Thick lens

We consider a lens consisting of two spherical surfaces centered on an optical axis and one cylindrical surface where the central axis of the cylinder is along the optical axis. The radius of curvature of the left spherical interface is $R_1$, the radius of curvature of the right spherical interface is $R_2$, and the radius of the cylinder is $R_c$. The thickness of the lens measured along the optical axis is $d$. The view shown below is looking down at the $x-y$ plane. It is possible to rotate the optical axis of the lens an angle $\phi$ with respect to the $x-$axis. Light rays leave an object $(x_o,y_o)$ and are reflected and refracted at the interfaces. The reflected rays have 1/10 the intensity of the incident rays and the refracted rays have 9/10 the intensity of the incident rays. The refraction can be calculated using Snell's law of refraction at a spherical interface. The index of refraction is wavelength dependent. The different colors are bent through different angles. This is called chromatic aberration. If the index of refraction is made the same for all three colors then it is still not always possible to focus the light to one point. This is called spherical aberration.

Light Source

$x_o = $ [cm]
$y_o = $ [cm]
$\phi = $ [deg]
$\lambda ('s) = $ an array of wavelengths in nm
$380 < \lambda <780$

 

Lens

$R_1 = $ [cm]
$R_2 = $ [cm]
$d = $ [cm]
$R_c = $ [cm]
$\phi = $ [deg]
$n = A + B/\lambda^2$, $A=$ , $B=$ [nm²]

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Lens types:

A three-dimensional version of this app is available here.