CASSEGRAIN AND GREGORIAN TELESCOPE DESIGNS



In the book "Telescope Optics, Evaluation and Design", by Harrie Rutten and Martin van Venrooij, the calculations for a Cassegrain system are given in Chapter 21.2. This note is a derivation from that source. The equation numbers assigned below match those given in that chapter. The basic Cassegrain layout is shown in Figure 1, below.



Figure 1: Cassegrain Layout

First, the definitions:

     S = f2 / f1 = r2 / r1
     T = D2 / D1
     M = f / f1
     B = b / f
     P = d / f

where:

     f1 and f2 are the primary and secondary focal lengths
     r1 and r2 are the primary and secondary radii of curvature
     D1 and D2 are the primary and secondary diameters
     f is the focal length of the system
     d is the separation between the primary and secondary
     b is distance of the final focal surface behind the primary

The equations to calculate the magnification are then:

     M = ( 1 - T ) / ( T - B )      21.2.1
     M = ( 1 - B - P ) / P      21.2.2

The auxilliary equations are:

     P = ( 1 - B ) / ( M + 1 )      21.2.3
     B = 1 - ( M + 1 ) * P      21.2.4
     T = P + B      21.2.5
     S = M * T / ( M - 1 )      21.2.6

     f1 = f / M
     f2 = S * f1
     d = f * P
     b = f * B

The Seidel coefficients are calculated from:

     alpha = ( ( M + 1 ) / ( M - 1 ) )2      21.2.10
     beta = ( ( M - 1 ) / M )3 * T      21.2.11
     gamma = ( ( M - 1 ) / M )3 * ( 1 - T )      21.2.12
     delta = 2 / M2      21.2.13
     epsilon = 4 * ( 1 - P ) / ( M * T )      21.2.14
     theta = ( M - 1 )3 * P2 / ( M * T )      21.2.15

With the Seidel coefficients themselves being:

   Spherical Aberration:
     Acass = 1 + SC1 - ( SC2 + alpha ) * beta      21.2.7
   Coma:
     Bcass = delta + ( SC2 + alpha ) * gamma      21.2.8
   Astigmatism:
     Ccass = epsilon - ( SC2 + alpha ) * theta      21.2.9

The equations above are consistent for Gregorian telescopes by letting the separation between the primary and secondary be larger than primary focal length, as shown in the Gregorian layout of Figure 2, below. Due to the crossover, the effect is that of making the secondary diameter appear negative (D2 < 0). This effect is extended to the net focal length and secondary magnification, making them appear negative, as well.


Figure 2: Gregorian Layout


The basic Cassegrain forms given in R&vV are still valid:

   Classical (paraboloidal primary):
     SC1 = -1
     SC2 = -alpha      21.2.16

   Dall-Kirkham (spherical secondary):
     SC1 = alpha * beta - 1      21.2.17
     SC2 = 0

   Ritchey-Chretien (aplanatic):
     SC1 = -( 1 + beta * ( delta / gamma ) )      21.2.18
     SC2 = -( alpha + delta / gamma )      21.2.19

   Pressman-Camichel (spherical primary):
     SC1 = 0
     SC2 = -( alpha - 1 / beta )      21.2.20


GEOMETRY

Solve the first equation and two of the remaining four

D1

*

f/#

=

f








D2

/

D1

=

T


b

/

f

=

B


d

/

f

=

P


f

/

f1

=

M








f1

f2

f

r1

r2

d

b

B

P

D1

D2

T

f/#

M

S

alpha

beta

gamma

delta

epsilon

theta


Ritchey-
Chretien

Classical

Dall-
Kirkham

Pressman-
Camichel


SC1


SC2


Acass


Bcass


Ccass


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