System Matrix for a Thick Lens

This is an examination of the system matrix for a thick lens in the form used by Meyer-Arendt. An alternative form of the system matrix is used by Hecht.

The example is for a lens with index of refraction n surrounded by air (n=1). It involves the surface powers of the lens and the thickness d between the vertexes. It also involves the principal planes H1 and H2. As with most ordinary geometrical optics, it is applicable only for small angles (paraxial rays). The development also follows the cartesian sign convention.

For glass with index of refraction
nlens = n =

the front surface power for lens radius
R1 = m is P1 = m-1

and the back surface power for lens radius
R2 = m is P2 = m-1

Lens thickness d = m

(Note that for a double convex lens, the front surface radius R1 is positive and the back surface radius R2 is negative according to the Cartesian sign convention.)

The symbols used by Meyer-Arendt for the elements of the system matrix will be used.

b = a =
d = c =

A number of other characteristics of the thick lens may be calculated from the system matrix.

The right-hand, or equivalent focal length of the lens is just the reciprocal of matrix element a: f2 = 1/a = m.

The distance V2H2 from the right vertex to the associated principal plane is given by V2H2= (c-1)/a = m.

The right vertex focal length (or back focal length) is given by fv2 = c/a = m.

Note that the equivalent focal length f2 is the sum of the back vertex focal length and the distance from the vertex to the principal plane: f2 = fv2 + V2H2. Similar relationships exist for the left-hand or front vertex.

The left vertex focal length (or front focal length) is given by fv1 = -b/a = m.

The distance V1H1 from the left vertex to the associated principal plane is given by V1H1= (1-b)/a = m.

The equivalent front focal length f1 is then given by f1 = -(b/a + V1H1) = m.

Image location for thick lens from system matrix
Image location for pair of thin lenses from system matrix
Index

Lens concepts

Thick lens concepts

References
Meyer-Arendt
Ch. 1.4

Hecht
 
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