{"id":4472,"date":"2019-05-24T02:35:05","date_gmt":"2019-05-24T02:35:05","guid":{"rendered":"http:\/\/fisicaevestibular.com.br\/novo\/?page_id=4472"},"modified":"2024-07-11T02:51:24","modified_gmt":"2024-07-11T02:51:24","slug":"afa-2018-2019","status":"publish","type":"page","link":"https:\/\/fisicaevestibular.com.br\/novo\/universidades-2019\/afa-2018-2019\/","title":{"rendered":"AFA – 2018\/2019"},"content":{"rendered":"

AFA – 2018\/2019<\/b><\/span><\/span><\/span><\/p>\n

<\/p>\n

Academia da For\u00e7a A\u00e9rea\u00a0(AFA)\u00a0\u00e9 um estabelecimento de ensino em n\u00edvel superior da\u00a0<\/b><\/span><\/span><\/span>For\u00e7a A\u00e9rea Brasileira<\/b><\/span><\/span><\/span><\/a>, <\/b><\/span><\/span><\/span>situado em\u00a0<\/b><\/span><\/span><\/span>Pirassununga<\/a>,\u00a0Estado de S\u00e3o Paulo<\/a>\u00a0e reconhecido pelo\u00a0Minist\u00e9rio da Educa\u00e7\u00e3o<\/a><\/b><\/span><\/span><\/span>.<\/b><\/span><\/span><\/span><\/p>\n

Integra o sistema de\u00a0<\/b><\/span><\/span><\/span>forma\u00e7\u00e3o e aperfei\u00e7oamento\u00a0<\/b><\/span><\/span><\/span>de pessoal do\u00a0<\/b><\/span><\/span><\/span>Comand<\/b><\/span><\/span><\/span><\/a>o<\/b><\/span><\/span><\/span><\/p>\n

o da Aeron\u00e1utica<\/b><\/span><\/span><\/span><\/a>\u00a0(COMAER)<\/b><\/span><\/span><\/span>e est\u00e1 subordinada ao Departamento de Ensino<\/b><\/span><\/span><\/span>\u00a0<\/b><\/span><\/span><\/span>(DEPENS) da\u00a0<\/b><\/span><\/span><\/span>For\u00e7a A\u00e9rea Brasileira<\/b><\/span><\/span><\/span><\/a>\u00a0(FAB<\/b><\/span><\/span><\/span>.<\/b><\/span><\/span><\/span><\/p>\n

Tem como finalidade a forma\u00e7\u00e3o de oficiais da ativa para os quadros de\u00a0aviadores,\u00a0intendentes<\/a>\u00a0e de infantaria da FAB.<\/b><\/span><\/span><\/span><\/p>\n

\u00c9 considerada uma das tr\u00eas melhores escolas de forma\u00e7\u00e3o de pilotos militares do mundo\u00a0<\/b><\/span><\/span><\/span>e forma n\u00e3o apenas\u00a0pilotos militares para a For\u00e7a A\u00e9rea Brasileira<\/b><\/span><\/span><\/span>,\u00a0<\/b><\/span><\/span><\/span>como tamb\u00e9m para\u00a0For\u00e7as A\u00e9reas de pa\u00edses da Am\u00e9rica Latina, \u00c1frica, \u00c1sia e Europa, mediante acordos internacionais de coopera\u00e7\u00e3o.<\/b><\/span><\/span><\/span><\/p>\n

O\u00a0ingresso na AFA ocorre mediante a aprova\u00e7\u00e3o em concursos p\u00fablicos anuais <\/b><\/span><\/span><\/span>de admiss\u00e3o, de \u00e2mbito nacional<\/b><\/span><\/span><\/span>.\u00a0<\/b><\/span><\/span><\/span>As<\/b><\/span><\/span><\/span>\u00a0<\/b><\/span><\/span><\/span>informa\u00e7\u00f5es\u00a0<\/b><\/span><\/span><\/span>sobre esses concursos est\u00e3o<\/b><\/span><\/span><\/span>\u00a0<\/b><\/span><\/span><\/span>dispon\u00edveis\u00a0<\/b><\/span><\/span><\/span>em todas as\u00a0<\/b><\/span><\/span><\/span>organiza\u00e7\u00f5es do Comando da Aeron\u00e1utica<\/b><\/span><\/span><\/span>.<\/b><\/span><\/span><\/span><\/p>\n

Atualmente, a Academia forma<\/b><\/span><\/span><\/span>\u00a0<\/b><\/span><\/span><\/span>cadetes dos seguintes cursos:<\/b><\/span><\/span><\/span><\/p>\n

\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0<\/span>Curso de Forma\u00e7\u00e3o de Oficiais de Infantaria da Aeron\u00e1utica (CFOINF)<\/b><\/span><\/span><\/span><\/p>\n

\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0<\/span>Curso de Forma\u00e7\u00e3o de Oficiais Aviadores (CFOAV)<\/b><\/span><\/span><\/span><\/p>\n

\u00a0\u00a0\u00a0\u00a0\u00a0\u00a0<\/span>Curso de Forma\u00e7\u00e3o de Oficiais Intendentes (CFOINT).<\/b><\/span><\/span><\/span><\/p>\n

Al\u00e9m disso<\/b><\/span><\/span><\/span>,\u00a0<\/b><\/span><\/span><\/span>todos os cadetes da Academia<\/b><\/span><\/span><\/span>, ao final do curso, recebem o\u00a0<\/b><\/span><\/span><\/span>t\u00edtulo de bachar\u00e9is em Administra\u00e7\u00e3o, com \u00eanfase\u00a0 em Administra\u00e7\u00e3o P\u00fablica.<\/b><\/span><\/span><\/span><\/p>\n

01 \u2013 (AFA-018\/019)<\/b><\/span><\/span><\/span><\/p>\n

<\/p>\n

Tr\u00eas part\u00edculas, A, B e C, movimentam-se, com velocidades constantes,<\/b><\/span><\/span><\/span> ao <\/b><\/span><\/span><\/span>longo<\/b><\/span><\/span><\/span> de uma <\/b><\/span><\/span><\/span>mesma dire\u00e7\u00e3o.<\/b><\/span><\/span><\/span> No <\/b><\/span><\/span><\/span>instante inicial, t<\/b><\/span><\/span><\/span>0<\/b><\/span><\/span><\/sub><\/span> = 0, a dist\u00e2ncia entre A e B vale x, e entre B e C vale y, <\/b><\/span><\/span><\/span>conforme indica a <\/b><\/span><\/span><\/span>figura a seguir.<\/b><\/span><\/span><\/span><\/p>\n

<\/p>\n

Em t = 2 s, a part\u00edcula A cruza com a part\u00edcula B.<\/b><\/span><\/span><\/span> <\/b>Em t = 3 s, a part\u00edcula A cruza com a part\u00edcula C.<\/b><\/span><\/span><\/span> <\/b><\/p>\n

A part\u00edcula C alcan\u00e7ar\u00e1 a part\u00edcula B no instante dado pela rela\u00e7\u00e3o<\/b><\/span><\/span><\/span><\/p>\n

<\/p>\n

02 \u2013 (AFA-018\/019)<\/b><\/span><\/span><\/span><\/p>\n

<\/p>\n

Uma <\/b><\/span><\/span><\/span>part\u00edcula, de massa 1 kg, descreve um movimento circular uniformemente variado, de raio 2,25 m, iniciando-o a partir do repouso no instante t0 = 0.<\/b><\/span><\/span><\/span> Em <\/b><\/span><\/span><\/span>t = 2 s,<\/b><\/span><\/span><\/span> o <\/b><\/span><\/span><\/span>m\u00f3dulo de sua velocidade vetorial (v) r \u00e9 de 6 m\/s, <\/b><\/span><\/span><\/span>conforme<\/b><\/span><\/span><\/span> figura abaixo. <\/b><\/span><\/span><\/span><\/p>\n

<\/p>\n

A <\/b><\/span><\/span><\/span>intensidade da for\u00e7a resultante sobre a part\u00edcula, no instante t = 1 s, em N<\/b><\/span><\/span><\/span>, vale<\/b><\/span><\/span><\/span><\/p>\n

a) <\/b><\/span><\/span><\/span>1 <\/b><\/span><\/span><\/span>b) <\/b><\/span><\/span><\/span>5 <\/b><\/span><\/span><\/span>c) <\/b><\/span><\/span><\/span>9 <\/b><\/span><\/span><\/span>d) <\/b><\/span><\/span><\/span>12 <\/b><\/span><\/span><\/span><\/p>\n

03 \u2013 (AFA-018\/019)<\/b><\/span><\/span><\/span><\/p>\n

<\/p>\n

Uma esfera, de dimens\u00f5es desprez\u00edveis,<\/b><\/span><\/span><\/span> <\/b>sob a\u00e7\u00e3o de um campo gravitacional constante, <\/b><\/span><\/span><\/span>est\u00e1 <\/b><\/span><\/span><\/span>inicialmente equilibrada na vertical por uma mola.<\/b><\/span><\/span><\/span> A <\/b><\/span><\/span><\/span>mola \u00e9 ideal <\/b><\/span><\/span><\/span>e se encontra com <\/b><\/span><\/span><\/span>uma deforma\u00e7\u00e3o x,<\/b><\/span><\/span><\/span> conforme ilustrado na <\/b><\/span><\/span><\/span>figura 1. <\/b><\/span><\/span><\/span>O <\/b><\/span><\/span><\/span>sistema esfera-mola \u00e9 posto, <\/b><\/span><\/span><\/span>em seguida, a <\/b><\/span><\/span><\/span>deslizar sobre uma superf\u00edcie horizontal, com velocidade constante,<\/b><\/span><\/span><\/span> conforme indicado na <\/b><\/span><\/span><\/span>figura 2.<\/b><\/span><\/span><\/span><\/p>\n

<\/p>\n

Nessa situa\u00e7\u00e3o, quando o \u00e2ngulo de inclina\u00e7\u00e3o da mola \u00e9 \u03b8 ,<\/b><\/span><\/span><\/span> em <\/b><\/span><\/span><\/span>rela\u00e7\u00e3o \u00e0 horizontal, <\/b><\/span><\/span><\/span>sua <\/b><\/span><\/span><\/span>deforma\u00e7\u00e3o \u00e9 y<\/b><\/span><\/span><\/span>. <\/b><\/span><\/span><\/span><\/p>\n

Nessas condi\u00e7\u00f5es, <\/b><\/span><\/span><\/span>o <\/b><\/span><\/span><\/span>coeficiente de atrito cin\u00e9tico entre a esfera e a superf\u00edcie horizontal vale <\/b><\/span><\/span><\/span><\/p>\n

a) \u00b5 = b) <\/b><\/span><\/span><\/span> <\/b>c) <\/b><\/span><\/span><\/span> <\/b>d) <\/b><\/span><\/span><\/span><\/p>\n

04 \u2013 (AFA-018\/019)<\/b><\/span><\/span><\/span><\/p>\n

<\/p>\n

Um <\/b><\/span><\/span><\/span>arm\u00e1rio, cujas dimens\u00f5es est\u00e3o indicadas <\/b><\/span><\/span><\/span>na figura abaixo, <\/b><\/span><\/span><\/span>est\u00e1 em repouso sobre um assoalho plano e horizontal.<\/b><\/span><\/span><\/span><\/p>\n

<\/p>\n

Uma pessoa aplica uma for\u00e7a F constante e horizontal<\/b><\/span><\/span><\/span>, cuja <\/b><\/span><\/span><\/span>linha de a\u00e7\u00e3o e o centro de massa (CM) do arm\u00e1rio est\u00e3o num mesmo plano vertical.<\/b><\/span><\/span><\/span> <\/b><\/p>\n

Sendo o <\/b><\/span><\/span><\/span>coeficiente de atrito est\u00e1tico entre o assoalho e o piso do arm\u00e1rio igual a \u00b5 <\/b><\/span><\/span><\/span>e estando o <\/b><\/span><\/span><\/span>arm\u00e1rio na imin\u00eancia de escorregar, <\/b><\/span><\/span><\/span>a <\/b><\/span><\/span><\/span>altura m\u00e1xima H na qual a pessoa poder\u00e1 aplicar a for\u00e7a para que a base do arm\u00e1rio continue completamente em contato com o assoalho <\/b><\/span><\/span><\/span>\u00e9<\/b><\/span><\/span><\/span><\/p>\n

<\/p>\n

05 \u2013 (AFA-018\/019)<\/b><\/span><\/span><\/span><\/p>\n

<\/p>\n

<\/p>\n

<\/p>\n

<\/p>\n

<\/p>\n

<\/p>\n

<\/a> 06 \u2013 (AFA-018\/019)<\/b><\/span><\/span><\/span><\/p>\n

<\/p>\n

A <\/b><\/span><\/span><\/span>montagem da figura a seguir ilustra a descida de uma part\u00edcula 1 <\/b><\/span><\/span><\/span>ao <\/b><\/span><\/span><\/span>longo de um trilho curvil\u00edneo. <\/b><\/span><\/span><\/span><\/p>\n

Partindo <\/b><\/span><\/span><\/span>do repouso em A, a part\u00edcula chega ao ponto B,<\/b><\/span><\/span><\/span> que est\u00e1 a uma <\/b><\/span><\/span><\/span>dist\u00e2ncia vertical H abaixo do ponto A, <\/b><\/span><\/span><\/span>de onde, ent\u00e3o, <\/b><\/span><\/span><\/span>\u00e9 lan\u00e7ada obliquamente, com um \u00e2ngulo de 45\u00ba com a horizontal.<\/b><\/span><\/span><\/span><\/p>\n

<\/p>\n

A <\/b><\/span><\/span><\/span>part\u00edcula, agora, descreve uma trajet\u00f3ria parab\u00f3lica <\/b><\/span><\/span><\/span>e, <\/b><\/span><\/span><\/span>ao atingir seu ponto de altura m\u00e1xima, nessa trajet\u00f3ria, ela se acopla a uma part\u00edcula 2, sofrendo, portanto, uma colis\u00e3o inel\u00e1stica. <\/b><\/span><\/span><\/span>Essa <\/b><\/span><\/span><\/span>segunda part\u00edcula possui o dobro de massa da primeira, <\/b><\/span><\/span><\/span>est\u00e1 em <\/b><\/span><\/span><\/span>repouso antes da colis\u00e3o e est\u00e1 presa ao teto por um fio ideal, de comprimento maior que H, <\/b><\/span><\/span><\/span>constituindo, assim, um <\/b><\/span><\/span><\/span>p\u00eandulo. Considerando<\/b><\/span><\/span><\/span> que <\/b><\/span><\/span><\/span>apenas na colis\u00e3o atuaram for\u00e7as dissipativas, <\/b><\/span><\/span><\/span>e que o <\/b><\/span><\/span><\/span>campo gravitacional local \u00e9 constante.<\/b><\/span><\/span><\/span> O <\/b><\/span><\/span><\/span>sistema formado pelas part\u00edculas 1 e 2 atinge uma altura m\u00e1xima h igual <\/b><\/span><\/span><\/span>a <\/b><\/span><\/span><\/span><\/p>\n

<\/p>\n

Resolu\u00e7\u00e3o comentada das quest\u00f5es de F\u00edsica da Academia da For\u00e7a A\u00e9rea \u2013 AFA \u2013 2018\/19<\/span><\/span><\/span><\/p>\n

01-<\/span><\/span><\/span><\/p>\n

<\/p>\n

R- A<\/b><\/span><\/span><\/span><\/p>\n

02-<\/span><\/span><\/span><\/p>\n

Acelera\u00e7\u00e3o tangencial<\/b><\/span><\/span><\/span><\/p>\n

<\/p>\n

Acelera\u00e7\u00e3o centr\u00edpeta<\/span><\/span><\/span><\/p>\n

<\/p>\n

Acelera\u00e7\u00e3o total<\/span><\/span><\/span><\/p>\n

<\/p>\n

<\/p>\n

R- B <\/b><\/span><\/span><\/span><\/p>\n

03-<\/span><\/span><\/span><\/p>\n

<\/p>\n

<\/p>\n

<\/p>\n

R- A<\/b><\/span><\/span><\/span><\/p>\n

04-<\/span><\/span><\/span><\/p>\n

<\/p>\n

Equil\u00edbrio na vertical (transla\u00e7\u00e3o)<\/b><\/span><\/span><\/span> <\/b> <\/b>N = P <\/b><\/span><\/span><\/span> <\/b> <\/b>equil\u00edbrio na horizontal <\/b><\/span><\/span><\/span> F = F<\/b><\/span><\/span><\/span>at<\/b><\/span><\/span><\/sub><\/span> <\/b> <\/b>F<\/b><\/span><\/span><\/span> = \u00b5.N <\/b><\/span><\/span><\/span>= \u00b5.P.<\/b><\/span><\/span><\/span><\/p>\n

Como o <\/b><\/span><\/span><\/span>arm\u00e1rio n\u00e3o pode perder contato com o solo, <\/b><\/span><\/span><\/span>ele deve estar na <\/b><\/span><\/span><\/span>imin\u00eancia de girar <\/b><\/span><\/span><\/span>sobre a<\/b><\/span><\/span><\/span><\/p>\n

<\/p>\n

quina direita onde vamos colocar o polo <\/b><\/span><\/span><\/span>e, veja que <\/b><\/span><\/span><\/span>somente as for\u00e7as <\/b><\/span><\/span><\/span> e <\/b><\/span><\/span><\/span> influem na tend\u00eancia de rota\u00e7\u00e3o <\/b><\/span><\/span><\/span>(para que ele n\u00e3o gire no sentido anti-hor\u00e1rio, j\u00e1 que a tend\u00eancia de rota\u00e7\u00e3o deve ser no sentido hor\u00e1rio).<\/b><\/span><\/span><\/span><\/p>\n

<\/p>\n

R- B<\/b><\/span><\/span><\/span><\/p>\n

05- <\/span><\/span><\/span><\/p>\n

Veja nas <\/b><\/span><\/span><\/span>figuras abaixo como varia o comportamento dos dois tipos de lentes de acordo com os valores dos \u00edndices de refra\u00e7\u00e3o do meio n<\/b><\/span><\/span><\/span>m <\/b><\/span><\/span><\/sub><\/span> e da lente n<\/b><\/span><\/span><\/span><\/p>\n

<\/p>\n

Resolu\u00e7\u00e3o<\/b><\/span><\/span><\/span>: <\/b><\/span><\/span><\/span>Na figura 1,<\/b><\/span><\/span><\/span> com <\/b><\/span><\/span><\/span>rela\u00e7\u00e3o ao objeto<\/b><\/span><\/span><\/span> a <\/b><\/span><\/span><\/span>lente 1 deve ser convergente, pois n<\/b><\/span><\/span><\/span>m<\/b><\/span><\/span><\/sub><\/span> > n<\/b><\/span><\/span><\/span>L <\/b><\/span><\/span><\/sub><\/span> <\/b>j\u00e1 que <\/b><\/span><\/span><\/span>lentes convergentes fornecem imagens maiores e invertidas do objeto (dependendo da posi\u00e7\u00e3o do mesmo). Na figura 2, <\/b><\/span><\/span><\/span>quando <\/b><\/span><\/span><\/span>n<\/b><\/span><\/span><\/span>m<\/b><\/span><\/span><\/sub><\/span> > n<\/b><\/span><\/span><\/span>L<\/b><\/span><\/span><\/sub><\/span> <\/b>a <\/b><\/span><\/span><\/span>imagem \u00e9 menor e direita <\/b><\/span><\/span><\/span>e a <\/b><\/span><\/span><\/span>lente \u00e9 divergente pois para qualquer posi\u00e7\u00e3o do objeto a imagem fornecida por lente divergente \u00e9 sempre menor e direita em rela\u00e7\u00e3o ao objeto.<\/b><\/span><\/span><\/span><\/p>\n

Ent\u00e3o, <\/b><\/span><\/span><\/span>para n\u2019 < n<\/b><\/span><\/span><\/span>1<\/b><\/span><\/span><\/sub><\/span> e n\u2019 < n<\/b><\/span><\/span><\/span>2<\/b><\/span><\/span><\/sub><\/span>,<\/b><\/span><\/span><\/span> a <\/b><\/span><\/span><\/span>situa\u00e7\u00e3o se inverte e a lente 1 ser\u00e1 divergente e a lente 2 ser\u00e1 convergente.<\/b><\/span><\/span><\/span> Como <\/b><\/span><\/span><\/span>lente divergente s\u00f3 forma imagem direita e menor (1<\/b><\/span><\/span><\/span>a<\/b><\/span><\/span><\/sup><\/span> figura da alternativa),<\/b><\/span><\/span><\/span> e a <\/b><\/span><\/span><\/span>lente convergente forma imagem invertida e menor <\/b><\/span><\/span><\/span> com o <\/b><\/span><\/span><\/span>objeto localizado antes do centro de curvatura, a \u00fanica op\u00e7\u00e3o poss\u00edvel \u00e9 a letra A.<\/b><\/span><\/span><\/span><\/p>\n

R- A<\/span><\/span><\/span><\/p>\n

06-<\/span><\/span><\/span><\/p>\n

C\u00e1lculo da velocidade V<\/b><\/span><\/span><\/span>B<\/b><\/span><\/span><\/sub><\/span> com que a <\/b><\/span><\/span><\/span>part\u00edcula 1 de massa m<\/b><\/span><\/span><\/span> que <\/b><\/span><\/span><\/span>partiu do repouso em A <\/b><\/span><\/span><\/span>(V<\/b><\/span><\/span><\/span>a<\/b><\/span><\/span><\/sub><\/span> = 0) na <\/b><\/span><\/span><\/span>altura H chega em B de altura nula e velocidade V<\/b><\/span><\/span><\/span>B,<\/b><\/span><\/span><\/sub><\/span> <\/b>pelo <\/b><\/span><\/span><\/span>teorema da conserva\u00e7\u00e3o da energia mec\u00e2nica. <\/b><\/span><\/span><\/span><\/p>\n

<\/p>\n

Lan\u00e7amento obl\u00edquo<\/b><\/span><\/span><\/span><\/p>\n

<\/p>\n

<\/p>\n

C\u00e1lculo<\/b><\/span><\/span><\/span> da <\/b><\/span><\/span><\/span>velocidade das esferas 1 e 2 de massa <\/b><\/span><\/span><\/span>(M = m + 2m= <\/b><\/span><\/span><\/span>3m<\/b><\/span><\/span><\/span>) que se<\/b><\/span><\/span><\/span> movem juntas ap\u00f3s o choque <\/b><\/span><\/span><\/span>com <\/b><\/span><\/span><\/span>velocidade comum V\u2019 <\/b><\/span><\/span><\/span>(colis\u00e3o inel\u00e1stica) <\/b><\/span><\/span><\/span>pela conserva\u00e7\u00e3o da quantidade de movimento.<\/b><\/span><\/span><\/span><\/p>\n

<\/p>\n

Agora <\/b><\/span><\/span><\/span>vamos calcular a altura m\u00e1xima atingida h <\/b><\/span><\/span><\/span>pelo <\/b><\/span><\/span><\/span>sistema formado pelas duas 1 e 2 <\/b><\/span><\/span><\/span>utilizando teorema da <\/b><\/span><\/span><\/span>conserva\u00e7\u00e3o da energia mec\u00e2nica quando se <\/b><\/span><\/span><\/span>deslocam <\/b><\/span><\/span><\/span>juntas do ponto P ao ponto Q.<\/b><\/span><\/span><\/span><\/p>\n

\"AFA\"<\/p>\n

R- D<\/b><\/span><\/span><\/span><\/p>\n

 <\/p>\n

Clique aqui para ver sobre o tema!<\/a><\/p>\n

Confira as v\u00eddeo aulas!<\/a><\/p>\n","protected":false},"excerpt":{"rendered":"

AFA – 2018\/2019 Academia da For\u00e7a A\u00e9rea\u00a0(AFA)\u00a0\u00e9 um estabelecimento de ensino em n\u00edvel superior da\u00a0For\u00e7a A\u00e9rea Brasileira, situado em\u00a0Pirassununga,\u00a0Estado de S\u00e3o Paulo\u00a0e reconhecido pelo\u00a0Minist\u00e9rio da Educa\u00e7\u00e3o. Integra o sistema de\u00a0forma\u00e7\u00e3o e aperfei\u00e7oamento\u00a0de pessoal do\u00a0Comando o da Aeron\u00e1utica\u00a0(COMAER)e est\u00e1 subordinada ao Departamento de Ensino\u00a0(DEPENS) da\u00a0For\u00e7a A\u00e9rea Brasileira\u00a0(FAB. Tem como finalidade a forma\u00e7\u00e3o de oficiais da ativa para os quadros de\u00a0aviadores,\u00a0intendentes\u00a0e de<\/p>\n","protected":false},"author":1,"featured_media":0,"parent":4337,"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-4472","page","type-page","status-publish","hentry"],"aioseo_notices":[],"_links":{"self":[{"href":"https:\/\/fisicaevestibular.com.br\/novo\/wp-json\/wp\/v2\/pages\/4472","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=4472"}],"version-history":[{"count":3,"href":"https:\/\/fisicaevestibular.com.br\/novo\/wp-json\/wp\/v2\/pages\/4472\/revisions"}],"predecessor-version":[{"id":10259,"href":"https:\/\/fisicaevestibular.com.br\/novo\/wp-json\/wp\/v2\/pages\/4472\/revisions\/10259"}],"up":[{"embeddable":true,"href":"https:\/\/fisicaevestibular.com.br\/novo\/wp-json\/wp\/v2\/pages\/4337"}],"wp:attachment":[{"href":"https:\/\/fisicaevestibular.com.br\/novo\/wp-json\/wp\/v2\/media?parent=4472"}],"curies":[{"name":"wp","href":"https:\/\/api.w.org\/{rel}","templated":true}]}}