OP - Principles of Paraxial Optics - Week 3 Flashcards
Define a paraxial ray.
A ray that travels very close to the optical axis, and always stay close to the axis.
Why are paraxial rays significant?
All the angles are very small relative to the optical axis, and so the trigonometric function more or less equals the angle. ie. sin(x) = x. This only occurs at small angles.
This only applies to radians, and not degrees.
Describe taylor series approximations for sin(x).
sin(x) = x - x^3/3! + x^5/5! + x^7/7! + …
Allows greater and greater approximations for sin (x).
Describe how snells law changes with respect to paraxial rays.
n’i’ = ni
Define the paraxial refraction equation.
n’u’ - nu = -hF
Define F and its equation.
F is the power of a surface.
F = C (n’ - n)
Define C’s equation.
C = curvature C = 1 / r
Describe the opening and closing equations (hint h=)
Opening
h = -ul
Closing
h = -u’l’
Describe the equation that proves paraxial rays are coincident.
(n’/l’) - (n/l) = F
Describe the paraxial transfer equation.
h’ = h + u’d
Describe the steps of ray-tracing through a number of steps.
- Choose a ray using the opening equation.
- Apply paraxial refraction equation to find u’
- Apply the paraxial transfer equation to find h’
- Repeat from step one, transforming u’ to u, h’ to h
- If final refraction, apply closing equation