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Polaryzacja światła

Polaryzacja światła. Polaryzacja światła. Tak widzimy przez okulary polaryzacyjne, górne zdjęcie wykonane jest bez filtru, a dolne z filtrem. liniowa. kołowa. eliptyczna. Światło niespolaryzowane. Polaryzacja kierunek drgań wektora E. Płaszczyzna polaryzacji. Filtry polaryzacyjne.

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Polaryzacja światła

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  1. Polaryzacja światła

  2. Polaryzacja światła Tak widzimy przez okulary polaryzacyjne, górne zdjęcie wykonane jest bez filtru, a dolne z filtrem

  3. liniowa kołowa eliptyczna

  4. Światło niespolaryzowane

  5. Polaryzacjakierunek drgań wektora E

  6. Płaszczyzna polaryzacji

  7. Filtry polaryzacyjne

  8. Światło spolaryzowane

  9. Światło spolaryzowane

  10. Światło spolaryzowane

  11. Jak spolaryzować światło?

  12. Polaryzacja światła przez odbicie

  13. Prawo Malusa

  14. optoelectronics Dwójłomność Halite (kubicznykryształ chlorku sodu, izotropowy optycznie Calcyt (optycznie anizotropowy) Kryształ kalcytu z dwoma skrzyżowanymi polaryzatorami Birefringence was first observed in the 17th century when sailors visiting Iceland brought back to Europe calcite cristals that showed double images of objects that were viewed through them. This effect was explained by Christiaan Huygens (1629 - 1695, Dutch physicist), as double refraction of what he called an ordinary and an extraordinary wave. With the help of a polarizer we can easily see what these ordinary and extraordinary beams are. Obviously these beams have orthogonal polarization, with one polarization (ordinary beam) passing undeflected throught the crystal and the other (extraordinary beam) being twice refracted.

  15. Dwójłomność

  16. optoelectronics Dwójłomność promień nadzwyczajny promień zwyczajny

  17. optoelectronics Dwójłomność promień zwyczajny promień nadzwyczajny

  18. Crystalline materials may have different indices of refraction associated with different crystallographic directions. A common situation with mineral crystals is that there are two distinct indices of refraction, and they are called birefringent materials.

  19. If the y- and z- directions are equivalent in terms of the crystalline forces, then the x-axis is unique and is called the optic axis of the material. • The propagation of light along the optic axis would be independent of its polarization; it's electric field is everywhere perpendicular to the optic axis and it is called the ordinary- or o-wave. The light wave with E-field parallel to the optic axis is called the extraordinary- or e-wave.

  20. Polarization through Scattering

  21. a J J* cos²a

  22. a ? N N* cos²a

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