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Relationships derived from Snell's law

  • Image position of a light ray incident on a material

The light rays before and after entering the material are shown in the figure below.

Description of light rays entering a material_001.png

Here, dw, dθ1 , and dθ2 are small quantities.

The conditions shown in the figure can be expressed as follows:

Description of light rays entering a material_002.png

Here,

Description of light rays entering a material_003.png

Therefore,

Description of light rays entering a material_004.png

Therefore,

Description of light rays entering a material_005.png
  • Image position when a parallel plate is placed perpendicular to the optical axis

Consider the following light beam that enters a plane-parallel plate and forms an image at the exit point. Calculate s in this case.

Image position of light perpendicularly incident on a parallel plate_001.png

Here, dh, dθ 1 , and dθ 2 are small quantities.

The conditions shown in the figure can be expressed as follows:

Image position of light perpendicularly incident on a parallel plate_002.png

Where:

Image position of light perpendicularly incident on a parallel plate_003.png

Therefore,

Image position of light perpendicularly incident on a parallel plate_004.png

Therefore,

Image position of light perpendicularly incident on a parallel plate_005.png
  • Image position when a parallel plate is placed at an angle to the optical axis

Consider the following light beam that is obliquely incident on a parallel plane plate and forms an image at the exit point. Calculate Δx and Δy in this case.

Parallel plane plate oblique incidence_001.png

Here, dh, dθ 1 , and dθ 2 are small quantities.

The conditions shown in the figure can be expressed as follows:

Differentiate both sides of ③ to get

From ①, ②, ③', ④, and ⑤, eliminating s, xA, xB, dh, dθ1, and dθ2, we get

Here, from ① and ⑥,

Also, from ③,

Therefore, the solution we seek can be expressed as follows:

Parallel plane plate oblique incidence_007.png

Furthermore, by applying ③ and eliminating θ2, we get

 

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