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Table of Contents

  1. What is Optics?
  2. Geometric Optics
    1. Index of Refraction
    2. Snell's Law
    3. Thin Lenses
    4. Thick Lenses
    5. Imaging
    6. Paraxial Raytracing
    7. Gaussian Reduction
    8. Stops and Pupils
  3. Aberrations
    1. Chromatic Aberration
    2. Spherical Aberration
    3. Coma
  4. Physical Optics
    1. Polarization

What is Optics?

Optics is the study of light.

Geometric Optics

Index of Refraction

There is a value that measures the ratio, n, between the speed of light in a vacuum, c, to the speed of light in a medium, v, particular for various mediums.

n = c v

Snell's Law (Law of Refraction)

Arguably one of the most important laws in optics, especially geometric optics, is Snell's Law, or the Law of Refraction. It defines how light hitting a surface changes angle behind the surface. More specifically, the product of the indicent light's angle to the surface normal, θ, and the index of refraction of the first medium, n, is equal to the product of the outward light's angle to the surface normal, θ', and the index of refraction of the medium incident upon, n'.

n sinθ = n' sinθ'

There's many reasons to like Snell's Law. For one, it produces extremely cool effects in our everyday life like the famous "Snell's Window" in pools of water.

I like Snell's Law because I imagine that a snail invented it 🐌

Total Internal Reflection:

Thin Lenses

Lenses are optical elements made of surfaces of glass which bend light across a front surface into its own material, often glass, and then through a second surface. The surfaces are often made with precise curvature to

In all optical elements, there are a set of characteristic points that we can measure to define a model of a system. These will be discussed in further detail later on.

Thick Lenses

Moving beyond the thin lens approximations, we can start analyzing systems taking into account the ray bending and transfer happening within the sag of lenses or other optical elements. This is extremely useful for building models of complex systems into

Any imaging system can be broken down into a few charactistic points known as cardinal points, which provide us reference points for things we want to image from object space into image space, using our imaging equations. There are six to be aware of:

And their conjugate rear versions, for image space:

The principal planes of an optical system represent the

Imaging

When we imagine everything in front of a lens as the "object space" of that system and every ray of light that propogates through the lens, cumulatively known as the ray bundle, as the "image space" of that system, we are able to consider the mathematics for imaging object space onto image space.

When an object is a distance away from the front principal plane of a system z (measured negative if in opposite direction of light; a vector measurement), it is imaged through a system with focal length f, to a distance away from the rear principal plane of the system z'

Thin Lens Imaging Equation: 1 z' = 1 z + 1 f

The optical "power" of an element is defined as the inverse of its focal length, often measured in mm^-1 known as diopters to opticians. It is represented by the symbol Φ

Φ = 1 f

Paraxial Raytracing

It is useful in many applications to trace a "ray" through an optical system to understand where key objects are being imaged or even occluded by objects in a system.

For convenience when doing raytrace calculations, we will denote the "optical angle" of a ray, the product of the index, n, and angle relative to the optical axis, u, as the optical angle, ω.

ω = n u

Transfer:

y' = y + ω' τ'

Refraction:

ω' = ω - y Φ

Gaussian Reduction

Reduced thickness.

τ = t n

Reduction of power between refractive surface 1, with power Φ1, and refractive surface 2, with power Φ2, and a reduced thickness between the surfaces τ to find the system power Φ

Φ = Φ1 + Φ2 - Φ1 Φ2 τ

By def

Stops and Pupils

Any optical system collects a limited amount of light, often restricted by a

There are two characteristic pupils

f/# ("F-Number")

The f/# of a system is a characteristic yadayada

f/# = f DEP

Aberrations

Spherical Aberration

Chromatic Aberration

Coma

Physical Optics

I'm still learning 😀

Polarization