{"id":2430,"date":"2016-09-11T00:36:48","date_gmt":"2016-09-11T00:36:48","guid":{"rendered":"http:\/\/fisicaevestibular.com.br\/novo\/?page_id=2430"},"modified":"2024-08-23T15:05:15","modified_gmt":"2024-08-23T15:05:15","slug":"exercicios-de-vestibulares-com-resolucoes-comentadas-sobre-equacao-da-onda","status":"publish","type":"page","link":"https:\/\/fisicaevestibular.com.br\/novo\/ondulatoria\/ondas\/equacao-da-onda-equacao-fundamental-da-ondulatoria\/exercicios-de-vestibulares-com-resolucoes-comentadas-sobre-equacao-da-onda\/","title":{"rendered":"Equa\u00e7\u00e3o da onda &#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><b> <\/b><\/p>\n<p align=\"CENTER\"><span style=\"color: #0000cc;\"><span style=\"font-family: Arial Black,serif;\"><span style=\"font-size: large;\"><b>Equa\u00e7\u00e3o da onda (Equa\u00e7\u00e3o fundamental da ondulat\u00f3ria)<\/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-(UFSM)<\/b><\/span><\/span><\/span><b> <\/b><span style=\"color: #000000;\"><span style=\"font-family: Arial,serif;\"><span style=\"font-size: medium;\"><b>&#8220;Os habitantes dos pinheirais formados por arauc\u00e1rias come\u00e7aram a produzir cer\u00e2micas e aperfei\u00e7oaram seus instrumentos de trabalho.&#8221;<\/b><\/span><\/span><\/span><\/p>\n<p><span style=\"color: #000000;\"><span style=\"font-family: Arial,serif;\"><span style=\"font-size: medium;\"><b>Para descascar e moer cereais, as \u00edndias usavam um pil\u00e3o de pedra. Se uma \u00edndia batesse nos cereais 20 vezes por minuto, a freq\u00fc\u00eancia das batidas, em Hz, seria de, aproximadamente,<\/b><\/span><\/span><\/span><\/p>\n<p><img decoding=\"async\" src=\"http:\/\/fisicaevestibular.com.br\/novo\/wp-content\/uploads\/migracao\/ondulatoria\/equacaoonda\/i_b8534983f3672ed3_html_f8106f09.png\" alt=\"\" width=\"765\" height=\"22\" name=\"Picture 54\" align=\"BOTTOM\" border=\"0\" \/><\/p>\n<p><span style=\"color: #000000;\">\u00a0<\/span><\/p>\n<p><span style=\"color: #0000cc;\"><span style=\"font-family: Arial Black,serif;\"><span style=\"font-size: medium;\"><b>02-(UFAL)<\/b><\/span><\/span><\/span><b> <\/b><span style=\"color: #000000;\"><span style=\"font-family: Arial,serif;\"><span style=\"font-size: medium;\"><b>Uma onda produzida numa corda se propaga com freq\u00fc\u00eancia de 25 Hz. O gr\u00e1fico a seguir representa a corda num dado instante.<\/b><\/span><\/span><\/span><\/p>\n<p><span style=\"color: #000000;\"><span style=\"font-family: Arial,serif;\"><span style=\"font-size: medium;\"><b>Considere a situa\u00e7\u00e3o apresentada e os dados do gr\u00e1fico para analisar as afirma\u00e7\u00f5es que seguem.<\/b><\/span><\/span><\/span><img fetchpriority=\"high\" decoding=\"async\" src=\"http:\/\/fisicaevestibular.com.br\/novo\/wp-content\/uploads\/migracao\/ondulatoria\/equacaoonda\/i_b8534983f3672ed3_html_45087cb7.gif\" alt=\"\" width=\"456\" height=\"276\" name=\"Picture 103\" align=\"LEFT\" border=\"0\" hspace=\"12\" \/><\/p>\n<p><span style=\"color: #000000;\"><span style=\"font-family: Arial,serif;\"><span style=\"font-size: medium;\"><b>(\u00a0\u00a0\u00a0\u00a0 ) O per\u00edodo de propaga\u00e7\u00e3o da onda na corda \u00e9 20 s.<\/b><\/span><\/span><\/span><\/p>\n<p><span style=\"color: #000000;\"><span style=\"font-family: Arial,serif;\"><span style=\"font-size: medium;\"><b>(\u00a0\u00a0\u00a0\u00a0 ) A amplitude da onda estabelecida na corda \u00e9 de 6,0cm.<\/b><\/span><\/span><\/span><\/p>\n<p><span style=\"color: #000000;\"><span style=\"font-family: Arial,serif;\"><span style=\"font-size: medium;\"><b>(\u00a0\u00a0\u00a0\u00a0 ) A velocidade de propaga\u00e7\u00e3o da onda na corda \u00e9 de 5,0 m\/s.<\/b><\/span><\/span><\/span><\/p>\n<p><span style=\"color: #000000;\"><span style=\"font-family: Arial,serif;\"><span style=\"font-size: medium;\"><b>(\u00a0\u00a0\u00a0\u00a0 ) A onda que se estabeleceu na corda \u00e9 do tipo transversal.<\/b><\/span><\/span><\/span><\/p>\n<p><span style=\"color: #000000;\"><span style=\"font-family: Arial,serif;\"><span style=\"font-size: medium;\"><b>(\u00a0\u00a0\u00a0\u00a0 ) A onda que se estabeleceu na corda tem comprimento de onda de 10 cm.<\/b><\/span><\/span><\/span><\/p>\n<p><span style=\"color: #000000;\">\u00a0<\/span><\/p>\n<p><span style=\"color: #0000cc;\"><span style=\"font-family: Arial Black,serif;\"><span style=\"font-size: medium;\"><b>03- (UFRS)<\/b><\/span><\/span><\/span><b> <\/b><span style=\"color: #000000;\"><span style=\"font-family: Arial,serif;\"><span style=\"font-size: medium;\"><b>Um trem de ondas senoidais, gerado por um dispositivo mec\u00e2nico oscilante, propaga-se ao longo de uma corda. A tabela a seguir descreve quatro grandezas que caracterizam essas ondas mec\u00e2nicas.<\/b><\/span><\/span><\/span><img decoding=\"async\" src=\"http:\/\/fisicaevestibular.com.br\/novo\/wp-content\/uploads\/migracao\/ondulatoria\/equacaoonda\/i_b8534983f3672ed3_html_418f7a77.png\" alt=\"\" width=\"444\" height=\"274\" name=\"Picture 55\" align=\"LEFT\" border=\"0\" hspace=\"12\" \/><\/p>\n<p><span style=\"color: #000000;\"><span style=\"font-family: Arial,serif;\"><span style=\"font-size: medium;\"><b>As grandezas 1, 2, 3 e 4 s\u00e3o denominadas, respectivamente,<\/b><\/span><\/span><\/span><\/p>\n<p><span style=\"color: #000000;\"><span style=\"font-family: Arial,serif;\"><span style=\"font-size: medium;\"><b>a) freq\u00fc\u00eancia, fase, amplitude e comprimento de onda.<\/b><\/span><\/span><\/span><\/p>\n<p><span style=\"color: #000000;\"><span style=\"font-family: Arial,serif;\"><span style=\"font-size: medium;\"><b>b) fase, freq\u00fc\u00eancia, comprimento de onda e amplitude.<\/b><\/span><\/span><\/span><\/p>\n<p><span style=\"color: #000000;\"><span style=\"font-family: Arial,serif;\"><span style=\"font-size: medium;\"><b>c) per\u00edodo, freq\u00fc\u00eancia, velocidade de propaga\u00e7\u00e3o e amplitude.<\/b><\/span><\/span><\/span><\/p>\n<p><span style=\"color: #000000;\"><span style=\"font-family: Arial,serif;\"><span style=\"font-size: medium;\"><b>d) per\u00edodo, freq\u00fc\u00eancia, amplitude e comprimento de onda.<\/b><\/span><\/span><\/span><\/p>\n<p><span style=\"color: #000000;\"><span style=\"font-family: Arial,serif;\"><span style=\"font-size: medium;\"><b>e) freq\u00fc\u00eancia, per\u00edodo, comprimento de onda e amplitude<\/b><\/span><\/span><\/span><\/p>\n<p><span style=\"color: #000000;\">\u00a0<\/span><\/p>\n<p><span style=\"color: #0000cc;\"><span style=\"font-family: Arial Black,serif;\"><span style=\"font-size: medium;\"><b>04-(UNESP-SP) <\/b><\/span><\/span><\/span><span style=\"color: #000000;\"><span style=\"font-family: Arial,serif;\"><span style=\"font-size: medium;\"><b>A sucess\u00e3o de pulsos representada na figura foi produzida em 1,5s. Determine a<\/b><\/span><\/span><\/span><\/p>\n<p align=\"CENTER\"><img loading=\"lazy\" decoding=\"async\" src=\"http:\/\/fisicaevestibular.com.br\/novo\/wp-content\/uploads\/migracao\/ondulatoria\/equacaoonda\/i_b8534983f3672ed3_html_3e6e0158.jpg\" alt=\"\" width=\"383\" height=\"83\" name=\"Picture 56\" align=\"BOTTOM\" border=\"0\" \/><\/p>\n<p><span style=\"color: #000000;\"> <span style=\"font-family: Arial,serif;\"><span style=\"font-size: medium;\"><b>freq\u00fc\u00eancia e o per\u00edodo da onda.<\/b><\/span><\/span><\/span><\/p>\n<p><img loading=\"lazy\" decoding=\"async\" src=\"http:\/\/fisicaevestibular.com.br\/novo\/wp-content\/uploads\/migracao\/ondulatoria\/equacaoonda\/i_b8534983f3672ed3_html_1b15c28c.png\" alt=\"\" width=\"775\" height=\"239\" name=\"Picture 23\" align=\"BOTTOM\" border=\"0\" \/><\/p>\n<p><span style=\"color: #0000cc;\"><span style=\"font-family: Arial Black,serif;\"><span style=\"font-size: medium;\"><b>06- (UFPE)<\/b><\/span><\/span><\/span><b> <\/b><\/p>\n<p><span style=\"color: #000000;\"><span style=\"font-family: Arial,serif;\"><span style=\"font-size: medium;\"><b>As curvas A e B representam duas fotografias sucessivas de uma onda transversal que se propaga numa corda. O intervalo entre as fotografias \u00e9 de 0,008 s e \u00e9 menor do que o per\u00edodo da onda. Calcule a velocidade de propaga\u00e7\u00e3o da onda na corda, em m\/s.<\/b><\/span><\/span><\/span><\/p>\n<p><img loading=\"lazy\" decoding=\"async\" src=\"http:\/\/fisicaevestibular.com.br\/novo\/wp-content\/uploads\/migracao\/ondulatoria\/equacaoonda\/i_b8534983f3672ed3_html_d39ee041.gif\" alt=\"\" width=\"366\" height=\"163\" name=\"Picture 107\" align=\"LEFT\" border=\"0\" hspace=\"12\" \/><\/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>07-(UFRJ-RJ)<\/b><\/span><\/span><\/span><span style=\"color: #000000;\"><span style=\"font-family: Arial,serif;\"><span style=\"font-size: medium;\"><b> Uma perturba\u00e7\u00e3o peri\u00f3dica em uma corda produz ondas de freq\u00fc\u00eancia 40 Hz e comprimento de onda 15 cm.<\/b><\/span><\/span><\/span><\/p>\n<p><span style=\"color: #000000;\"><span style=\"font-family: Arial,serif;\"><span style=\"font-size: medium;\"><b>Neste caso, calcule:<\/b><\/span><\/span><\/span><\/p>\n<p><span style=\"color: #000000;\"><span style=\"font-family: Arial,serif;\"><span style=\"font-size: medium;\"><b>a) o per\u00edodo da onda.<\/b><\/span><\/span><\/span><\/p>\n<p><span style=\"color: #000000;\"><span style=\"font-family: Arial,serif;\"><span style=\"font-size: medium;\"><b>b) a velocidade da onda.<\/b><\/span><\/span><\/span><\/p>\n<p><span style=\"color: #000000;\">\u00a0<\/span><\/p>\n<p><span style=\"color: #0000cc;\"><span style=\"font-family: Arial Black,serif;\"><span style=\"font-size: medium;\"><b>08-(UFRJ-RJ)<\/b><\/span><\/span><\/span><b> <\/b><span style=\"color: #000000;\"><span style=\"font-family: Arial,serif;\"><span style=\"font-size: medium;\"><b>Atrav\u00e9s de um dispositivo adequado, produzem-se ondas em um meio el\u00e1stico, de tal modo que as freq\u00fc\u00eancias das ondas obtidas se encontram no intervalo de 15Hz a 60Hz. O gr\u00e1fico mostra como varia o comprimento de onda (\u03bb) em fun\u00e7\u00e3o da freq\u00fc\u00eancia (f).<\/b><\/span><\/span><\/span><img loading=\"lazy\" decoding=\"async\" src=\"http:\/\/fisicaevestibular.com.br\/novo\/wp-content\/uploads\/migracao\/ondulatoria\/equacaoonda\/i_b8534983f3672ed3_html_6aad1af9.jpg\" alt=\"\" width=\"505\" height=\"218\" name=\"Picture 108\" align=\"LEFT\" border=\"0\" hspace=\"12\" \/><\/p>\n<p><span style=\"color: #000000;\"><span style=\"font-family: Arial,serif;\"><span style=\"font-size: medium;\"><b>a) Calcule o menor comprimento de onda produzido nessa experi\u00eancia.<\/b><\/span><\/span><\/span><\/p>\n<p><span style=\"color: #000000;\"><span style=\"font-family: Arial,serif;\"><span style=\"font-size: medium;\"><b>b) Para um comprimento de onda de 12m, calcule o per\u00edodo da onda.<\/b><\/span><\/span><\/span><\/p>\n<p><span style=\"color: #000000;\">\u00a0<\/span><\/p>\n<p><span style=\"color: #0000cc;\"><span style=\"font-family: Arial Black,serif;\"><span style=\"font-size: medium;\"><b>09-(PUC-SP)<\/b><\/span><\/span><\/span><b> <\/b><span style=\"color: #000000;\"><span style=\"font-family: Arial,serif;\"><span style=\"font-size: medium;\"><b>A velocidade de propaga\u00e7\u00e3o de uma perturba\u00e7\u00e3o transversal numa corda de massa espec\u00edfica linear igual a 0,01kg\/m, tracionada por uma for\u00e7a de 64N, \u00e9, em metros por segundo, de:<\/b><\/span><\/span><\/span><\/p>\n<p><img loading=\"lazy\" decoding=\"async\" src=\"http:\/\/fisicaevestibular.com.br\/novo\/wp-content\/uploads\/migracao\/ondulatoria\/equacaoonda\/i_b8534983f3672ed3_html_c9b1567f.png\" alt=\"\" width=\"764\" height=\"19\" name=\"Picture 40\" align=\"BOTTOM\" border=\"0\" \/><\/p>\n<p><span style=\"color: #0000cc;\"><span style=\"font-family: Arial Black,serif;\"><span style=\"font-size: medium;\"><b>10-(MACKENZIE-SP)<\/b><\/span><\/span><\/span><b> <\/b><span style=\"color: #000000;\"><span style=\"font-family: Arial,serif;\"><span style=\"font-size: medium;\"><b>Um fio met\u00e1lico de 2m de comprimento e 10g de massa \u00e9 tracionado mediante uma for\u00e7a de 200N. Determine a velocidade de propaga\u00e7\u00e3o de um pulso transversal nesse fio.<\/b><\/span><\/span><\/span><\/p>\n<p><span style=\"color: #000000;\">\u00a0<\/span><\/p>\n<p><span style=\"color: #0000cc;\"><span style=\"font-family: Arial Black,serif;\"><span style=\"font-size: medium;\"><b>11-(FMJ-CE<\/b><\/span><\/span><\/span><span style=\"color: #000000;\"><span style=\"font-family: Arial,serif;\"><span style=\"font-size: medium;\"><b>) A figura mostra uma corda de massa m, submetida a uma for\u00e7a de tra\u00e7\u00e3o\u00a0 de intensidade T=24N, tendo suas extremidades presas a dois suportes fixos A e B.<\/b><\/span><\/span><\/span><img loading=\"lazy\" decoding=\"async\" src=\"http:\/\/fisicaevestibular.com.br\/novo\/wp-content\/uploads\/migracao\/ondulatoria\/equacaoonda\/i_b8534983f3672ed3_html_ebd8c04e.jpg\" alt=\"\" width=\"545\" height=\"144\" name=\"Picture 109\" align=\"LEFT\" border=\"0\" hspace=\"12\" \/><\/p>\n<p><span style=\"color: #000000;\"><span style=\"font-family: Arial,serif;\"><span style=\"font-size: medium;\"><b>Determine a massa de m, em quilogramas, sabendo que a velocidade de propaga\u00e7\u00e3o do pulso \u00e9 V=40m\/s.<\/b><\/span><\/span><\/span><\/p>\n<p><span style=\"color: #000000;\">\u00a0<\/span><\/p>\n<p><span style=\"color: #0000cc;\"><span style=\"font-family: Arial Black,serif;\"><span style=\"font-size: medium;\"><b>12-(UFPE)<\/b><\/span><\/span><\/span><b> <\/b><span style=\"color: #000000;\"><span style=\"font-family: Arial,serif;\"><span style=\"font-size: medium;\"><b>Uma onda transversal propaga-se em um fio de densidade d=10 g\/m. O fio est\u00e1 submetido a uma tra\u00e7\u00e3o F = 16 N. Verifica-se que a menor dist\u00e2ncia entre duas cristas da onda \u00e9 igual a 4,0 m. Calcule a freq\u00fc\u00eancia desta onda, em Hz.<\/b><\/span><\/span><\/span><\/p>\n<p><span style=\"color: #000000;\">\u00a0<\/span><\/p>\n<p><span style=\"color: #0000cc;\"><span style=\"font-family: Arial Black,serif;\"><span style=\"font-size: medium;\"><b>13-(UFMS)<\/b><\/span><\/span><\/span><b> <\/b><span style=\"color: #000000;\"><span style=\"font-family: Arial,serif;\"><span style=\"font-size: medium;\"><b>Uma corda de comprimento L=50cm est\u00e1 tensionada por um peso P=52,9N. (figura)<\/b><\/span><\/span><\/span><\/p>\n<p align=\"CENTER\"><img loading=\"lazy\" decoding=\"async\" src=\"http:\/\/fisicaevestibular.com.br\/novo\/wp-content\/uploads\/migracao\/ondulatoria\/equacaoonda\/i_b8534983f3672ed3_html_ec35a26c.jpg\" alt=\"\" width=\"407\" height=\"155\" name=\"Picture 110\" align=\"BOTTOM\" border=\"0\" \/><\/p>\n<p><span style=\"color: #000000;\"><span style=\"font-family: Arial,serif;\"><span style=\"font-size: medium;\"><b>Calcule a velocidade de propaga\u00e7\u00e3o da onda nessa corda, em m\/s.<\/b><\/span><\/span><\/span><\/p>\n<p><span style=\"color: #000000;\">\u00a0<\/span><\/p>\n<p><span style=\"color: #0000cc;\"><span style=\"font-family: Arial Black,serif;\"><span style=\"font-size: medium;\"><b>14-(UFES)<\/b><\/span><\/span><\/span><b> <\/b><span style=\"color: #000000;\"><span style=\"font-family: Arial,serif;\"><span style=\"font-size: medium;\"><b>Os morcegos emitem ultra-sons (movimento vibrat\u00f3rio, cuja freq\u00fc\u00eancia \u00e9 superior a 20.000 Hz). Considere-se que o menor comprimento de onda emitido por um morcego \u00e9 de 3,4.<\/b><\/span><\/span><\/span><\/p>\n<p><span style=\"color: #000000;\"><span style=\"font-family: Arial,serif;\"><span style=\"font-size: medium;\"><b>10<\/b><\/span><\/span><\/span><span style=\"color: #000000;\"><sup><span style=\"font-family: Arial,serif;\"><span style=\"font-size: medium;\"><b>-3<\/b><\/span><\/span><\/sup><\/span><span style=\"color: #000000;\"><span style=\"font-family: Arial,serif;\"><span style=\"font-size: medium;\"><b>\u00a0m.<\/b><\/span><\/span><\/span><\/p>\n<p align=\"CENTER\"><img loading=\"lazy\" decoding=\"async\" src=\"http:\/\/fisicaevestibular.com.br\/novo\/wp-content\/uploads\/migracao\/ondulatoria\/equacaoonda\/i_b8534983f3672ed3_html_be7ffc30.jpg\" alt=\"\" width=\"458\" height=\"216\" name=\"Picture 111\" align=\"BOTTOM\" border=\"0\" \/><\/p>\n<p><span style=\"color: #000000;\"><span style=\"font-family: Arial,serif;\"><span style=\"font-size: medium;\"><b>Supondo-se que a velocidade do som no ar \u00e9 de 340 m\/s, determine a freq\u00fc\u00eancia mais alta que um morcego emite.<\/b><\/span><\/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>15-(FUVEST-SP)<\/b><\/span><\/span><\/span><b> <\/b><span style=\"color: #000000;\"><span style=\"font-family: Arial,serif;\"><span style=\"font-size: medium;\"><b>Um grande aqu\u00e1rio, com paredes laterais de vidro, permite visualizar, na superf\u00edcie da \u00e1gua, uma onda que se propaga. A figura representa o perfil de tal onda no instante T<\/b><\/span><\/span><\/span><span style=\"color: #000000;\"><sub><span style=\"font-family: Arial,serif;\"><span style=\"font-size: medium;\"><b>o<\/b><\/span><\/span><\/sub><\/span><span style=\"color: #000000;\"><span style=\"font-family: Arial,serif;\"><span style=\"font-size: medium;\"><b>. Durante sua passagem, uma b\u00f3ia, em dada posi\u00e7\u00e3o, oscila para cima e para baixo e seu deslocamento vertical (y), em fun\u00e7\u00e3o do tempo, est\u00e1 representado no gr\u00e1fico<\/b><\/span><\/span><\/span><img loading=\"lazy\" decoding=\"async\" src=\"http:\/\/fisicaevestibular.com.br\/novo\/wp-content\/uploads\/migracao\/ondulatoria\/equacaoonda\/i_b8534983f3672ed3_html_2403934e.jpg\" alt=\"\" width=\"476\" height=\"213\" name=\"Picture 112\" align=\"LEFT\" border=\"0\" hspace=\"12\" \/><\/p>\n<p><span style=\"color: #000000;\"><span style=\"font-family: Arial,serif;\"><span style=\"font-size: medium;\"><b>Com essas informa\u00e7\u00f5es, \u00e9 poss\u00edvel concluir que a onda se propaga com uma velocidade, aproximadamente, de<\/b><\/span><\/span><\/span><\/p>\n<p><span style=\"color: #000000;\"><span style=\"font-family: Arial,serif;\"><span style=\"font-size: medium;\"><b>a) 2,0 m\/s<\/b><\/span><\/span><\/span><\/p>\n<p><span style=\"color: #000000;\"><span style=\"font-family: Arial,serif;\"><span style=\"font-size: medium;\"><b>b) 2,5 m\/s<\/b><\/span><\/span><\/span><\/p>\n<p><span style=\"color: #000000;\"><span style=\"font-family: Arial,serif;\"><span style=\"font-size: medium;\"><b>c) 5,0 m\/s<\/b><\/span><\/span><\/span><\/p>\n<p><span style=\"color: #000000;\"><span style=\"font-family: Arial,serif;\"><span style=\"font-size: medium;\"><b>d) 10 m\/s<\/b><\/span><\/span><\/span><\/p>\n<p><span style=\"color: #000000;\"><span style=\"font-family: Arial,serif;\"><span style=\"font-size: medium;\"><b>e) 20 m\/s<\/b><\/span><\/span><\/span><\/p>\n<p><span style=\"color: #000000;\">\u00a0<\/span><\/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=\"color: #000000;\"><span style=\"font-family: Arial,serif;\"><span style=\"font-size: medium;\"><b>Daniel brinca produzindo ondas ao bater com uma varinha na superf\u00edcie de um lago. A varinha toca a \u00e1gua a cada 5 segundos. Se Daniel passar a bater a varinha na \u00e1gua a cada 3 segundos, as ondas produzidas ter\u00e3o maior:<\/b><\/span><\/span><\/span><\/p>\n<p><span style=\"color: #000000;\"><span style=\"font-family: Arial,serif;\"><span style=\"font-size: medium;\"><b>a) comprimento de onda.<br \/>\nb) freq\u00fc\u00eancia.<br \/>\nc) per\u00edodo.<br \/>\nd) velocidade<\/b><\/span><\/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=\"color: #000000;\"><span style=\"font-family: Arial,serif;\"><span style=\"font-size: medium;\"><b>Radia\u00e7\u00f5es, como raios X, luz verde, luz ultravioleta, microondas ou ondas de r\u00e1dio, s\u00e3o caracterizadas por seu comprimento de onda (\u03bb) e por sua freq\u00fc\u00eancia (f). Quando essas radia\u00e7\u00f5es propagam-se no v\u00e1cuo, todas apresentam o mesmo valor para:<\/b><\/span><\/span><\/span><\/p>\n<p><img loading=\"lazy\" decoding=\"async\" src=\"http:\/\/fisicaevestibular.com.br\/novo\/wp-content\/uploads\/migracao\/ondulatoria\/equacaoonda\/i_b8534983f3672ed3_html_53aac25b.png\" alt=\"\" width=\"765\" height=\"21\" name=\"Picture 49\" align=\"BOTTOM\" border=\"0\" \/><\/p>\n<p><span style=\"color: #0000cc;\"><span style=\"font-family: Arial Black,serif;\"><span style=\"font-size: medium;\"><b>18-(UFPE)<\/b><\/span><\/span><\/span><b> <\/b><span style=\"color: #000000;\"><span style=\"font-family: Arial,serif;\"><span style=\"font-size: medium;\"><b>A figura a seguir mostra esquematicamente as ondas na superf\u00edcie d&#8217;\u00e1gua de um lago, produzidas por uma fonte de freq\u00fc\u00eancia 6,0 Hz, localizada no ponto A.<\/b><\/span><\/span><\/span><\/p>\n<p align=\"CENTER\"><img loading=\"lazy\" decoding=\"async\" src=\"http:\/\/fisicaevestibular.com.br\/novo\/wp-content\/uploads\/migracao\/ondulatoria\/equacaoonda\/i_b8534983f3672ed3_html_3adb0ca3.jpg\" alt=\"\" width=\"383\" height=\"195\" name=\"Picture 114\" align=\"BOTTOM\" border=\"0\" \/><\/p>\n<p><span style=\"color: #000000;\">\u00a0<span style=\"font-family: Arial,serif;\"><span style=\"font-size: medium;\"><b>As linhas cheias correspondem \u00e0s cristas, e as pontilhadas representam os vales em um certo instante de tempo. Qual o intervalo de tempo, em segundos, para que uma frente de onda percorra a dist\u00e2ncia da fonte at\u00e9 o ponto B, distante 60 cm<\/b><\/span><\/span><\/span><span style=\"color: #000000;\"><span style=\"font-family: Arial,serif;\"><span style=\"font-size: medium;\"><b>?<\/b><\/span><\/span><\/span><\/p>\n<p><span style=\"color: #000000;\">\u00a0<\/span><\/p>\n<p><span style=\"color: #0000cc;\"><span style=\"font-family: Arial Black,serif;\"><span style=\"font-size: medium;\"><b>19-(PUC-SP)<\/b><\/span><\/span><\/span><b> <\/b><span style=\"color: #000000;\"><span style=\"font-family: Arial,serif;\"><span style=\"font-size: medium;\"><b>Em dezembro de 2004 um terremoto no fundo do oceano, pr\u00f3ximo \u00e0 costa oeste da ilha de Sumatra, foi a perturba\u00e7\u00e3o necess\u00e1ria para a gera\u00e7\u00e3o de uma onda gigante, uma &#8220;tsunami&#8221;. A onda arrasou v\u00e1rias ilhas e localidades costeiras na \u00cdndia, no Sri Lanka, na Indon\u00e9sia, na Mal\u00e1sia, na Tail\u00e2ndia, dentre outras.<\/b><\/span><\/span><\/span><\/p>\n<p><span style=\"color: #000000;\"><span style=\"font-family: Arial,serif;\"><span style=\"font-size: medium;\"><b>Uma &#8220;tsunami&#8221; de comprimento de onda 150 quil\u00f4metros pode se deslocar com velocidade de 750 km\/h. Quando a profundidade das \u00e1guas \u00e9 grande, a amplitude da onda n\u00e3o atinge mais do que 1 metro, de maneira que um barco nessa regi\u00e3o praticamente n\u00e3o percebe a passagem da onda.<\/b><\/span><\/span><\/span><\/p>\n<p><span style=\"color: #000000;\"><span style=\"font-family: Arial,serif;\"><span style=\"font-size: medium;\"><b>Quanto tempo demora para um comprimento de onda dessa &#8220;tsunami&#8221; passar pelo barco?<\/b><\/span><\/span><\/span><\/p>\n<p><img loading=\"lazy\" decoding=\"async\" src=\"http:\/\/fisicaevestibular.com.br\/novo\/wp-content\/uploads\/migracao\/ondulatoria\/equacaoonda\/i_b8534983f3672ed3_html_b0b34284.png\" alt=\"\" width=\"764\" height=\"20\" name=\"Picture 51\" align=\"BOTTOM\" border=\"0\" \/><\/p>\n<p><span style=\"color: #000000;\">\u00a0<\/span><\/p>\n<p><span style=\"color: #0000cc;\"><span style=\"font-family: Arial Black,serif;\"><span style=\"font-size: medium;\"><b>20-(FUVEST-SP)<\/b><\/span><\/span><\/span><b> <\/b><span style=\"color: #000000;\"><span style=\"font-family: Arial,serif;\"><span style=\"font-size: medium;\"><b>Um sensor, montado em uma plataforma da Petrobr\u00e1s, com posi\u00e7\u00e3o fixa em rela\u00e7\u00e3o ao fundo do mar, registra as sucessivas posi\u00e7\u00f5es de uma pequena bola que flutua sobre a superf\u00edcie da \u00e1gua, \u00e0 medida que uma onda do mar passa por essa bola continuamente. A bola descreve um movimento aproximadamente circular, no plano vertical, mantendo-se em torno da mesma posi\u00e7\u00e3o m\u00e9dia, tal como reproduzido na seq\u00fc\u00eancia de registros adiante, nos tempos indicados. O intervalo entre registros \u00e9 menor do que o per\u00edodo da onda. A velocidade de propaga\u00e7\u00e3o dessa onda senoidal \u00e9 de 1,5 m\/s.<\/b><\/span><\/span><\/span><\/p>\n<p><img loading=\"lazy\" decoding=\"async\" src=\"http:\/\/fisicaevestibular.com.br\/novo\/wp-content\/uploads\/migracao\/ondulatoria\/equacaoonda\/i_b8534983f3672ed3_html_7a7471cb.png\" alt=\"\" width=\"610\" height=\"214\" name=\"Picture 57\" align=\"LEFT\" border=\"0\" hspace=\"12\" \/><\/p>\n<p><span style=\"color: #000000;\"><span style=\"font-family: Arial,serif;\"><span style=\"font-size: medium;\"><b>Para essas condi\u00e7\u00f5es:<\/b><\/span><\/span><\/span><\/p>\n<p><span style=\"color: #000000;\"><span style=\"font-family: Arial,serif;\"><span style=\"font-size: medium;\"><b>a) Determine o per\u00edodo T, em segundos, dessa onda do mar.<\/b><\/span><\/span><\/span><\/p>\n<p><span style=\"color: #000000;\"><span style=\"font-family: Arial,serif;\"><span style=\"font-size: medium;\"><b>b) Determine o comprimento de onda \u2014, em m, dessa onda do mar.<\/b><\/span><\/span><\/span><\/p>\n<p><span style=\"color: #000000;\"><span style=\"font-family: Arial,serif;\"><span style=\"font-size: medium;\"><b>c) Represente, um esquema do perfil dessa onda, para o instante t = 14 s, tal como visto da plataforma fixa. Indique os valores apropriados nos eixos horizontal e vertical.<\/b><\/span><\/span><\/span><\/p>\n<p><span style=\"color: #000000;\">\u00a0<\/span><\/p>\n<p><span style=\"color: #0000cc;\"><span style=\"font-family: Arial Black,serif;\"><span style=\"font-size: medium;\"><b>21-(UNICAMP-SP)<\/b><\/span><\/span><\/span><b> <\/b><span style=\"color: #000000;\"><span style=\"font-family: Arial,serif;\"><span style=\"font-size: medium;\"><b>Uma das formas de se controlar misturas de gases de maneira r\u00e1pida, sem precisar retirar amostras, \u00e9 medir a varia\u00e7\u00e3o da velocidade do som no interior desses gases. Uma onda sonora com freq\u00fc\u00eancia de 800 kHz \u00e9 enviada de um emissor a um receptor (vide esquema), sendo ent\u00e3o medida eletronicamente sua velocidade de propaga\u00e7\u00e3o em uma mistura gasosa. O gr\u00e1fico adiante apresenta a velocidade do som para uma mistura de arg\u00f4nio e nitrog\u00eanio em fun\u00e7\u00e3o da fra\u00e7\u00e3o molar de Ar em N.<\/b><\/span><\/span><\/span><\/p>\n<p><img loading=\"lazy\" decoding=\"async\" src=\"http:\/\/fisicaevestibular.com.br\/novo\/wp-content\/uploads\/migracao\/ondulatoria\/equacaoonda\/i_b8534983f3672ed3_html_69723543.jpg\" alt=\"\" width=\"518\" height=\"229\" name=\"Picture 116\" align=\"LEFT\" border=\"0\" hspace=\"12\" \/><\/p>\n<p><span style=\"color: #000000;\"><span style=\"font-family: Arial,serif;\"><span style=\"font-size: medium;\"><b>a) Qual o comprimento de onda da onda sonora no N\u201a puro?<\/b><\/span><\/span><\/span><\/p>\n<p><span style=\"color: #000000;\"><span style=\"font-family: Arial,serif;\"><span style=\"font-size: medium;\"><b>b) Qual o tempo para a onda sonora atravessar um tubo de 10 cm de comprimento contendo uma mistura com uma fra\u00e7\u00e3o molar de Ar de 60%?<\/b><\/span><\/span><\/span><\/p>\n<p><span style=\"color: #000000;\">\u00a0<\/span><\/p>\n<p><span style=\"color: #0000cc;\"><span style=\"font-family: Arial Black,serif;\"><span style=\"font-size: medium;\"><b>22- (UNICAMP-SP)<\/b><\/span><\/span><\/span><b> <\/b><span style=\"color: #000000;\"><span style=\"font-family: Arial,serif;\"><span style=\"font-size: medium;\"><b>O sistema GPS (&#8220;Global Positioning System&#8221;) consiste em um conjunto de sat\u00e9lites em \u00f3rbita em torno da Terra que transmitem sinais eletromagn\u00e9ticos para receptores na superf\u00edcie terrestre. A velocidade de propaga\u00e7\u00e3o dos sinais \u00e9 de 300.000 km\/s. Para que o sistema funcione bem, a absor\u00e7\u00e3o atmosf\u00e9rica desse sinal eletromagn\u00e9tico deve ser pequena. A figura a seguir mostra a porcentagem de radia\u00e7\u00e3o eletromagn\u00e9tica absorvida pela atmosfera em fun\u00e7\u00e3o do comprimento de onda<\/b><\/span><\/span><\/span><\/p>\n<p><img loading=\"lazy\" decoding=\"async\" src=\"http:\/\/fisicaevestibular.com.br\/novo\/wp-content\/uploads\/migracao\/ondulatoria\/equacaoonda\/i_b8534983f3672ed3_html_28adae8b.jpg\" alt=\"\" width=\"486\" height=\"264\" name=\"Picture 117\" align=\"BOTTOM\" border=\"0\" \/><\/p>\n<p><span style=\"color: #000000;\"><span style=\"font-family: Arial,serif;\"><span style=\"font-size: medium;\"><b>a) A freq\u00fc\u00eancia do sinal GPS \u00e9 igual a 1.500 MHz. Qual o comprimento de onda correspondente? Qual a porcentagem de absor\u00e7\u00e3o do sinal pela atmosfera?<\/b><\/span><\/span><\/span><\/p>\n<p><span style=\"color: #000000;\"><span style=\"font-family: Arial,serif;\"><span style=\"font-size: medium;\"><b>b) Uma das aplica\u00e7\u00f5es mais importantes do sistema GPS \u00e9 a determina\u00e7\u00e3o da posi\u00e7\u00e3o de um certo receptor na Terra. Essa determina\u00e7\u00e3o \u00e9 feita atrav\u00e9s da medida do tempo que o sinal leva para ir do sat\u00e9lite at\u00e9 o receptor. Qual \u00e9 a varia\u00e7\u00e3o\u00a0Dt na medida do tempo feita pelo receptor que corresponde a uma varia\u00e7\u00e3o na dist\u00e2ncia sat\u00e9lite-receptor de\u00a0Dx = 100m? Considere\u00a0 \u00a0que a trajet\u00f3ria do sinal seja retil\u00ednea.<\/b><\/span><\/span><\/span><\/p>\n<p><span style=\"color: #000000;\">\u00a0<\/span><\/p>\n<p><span style=\"color: #0000cc;\"><span style=\"font-family: Arial Black,serif;\"><span style=\"font-size: medium;\"><b>23-(UNICAMP-SP)<\/b><\/span><\/span><\/span><b> <\/b><span style=\"color: #000000;\"><span style=\"font-family: Arial,serif;\"><span style=\"font-size: medium;\"><b>Ondas s\u00e3o fen\u00f4menos nos quais h\u00e1 transporte de energia sem que seja necess\u00e1rio o transporte de massa. Um exemplo particularmente extremo s\u00e3o os &#8220;tsunamis&#8221;, ondas que se formam no oceano, como conseq\u00fc\u00eancia, por exemplo, de terremotos submarinos.<\/b><\/span><\/span><\/span><\/p>\n<p><span style=\"color: #000000;\"><span style=\"font-family: Arial,serif;\"><span style=\"font-size: medium;\"><b>a) Se, na regi\u00e3o de forma\u00e7\u00e3o, o comprimento de onda de um&#8221;tsunami&#8221; \u00e9 de 150 km e sua velocidade \u00e9 de 200 m\/s, qual \u00e9 o per\u00edodo da onda?<\/b><\/span><\/span><\/span><\/p>\n<p><span style=\"color: #000000;\"><span style=\"font-family: Arial,serif;\"><span style=\"font-size: medium;\"><b>b) A velocidade de propaga\u00e7\u00e3o da onda \u00e9 dada por v =\u00a0<img decoding=\"async\" src=\"http:\/\/fisicaevestibular.com.br\/novo\/wp-content\/uploads\/migracao\/ondulatoria\/equacaoonda\/i_b8534983f3672ed3_html_e3f6168.gif\" alt=\"\" align=\"ABSMIDDLE\" hspace=\"8\" \/>(gh) , onde h \u00e9 a profundidade local do oceano e g \u00e9 a acelera\u00e7\u00e3o da gravidade (10m\/s<\/b><\/span><\/span><\/span><span style=\"color: #000000;\"><sup><span style=\"font-family: Arial,serif;\"><span style=\"font-size: medium;\"><b>2<\/b><\/span><\/span><\/sup><\/span><span style=\"color: #000000;\"><span style=\"font-family: Arial,serif;\"><span style=\"font-size: medium;\"><b>). Qual \u00e9 a velocidade numa regi\u00e3o pr\u00f3xima \u00e0 costa, onde a profundidade \u00e9 de 6,4 m?<\/b><\/span><\/span><\/span><\/p>\n<p><span style=\"color: #000000;\"><span style=\"font-family: Arial,serif;\"><span style=\"font-size: medium;\"><b>c) Sendo A a amplitude (altura) da onda e supondo-se que a energia do &#8220;tsunami&#8221; se conserva, o produto V.A<\/b><\/span><\/span><\/span><span style=\"color: #000000;\"><sup><span style=\"font-family: Arial,serif;\"><span style=\"font-size: medium;\"><b>2<\/b><\/span><\/span><\/sup><\/span><span style=\"color: #000000;\"><span style=\"font-family: Arial,serif;\"><span style=\"font-size: medium;\"><b>\u00a0mant\u00e9m-se constante durante a propaga\u00e7\u00e3o. Se a amplitude da onda na regi\u00e3o de forma\u00e7\u00e3o for de 1,0 m, qual ser\u00e1 a amplitude perto da costa, onde a profundidade \u00e9 de 6,4 m?<\/b><\/span><\/span><\/span><\/p>\n<p><span style=\"color: #000000;\">\u00a0<\/span><\/p>\n<p><span style=\"color: #0000cc;\"><span style=\"font-family: Arial Black,serif;\"><span style=\"font-size: medium;\"><b>24-(UNIFESP-SP)<\/b><\/span><\/span><\/span><b> <\/b><span style=\"color: #000000;\"><span style=\"font-family: Arial,serif;\"><span style=\"font-size: medium;\"><b>O gr\u00e1fico representa a profundidade (y) no mar em fun\u00e7\u00e3o da velocidade do som (v). A freq\u00fc\u00eancia do som \u00e9 de 3000 Hz; essa curva \u00e9 v\u00e1lida para condi\u00e7\u00f5es determinadas de press\u00e3o e salinidade da \u00e1gua do mar.<\/b><\/span><\/span><\/span><img loading=\"lazy\" decoding=\"async\" src=\"http:\/\/fisicaevestibular.com.br\/novo\/wp-content\/uploads\/migracao\/ondulatoria\/equacaoonda\/i_b8534983f3672ed3_html_2f1124c8.png\" alt=\"\" width=\"289\" height=\"239\" name=\"Picture 62\" align=\"LEFT\" border=\"0\" hspace=\"12\" \/><\/p>\n<p><span style=\"color: #000000;\"><span style=\"font-family: Arial,serif;\"><span style=\"font-size: medium;\"><b>a) Nessas condi\u00e7\u00f5es, fa\u00e7a uma avalia\u00e7\u00e3o aproximada do valor m\u00ednimo atingido pela velocidade do som no mar e da profundidade em que isso ocorre.<\/b><\/span><\/span><\/span><\/p>\n<p><span style=\"color: #000000;\"><span style=\"font-family: Arial,serif;\"><span style=\"font-size: medium;\"><b>b) Desenhe na folha de respostas o esbo\u00e7o do correspondente gr\u00e1fico profundidade (y) em fun\u00e7\u00e3o do comprimento de onda (\u2014) do som. Adote o mesmo eixo e a mesma escala para a profundidade e coloque o comprimento de onda no eixo das abscissas. Represente tr\u00eas valores de \u2014, escritos com tr\u00eas algarismos significativos.<\/b><\/span><\/span><\/span><\/p>\n<p><span style=\"color: #000000;\">\u00a0<\/span><\/p>\n<p><span style=\"color: #0000cc;\"><span style=\"font-family: Arial Black,serif;\"><span style=\"font-size: medium;\"><b>25-(UNESP-SP)<\/b><\/span><\/span><\/span><b> <\/b><span style=\"color: #000000;\"><span style=\"font-family: Arial,serif;\"><span style=\"font-size: medium;\"><b>A propaga\u00e7\u00e3o de uma onda no mar da esquerda para a direita \u00e9 registrada em intervalos de 0,5 s e apresentada atrav\u00e9s da seq\u00fc\u00eancia dos gr\u00e1ficos da figura, tomados dentro de um mesmo ciclo<\/b><\/span><\/span><\/span><img loading=\"lazy\" decoding=\"async\" src=\"http:\/\/fisicaevestibular.com.br\/novo\/wp-content\/uploads\/migracao\/ondulatoria\/equacaoonda\/i_b8534983f3672ed3_html_19f05f37.png\" alt=\"\" width=\"504\" height=\"234\" name=\"Picture 65\" align=\"LEFT\" border=\"0\" hspace=\"12\" \/><\/p>\n<p><span style=\"color: #000000;\"><span style=\"font-family: Arial,serif;\"><span style=\"font-size: medium;\"><b>Analisando os gr\u00e1ficos, podemos afirmar que a velocidade da onda, em m\/s, \u00e9 de<\/b><\/span><\/span><\/span><\/p>\n<p><span style=\"color: #000000;\"><span style=\"font-family: Arial,serif;\"><span style=\"font-size: medium;\"><b>a) 1,5.\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0<\/b><\/span><\/span><\/span><\/p>\n<p><span style=\"color: #000000;\"><span style=\"font-family: Arial,serif;\"><span style=\"font-size: medium;\"><b>b) 2,0.\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0 <\/b><\/span><\/span><\/span><\/p>\n<p><span style=\"color: #000000;\"><span style=\"font-family: Arial,serif;\"><span style=\"font-size: medium;\"><b>c) 4,0.\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0 <\/b><\/span><\/span><\/span><\/p>\n<p><span style=\"color: #000000;\"><span style=\"font-family: Arial,serif;\"><span style=\"font-size: medium;\"><b>d) 4,5.\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><\/span><\/p>\n<p><span style=\"color: #000000;\"><span style=\"font-family: Arial,serif;\"><span style=\"font-size: medium;\"><b>e) 5,0.<\/b><\/span><\/span><\/span><\/p>\n<p><span style=\"color: #000000;\">\u00a0<\/span><\/p>\n<p><span style=\"color: #0000cc;\"><span style=\"font-family: Arial Black,serif;\"><span style=\"font-size: medium;\"><b>26-(UNICAMP-SP)<\/b><\/span><\/span><\/span><b> <\/b><span style=\"color: #000000;\"><span style=\"font-family: Arial,serif;\"><span style=\"font-size: medium;\"><b>O diagn\u00f3stico precoce de doen\u00e7as graves, como o c\u00e2ncer, aumenta de maneira significativa a chance de cura ou controle da doen\u00e7a. A tomografia de Resson\u00e2ncia Magn\u00e9tica Nuclear \u00e9 uma t\u00e9cnica de diagnostico m\u00e9dico que utiliza imagens obtidas a partir da absor\u00e7\u00e3o de radiofreq\u00fc\u00eancia pelos pr\u00f3tons do hidrog\u00eanio submetidos a um campo magn\u00e9tico. A condi\u00e7\u00e3o necess\u00e1ria para que a absor\u00e7\u00e3o ocorra, chamada condi\u00e7\u00e3o de resson\u00e2ncia, \u00e9 dada pela equa\u00e7\u00e3o f =\u03bbB, sendo f a frequ\u00eancia da radia\u00e7\u00e3o, B o campo magn\u00e9tico na posi\u00e7\u00e3o do pr\u00f3ton, e \u03bb= 42 MHz\/T<\/b><\/span><\/span><\/span><\/p>\n<p><img loading=\"lazy\" decoding=\"async\" src=\"http:\/\/fisicaevestibular.com.br\/novo\/wp-content\/uploads\/migracao\/ondulatoria\/equacaoonda\/i_b8534983f3672ed3_html_5307d04a.jpg\" alt=\"\" width=\"435\" height=\"253\" name=\"Picture 120\" align=\"LEFT\" border=\"0\" hspace=\"12\" \/><\/p>\n<p><span style=\"color: #000000;\"><span style=\"font-family: Arial,serif;\"><span style=\"font-size: medium;\"><b>Para se mapear diferentes partes do corpo, o campo magn\u00e9tico aplicado varia com a posi\u00e7\u00e3o ao longo do corpo do paciente.<\/b><\/span><\/span><\/span><\/p>\n<p><span style=\"color: #000000;\"><span style=\"font-family: Arial,serif;\"><span style=\"font-size: medium;\"><b>a) Observa-se que a radia\u00e7\u00e3o de freq\u00fc\u00eancia igual a 63MHz \u00e9 absorvida quando um paciente \u00e9 submetido a um campo magn\u00e9tico que varia conforme o gr\u00e1fico acima. Em que posi\u00e7\u00e3o x do corpo do paciente esta absor\u00e7\u00e3o ocorre?<\/b><\/span><\/span><\/span><\/p>\n<p><span style=\"color: #000000;\"><span style=\"font-family: Arial,serif;\"><span style=\"font-size: medium;\"><b>b) O comprimento de onda \u00e9 a dist\u00e2ncia percorrida pela onda durante o tempo de um per\u00edodo. O per\u00edodo \u00e9 igual ao inverso da freq\u00fc\u00eancia da onda. Qual \u00e9 o comprimento de onda da radiofreq\u00fc\u00eancia de 63 MHz no ar, sabendo-se que sua velocidade \u00e9 igual a 3,0 . 10<\/b><\/span><\/span><\/span><span style=\"color: #000000;\"><sup><span style=\"font-family: Arial,serif;\"><span style=\"font-size: medium;\"><b>8<\/b><\/span><\/span><\/sup><\/span><span style=\"color: #000000;\"><span style=\"font-family: Arial,serif;\"><span style=\"font-size: medium;\"><b>\u00a0m\/s?<\/b><\/span><\/span><\/span><\/p>\n<p><span style=\"color: #000000;\">\u00a0<\/span><\/p>\n<p><span style=\"color: #0000cc;\"><span style=\"font-family: Arial Black,serif;\"><span style=\"font-size: medium;\"><b>27-(UNESP-SP)<\/b><\/span><\/span><\/span><b> <\/b><span style=\"color: #000000;\"><span style=\"font-family: Arial,serif;\"><span style=\"font-size: medium;\"><b>Considere um lago onde a velocidade de propaga\u00e7\u00e3o das ondas na superf\u00edcie n\u00e3o <\/b><\/span><\/span><\/span><\/p>\n<p><span style=\"color: #000000;\"><span style=\"font-family: Arial,serif;\"><span style=\"font-size: medium;\"><b>dependa do comprimento de onda, mas apenas da profundidade. Essa rela\u00e7\u00e3o pode ser dada por v =\u00a0<img decoding=\"async\" src=\"http:\/\/fisicaevestibular.com.br\/novo\/wp-content\/uploads\/migracao\/ondulatoria\/equacaoonda\/i_b8534983f3672ed3_html_116c0bba.gif\" alt=\"\" align=\"ABSMIDDLE\" hspace=\"8\" \/>gd) , onde g \u00e9 a acelera\u00e7\u00e3o da gravidade e d \u00e9 a profundidade. Duas regi\u00f5es desse lago t\u00eam diferentes profundidades, como ilustrado na figura.<\/b><\/span><\/span><\/span><img loading=\"lazy\" decoding=\"async\" src=\"http:\/\/fisicaevestibular.com.br\/novo\/wp-content\/uploads\/migracao\/ondulatoria\/equacaoonda\/i_b8534983f3672ed3_html_c4265e9b.png\" alt=\"\" width=\"386\" height=\"228\" name=\"Picture 66\" align=\"LEFT\" border=\"0\" hspace=\"12\" \/><\/p>\n<p><span style=\"color: #000000;\"><span style=\"font-family: Arial,serif;\"><span style=\"font-size: medium;\"><b>O fundo do lago e formado por extensas plataformas planas em dois n\u00edveis; um degrau separa uma regi\u00e3o com 2,5 m de profundidade de outra com 10 m de profundidade. Uma onda plana, com comprimento de onda\u00a0l, forma-se na superf\u00edcie da regi\u00e3o rasa do lago e propaga-se para a direita, passando pelo desn\u00edvel. Considerando que a onda em ambas as regi\u00f5es possui mesma freq\u00fc\u00eancia, pode-se dizer que o comprimento de onda na regi\u00e3o mais profunda \u00e9 (g=10m\/s<\/b><\/span><\/span><\/span><span style=\"color: #000000;\"><sup><span style=\"font-family: Arial,serif;\"><span style=\"font-size: medium;\"><b>2<\/b><\/span><\/span><\/sup><\/span><span style=\"color: #000000;\"><span style=\"font-family: Arial,serif;\"><span style=\"font-size: medium;\"><b>)<\/b><\/span><\/span><\/span><\/p>\n<p><img loading=\"lazy\" decoding=\"async\" src=\"http:\/\/fisicaevestibular.com.br\/novo\/wp-content\/uploads\/migracao\/ondulatoria\/equacaoonda\/i_b8534983f3672ed3_html_9bead931.png\" alt=\"\" width=\"765\" height=\"22\" name=\"Picture 68\" align=\"BOTTOM\" border=\"0\" \/><\/p>\n<p><span style=\"color: #0000cc;\"><span style=\"font-family: Arial Black,serif;\"><span style=\"font-size: medium;\"><b>28-(FUVEST-SP)<\/b><\/span><\/span><\/span><b> <\/b><span style=\"color: #000000;\"><span style=\"font-family: Arial,serif;\"><span style=\"font-size: medium;\"><b>A propaga\u00e7\u00e3o de ondas na \u00e1gua \u00e9 estudada em grandes tanques, com detectores e softwares apropriados. Em uma das extremidades de um tanque (Figura 1), de 200 m de comprimento, um dispositivo D produz ondas na \u00e1gua, sendo que o perfil da superf\u00edcie da \u00e1gua, ao longo de toda a extens\u00e3o do tanque, \u00e9 registrado por detectores em instantes subseq\u00fcentes. Um conjunto de ondas, produzidas com freq\u00fc\u00eancia constante, tem seu deslocamento y, em FUN\u00c7\u00c3O DO TEMPO, representado na Figura 1, tal como registrado por detectores fixos na posi\u00e7\u00e3o x = 15 m.<\/b><\/span><\/span><\/span><\/p>\n<p><img loading=\"lazy\" decoding=\"async\" src=\"http:\/\/fisicaevestibular.com.br\/novo\/wp-content\/uploads\/migracao\/ondulatoria\/equacaoonda\/i_b8534983f3672ed3_html_4997f31.gif\" alt=\"\" width=\"772\" height=\"360\" name=\"Picture 122\" align=\"BOTTOM\" border=\"0\" \/><span style=\"color: #000000;\">\u00a0<span style=\"font-family: Arial,serif;\"><span style=\"font-size: medium;\"><b>Para esse mesmo conjunto de ondas, os resultados das medidas de sua propaga\u00e7\u00e3o ao longo do tanque s\u00e3o apresentados a seguir. Esses resultados correspondem aos deslocamentos y do n\u00edvel da \u00e1gua em rela\u00e7\u00e3o ao n\u00edvel de equil\u00edbrio (y = 0) medidos no instante t = 25 s para diversos valores de x. A partir desses resultados:<\/b><\/span><\/span><\/span><\/p>\n<p><span style=\"color: #000000;\"><span style=\"font-family: Arial,serif;\"><span style=\"font-size: medium;\"><b>a) Estime a freq\u00fc\u00eancia f, em Hz, com que as ondas foram produzidas.<\/b><\/span><\/span><\/span><\/p>\n<p><span style=\"color: #000000;\"><span style=\"font-family: Arial,serif;\"><span style=\"font-size: medium;\"><b>b) Estime o comprimento de onda L, em metros, das ondas formadas.<\/b><\/span><\/span><\/span><\/p>\n<p><span style=\"color: #000000;\"><span style=\"font-family: Arial,serif;\"><span style=\"font-size: medium;\"><b>c) Estime a velocidade V, em m\/s, de propaga\u00e7\u00e3o das ondas no tanque.<\/b><\/span><\/span><\/span><\/p>\n<p><span style=\"color: #000000;\"><span style=\"font-family: Arial,serif;\"><span style=\"font-size: medium;\"><b>d) Identifique, no gr\u00e1fico da Figura 2 (t = 25 s), as posi\u00e7\u00f5es das ondas A, B, C, D e E, assinaladas na Figura 1, ainda que, como pode ser observado, as amplitudes dessas ondas diminuam com sua propaga\u00e7\u00e3o.<\/b><\/span><\/span><\/span><\/p>\n<p><span style=\"color: #000000;\">\u00a0<\/span><\/p>\n<p><span style=\"color: #0000cc;\"><span style=\"font-family: Arial Black,serif;\"><span style=\"font-size: medium;\"><b>29-(FUVEST-SP)<\/b><\/span><\/span><\/span><b> <\/b><span style=\"color: #000000;\"><span style=\"font-family: Arial,serif;\"><span style=\"font-size: medium;\"><b>Um vibrador produz, numa superf\u00edcie l\u00edquida, ondas de comprimento 5,0cm que se propagam a velocidade de 3,0cm\/s.<\/b><\/span><\/span><\/span><\/p>\n<p><span style=\"color: #000000;\"><span style=\"font-family: Arial,serif;\"><span style=\"font-size: medium;\"><b>a) Qual a freq\u00fc\u00eancia das ondas?<\/b><\/span><\/span><\/span><\/p>\n<p><span style=\"color: #000000;\"><span style=\"font-family: Arial,serif;\"><span style=\"font-size: medium;\"><b>b) Caso o vibrador aumente apenas sua amplitude de vibra\u00e7\u00e3o, o que ocorre com a velocidade de propaga\u00e7\u00e3o, o comprimento e a freq\u00fc\u00eancia das ondas?<\/b><\/span><\/span><\/span><\/p>\n<p><span style=\"color: #000000;\">\u00a0<\/span><\/p>\n<p><span style=\"color: #0000cc;\"><span style=\"font-family: Arial Black,serif;\"><span style=\"font-size: medium;\"><b>30-(FUVEST-SP)<\/b><\/span><\/span><\/span><b> <\/b><span style=\"color: #000000;\"><span style=\"font-family: Arial,serif;\"><span style=\"font-size: medium;\"><b>Num lago o vento produz ondas peri\u00f3dicas que se propagam com a velocidade de 2m\/s. O comprimento de onda \u00e9 10m. Determine o per\u00edodo de oscila\u00e7\u00e3o de um barco<\/b><\/span><\/span><\/span><\/p>\n<p><span style=\"color: #000000;\"><span style=\"font-family: Arial,serif;\"><span style=\"font-size: medium;\"><b>a) quando ancorado nesse lago.<\/b><\/span><\/span><\/span><\/p>\n<p><span style=\"color: #000000;\"><span style=\"font-family: Arial,serif;\"><span style=\"font-size: medium;\"><b>b) quando se movimenta em sentido contr\u00e1rio ao da propaga\u00e7\u00e3o das ondas, com uma velocidade de 8m\/s.<\/b><\/span><\/span><\/span><\/p>\n<p><span style=\"color: #000000;\">\u00a0<\/span><\/p>\n<p><span style=\"color: #0000cc;\"><span style=\"font-family: Arial Black,serif;\"><span style=\"font-size: medium;\"><b>31-(UECE-CE)<\/b><\/span><\/span><\/span><\/p>\n<p><span style=\"color: #000000;\"><span style=\"font-family: Arial,serif;\"><span style=\"font-size: medium;\"><b>Fornos de micro-ondas usam ondas de r\u00e1dio de comprimento de onda aproximadamente 12 cm para aquecer os alimentos.<\/b><\/span><\/span><\/span><img loading=\"lazy\" decoding=\"async\" src=\"http:\/\/fisicaevestibular.com.br\/novo\/wp-content\/uploads\/migracao\/ondulatoria\/equacaoonda\/i_b8534983f3672ed3_html_6d0d92ca.jpg\" alt=\"\" width=\"322\" height=\"123\" name=\"Picture 124\" align=\"LEFT\" border=\"0\" hspace=\"12\" \/><\/p>\n<p><span style=\"color: #000000;\"><span style=\"font-family: Arial,serif;\"><span style=\"font-size: medium;\"><b>Considerando a velocidade da luz igual a 300 000 km\/s a frequ\u00eancia das ondas utilizadas \u00e9<\/b><\/span><\/span><\/span><\/p>\n<p><span style=\"color: #000000;\"><span style=\"font-family: Arial,serif;\"><span style=\"font-size: medium;\"><b>a)\u00a0360 Hz.\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\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0<\/b><\/span><\/span><\/span><\/p>\n<p><span style=\"color: #000000;\"><span style=\"font-family: Arial,serif;\"><span style=\"font-size: medium;\"><b>b)\u00a0250 kHz.\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\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0<\/b><\/span><\/span><\/span><\/p>\n<p><span style=\"color: #000000;\"><span style=\"font-family: Arial,serif;\"><span style=\"font-size: medium;\"><b>c)\u00a03,6 MHz.\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\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0<\/b><\/span><\/span><\/span><\/p>\n<p><span style=\"color: #000000;\"><span style=\"font-family: Arial,serif;\"><span style=\"font-size: medium;\"><b>d)\u00a02,5 GHz.\u00a0\u00a0<\/b><\/span><\/span><\/span><\/p>\n<p><span style=\"color: #000000;\">\u00a0<\/span><\/p>\n<p><span style=\"color: #0000cc;\"><span style=\"font-family: Arial Black,serif;\"><span style=\"font-size: medium;\"><b>32-(PUC-PR)<\/b><\/span><\/span><\/span><\/p>\n<p><img loading=\"lazy\" decoding=\"async\" src=\"http:\/\/fisicaevestibular.com.br\/novo\/wp-content\/uploads\/migracao\/ondulatoria\/equacaoonda\/i_b8534983f3672ed3_html_b32aaf04.jpg\" alt=\"\" width=\"77\" height=\"90\" name=\"Picture 125\" align=\"BOTTOM\" border=\"0\" \/><span style=\"color: #000000;\">\u00a0<img loading=\"lazy\" decoding=\"async\" src=\"http:\/\/fisicaevestibular.com.br\/novo\/wp-content\/uploads\/migracao\/ondulatoria\/equacaoonda\/i_b8534983f3672ed3_html_843cf77c.jpg\" alt=\"\" width=\"148\" height=\"89\" name=\"Picture 126\" align=\"BOTTOM\" border=\"0\" \/>\u00a0<img loading=\"lazy\" decoding=\"async\" src=\"http:\/\/fisicaevestibular.com.br\/novo\/wp-content\/uploads\/migracao\/ondulatoria\/equacaoonda\/i_b8534983f3672ed3_html_27018a87.jpg\" alt=\"\" width=\"151\" height=\"93\" name=\"Picture 127\" align=\"BOTTOM\" border=\"0\" \/>\u00a0<img loading=\"lazy\" decoding=\"async\" src=\"http:\/\/fisicaevestibular.com.br\/novo\/wp-content\/uploads\/migracao\/ondulatoria\/equacaoonda\/i_b8534983f3672ed3_html_8507b4f7.jpg\" alt=\"\" width=\"178\" height=\"94\" name=\"Picture 128\" align=\"BOTTOM\" border=\"0\" \/>\u00a0<img loading=\"lazy\" decoding=\"async\" src=\"http:\/\/fisicaevestibular.com.br\/novo\/wp-content\/uploads\/migracao\/ondulatoria\/equacaoonda\/i_b8534983f3672ed3_html_47310084.jpg\" alt=\"\" width=\"185\" height=\"104\" name=\"Picture 129\" align=\"BOTTOM\" border=\"0\" \/><\/span><\/p>\n<p><span style=\"color: #000000;\"><span style=\"font-family: Arial,serif;\"><span style=\"font-size: medium;\"><b>Para que um objeto possa ser vis\u00edvel em um microsc\u00f3pio qualquer, o comprimento de onda da radia\u00e7\u00e3o incidente deve ser pelo menos compar\u00e1vel ao tamanho do objeto. Na f\u00edsica qu\u00e2ntica, o princ\u00edpio da dualidade onda-part\u00edcula, introduzido por Louis de Broglie, prop\u00f5e que part\u00edculas de mat\u00e9ria, como os el\u00e9trons, podem comportar-se como ondas de maneira similar \u00e0 luz. Um exemplo de aplica\u00e7\u00e3o desse princ\u00edpio \u00e9 o que ocorre no microsc\u00f3pio eletr\u00f4nico, em que um feixe de el\u00e9trons \u00e9 produzido para \u201ciluminar\u201d a amostra. O comprimento de onda dos el\u00e9trons do feixe \u00e9 muito menor que o da luz; com isso, consegue-se obter amplia\u00e7\u00f5es mil vezes maiores do que as de um microsc\u00f3pio \u00f3ptico.<\/b><\/span><\/span><\/span><\/p>\n<p><span style=\"color: #000000;\"><span style=\"font-family: Arial,serif;\"><span style=\"font-size: medium;\"><b>Suponha que, para visualizar o v\u00edrus H<\/b><\/span><\/span><\/span><span style=\"color: #000000;\"><sub><span style=\"font-family: Arial,serif;\"><span style=\"font-size: medium;\"><b>1<\/b><\/span><\/span><\/sub><\/span><span style=\"color: #000000;\"><span style=\"font-family: Arial,serif;\"><span style=\"font-size: medium;\"><b>N<\/b><\/span><\/span><\/span><span style=\"color: #000000;\"><sub><span style=\"font-family: Arial,serif;\"><span style=\"font-size: medium;\"><b>1<\/b><\/span><\/span><\/sub><\/span><span style=\"color: #000000;\"><span style=\"font-family: Arial,serif;\"><span style=\"font-size: medium;\"><b>\u00a0em um microsc\u00f3pio eletr\u00f4nico, um feixe de el\u00e9trons tenha sido ajustado para fornecerel\u00e9trons que se propagam com comprimento de onda igual ao di\u00e2metro do v\u00edrus (supondo forma esf\u00e9rica). Se a velocidade de propaga\u00e7\u00e3o da onda do feixe for de 10<\/b><\/span><\/span><\/span><span style=\"color: #000000;\"><sup><span style=\"font-family: Arial,serif;\"><span style=\"font-size: medium;\"><b>4<\/b><\/span><\/span><\/sup><\/span><span style=\"color: #000000;\"><span style=\"font-family: Arial,serif;\"><span style=\"font-size: medium;\"><b>\u00a0m\/s e a frequ\u00eancia for de 10<\/b><\/span><\/span><\/span><span style=\"color: #000000;\"><sup><span style=\"font-family: Arial,serif;\"><span style=\"font-size: medium;\"><b>11<\/b><\/span><\/span><\/sup><\/span><span style=\"color: #000000;\"><span style=\"font-family: Arial,serif;\"><span style=\"font-size: medium;\"><b>\u00a0Hz, assinale a alternativa que corresponde ao di\u00e2metro do v\u00edrus H<\/b><\/span><\/span><\/span><span style=\"color: #000000;\"><sub><span style=\"font-family: Arial,serif;\"><span style=\"font-size: medium;\"><b>1<\/b><\/span><\/span><\/sub><\/span><span style=\"color: #000000;\"><span style=\"font-family: Arial,serif;\"><span style=\"font-size: medium;\"><b>N<\/b><\/span><\/span><\/span><span style=\"color: #000000;\"><sub><span style=\"font-family: Arial,serif;\"><span style=\"font-size: medium;\"><b>1<\/b><\/span><\/span><\/sub><\/span><span style=\"color: #000000;\"><span style=\"font-family: Arial,serif;\"><span style=\"font-size: medium;\"><b>. Dado: 1 nm (nan\u00f4metro) = 10<\/b><\/span><\/span><\/span><span style=\"color: #000000;\"><sup><span style=\"font-family: Arial,serif;\"><span style=\"font-size: medium;\"><b>-9<\/b><\/span><\/span><\/sup><\/span><span style=\"color: #000000;\"><span style=\"font-family: Arial,serif;\"><span style=\"font-size: medium;\"><b>\u00a0m.<\/b><\/span><\/span><\/span><img loading=\"lazy\" decoding=\"async\" src=\"http:\/\/fisicaevestibular.com.br\/novo\/wp-content\/uploads\/migracao\/ondulatoria\/equacaoonda\/i_b8534983f3672ed3_html_4c4893ea.jpg\" alt=\"\" width=\"366\" height=\"251\" name=\"Picture 130\" align=\"LEFT\" border=\"0\" hspace=\"12\" \/><\/p>\n<p><span style=\"color: #000000;\"><span style=\"font-family: Arial,serif;\"><span style=\"font-size: medium;\"><b>a) 10 nm\u00a0 \u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0<\/b><\/span><\/span><\/span><\/p>\n<p><span style=\"color: #000000;\"><span style=\"font-family: Arial,serif;\"><span style=\"font-size: medium;\"><b>b) 1 nm\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><\/span><\/p>\n<p><span style=\"color: #000000;\"><span style=\"font-family: Arial,serif;\"><span style=\"font-size: medium;\"><b>c) 100 nm\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><\/span><\/p>\n<p><span style=\"color: #000000;\"><span style=\"font-family: Arial,serif;\"><span style=\"font-size: medium;\"><b>d) 10 \u00b5m\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\u00a0\u00a0\u00a0\u00a0<\/b><\/span><\/span><\/span><\/p>\n<p><span style=\"color: #000000;\"><span style=\"font-family: Arial,serif;\"><span style=\"font-size: medium;\"><b>e) 1 \u00b5m\u00a0<\/b><\/span><\/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>33-(FGV-SP)\u00a0<\/b><\/span><\/span><\/span><\/p>\n<p><img loading=\"lazy\" decoding=\"async\" src=\"http:\/\/fisicaevestibular.com.br\/novo\/wp-content\/uploads\/migracao\/ondulatoria\/equacaoonda\/i_b8534983f3672ed3_html_1017321b.jpg\" alt=\"\" width=\"240\" height=\"70\" name=\"Picture 131\" align=\"BOTTOM\" border=\"0\" \/><\/p>\n<p><span style=\"color: #000000;\"><span style=\"font-family: Arial,serif;\"><span style=\"font-size: medium;\"><b>Veja esse quadro. Nele, o artista mostra os efeitos dos golpes intermitentes do vento sobre um trigal.<\/b><\/span><\/span><\/span><img loading=\"lazy\" decoding=\"async\" src=\"http:\/\/fisicaevestibular.com.br\/novo\/wp-content\/uploads\/migracao\/ondulatoria\/equacaoonda\/i_b8534983f3672ed3_html_6b9e1fcd.jpg\" alt=\"\" width=\"475\" height=\"155\" name=\"Picture 132\" align=\"LEFT\" border=\"0\" hspace=\"12\" \/><\/p>\n<p><span style=\"color: #000000;\"><span style=\"font-family: Arial,serif;\"><span style=\"font-size: medium;\"><b>Admitindo que a dist\u00e2ncia entre as duas \u00e1rvores seja de 120 m e, supondo que a frequ\u00eancia dos golpes de ar e consequentemente do trigo balan\u00e7ando seja de 0,50 Hz, a velocidade do vento na ocasi\u00e3o retratada pela pintura \u00e9, em m\/s,<\/b><\/span><\/span><\/span><\/p>\n<p><img loading=\"lazy\" decoding=\"async\" src=\"http:\/\/fisicaevestibular.com.br\/novo\/wp-content\/uploads\/migracao\/ondulatoria\/equacaoonda\/i_b8534983f3672ed3_html_bebb6da6.png\" alt=\"\" width=\"765\" height=\"25\" name=\"Picture 70\" align=\"BOTTOM\" border=\"0\" \/><\/p>\n<p><span style=\"color: #000000;\">\u00a0<\/span><span style=\"color: #0000cc;\"><span style=\"font-family: Arial Black,serif;\"><span style=\"font-size: medium;\"><b>34-(UPE-PE)\u00a0<\/b><\/span><\/span><\/span><\/p>\n<p><img loading=\"lazy\" decoding=\"async\" src=\"http:\/\/fisicaevestibular.com.br\/novo\/wp-content\/uploads\/migracao\/ondulatoria\/equacaoonda\/i_b8534983f3672ed3_html_7ff83b06.jpg\" alt=\"\" width=\"175\" height=\"70\" name=\"Picture 133\" align=\"BOTTOM\" border=\"0\" \/><\/p>\n<p><span style=\"color: #000000;\"><span style=\"font-family: Arial,serif;\"><span style=\"font-size: medium;\"><b>Um pulso ondulat\u00f3rio senoidal \u00e9 produzido em uma extremidade de uma corda longa e se propaga por toda a sua extens\u00e3o. A onda\u00a0possui uma frequ\u00eancia de 50 Hz e comprimento de onda 0,5 m. O tempo que a onda leva para percorrer uma dist\u00e2ncia de 10m na corda vale em segundos:<\/b><\/span><\/span><\/span><img loading=\"lazy\" decoding=\"async\" src=\"http:\/\/fisicaevestibular.com.br\/novo\/wp-content\/uploads\/migracao\/ondulatoria\/equacaoonda\/i_b8534983f3672ed3_html_86f615c7.jpg\" alt=\"\" width=\"318\" height=\"68\" name=\"Picture 134\" align=\"LEFT\" border=\"0\" hspace=\"12\" \/><\/p>\n<p><img loading=\"lazy\" decoding=\"async\" src=\"http:\/\/fisicaevestibular.com.br\/novo\/wp-content\/uploads\/migracao\/ondulatoria\/equacaoonda\/i_b8534983f3672ed3_html_c30e1426.png\" alt=\"\" width=\"765\" height=\"21\" name=\"Picture 71\" align=\"BOTTOM\" border=\"0\" \/><\/p>\n<p><span style=\"color: #0000cc;\"><span style=\"font-family: Arial Black,serif;\"><span style=\"font-size: medium;\"><b>35-(PUC-SP) <\/b><\/span><\/span><\/span><span style=\"color: #000000;\"><span style=\"font-family: Arial,serif;\"><span style=\"font-size: medium;\"><b>O fone de ouvido tem se tornado cada vez mais um acess\u00f3rio indispens\u00e1vel para os adolescentes que curtem suas m\u00fasicas em todos os ambientes e hor\u00e1rios. Antes do advento do\u00a0<\/b><\/span><\/span><\/span><span style=\"color: #000000;\"><span style=\"font-family: Arial,serif;\"><span style=\"font-size: medium;\"><i><b>iPod<\/b><\/i><\/span><\/span><\/span><span style=\"color: #000000;\"><span style=\"font-family: Arial,serif;\"><span style=\"font-size: medium;\"><b>\u00a0e outros cong\u00eaneres, para ouvir as m\u00fasicas da parada de sucessos, os jovens tinham que carregar seu radinho port\u00e1til sintonizado em FM (frequ\u00eancia modulada).<\/b><\/span><\/span><\/span><img loading=\"lazy\" decoding=\"async\" src=\"http:\/\/fisicaevestibular.com.br\/novo\/wp-content\/uploads\/migracao\/ondulatoria\/equacaoonda\/i_b8534983f3672ed3_html_e29a55c5.jpg\" alt=\"\" width=\"448\" height=\"144\" name=\"Picture 136\" align=\"LEFT\" border=\"0\" hspace=\"12\" \/><\/p>\n<p><span style=\"color: #000000;\"><span style=\"font-family: Arial,serif;\"><span style=\"font-size: medium;\"><b>Observando o painel de um desses r\u00e1dios, calcule a raz\u00e3o aproximada entre o maior e o menor comprimento de onda para a faixa de valores correspondentes a FM.<\/b><\/span><\/span><\/span><\/p>\n<p><img loading=\"lazy\" decoding=\"async\" src=\"http:\/\/fisicaevestibular.com.br\/novo\/wp-content\/uploads\/migracao\/ondulatoria\/equacaoonda\/i_b8534983f3672ed3_html_de908624.png\" alt=\"\" width=\"765\" height=\"18\" name=\"Picture 72\" align=\"BOTTOM\" border=\"0\" \/><\/p>\n<p><span style=\"color: #0000cc;\"><span style=\"font-family: Arial Black,serif;\"><span style=\"font-size: medium;\"><b>36-(CPS)<\/b><\/span><\/span><\/span><\/p>\n<p><img loading=\"lazy\" decoding=\"async\" src=\"http:\/\/fisicaevestibular.com.br\/novo\/wp-content\/uploads\/migracao\/ondulatoria\/equacaoonda\/i_b8534983f3672ed3_html_2dbf1545.jpg\" alt=\"\" width=\"294\" height=\"83\" name=\"Picture 137\" align=\"BOTTOM\" border=\"0\" \/><\/p>\n<p><span style=\"color: #000000;\">\u00a0<span style=\"font-family: Arial,serif;\"><span style=\"font-size: medium;\"><b>Na Copa do Mundo de 2010, a Fifa determinou que nenhum atleta poderia participar sem ter feito uma minuciosa avalia\u00e7\u00e3o cardiol\u00f3gica pr\u00e9via. Um dos testes a ser realizado, no exame ergom\u00e9trico, era o eletrocardiograma. Nele \u00e9 feito o registro da varia\u00e7\u00e3o dos potenciais el\u00e9tricos gerados pela atividade do cora\u00e7\u00e3o.<\/b><\/span><\/span><\/span><img loading=\"lazy\" decoding=\"async\" src=\"http:\/\/fisicaevestibular.com.br\/novo\/wp-content\/uploads\/migracao\/ondulatoria\/equacaoonda\/i_b8534983f3672ed3_html_3b6dd2be.jpg\" alt=\"\" width=\"552\" height=\"212\" name=\"Picture 138\" align=\"LEFT\" border=\"0\" hspace=\"12\" \/><\/p>\n<p><span style=\"color: #000000;\"><span style=\"font-family: Arial,serif;\"><span style=\"font-size: medium;\"><b>Considere a figura que representa parte do eletrocardiograma de um determinado atleta.<\/b><\/span><\/span><\/span><\/p>\n<p><span style=\"color: #000000;\"><span style=\"font-family: Arial,serif;\"><span style=\"font-size: medium;\"><b>Sabendo que o pico m\u00e1ximo representa a fase final da di\u00e1stole, conclui-se que a frequ\u00eancia card\u00edaca desse atleta \u00e9, em batimentos por minuto,<\/b><\/span><\/span><\/span><\/p>\n<p><span style=\"color: #000000;\"><span style=\"font-family: Arial,serif;\"><span style=\"font-size: medium;\"><b>a) 60.\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><\/span><\/p>\n<p><span style=\"color: #000000;\"><span style=\"font-family: Arial,serif;\"><span style=\"font-size: medium;\"><b>b) 80.\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><\/span><\/p>\n<p><span style=\"color: #000000;\"><span style=\"font-family: Arial,serif;\"><span style=\"font-size: medium;\"><b>c) 100.\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><\/span><\/p>\n<p><span style=\"color: #000000;\"><span style=\"font-family: Arial,serif;\"><span style=\"font-size: medium;\"><b>d) 120.\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\u00a0\u00a0\u00a0\u00a0\u00a0<\/b><\/span><\/span><\/span><\/p>\n<p><span style=\"color: #000000;\"><span style=\"font-family: Arial,serif;\"><span style=\"font-size: medium;\"><b>e) 140.\u00a0<\/b><\/span><\/span><\/span><\/p>\n<p><span style=\"color: #000000;\">\u00a0<\/span><\/p>\n<p><span style=\"color: #0000cc;\"><span style=\"font-family: Arial Black,serif;\"><span style=\"font-size: medium;\"><b>37-(FUVEST-SP)<\/b><\/span><\/span><\/span><\/p>\n<p><img loading=\"lazy\" decoding=\"async\" src=\"http:\/\/fisicaevestibular.com.br\/novo\/wp-content\/uploads\/migracao\/ondulatoria\/equacaoonda\/i_b8534983f3672ed3_html_b1985049.jpg\" alt=\"\" width=\"125\" height=\"35\" name=\"Picture 139\" align=\"BOTTOM\" border=\"0\" \/><\/p>\n<p><span style=\"color: #000000;\">\u00a0<span style=\"font-family: Arial,serif;\"><span style=\"font-size: medium;\"><b>Em um ponto fixo do espa\u00e7o, o campo el\u00e9trico de uma radia\u00e7\u00e3o eletromagn\u00e9tica tem sempre a mesma dire\u00e7\u00e3o e oscila no tempo, como mostra o gr\u00e1fico abaixo, que representa sua proje\u00e7\u00e3o\u00a0<\/b><\/span><\/span><\/span><span style=\"color: #000000;\"><span style=\"font-family: Arial,serif;\"><span style=\"font-size: medium;\"><i><b>E\u00a0<\/b><\/i><\/span><\/span><\/span><span style=\"color: #000000;\"><span style=\"font-family: Arial,serif;\"><span style=\"font-size: medium;\"><b>nessa dire\u00e7\u00e3o fixa;\u00a0<\/b><\/span><\/span><\/span><span style=\"color: #000000;\"><span style=\"font-family: Arial,serif;\"><span style=\"font-size: medium;\"><i><b>E\u00a0<\/b><\/i><\/span><\/span><\/span><span style=\"color: #000000;\"><span style=\"font-family: Arial,serif;\"><span style=\"font-size: medium;\"><b>\u00e9 positivo ou negativo conforme o sentido do campo.<\/b><\/span><\/span><\/span><\/p>\n<p><img loading=\"lazy\" decoding=\"async\" src=\"http:\/\/fisicaevestibular.com.br\/novo\/wp-content\/uploads\/migracao\/ondulatoria\/equacaoonda\/i_b8534983f3672ed3_html_7e1f0858.jpg\" alt=\"\" width=\"380\" height=\"168\" name=\"Picture 140\" align=\"BOTTOM\" border=\"0\" \/><span style=\"color: #000000;\">\u00a0\u00a0\u00a0<img loading=\"lazy\" decoding=\"async\" src=\"http:\/\/fisicaevestibular.com.br\/novo\/wp-content\/uploads\/migracao\/ondulatoria\/equacaoonda\/i_b8534983f3672ed3_html_d2d62b91.jpg\" alt=\"\" width=\"370\" height=\"170\" name=\"Picture 141\" align=\"BOTTOM\" border=\"0\" \/><\/span><\/p>\n<p><span style=\"color: #000000;\"><span style=\"font-family: Arial,serif;\"><span style=\"font-size: medium;\"><b>Consultando a tabela acima, que fornece os valores t\u00edpicos de frequ\u00eancia\u00a0<\/b><\/span><\/span><\/span><span style=\"color: #000000;\"><span style=\"font-family: Arial,serif;\"><span style=\"font-size: medium;\"><i><b>f\u00a0<\/b><\/i><\/span><\/span><\/span><span style=\"color: #000000;\"><span style=\"font-family: Arial,serif;\"><span style=\"font-size: medium;\"><b>para diferentes regi\u00f5es do espectro eletromagn\u00e9tico, e analisando o gr\u00e1fico de\u00a0<\/b><\/span><\/span><\/span><span style=\"color: #000000;\"><span style=\"font-family: Arial,serif;\"><span style=\"font-size: medium;\"><i><b>E<\/b><\/i><\/span><\/span><\/span><span style=\"color: #000000;\"><span style=\"font-family: Arial,serif;\"><span style=\"font-size: medium;\"><b>\u00a0em fun\u00e7\u00e3o do tempo, \u00e9 poss\u00edvel classificar essa radia\u00e7\u00e3o como<\/b><\/span><\/span><\/span><\/p>\n<p><img loading=\"lazy\" decoding=\"async\" src=\"http:\/\/fisicaevestibular.com.br\/novo\/wp-content\/uploads\/migracao\/ondulatoria\/equacaoonda\/i_b8534983f3672ed3_html_c8a66107.png\" alt=\"\" width=\"764\" height=\"16\" name=\"Picture 73\" align=\"BOTTOM\" border=\"0\" \/><\/p>\n<p><span style=\"color: #0000cc;\"><span style=\"font-family: Arial Black,serif;\"><span style=\"font-size: medium;\"><b>38-(UERJ-RJ)\u00a0<\/b><\/span><\/span><\/span><span style=\"color: #000000;\"><span style=\"font-family: Arial,serif;\"><span style=\"font-size: medium;\"><b>A sirene de uma f\u00e1brica produz sons com frequ\u00eancia igual a 2640 Hz.<\/b><\/span><\/span><\/span><\/p>\n<p><span style=\"color: #000000;\"><span style=\"font-family: Arial,serif;\"><span style=\"font-size: medium;\"><b>Determine o comprimento de onda do som produzido pela sirene em um dia cuja velocidade de propaga\u00e7\u00e3o das ondas sonoras no ar seja igual a 1.188 km\/h.<\/b><\/span><\/span><\/span><\/p>\n<p><span style=\"color: #000000;\">\u00a0<\/span><\/p>\n<p><span style=\"color: #0000cc;\"><span style=\"font-family: Arial Black,serif;\"><span style=\"font-size: medium;\"><b>39-(UFPR-PR)<\/b><\/span><\/span><\/span><b> <\/b><span style=\"color: #000000;\"><span style=\"font-family: Arial,serif;\"><span style=\"font-size: medium;\"><b>Uma fila de carros, igualmente espa\u00e7ados, de tamanhos e massas iguais faz a travessia de uma ponte com velocidades iguais e constantes, conforme mostra a figura abaixo. Cada vez que um carro entra na ponte, o impacto de seu peso provoca nela uma perturba\u00e7\u00e3o em forma de um pulso de onda. Esse pulso se propaga com velocidade de m\u00f3dulo 10 m\/s no sentido de A para B. Como resultado, a ponte oscila, formando uma onda estacion\u00e1ria com 3 ventres e 4 n\u00f3s.<\/b><\/span><\/span><\/span><img loading=\"lazy\" decoding=\"async\" src=\"http:\/\/fisicaevestibular.com.br\/novo\/wp-content\/uploads\/migracao\/ondulatoria\/equacaoonda\/i_b8534983f3672ed3_html_f2aba459.jpg\" alt=\"\" width=\"425\" height=\"155\" name=\"Picture 146\" align=\"LEFT\" border=\"0\" hspace=\"12\" \/><\/p>\n<p><span style=\"color: #000000;\"><span style=\"font-family: Arial,serif;\"><span style=\"font-size: medium;\"><b>Considerando que o fluxo de carros produza na ponte uma oscila\u00e7\u00e3o de 1 Hz, assinale a alternativa correta para o comprimento da ponte.<\/b><\/span><\/span><\/span><\/p>\n<p><img loading=\"lazy\" decoding=\"async\" src=\"http:\/\/fisicaevestibular.com.br\/novo\/wp-content\/uploads\/migracao\/ondulatoria\/equacaoonda\/i_b8534983f3672ed3_html_4111fd1.png\" alt=\"\" width=\"765\" height=\"18\" name=\"Picture 74\" align=\"BOTTOM\" border=\"0\" \/><\/p>\n<p><span style=\"color: #0000cc;\"><span style=\"font-family: Arial Black,serif;\"><span style=\"font-size: medium;\"><b>40-(UFPE-PE)<\/b><\/span><\/span><\/span><\/p>\n<p><img loading=\"lazy\" decoding=\"async\" src=\"http:\/\/fisicaevestibular.com.br\/novo\/wp-content\/uploads\/migracao\/ondulatoria\/equacaoonda\/i_b8534983f3672ed3_html_43346cc6.jpg\" alt=\"\" width=\"508\" height=\"128\" name=\"Picture 147\" align=\"BOTTOM\" border=\"0\" \/><\/p>\n<p><span style=\"color: #000000;\"><span style=\"font-family: Arial,serif;\"><span style=\"font-size: medium;\"><b>Na figura abaixo, mostra-se uma onda mec\u00e2nica se propagando em um el\u00e1stico submetido a um <\/b><\/span><\/span><\/span><\/p>\n<p align=\"CENTER\"><img loading=\"lazy\" decoding=\"async\" src=\"http:\/\/fisicaevestibular.com.br\/novo\/wp-content\/uploads\/migracao\/ondulatoria\/equacaoonda\/i_b8534983f3672ed3_html_c10b5d06.jpg\" alt=\"\" width=\"472\" height=\"210\" name=\"Picture 148\" align=\"BOTTOM\" border=\"0\" \/><\/p>\n<p><span style=\"color: #000000;\"><span style=\"font-family: Arial,serif;\"><span style=\"font-size: medium;\"><b>certa tens\u00e3o, na horizontal. A freq\u00fc\u00eancia da onda \u00e9 f = 740 Hz.<\/b><\/span><\/span><\/span><\/p>\n<p><span style=\"color: #000000;\"><span style=\"font-family: Arial,serif;\"><span style=\"font-size: medium;\"><b>Calcule a velocidade de propaga\u00e7\u00e3o da onda, em m\/s.<\/b><\/span><\/span><\/span><\/p>\n<p><span style=\"color: #000000;\">\u00a0<\/span><\/p>\n<p><span style=\"color: #0000cc;\"><span style=\"font-family: Arial Black,serif;\"><span style=\"font-size: medium;\"><b>41-(IFNMG-MG)<\/b><\/span><\/span><\/span><\/p>\n<p><img loading=\"lazy\" decoding=\"async\" src=\"http:\/\/fisicaevestibular.com.br\/novo\/wp-content\/uploads\/migracao\/ondulatoria\/equacaoonda\/i_b8534983f3672ed3_html_f81ee094.jpg\" alt=\"\" width=\"475\" height=\"146\" name=\"Picture 149\" align=\"BOTTOM\" border=\"0\" \/><\/p>\n<p><span style=\"color: #000000;\"><span style=\"font-family: Arial,serif;\"><span style=\"font-size: medium;\"><b>Algumas aranhas, valendo-se da tens\u00e3o superficial, podem caminhar sobre a superf\u00edcie livre da \u00e1gua. Para atrair eventuais presas, a aranha produz pequenas vibra\u00e7\u00f5es, gerando ondas superficiais, as quais apresentam comprimento de onda<\/b><\/span><\/span><\/span><img loading=\"lazy\" decoding=\"async\" src=\"http:\/\/fisicaevestibular.com.br\/novo\/wp-content\/uploads\/migracao\/ondulatoria\/equacaoonda\/i_b8534983f3672ed3_html_1eb296b7.jpg\" alt=\"\" width=\"592\" height=\"198\" name=\"Picture 150\" align=\"LEFT\" border=\"0\" hspace=\"12\" \/><\/p>\n<p><span style=\"color: #000000;\"><span style=\"font-family: Arial,serif;\"><span style=\"font-size: medium;\"><b>igual a 2,0 mm. O deslocamento vertical das part\u00edculas de \u00e1gua varia com o tempo (dado em milissegundos, ms) conforme o gr\u00e1fico apresentado na figura acima.<\/b><\/span><\/span><\/span><\/p>\n<p><span style=\"color: #000000;\"><span style=\"font-family: Arial,serif;\"><span style=\"font-size: medium;\"><b>Nessas condi\u00e7\u00f5es, o valor da velocidade de propaga\u00e7\u00e3o de tais ondas, expresso em cm\/s, est\u00e1 corretamente apresentado na alternativa:<\/b><\/span><\/span><\/span><\/p>\n<p><img loading=\"lazy\" decoding=\"async\" src=\"http:\/\/fisicaevestibular.com.br\/novo\/wp-content\/uploads\/migracao\/ondulatoria\/equacaoonda\/i_b8534983f3672ed3_html_62469a5a.png\" alt=\"\" width=\"765\" height=\"19\" name=\"Picture 75\" align=\"BOTTOM\" border=\"0\" \/><\/p>\n<p><span style=\"color: #000000;\">\u00a0<\/span><\/p>\n<p><span style=\"color: #0000cc;\"><span style=\"font-family: Arial Black,serif;\"><span style=\"font-size: medium;\"><b>42-(UNICAMP-SP)<\/b><\/span><\/span><\/span><\/p>\n<p><img loading=\"lazy\" decoding=\"async\" src=\"http:\/\/fisicaevestibular.com.br\/novo\/wp-content\/uploads\/migracao\/ondulatoria\/equacaoonda\/i_b8534983f3672ed3_html_ad38ae40.jpg\" alt=\"\" width=\"643\" height=\"128\" name=\"Picture 151\" align=\"BOTTOM\" border=\"0\" \/><\/p>\n<p><span style=\"color: #000000;\"><span style=\"font-family: Arial,serif;\"><span style=\"font-size: medium;\"><b>Nos \u00faltimos anos, o Brasil vem implantando em diversas cidades o\u00a0 sinal de televis\u00e3o digital. O sinal de televis\u00e3o \u00e9 transmitido<\/b><\/span><\/span><\/span><\/p>\n<p align=\"CENTER\"><img loading=\"lazy\" decoding=\"async\" src=\"http:\/\/fisicaevestibular.com.br\/novo\/wp-content\/uploads\/migracao\/ondulatoria\/equacaoonda\/i_b8534983f3672ed3_html_c4a3c510.jpg\" alt=\"\" width=\"435\" height=\"154\" name=\"Picture 152\" align=\"BOTTOM\" border=\"0\" \/><\/p>\n<p><span style=\"color: #000000;\"><span style=\"font-family: Arial,serif;\"><span style=\"font-size: medium;\"><b>atrav\u00e9s de antenas e cabos, por ondas eletromagn\u00e9ticas cuja velocidade no ar \u00e9 aproximadamente igual \u00e0 da luz no v\u00e1cuo.<\/b><\/span><\/span><\/span><\/p>\n<p><span style=\"color: #000000;\"><span style=\"font-family: Arial,serif;\"><span style=\"font-size: medium;\"><b>Um tipo de antena usada na recep\u00e7\u00e3o do sinal \u00e9 a log-peri\u00f3dica, representada na figura abaixo, na qual o comprimento das hastes met\u00e1licas de uma extremidade \u00e0 outra, L , \u00e9 vari\u00e1vel. A maior efici\u00eancia de recep\u00e7\u00e3o \u00e9 obtida quando\u00a0 L \u00e9 cerca de meio comprimento de onda da onda eletromagn\u00e9tica que transmite o sinal no ar ( L \u2248 \u03bb\/2 ). Encontre a menor frequ\u00eancia que a antena ilustrada na figura consegue sintonizar de forma eficiente, e marque na figura a haste correspondente.<\/b><\/span><\/span><\/span><\/p>\n<p align=\"CENTER\"><img loading=\"lazy\" decoding=\"async\" src=\"http:\/\/fisicaevestibular.com.br\/novo\/wp-content\/uploads\/migracao\/ondulatoria\/equacaoonda\/i_b8534983f3672ed3_html_9439339.jpg\" alt=\"\" width=\"510\" height=\"151\" name=\"Picture 153\" align=\"BOTTOM\" border=\"0\" \/><\/p>\n<p><span style=\"color: #000000;\">\u00a0<\/span><\/p>\n<p><span style=\"color: #0000cc;\"><span style=\"font-family: Arial Black,serif;\"><span style=\"font-size: medium;\"><b>43-(FUVEST-SP)<\/b><\/span><\/span><\/span><\/p>\n<p><span style=\"color: #000000;\">\u00a0<img loading=\"lazy\" decoding=\"async\" src=\"http:\/\/fisicaevestibular.com.br\/novo\/wp-content\/uploads\/migracao\/ondulatoria\/equacaoonda\/i_b8534983f3672ed3_html_1d8fcff6.jpg\" alt=\"\" width=\"733\" height=\"144\" name=\"Picture 154\" align=\"BOTTOM\" border=\"0\" \/><\/span><\/p>\n<p><span style=\"color: #000000;\"><span style=\"font-family: Arial,serif;\"><span style=\"font-size: medium;\"><b>A figura abaixo representa imagens instant\u00e2neas de duas cordas flex\u00edveis id\u00eanticas, C<\/b><\/span><\/span><\/span><span style=\"color: #000000;\"><sub><span style=\"font-family: Arial,serif;\"><span style=\"font-size: medium;\"><b>1<\/b><\/span><\/span><\/sub><\/span><span style=\"color: #000000;\"><span style=\"font-family: Arial,serif;\"><span style=\"font-size: medium;\"><b>\u00a0e C<\/b><\/span><\/span><\/span><span style=\"color: #000000;\"><sub><span style=\"font-family: Arial,serif;\"><span style=\"font-size: medium;\"><b>2<\/b><\/span><\/span><\/sub><\/span><span style=\"color: #000000;\"><span style=\"font-family: Arial,serif;\"><span style=\"font-size: medium;\"><b>, tracionadas por for\u00e7as diferentes, nas quais se propagam ondas.<\/b><\/span><\/span><\/span><img loading=\"lazy\" decoding=\"async\" src=\"http:\/\/fisicaevestibular.com.br\/novo\/wp-content\/uploads\/migracao\/ondulatoria\/equacaoonda\/i_b8534983f3672ed3_html_c7bba788.jpg\" alt=\"\" width=\"405\" height=\"145\" name=\"Picture 155\" align=\"LEFT\" border=\"0\" hspace=\"12\" \/><\/p>\n<p><span style=\"color: #000000;\"><span style=\"font-family: Arial,serif;\"><span style=\"font-size: medium;\"><b>Durante uma aula, estudantes afirmaram que as ondas nas cordas C<\/b><\/span><\/span><\/span><span style=\"color: #000000;\"><sub><span style=\"font-family: Arial,serif;\"><span style=\"font-size: medium;\"><b>1<\/b><\/span><\/span><\/sub><\/span><span style=\"color: #000000;\"><span style=\"font-family: Arial,serif;\"><span style=\"font-size: medium;\"><b>\u00a0e C<\/b><\/span><\/span><\/span><span style=\"color: #000000;\"><sub><span style=\"font-family: Arial,serif;\"><span style=\"font-size: medium;\"><b>2<\/b><\/span><\/span><\/sub><\/span><span style=\"color: #000000;\"><span style=\"font-family: Arial,serif;\"><span style=\"font-size: medium;\"><b>\u00a0t\u00eam:<\/b><\/span><\/span><\/span><\/p>\n<p><span style=\"color: #000000;\"><span style=\"font-family: Arial,serif;\"><span style=\"font-size: medium;\"><b>I. A mesma velocidade de propaga\u00e7\u00e3o.<\/b><\/span><\/span><\/span><\/p>\n<p><span style=\"color: #000000;\"><span style=\"font-family: Arial,serif;\"><span style=\"font-size: medium;\"><b>II. O mesmo comprimento de onda.<\/b><\/span><\/span><\/span><\/p>\n<p><span style=\"color: #000000;\"><span style=\"font-family: Arial,serif;\"><span style=\"font-size: medium;\"><b>III. A mesma frequ\u00eancia.<\/b><\/span><\/span><\/span><\/p>\n<p><span style=\"color: #000000;\"><span style=\"font-family: Arial,serif;\"><span style=\"font-size: medium;\"><b>Est\u00e1 correto apenas o que se afirma em<\/b><\/span><\/span><\/span><\/p>\n<p align=\"CENTER\"><img loading=\"lazy\" decoding=\"async\" src=\"http:\/\/fisicaevestibular.com.br\/novo\/wp-content\/uploads\/migracao\/ondulatoria\/equacaoonda\/i_b8534983f3672ed3_html_5b93d0e8.jpg\" alt=\"\" width=\"270\" height=\"120\" name=\"Picture 156\" align=\"BOTTOM\" border=\"0\" \/><\/p>\n<p><span style=\"color: #000000;\"><span style=\"font-family: Arial,serif;\"><span style=\"font-size: medium;\"><b>a) I. \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><\/span><\/p>\n<p><span style=\"color: #000000;\"><span style=\"font-family: Arial,serif;\"><span style=\"font-size: medium;\"><b>b) II. \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><\/span><\/p>\n<p><span style=\"color: #000000;\"><span style=\"font-family: Arial,serif;\"><span style=\"font-size: medium;\"><b>c) III. \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\u00a0\u00a0\u00a0<\/b><\/span><\/span><\/span><\/p>\n<p><span style=\"color: #000000;\"><span style=\"font-family: Arial,serif;\"><span style=\"font-size: medium;\"><b>d) I e II. \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\u00a0\u00a0\u00a0<\/b><\/span><\/span><\/span><\/p>\n<p><span style=\"color: #000000;\"><span style=\"font-family: Arial,serif;\"><span style=\"font-size: medium;\"><b>e) II e III.<\/b><\/span><\/span><\/span><\/p>\n<p><span style=\"color: #000000;\">\u00a0<\/span><\/p>\n<p><span style=\"color: #0000cc;\"><span style=\"font-family: Arial Black,serif;\"><span style=\"font-size: medium;\"><b>44-(COL\u00c9GIO NAVAL)<\/b><\/span><\/span><\/span><\/p>\n<p><img loading=\"lazy\" decoding=\"async\" src=\"http:\/\/fisicaevestibular.com.br\/novo\/wp-content\/uploads\/migracao\/ondulatoria\/equacaoonda\/i_b8534983f3672ed3_html_879a7069.jpg\" alt=\"\" width=\"574\" height=\"148\" name=\"Picture 157\" align=\"BOTTOM\" border=\"0\" \/><\/p>\n<p><span style=\"color: #000000;\"><span style=\"font-family: Arial,serif;\"><span style=\"font-size: medium;\"><b>Analise\u00a0 a\u00a0 figura\u00a0 a\u00a0 seguir.<\/b><\/span><\/span><\/span><\/p>\n<p align=\"CENTER\"><img loading=\"lazy\" decoding=\"async\" src=\"http:\/\/fisicaevestibular.com.br\/novo\/wp-content\/uploads\/migracao\/ondulatoria\/equacaoonda\/i_b8534983f3672ed3_html_fcc3aeeb.png\" alt=\"\" width=\"616\" height=\"192\" name=\"Picture 76\" align=\"BOTTOM\" border=\"0\" \/><\/p>\n<p><span style=\"color: #000000;\"><span style=\"font-family: Arial,serif;\"><span style=\"font-size: medium;\"><b>Uma\u00a0 pessoa\u00a0 encontra-se\u00a0 parada\u00a0 em\u00a0 um\u00a0 ponto\u00a0 P, distante\u00a0 de\u00a0 um obst\u00e1culo\u00a0 e\u00a0 de\u00a0 uma\u00a0 fonte\u00a0 sonora\u00a0 que\u00a0 emite\u00a0 ondas\u00a0 conforme\u00a0 a configura\u00e7\u00e3o\u00a0 mostrada\u00a0 na\u00a0 figura\u00a0 acima.\u00a0 Um\u00a0 som\u00a0 emitido\u00a0 pela fonte\u00a0 no\u00a0 instante\u00a0 t<\/b><\/span><\/span><\/span><span style=\"color: #000000;\"><sub><span style=\"font-family: Arial,serif;\"><span style=\"font-size: medium;\"><b>o<\/b><\/span><\/span><\/sub><\/span><span style=\"color: #000000;\"><span style=\"font-family: Arial,serif;\"><span style=\"font-size: medium;\"><b>\u00a0= Os\u00a0 passa\u00a0 pelo\u00a0 ponto\u00a0 P\u00a0 no\u00a0 instante t<\/b><\/span><\/span><\/span><span style=\"color: #000000;\"><sub><span style=\"font-family: Arial,serif;\"><span style=\"font-size: medium;\"><b>1<\/b><\/span><\/span><\/sub><\/span><span style=\"color: #000000;\"><span style=\"font-family: Arial,serif;\"><span style=\"font-size: medium;\"><b>\u00a0= 0,5 s\u00a0 e\u00a0 retorna\u00a0 ao\u00a0 ouvido\u00a0 da\u00a0 pessoa\u00a0 no\u00a0 instante t<\/b><\/span><\/span><\/span><span style=\"color: #000000;\"><sub><span style=\"font-family: Arial,serif;\"><span style=\"font-size: medium;\"><b>2\u00a0<\/b><\/span><\/span><\/sub><\/span><span style=\"color: #000000;\"><span style=\"font-family: Arial,serif;\"><span style=\"font-size: medium;\"><b>=2,5s, ap\u00f3s\u00a0 ter\u00a0 colidido\u00a0 com\u00a0 o\u00a0 obst\u00e1culo.\u00a0 Considerando\u00a0 a velocidade\u00a0 do\u00a0 som\u00a0 no\u00a0 ar\u00a0 como\u00a0 sendo\u00a0 constante\u00a0 e\u00a0 igual\u00a0 a 340m\/ s, \u00e9\u00a0 correto\u00a0 afirmar\u00a0 que\u00a0 o\u00a0 comprimento\u00a0 de\u00a0 onda, a\u00a0 frequ\u00eancia\u00a0 da\u00a0 fonte\u00a0 emissora\u00a0 e\u00a0 a\u00a0 dist\u00e2ncia\u00a0 da\u00a0 pessoa\u00a0 at\u00e9\u00a0 o obst\u00e1culo\u00a0 valem, respectivamente:<\/b><\/span><\/span><\/span><\/p>\n<p><span style=\"color: #000000;\"><span style=\"font-family: Arial,serif;\"><span style=\"font-size: medium;\"><b>(A) \u03bb=0,17m; f =1000Hz; d = 170m\u00a0\u00a0\u00a0\u00a0\u00a0 <\/b><\/span><\/span><\/span><\/p>\n<p><span style=\"color: #000000;\"><span style=\"font-family: Arial,serif;\"><span style=\"font-size: medium;\"><b>(B) \u03bb = 0,34m; f =1000Hz; d=340m.\u00a0\u00a0\u00a0\u00a0\u00a0 <\/b><\/span><\/span><\/span><\/p>\n<p><span style=\"color: #000000;\"><span style=\"font-family: Arial,serif;\"><span style=\"font-size: medium;\"><b>(C)\u00a0 \u03bb =0,34m; f=2000Hz; d=170m<\/b><\/span><\/span><\/span><\/p>\n<p><span style=\"color: #000000;\"><span style=\"font-family: Arial,serif;\"><span style=\"font-size: medium;\"><b>(D) \u03bb =0,51m; f=1000Hz; d=340m\u00a0\u00a0\u00a0 \u00a0\u00a0\u00a0\u00a0<\/b><\/span><\/span><\/span><\/p>\n<p><span style=\"color: #000000;\"><span style=\"font-family: Arial,serif;\"><span style=\"font-size: medium;\"><b>(E)\u00a0 \u03bb =0, 51m; f =2000Hz; d=680m<\/b><\/span><\/span><\/span><\/p>\n<p><span style=\"color: #000000;\">\u00a0<\/span><\/p>\n<h3><span style=\"color: #000080;\"><a style=\"color: #000080;\" title=\"Resolu\u00e7\u00e3o comentada dos exerc\u00edcios de vestibulares sobre Equa\u00e7\u00e3o da Onda\" href=\"http:\/\/fisicaevestibular.com.br\/novo\/ondulatoria\/ondas\/equacao-da-onda-equacao-fundamental-da-ondulatoria\/resolucao-comentada-dos-exercicios-de-vestibulares-sobre-equacao-da-onda\/\">Confira as resolu\u00e7\u00f5es comentadas<\/a><\/span><\/h3>\n","protected":false},"excerpt":{"rendered":"<p>Exerc\u00edcios de vestibulares com resolu\u00e7\u00f5es comentadas sobre Equa\u00e7\u00e3o da onda (Equa\u00e7\u00e3o fundamental da ondulat\u00f3ria) 01-(UFSM) &#8220;Os habitantes dos pinheirais formados por arauc\u00e1rias come\u00e7aram a produzir cer\u00e2micas e aperfei\u00e7oaram seus instrumentos de trabalho.&#8221; Para descascar e moer cereais, as \u00edndias usavam um pil\u00e3o de pedra. Se uma \u00edndia batesse nos cereais 20 vezes por minuto, a freq\u00fc\u00eancia das batidas, em Hz,<\/p>\n","protected":false},"author":1,"featured_media":0,"parent":2428,"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-2430","page","type-page","status-publish","hentry"],"aioseo_notices":[],"_links":{"self":[{"href":"https:\/\/fisicaevestibular.com.br\/novo\/wp-json\/wp\/v2\/pages\/2430","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=2430"}],"version-history":[{"count":4,"href":"https:\/\/fisicaevestibular.com.br\/novo\/wp-json\/wp\/v2\/pages\/2430\/revisions"}],"predecessor-version":[{"id":10914,"href":"https:\/\/fisicaevestibular.com.br\/novo\/wp-json\/wp\/v2\/pages\/2430\/revisions\/10914"}],"up":[{"embeddable":true,"href":"https:\/\/fisicaevestibular.com.br\/novo\/wp-json\/wp\/v2\/pages\/2428"}],"wp:attachment":[{"href":"https:\/\/fisicaevestibular.com.br\/novo\/wp-json\/wp\/v2\/media?parent=2430"}],"curies":[{"name":"wp","href":"https:\/\/api.w.org\/{rel}","templated":true}]}}