=\"font-family: Arial,serif;\"><span style=\"font-size: medium;\"><b>Para que os raios retornem paralelos a l\u00e2mpada L deve estar no foco de E\u2019 (todo raio de luz que incide passando pelo foco retorna paralelamente ao eixo principal) e no centro de curvatura de E\u2019\u2019 ( todo raio de luz que incide passando pelo centro de curvatura\u00a0 retorna sobre ele mesmo).<\/b><\/span><\/span><\/p>\n<p align=\"CENTER\"><img loading=\"lazy\" decoding=\"async\" src=\"http:\/\/fisicaevestibular.com.br\/novo\/wp-content\/uploads\/migracao\/optica\/espelhos-efericos\/i_5cc0b4c3c9fe01ca_html_88d68bfc.jpg\" alt=\"\" width=\"433\" height=\"265\" name=\"Imagem 146\" align=\"BOTTOM\" border=\"0\" \/><\/p>\n<p>\u00a0<span style=\"font-family: Arial,serif;\"><span style=\"font-size: medium;\"><b>Assim, todo raio de luz que emerge \u00e0 esquerda de L e incide sobre E\u2019\u2019 retorna sobre si mesmo, passa pelo foco de E\u2019 e retorna novamente de forma paralela.\u00a0<\/b><\/span><\/span><span style=\"font-family: Arial,serif;\"><span style=\"font-size: medium;\"><b>R- E<\/b><\/span><\/span><\/p>\n<p><span style=\"color: #c00000;\"><span style=\"font-family: Arial Black,serif;\"><span style=\"font-size: medium;\"><b>26-<\/b><\/span><\/span><\/span><b> <\/b><span style=\"font-family: Arial,serif;\"><span style=\"font-size: medium;\"><b>Se a imagem\u00a0 do cartaz est\u00e1 \u201cdentro\u201d do espelho, o objeto est\u00e1 entre o foco e o espelho e, nesse caso, a imagem \u00e9 virtual, direita, maior que o objeto e revertida (troca direita pela esquerda)\u00a0<\/b><\/span><\/span><span style=\"font-family: Arial,serif;\"><span style=\"font-size: medium;\"><b>R- D<\/b><\/span><\/span><\/p>\n<p><span style=\"color: #c00000;\"><span style=\"font-family: Arial Black,serif;\"><span style=\"font-size: medium;\"><b>26a)<\/b><\/span><\/span><\/span><b> <\/b><span style=\"font-family: Arial,serif;\"><span style=\"font-size: medium;\"><b>Em um espelho c\u00f4ncavo, com dist\u00e2ncia focal de 10 cm, se o objeto est\u00e1 a 20 cm, ou seja, no dobro da dist\u00e2ncia focal, ele est\u00e1 no ponto antiprincipal objeto do espelho\u00a0 &#8212;\u00a0 neste ponto a imagem \u00e9 real, invertida e possui o mesmo tamanho do objeto\u00a0 &#8212;\u00a0 veja<\/b><\/span><\/span><\/p>\n<p align=\"CENTER\"><img loading=\"lazy\" decoding=\"async\" src=\"http:\/\/fisicaevestibular.com.br\/novo\/wp-content\/uploads\/migracao\/optica\/espelhos-efericos\/i_5cc0b4c3c9fe01ca_html_849739b8.jpg\" alt=\"\" width=\"399\" height=\"209\" name=\"Imagem 147\" align=\"BOTTOM\" border=\"0\" \/><\/p>\n<p><span style=\"font-family: Arial,serif;\"><span style=\"font-size: medium;\"><b>constru\u00e7\u00e3o gr\u00e1fica\u00a0 &#8212;\u00a0 \u00e9 poss\u00edvel tamb\u00e9m analisar esta quest\u00e3o pela equa\u00e7\u00e3o dos pontos conjugados de Gauss, ou seja, 1\/f=1\/P + 1\/P\u2019\u00a0 &#8212;\u00a0 1\/10=1\/20 + 1\/P\u2019\u00a0 &#8212;\u00a0 P\u2019=20cm\u00a0 &#8212;\u00a0 como p\u2019 \u00e9 positivo isto implica que a imagem \u00e9 real\u00a0 &#8212;\u00a0 \u00a0imagem real conjugada por um \u00fanico espelho a partir de um objeto real s\u00f3 pode ser invertida\u00a0 &#8212;\u00a0<\/b><\/span><\/span><span style=\"font-family: Arial,serif;\"><span style=\"font-size: medium;\"><b>\u00a0R- B<\/b><\/span><\/span><span style=\"font-family: Arial,serif;\"><span style=\"font-size: medium;\"><b>\u00a0<\/b><\/span><\/span><\/p>\n<p><span style=\"color: #c00000;\"><span style=\"font-family: Arial Black,serif;\"><span style=\"font-size: medium;\"><b>27-<\/b><\/span><\/span><\/span><span style=\"color: #c00000;\"><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>Os raios solares que atingem a Terra s\u00e3o praticamente paralelos devido \u00e0 grande dist\u00e2ncia entre o Sol e a Terra\u00a0 &#8212;\u00a0 de acordo com o enunciado, esses raios solares s\u00e3o verticais, atingindo o espelho paralelamente ao eixo principal\u00a0 &#8212;\u00a0 como o espelho \u00e9 gaussiano, os raios refletidos passam pelo foco principal, que fica \u00e0 dist\u00e2ncia R\/2 do v\u00e9rtice do espelho\u00a0 &#8212;\u00a0<\/b><\/span><\/span><span style=\"font-family: Arial,serif;\"><span style=\"font-size: medium;\"><b>\u00a0R- A<\/b><\/span><\/span><\/p>\n<p><span style=\"color: #c00000;\"><span style=\"font-family: Arial Black,serif;\"><span style=\"font-size: medium;\"><b>28-<\/b><\/span><\/span><\/span><span style=\"color: #c00000;\"><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>Observe na figura fornecida, que a imagem do objeto real est\u00e1 invertida e ampliada\u00a0 &#8212;\u00a0 esse caso s\u00f3 acontece para um espelho esf\u00e9rico c\u00f4ncavo, quando o objeto est\u00e1 entre o centro de curvatura (C) e o foco (F) , como mostra a constru\u00e7\u00e3o geom\u00e9trica da imagem abaixo:<\/b><\/span><\/span><\/p>\n<p align=\"CENTER\"><img loading=\"lazy\" decoding=\"async\" src=\"http:\/\/fisicaevestibular.com.br\/novo\/wp-content\/uploads\/migracao\/optica\/espelhos-efericos\/i_5cc0b4c3c9fe01ca_html_a47ced7d.jpg\" alt=\"\" width=\"530\" height=\"238\" name=\"Imagem 148\" align=\"BOTTOM\" border=\"0\" \/><\/p>\n<p><span style=\"font-family: Arial,serif;\"><span style=\"font-size: medium;\"><b>R- D \u00a0<\/b><\/span><\/span><\/p>\n<p><span style=\"color: #c00000;\"><span style=\"font-family: Arial Black,serif;\"><span style=\"font-size: medium;\"><b>29-<\/b><\/span><\/span><\/span><span style=\"color: #c00000;\"><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>Nossos olhos est\u00e3o acostumados com imagens em espelhos planos, onde imagens de objetos mais distantes nos parecem cada vez menores\u00a0 &#8212;\u00a0 esse condicionamento \u00e9 levado para o espelho convexo\u00a0 &#8212;\u00a0 o fato de a imagem ser menor que o objeto \u00e9 interpretado pelo c\u00e9rebro como se o objeto estivesse mais distante do que realmente est\u00e1\u00a0 &#8212;\u00a0 essa falsa impress\u00e3o \u00e9 desfeita quando o motorista est\u00e1, por exemplo, dando marcha a r\u00e9 em uma garagem, vendo apenas a imagem dessa parede pelo espelho convexo\u00a0 &#8212;\u00a0 ele para o carro quando percebe pela imagem do espelho convexo que est\u00e1 quase batendo na parede\u00a0 &#8212;\u00a0 ao olhar para tr\u00e1s, por vis\u00e3o direta, ele percebe que n\u00e3o estava t\u00e3o pr\u00f3ximo assim da parede\u00a0 &#8212;\u00a0<\/b><\/span><\/span><span style=\"font-family: Arial,serif;\"><span style=\"font-size: medium;\"><b>\u00a0R- C\u00a0<\/b><\/span><\/span><span style=\"font-family: Arial,serif;\"><span style=\"font-size: medium;\"><b>\u00a0<\/b><\/span><\/span><\/p>\n<p><span style=\"color: #c00000;\"><span style=\"font-family: Arial Black,serif;\"><span style=\"font-size: medium;\"><b>30-<\/b><\/span><\/span><\/span><span style=\"color: #c00000;\"><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>Sabemos que num espelho esf\u00e9rico c\u00f4ncavo gaussiano a dist\u00e2ncia focal (f) \u00e9 metade do raio de <\/b><\/span><\/span><\/p>\n<p align=\"CENTER\"><img loading=\"lazy\" decoding=\"async\" src=\"http:\/\/fisicaevestibular.com.br\/novo\/wp-content\/uploads\/migracao\/optica\/espelhos-efericos\/i_5cc0b4c3c9fe01ca_html_3487bdea.jpg\" alt=\"\" width=\"435\" height=\"212\" name=\"Imagem 149\" align=\"BOTTOM\" border=\"0\" \/><\/p>\n<p><span style=\"font-family: Arial,serif;\"><span style=\"font-size: medium;\"><b>curvatura (R), que, por sua vez,\u00e9 metade do di\u00e2metro (d)\u00a0 &#8212;\u00a0 f=R\/2=(d\/2)\/2\u00a0 &#8212;\u00a0 f=d\/4\u00a0 &#8212;\u00a0 d=4f\u00a0 &#8212;\u00a0<\/b><\/span><\/span><span style=\"font-family: Arial,serif;\"><span style=\"font-size: medium;\"><b>\u00a0R- D<\/b><\/span><\/span><\/p>\n<p><span style=\"color: #c00000;\"><span style=\"font-family: Arial Black,serif;\"><span style=\"font-size: medium;\"><b>31-<\/b><\/span><\/span><\/span><b> <\/b><span style=\"font-family: Arial,serif;\"><span style=\"font-size: medium;\"><b>a) Para o pequeno espelho, o objeto em F \u00e9 virtual porque \u00e9 obtido no prolongamento dos raios luminosos.<\/b><\/span><\/span><\/p>\n<p><span style=\"font-family: Arial,serif;\"><span style=\"font-size: medium;\"><b>b) De F ao espelho grande\u00a0 a dist\u00e2ncia \u00e9 R\/2=2,5m\u00a0 &#8212;\u00a0 como o objeto em F \u00e9 virtual\u00a0 &#8212;\u00a0 P=(2,5 \u2013 2,0)= &#8211; 0,5m \u00a0&#8212;\u00a0 1\/f=1\/P + 1\/P\u2019\u00a0 &#8212;\u00a0 1\/f=1\/-0,5 + \u00bd\u00a0 &#8212;\u00a0 f= &#8211; 0,67m\u00a0 &#8212;\u00a0\u00a0<\/b><\/span><\/span><span style=\"font-family: Arial,serif;\"><span style=\"font-size: medium;\"><b>r=2f= &#8211; 1,3m<\/b><\/span><\/span><\/p>\n<p><span style=\"font-family: Arial,serif;\"><span style=\"font-size: medium;\"><b>c) Como r &lt; 0 , ent\u00e3o o pequeno espelho \u00e9 convexo<\/b><\/span><\/span><\/p>\n<p>&nbsp;<\/p>\n<p><span style=\"color: #c00000;\"><span style=\"font-family: Arial Black,serif;\"><span style=\"font-size: medium;\"><b>32-<\/b><\/span><\/span><\/span><b> <\/b><span style=\"font-family: Arial,serif;\"><span style=\"font-size: medium;\"><b>Primeira imagem, invertida e aumentada &#8211; \u00a0espelho c\u00f4ncavo &#8211; Objeto entre C e F<\/b><\/span><\/span><\/p>\n<p align=\"CENTER\"><img loading=\"lazy\" decoding=\"async\" src=\"http:\/\/fisicaevestibular.com.br\/novo\/wp-content\/uploads\/migracao\/optica\/espelhos-efericos\/i_5cc0b4c3c9fe01ca_html_413f2b2e.jpg\" alt=\"\" width=\"611\" height=\"252\" name=\"Imagem 150\" align=\"BOTTOM\" border=\"0\" \/><\/p>\n<p><span style=\"font-family: Arial,serif;\"><span style=\"font-size: medium;\"><b>A imagem ter\u00e1: Natureza \u2013 real\u00a0 &#8212;\u00a0 Localiza\u00e7\u00e3o \u2013 antes de C\u00a0 &#8212;\u00a0 Tamanho \u2013 maior que o do objeto\u00a0 &#8212;\u00a0 Orienta\u00e7\u00e3o \u2013 invertida em rela\u00e7\u00e3o ao objeto<\/b><\/span><\/span><\/p>\n<p><span style=\"font-family: Arial,serif;\"><span style=\"font-size: medium;\"><b>Segunda imagem, invertida e reduzida \u2013 espelho c\u00f4ncavo &#8211; Objeto antes do centro de curvatura C<\/b><\/span><\/span><\/p>\n<p><img loading=\"lazy\" decoding=\"async\" src=\"http:\/\/fisicaevestibular.com.br\/novo\/wp-content\/uploads\/migracao\/optica\/espelhos-efericos\/i_5cc0b4c3c9fe01ca_html_547233a3.jpg\" alt=\"\" width=\"587\" height=\"254\" name=\"Imagem 151\" align=\"BOTTOM\" border=\"0\" \/><\/p>\n<p><span style=\"font-family: Arial,serif;\"><span style=\"font-size: medium;\"><b>A imagem ter\u00e1:Natureza \u2013 real (obtida na interse\u00e7\u00e3o do pr\u00f3prio raio de luz \u2013 linha cheia) \u2013 pode ser projetada, fotografada, etc.\u00a0 &#8212;\u00a0 Localiza\u00e7\u00e3o \u2013 entre C e F\u00a0 &#8212;\u00a0 Dimens\u00e3o (tamanho) \u2013 menor que o do objeto\u00a0 &#8212;\u00a0 Orienta\u00e7\u00e3o \u2013 invertida em rela\u00e7\u00e3o ao objeto<\/b><\/span><\/span><\/p>\n<p><span style=\"font-family: Arial,serif;\"><span style=\"font-size: medium;\"><b>Terceira imagem, direita e reduzida \u2013 espelho convexo &#8211; Espelho convexo &#8212; Para qualquer localiza\u00e7\u00e3o do objeto a imagem ter\u00e1 sempre:<\/b><\/span><\/span><\/p>\n<p><img loading=\"lazy\" decoding=\"async\" src=\"http:\/\/fisicaevestibular.com.br\/novo\/wp-content\/uploads\/migracao\/optica\/espelhos-efericos\/i_5cc0b4c3c9fe01ca_html_1d8ac364.jpg\" alt=\"\" width=\"348\" height=\"164\" name=\"Imagem 152\" align=\"BOTTOM\" border=\"0\" \/>\u00a0\u00a0\u00a0<img loading=\"lazy\" decoding=\"async\" src=\"http:\/\/fisicaevestibular.com.br\/novo\/wp-content\/uploads\/migracao\/optica\/espelhos-efericos\/i_5cc0b4c3c9fe01ca_html_d7507c94.jpg\" alt=\"\" width=\"384\" height=\"159\" name=\"Imagem 153\" align=\"BOTTOM\" border=\"0\" \/><\/p>\n<p><span style=\"font-family: Arial,serif;\"><span style=\"font-size: medium;\"><b>Natureza \u2013 virtual\u00a0 &#8212;\u00a0 Localiza\u00e7\u00e3o \u2013 atr\u00e1s do espelho e entre V e F e observe que \u00e0 medida que o objeto se aproxima do espelho, a imagem tamb\u00e9m se aproxima e aumenta de tamanho, mas est\u00e1 sempre entre V e F\u00a0 &#8212;\u00a0 \u00a0Tamanho \u2013 menor que o do objeto\u00a0 &#8212;\u00a0 Orienta\u00e7\u00e3o \u2013 direita em rela\u00e7\u00e3o ao objeto\u00a0 &#8212;\u00a0 Utilidades: Os espelhos convexos s\u00e3o empregados como retrovisores em ve\u00edculos, cabines de seguran\u00e7a, elevadores, etc. Sua vantagem sobre o espelho plano, nesse particular, \u00e9 ter maior campo visual. T\u00eam, entretanto, o inconveniente de n\u00e3o darem no\u00e7\u00e3o da dist\u00e2ncia.<\/b><\/span><\/span><\/p>\n<p><span style=\"font-family: Arial,serif;\"><span style=\"font-size: medium;\"><b>R- E<\/b><\/span><\/span><span style=\"font-family: Arial,serif;\"><span style=\"font-size: medium;\"><b>.\u00a0<\/b><\/span><\/span><\/p>\n<p><span style=\"color: #c00000;\"><span style=\"font-family: Arial Black,serif;\"><span style=\"font-size: medium;\"><b>33-(ACAFE-SC)<\/b><\/span><\/span><\/span><\/p>\n<p><span style=\"font-family: Arial,serif;\"><span style=\"font-size: medium;\"><b>Todo espelho esf\u00e9rico convexo, independentemente da posi\u00e7\u00e3o do objeto fornece sempre imagens virtuais, direitas e menores que o objeto\u00a0 &#8212;\u00a0 o fato das imagens serem menores que os objetos aumenta o campo visual do espelho\u00a0 &#8212;\u00a0 t\u00eam, entretanto, o inconveniente de n\u00e3o darem no\u00e7\u00e3o da dist\u00e2ncia.<\/b><\/span><\/span><\/p>\n<p><span style=\"font-family: Arial,serif;\"><span style=\"font-size: medium;\"><b>R- A<\/b><\/span><\/span><\/p>\n<p>&nbsp;<\/p>\n<h3><a title=\"Exerc\u00edcios de vestibulares sobre Espelhos esf\u00e9ricos \u2013 Constru\u00e7\u00e3o geom\u00e9trica de imagens\" href=\"http:\/\/fisicaevestibular.com.br\/novo\/optica\/optica-geometrica\/espelhos-esfericos-construcao-geometrica-de-imagens\/2172-2\/\"><span style=\"color: #000080;\">Voltar para os exerc\u00edcios<\/span><\/a><\/h3>\n","protected":false},"excerpt":{"rendered":"<p>Resolu\u00e7\u00e3o comentada dos exerc\u00edcios de vestibulares sobre Espelhos esf\u00e9ricos \u2013 Constru\u00e7\u00e3o geom\u00e9trica de imagens \u00a001- Trata-se de um espelho convexo e nele a imagem \u00e9 sempre virtual, direita,\u00a0 menor que o objeto e est\u00e1 sempre atr\u00e1s do espelho e entre\u00a0 o v\u00e9rtice V e o foco F, para qualquer posi\u00e7\u00e3o do objeto. R- D 02- R- A\u00a0 (veja esquema abaixo)<\/p>\n","protected":false},"author":1,"featured_media":0,"parent":2170,"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-2175","page","type-page","status-publish","hentry"],"aioseo_notices":[],"_links":{"self":[{"href":"https:\/\/fisicaevestibular.com.br\/novo\/wp-json\/wp\/v2\/pages\/2175","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=2175"}],"version-history":[{"count":3,"href":"https:\/\/fisicaevestibular.com.br\/novo\/wp-json\/wp\/v2\/pages\/2175\/revisions"}],"predecessor-version":[{"id":10935,"href":"https:\/\/fisicaevestibular.com.br\/novo\/wp-json\/wp\/v2\/pages\/2175\/revisions\/10935"}],"up":[{"embeddable":true,"href":"https:\/\/fisicaevestibular.com.br\/novo\/wp-json\/wp\/v2\/pages\/2170"}],"wp:attachment":[{"href":"https:\/\/fisicaevestibular.com.br\/novo\/wp-json\/wp\/v2\/media?parent=2175"}],"curies":[{"name":"wp","href":"https:\/\/api.w.org\/{rel}","templated":true}]}}