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Conducting (metallic) surfaces can be substituted for the dielectric surfaces, showing that there is no polarization in reflection from conducting surfaces.
The sequence of photographs above show the following physical situations:
-two dielectric surfaces with parallel surfaces.
-two dielectric surfaces with perpendicular surfaces.
-two conducting surfaces with parallel surfaces.
-two conducting surfaces with perpendicular surfaces.
-lower conducting surface parallel to upper dielectric surface.
-lower conducting surface perpendicular to upper dielectric surface.
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Demonstrates polarization of light
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