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N 21 < 1: faasiseosed

N 21 < 1: faasiseosed. a < a p. E  10 /E  00 =. E  10 / E  00 =. E  10 /E  00 =. E  10 / E  00 =. Alati!. =. =. tan( d  /2). tan( d  /2). 3. 1. 3. 2. 2. 1. 3. 2. 1. Langev laine lineaarselt polariseeritud , asimuut 45 0. Täielik peegeldumine. ?. , aga.

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N 21 < 1: faasiseosed

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  1. N21 < 1: faasiseosed a < ap E10/E00= E10 /E00= E10/E00 = E10 /E00= Alati! = =

  2. tan(d/2) tan(d/2) 3 1 3 2 2 1 3 2 1 Langevlainelineaarseltpolariseeritud, asimuut 450

  3. Täielik peegeldumine ? , aga Kui n1 > n2 = x n2 z Kehtib alati Amplituud Faas Amplituud: Amplituud

  4. Pindlaine (tunnelefekt) G M (n2 < n1) 1 2 < l Amplituud a > ap z l x Kui vahe risttahukate vahel on suur, siis pöördub laine täielikult tagasi T T Kui vahe on  l, siis tungib laine ka teise risttahukasse Auditoorium

  5. Valguse levik neelavas keskkonnas I0 I I0/e dz z z =1/a - a dI  I dz Tasalaine ja teisendame Neeldumise arvestamiseks loeme, et Amplituud

  6. kompleksne e : faasinihe E ja H vahel 2 2 2 a - - a N cos( ) N sin ( ) 21 21 - || || || || E E /E /E = 10 10 00 00 2 2 2 a + - a N cos( ) N sin ( ) 21 21 - kompleksne Kompleksne murdumisnäitaja Metallid  1 Kuna z = l0 , siis vahemaa läbimisel Fresneli valemid N21 - kompleksne Polariseeritud valguse langemisel metallile on peegelduv valgus elliptiliselt polariseeritud.

  7. Metalli omadused optilistel sagedustel ja Mõõdetavad suurused: R ja d = d - d Fresneli valemitest:

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