2. <latexit sha1_base64="ZHNFm7aul4+awZu3cbU6m4LJoVo=">AAACCnicbVDLSsNAFJ3UV62vqEs3g0VwVRIRdFl047KCtYWmhMl02g6dR5iZFEPI1o2/4saFgrj1C9z5N07TLLT1wIXDOffO3HuimFFtPO/bqaysrq1vVDdrW9s7u3vu/sG9lonCpI0lk6obIU0YFaRtqGGkGyuCeMRIJ5pcz/zOlChNpbgzaUz6HI0EHVKMjJVCFwbFG5kigxxOwyzgkXzIAkNFCrXkeR66da/hFYDLxC9JHZRohe5XMJA44UQYzJDWPd+LTT9DylDMSF4LEk1ihCdoRHqWCsSJ7mfFFjk8scoADqWyJQws1N8TGeJapzyynRyZsV70ZuJ/Xi8xw8t+RkWcGCLw/KNhwqCRcBYLHFBFsGGpJQgraneFeIwUwsaGV7Mh+IsnL5POWcM/b/j+7Xm9eVXmUQVH4BicAh9cgCa4AS3QBhg8gmfwCt6cJ+fFeXc+5q0Vp5w5BH/gfP4Al8ebWA==</latexit>
vsom
<latexit sha1_base64="OoHnUMTfKHKutCSpgX5+xyUTuug=">AAACCHicbVDLSsNAFJ34rPUVdSnIYBFclUQKuiwK4rKCtYUmhMlk0g6dTMLMpBhCdm78FTcuFMStn+DOv3GaZqGtBy4czrl35t7jJ4xKZVnfxtLyyuraem2jvrm1vbNr7u3fyzgVmHRxzGLR95EkjHLSVVQx0k8EQZHPSM8fX0393oQISWN+p7KEuBEachpSjJSWPPPIKd/IBQkKOPFyJ/Ljh9xRlGfwuig8s2E1rRJwkdgVaYAKHc/8coIYpxHhCjMk5cC2EuXmSCiKGSnqTipJgvAYDclAU44iIt283KGAJ1oJYBgLXVzBUv09kaNIyizydWeE1EjOe1PxP2+QqvDCzSlPUkU4nn0UpgyqGE5DgQEVBCuWaYKwoHpXiEdIIKx0dHUdgj1/8iLpnTXtVtO2b1uN9mWVRw0cgmNwCmxwDtrgBnRAF2DwCJ7BK3gznowX4934mLUuGdXMAfgD4/MHoUGaOw==</latexit>
vF
<latexit sha1_base64="VHzpmnisfK3i/tDtRu5z2TTD20Q=">AAAB9HicbVBNS8NAEJ3Ur1q/qh69LBbBU0mkoBehqAePFVpbaELZbDft0s0m7E6EUvo3vHhQEK/+GG/+G7dtDtr6YODx3gwz88JUCoOu++0U1tY3NreK26Wd3b39g/Lh0aNJMs14iyUy0Z2QGi6F4i0UKHkn1ZzGoeTtcHQ789tPXBuRqCaOUx7EdKBEJBhFK/n+HZdICZJr0uyVK27VnYOsEi8nFcjR6JW//H7CspgrZJIa0/XcFIMJ1SiY5NOSnxmeUjaiA961VNGYm2Ayv3lKzqzSJ1GibSkkc/X3xITGxozj0HbGFIdm2ZuJ/3ndDKOrYCJUmiFXbLEoyiTBhMwCIH2hOUM5toQyLeythA2ppgxtTCUbgrf88ippX1S9WtXzHmqV+k2eRxFO4BTOwYNLqMM9NKAFDFJ4hld4czLnxXl3PhatBSefOYY/cD5/AAXrkNY=</latexit>
t = T
<latexit sha1_base64="+8FUkWl9JVjn0Yhmp09+PMq7Ym0=">AAAB9XicbVA9SwNBEJ3zM8avqKXNYhCswl0IaCMEtbCMkJhAcoS9zV6yZG/v3J0LhJDfYWOhILb+Fzv/jZvkCk18MPB4b4aZeUEihUHX/XbW1jc2t7ZzO/ndvf2Dw8LR8aOJU814g8Uy1q2AGi6F4g0UKHkr0ZxGgeTNYHg785sjro2IVR3HCfcj2lciFIyilfzOHZdICZJrUq53C0W35M5BVomXkSJkqHULX51ezNKIK2SSGtP23AT9CdUomOTTfCc1PKFsSPu8bamiETf+ZH70lJxbpUfCWNtSSObq74kJjYwZR4HtjCgOzLI3E//z2imGV/5EqCRFrthiUZhKgjGZJUB6QnOGcmwJZVrYWwkbUE0Z2pzyNgRv+eVV0iyXvErJ8x4qxepNlkcOTuEMLsCDS6jCPdSgAQye4Ble4c0ZOS/Ou/OxaF1zspkT+APn8wd6aZES</latexit>
t = 2T
<latexit sha1_base64="O0RPvHRw/IJZ09PwLbtl4k96bM0=">AAAB9XicbVA9SwNBEN2LXzF+RS1tFoNgFe40oI0Q1MIyQmICyRH2NnPJkr29c3cuEEJ+h42Fgtj6X+z8N26SKzT6YODx3gwz84JECoOu++XkVlbX1jfym4Wt7Z3dveL+wYOJU82hwWMZ61bADEihoIECJbQSDSwKJDSD4c3Mb45AGxGrOo4T8CPWVyIUnKGV/M4tSGQU6RU9r3eLJbfszkH/Ei8jJZKh1i1+dnoxTyNQyCUzpu25CfoTplFwCdNCJzWQMD5kfWhbqlgExp/Mj57SE6v0aBhrWwrpXP05MWGRMeMosJ0Rw4FZ9mbif147xfDSnwiVpAiKLxaFqaQY01kCtCc0cJRjSxjXwt5K+YBpxtHmVLAheMsv/yXNs7JXKXvefaVUvc7yyJMjckxOiUcuSJXckRppEE4eyRN5Ia/OyHl23pz3RWvOyWYOyS84H99775ET</latexit>
t = 3T
<latexit sha1_base64="Ztha2fo3iGVJ75b//X8HaS3m094=">AAAB8XicbVBNSwMxFHzrZ61fVY9egkX0VDZS0GPRi8cK1lbapWSz2TY0yS5JVihLf4UXDwri1X/jzX9j2u5BWwcCw8w88t6EqeDG+v63t7K6tr6xWdoqb+/s7u1XDg4fTJJpylo0EYnuhMQwwRVrWW4F66SaERkK1g5HN1O//cS04Ym6t+OUBZIMFI85JdZJjz3hohFBZ/1K1a/5M6BlggtShQLNfuWrFyU0k0xZKogxXeynNsiJtpwKNin3MsNSQkdkwLqOKiKZCfLZwhN06pQIxYl2T1k0U39P5EQaM5ahS0pih2bRm4r/ed3MxldBzlWaWabo/KM4E8gmaHo9irhm1IqxI4Rq7nZFdEg0odZ1VHYl4MWTl0n7oobrNYzv6tXGddFHCY7hBM4BwyU04Baa0AIKEp7hFd487b14797HPLriFTNH8Afe5w+QkZAR</latexit>
0
<latexit sha1_base64="Ztha2fo3iGVJ75b//X8HaS3m094=">AAAB8XicbVBNSwMxFHzrZ61fVY9egkX0VDZS0GPRi8cK1lbapWSz2TY0yS5JVihLf4UXDwri1X/jzX9j2u5BWwcCw8w88t6EqeDG+v63t7K6tr6xWdoqb+/s7u1XDg4fTJJpylo0EYnuhMQwwRVrWW4F66SaERkK1g5HN1O//cS04Ym6t+OUBZIMFI85JdZJjz3hohFBZ/1K1a/5M6BlggtShQLNfuWrFyU0k0xZKogxXeynNsiJtpwKNin3MsNSQkdkwLqOKiKZCfLZwhN06pQIxYl2T1k0U39P5EQaM5ahS0pih2bRm4r/ed3MxldBzlWaWabo/KM4E8gmaHo9irhm1IqxI4Rq7nZFdEg0odZ1VHYl4MWTl0n7oobrNYzv6tXGddFHCY7hBM4BwyU04Baa0AIKEp7hFd487b14797HPLriFTNH8Afe5w+QkZAR</latexit>
0
<latexit sha1_base64="Ztha2fo3iGVJ75b//X8HaS3m094=">AAAB8XicbVBNSwMxFHzrZ61fVY9egkX0VDZS0GPRi8cK1lbapWSz2TY0yS5JVihLf4UXDwri1X/jzX9j2u5BWwcCw8w88t6EqeDG+v63t7K6tr6xWdoqb+/s7u1XDg4fTJJpylo0EYnuhMQwwRVrWW4F66SaERkK1g5HN1O//cS04Ym6t+OUBZIMFI85JdZJjz3hohFBZ/1K1a/5M6BlggtShQLNfuWrFyU0k0xZKogxXeynNsiJtpwKNin3MsNSQkdkwLqOKiKZCfLZwhN06pQIxYl2T1k0U39P5EQaM5ahS0pih2bRm4r/ed3MxldBzlWaWabo/KM4E8gmaHo9irhm1IqxI4Rq7nZFdEg0odZ1VHYl4MWTl0n7oobrNYzv6tXGddFHCY7hBM4BwyU04Baa0AIKEp7hFd487b14797HPLriFTNH8Afe5w+QkZAR</latexit>
0
EFEITO DOPPLER:
LEMBRANDO DO QUE OCORRIA QUANTO A FONTE SE MOVIMENTAVA
Quando discutimos o efeito Doppler
devido ao movimento das fontes
observamos que a mudança de
frequência se dava porque a fonte
estava mudando de lugar e gerando
cada nova frente de onda num ponto
diferente no espaço. Assim as
frentes de ondas acabavam todas
excêntricas.
3. FONTE EM MOVIMENTO SUPERSÔNICO E OBSERVADOR EM REPOUSO
<latexit sha1_base64="OoHnUMTfKHKutCSpgX5+xyUTuug=">AAACCHicbVDLSsNAFJ34rPUVdSnIYBFclUQKuiwK4rKCtYUmhMlk0g6dTMLMpBhCdm78FTcuFMStn+DOv3GaZqGtBy4czrl35t7jJ4xKZVnfxtLyyuraem2jvrm1vbNr7u3fyzgVmHRxzGLR95EkjHLSVVQx0k8EQZHPSM8fX0393oQISWN+p7KEuBEachpSjJSWPPPIKd/IBQkKOPFyJ/Ljh9xRlGfwuig8s2E1rRJwkdgVaYAKHc/8coIYpxHhCjMk5cC2EuXmSCiKGSnqTipJgvAYDclAU44iIt283KGAJ1oJYBgLXVzBUv09kaNIyizydWeE1EjOe1PxP2+QqvDCzSlPUkU4nn0UpgyqGE5DgQEVBCuWaYKwoHpXiEdIIKx0dHUdgj1/8iLpnTXtVtO2b1uN9mWVRw0cgmNwCmxwDtrgBnRAF2DwCJ7BK3gznowX4934mLUuGdXMAfgD4/MHoUGaOw==</latexit>
vF
O movimento supersônico é o caso extremo deste
fenômeno. A fonte tem velocidade maior
que a velocidade de fase no gás e de fato vence
a frente de onda que ela própria gerou.
<latexit sha1_base64="ZHNFm7aul4+awZu3cbU6m4LJoVo=">AAACCnicbVDLSsNAFJ3UV62vqEs3g0VwVRIRdFl047KCtYWmhMl02g6dR5iZFEPI1o2/4saFgrj1C9z5N07TLLT1wIXDOffO3HuimFFtPO/bqaysrq1vVDdrW9s7u3vu/sG9lonCpI0lk6obIU0YFaRtqGGkGyuCeMRIJ5pcz/zOlChNpbgzaUz6HI0EHVKMjJVCFwbFG5kigxxOwyzgkXzIAkNFCrXkeR66da/hFYDLxC9JHZRohe5XMJA44UQYzJDWPd+LTT9DylDMSF4LEk1ihCdoRHqWCsSJ7mfFFjk8scoADqWyJQws1N8TGeJapzyynRyZsV70ZuJ/Xi8xw8t+RkWcGCLw/KNhwqCRcBYLHFBFsGGpJQgraneFeIwUwsaGV7Mh+IsnL5POWcM/b/j+7Xm9eVXmUQVH4BicAh9cgCa4AS3QBhg8gmfwCt6cJ+fFeXc+5q0Vp5w5BH/gfP4Al8ebWA==</latexit>
vsom
10. Efeito Doppler da Luz
Não há meio de propagação. As ondas eletromagnéticas
se propagam no vácuo. Importa somente a velocidade
relativa entre fonte e observador
<latexit sha1_base64="94pNZEITFn/llWrV3hLk/Fnd0PY=">AAACE3icbZDNSgMxFIUz9a/Wv1GXboJFVMQ6kYKCCEU3LitYW+iUkkkzbWgmMyaZQhn6DG58FTcuFMStG3e+jZl2Ftp6IPBx7r3c3ONFnCntON9Wbm5+YXEpv1xYWV1b37A3t+5VGEtCayTkoWx4WFHOBK1ppjltRJLiwOO07vWv03p9QKViobjTw4i2AtwVzGcEa2O17UN//xL60L2ArnqQ2vUlJglE8AgOTggcpXg8wbZddErOWHAWUAZFkKnatr/cTkjigApNOFaqiZxItxIsNSOcjgpurGiESR93adOgwAFVrWR80gjuGacD/VCaJzQcu78nEhwoNQw80xlg3VPTtdT8r9aMtX/eSpiIYk0FmSzyYw51CNN8YIdJSjQfGsBEMvNXSHrYpKJNigUTApo+eRbqpyVULiF0Wy5WrrI88mAH7IIDgMAZqIAbUAU1QMAjeAav4M16sl6sd+tj0pqzsplt8EfW5w88Q5p9</latexit>
f0
= f
s
1 + v/c
1 v/c
A expressão Doppler Relativística para a frequência observada é
onde “v" é a velocidade relativa entre fonte e observador e seu sinal indica se estão
se aproximando (+) ou se afastando (-) e “c" é a velocidade da luz.
<latexit sha1_base64="bBl4i2oJ8KP1Oode6I/v2G4pSv4=">AAACBXicbVDLSgMxFM3UV62vUZfdBIvgqs6USluKUHTjsoK1hc5QMmmmDU0yQ5IRytCFG3/FjQsFces/uPNvTB8LbT1wL4dz7iW5J4gZVdpxvq3M2vrG5lZ2O7ezu7d/YB8e3asokZi0cMQi2QmQIowK0tJUM9KJJUE8YKQdjK6nfvuBSEUjcafHMfE5GggaUoy0kXp2HsNLWKrVoFev1EpeHZYvqqZzeA5Vzy44RWcGuErcBSmABZo9+8vrRzjhRGjMkFJd14m1nyKpKWZkkvMSRWKER2hAuoYKxIny09kRE3hqlD4MI2lKaDhTf2+kiCs15oGZ5EgP1bI3Ff/zuokOq35KRZxoIvD8oTBhUEdwmgjsU0mwZmNDEJbU/BXiIZIIa5NbzoTgLp+8Stqlolsuuu5tudC4WuSRBXlwAs6ACyqgAW5AE7QABo/gGbyCN+vJerHerY/5aMZa7ByDP7A+fwDIhZQt</latexit>
c = 299 792 458 m/s
11. Efeito Doppler da Luz
Desvio para o vermelho ( REDSHIFT )
Uma fonte de luz vai parecer mais avermelhada* quando for
for vista se afastando do observador
<latexit sha1_base64="7WoEwgk+3mN0flfHUZtQdxHTihU=">AAAB73icbVBNS8NAEJ34WetX1aOXxSJ6KokU9OCh6MVjBWsKbSib7aRdutmE3Y1QQn+EFw8K4tW/481/47bNQVsfDDzem2FmXpgKro3rfjsrq2vrG5ulrfL2zu7efuXg8FEnmWLYYolIVDukGgWX2DLcCGynCmkcCvTD0e3U959QaZ7IBzNOMYjpQPKIM2qs5Edn5JpEpFepujV3BrJMvIJUoUCzV/nq9hOWxSgNE1TrjuemJsipMpwJnJS7mcaUshEdYMdSSWPUQT47d0JOrdInUaJsSUNm6u+JnMZaj+PQdsbUDPWiNxX/8zqZia6CnMs0MyjZfFGUCWISMv2d9LlCZsTYEsoUt7cSNqSKMmMTKtsQvMWXl4l/UfPqNc+7r1cbN0UeJTiGEzgHDy6hAXfQhBYwGMEzvMKbkzovzrvzMW9dcYqZI/gD5/MHBvaOiA==</latexit>
f0
< f
* O efeito Doppler relativístico vale para todo o espectro de ondas-eletromagnéticas
não só para a porção visível ao olho humano. Assim “avermelhar" e “azular" neste contexto
devem ser considerados metaforicamente no sentido de abaixar ou aumentar a frequência.
12. Efeito Doppler da Luz
Desvio para o azul ( BLUESHIFT )
Uma fonte de luz vai parecer mais azulada* quando for
for vista se aproximando do observador
* O efeito Doppler relativístico vale para todo o espectro de ondas-eletromagnéticas
não só para a porção visível ao olho humano. Assim “avermelhar" e “azular" neste contexto
devem ser considerados metaforicamente no sentido de abaixar ou aumentar a frequência.
<latexit sha1_base64="vS0HrCHaQFArtjWxTTQu3ErfbnE=">AAAB73icbVBNS8NAEJ34WetX1aOXxSJ6KokU9CRFLx4rWFNoQ9lsJ+3SzSbsboQS+iO8eFAQr/4db/4bt20O2vpg4PHeDDPzwlRwbVz321lZXVvf2Cxtlbd3dvf2KweHjzrJFMMWS0Si2iHVKLjEluFGYDtVSONQoB+Obqe+/4RK80Q+mHGKQUwHkkecUWMlPzoj1yQivUrVrbkzkGXiFaQKBZq9yle3n7AsRmmYoFp3PDc1QU6V4UzgpNzNNKaUjegAO5ZKGqMO8tm5E3JqlT6JEmVLGjJTf0/kNNZ6HIe2M6ZmqBe9qfif18lMdBXkXKaZQcnmi6JMEJOQ6e+kzxUyI8aWUKa4vZWwIVWUGZtQ2YbgLb68TPyLmleved59vdq4KfIowTGcwDl4cAkNuIMmtIDBCJ7hFd6c1Hlx3p2PeeuKU8wcwR84nz8KBo6K</latexit>
f0
> f
13. Efeito Doppler da Luz
Aproximação para velocidades relativas pequenas em
relação à velocidade da Luz
<latexit sha1_base64="94pNZEITFn/llWrV3hLk/Fnd0PY=">AAACE3icbZDNSgMxFIUz9a/Wv1GXboJFVMQ6kYKCCEU3LitYW+iUkkkzbWgmMyaZQhn6DG58FTcuFMStG3e+jZl2Ftp6IPBx7r3c3ONFnCntON9Wbm5+YXEpv1xYWV1b37A3t+5VGEtCayTkoWx4WFHOBK1ppjltRJLiwOO07vWv03p9QKViobjTw4i2AtwVzGcEa2O17UN//xL60L2ArnqQ2vUlJglE8AgOTggcpXg8wbZddErOWHAWUAZFkKnatr/cTkjigApNOFaqiZxItxIsNSOcjgpurGiESR93adOgwAFVrWR80gjuGacD/VCaJzQcu78nEhwoNQw80xlg3VPTtdT8r9aMtX/eSpiIYk0FmSzyYw51CNN8YIdJSjQfGsBEMvNXSHrYpKJNigUTApo+eRbqpyVULiF0Wy5WrrI88mAH7IIDgMAZqIAbUAU1QMAjeAav4M16sl6sd+tj0pqzsplt8EfW5w88Q5p9</latexit>
f0
= f
s
1 + v/c
1 v/c
Se então a expressão
<latexit sha1_base64="/TzzH7hQKdcBYC2rHqz9iEgNAjA=">AAAB8HicbVA9SwNBEJ2LXzF+nVraLAbBKt5KQIsUQRvLCMYEkiPsbfaSJXt75+5eIBz5EzYWCmLrz7Hz37hJrtDEBwOP92aYmRckgmvjed9OYW19Y3OruF3a2d3bP3APjx51nCrKmjQWsWoHRDPBJWsabgRrJ4qRKBCsFYxuZ35rzJTmsXwwk4T5ERlIHnJKjJXa4wuKajWEe27Zq3hzoFWCc1KGHI2e+9XtxzSNmDRUEK072EuMnxFlOBVsWuqmmiWEjsiAdSyVJGLaz+b3TtGZVfoojJUtadBc/T2RkUjrSRTYzoiYoV72ZuJ/Xic14bWfcZmkhkm6WBSmApkYzZ5Hfa4YNWJiCaGK21sRHRJFqLERlWwIePnlVdK6rOBqBeP7arl+k+dRhBM4hXPAcAV1uIMGNIGCgGd4hTfnyXlx3p2PRWvByWeO4Q+czx/D3470</latexit>
v/c << 1
usando que e para
fica
<latexit sha1_base64="smMCUqEkeOrXP0BBb9ouHfSy3Dc=">AAACBHicbVBNSwMxEM3Wr1q/Vr3pJVgEoVA3paDHohePFawtdJeSTbNtaLK7TbLSshS8+Fe8eFAQr/4Ib/4b03YP2vpg4PHeDDPz/JgzpR3n28qtrK6tb+Q3C1vbO7t79v7BvYoSSWiDRDySLR8ryllIG5ppTluxpFj4nDb9wfXUbz5QqVgU3ulxTD2BeyELGMHaSB37yFVDqVNUGk2gq5igQ4hgCY7OK7BjF52yMwNcJigjRZCh3rG/3G5EEkFDTThWqo2cWHsplpoRTicFN1E0xmSAe7RtaIgFVV46+2ECT43ShUEkTYUaztTfEykWSo2FbzoF1n216E3F/7x2ooNLL2VhnGgakvmiIOFQR3AaCOwySYnmY0MwkczcCkkfS0y0ia1gQkCLLy+TZqWMqmWEbqvF2lWWRx4cgxNwBhC4ADVwA+qgAQh4BM/gFbxZT9aL9W59zFtzVjZzCP7A+vwB3wyWKg==</latexit>
p
1 + x ' 1 + x/2
<latexit sha1_base64="hh1ucMgh4FxmHcc8f+jEwjPVDq8=">AAAB7nicbVBNSwMxEJ2tX7V+VT16CRbBU9lIQQ89FL14rGA/oF1KNs22sdlkSbJiKf0PXjwoiFd/jzf/jWm7B219MPB4b4aZeWEiuLG+/+3l1tY3Nrfy24Wd3b39g+LhUdOoVFPWoEoo3Q6JYYJL1rDcCtZONCNxKFgrHN3M/NYj04YreW/HCQtiMpA84pRYJzWfULWKcK9Y8sv+HGiV4IyUIEO9V/zq9hVNYyYtFcSYDvYTG0yItpwKNi10U8MSQkdkwDqOShIzE0zm107RmVP6KFLalbRorv6emJDYmHEcus6Y2KFZ9mbif14ntdFVMOEySS2TdLEoSgWyCs1eR32uGbVi7AihmrtbER0STah1ARVcCHj55VXSuijjShnju0qpdp3lkYcTOIVzwHAJNbiFOjSAwgM8wyu8ecp78d69j0VrzstmjuEPvM8fmzWOUA==</latexit>
x << 1
<latexit sha1_base64="lINLq3kYen0+1kNJv4aaqDL5jRc=">AAAB/3icbVBNSwMxEM3Wr1q/VsWTl2ARK0LdSEGPRS8eK1hbaJeSTbNtaJJdk2yhLAX/ihcPCuLVv+HNf2Pa7kFbHww83pthZl4Qc6aN5307uaXlldW1/HphY3Nre8fd3XvQUaIIrZOIR6oZYE05k7RumOG0GSuKRcBpIxjcTPzGkCrNInlvRjH1Be5JFjKCjZU67kF40tZM0EcYwhJE8AwOz8lpxy16ZW8KuEhQRoogQ63jfrW7EUkElYZwrHULebHxU6wMI5yOC+1E0xiTAe7RlqUSC6r9dHr+GB5bpQvDSNmSBk7V3xMpFlqPRGA7BTZ9Pe9NxP+8VmLCKz9lMk4MlWS2KEw4NBGcZAG7TFFi+MgSTBSzt0LSxwoTYxMr2BDQ/MuLpHFRRpUyQneVYvU6yyMPDsERKAEELkEV3IIaqAMCUvAMXsGb8+S8OO/Ox6w152Qz++APnM8fJDuTeQ==</latexit>
f0
' f(1 + v/c)
O que é semelhante ao caso do Doppler no som para o caso que as velocidades
de fonte e de observador são muito menores que a velocidade do som.
1
p
1 x
' 1 + x/2