Transcript Day 5

Announcements
•Lab tonight: planetarium
•Homework: Chapter 6 # 1, 2, 3, 4, 5 & 6
•First Quarter Observing Night
Wednesday after fall break. Set-up
starts around 6:45pm
Telescopes
Galileo’s early
telescope and lens
Newton’s original
telescope with mirror
Telescope basics
Telescopes either use refraction or reflection to focus
light to a point. For refraction, the basic law is Snell’s
Law: n1sinq1 = n2sinq2. The law of reflection is a much
simpler: i  r
If the surfaces of a piece of
glass are curved, they will
focus light to a point
 1 1 n  1d 
1
 n  1  

f
R
R
nR
R
2
1 2 
 1
R1 and R2 are the radii of
curvature of the two faces, n
is the index of refraction of
the glass and d is the center
thickness of the lens.
Assumes lens is used in air
The focal length, f, is the distance from the lens
axis to the focal point or focal plane. The focal
length of a lens depends on the material of the
lens and the curvature of the surfaces
A concave mirror will also
focus light to a point
r
f 
2
For a spherical mirror the focal
length is just half the radius of
curvature of the mirror. For
other shapes the formula is
somewhat more complicated
For any telescope, the most
important property is the
Light Gathering Power (LGP)
2
0
d
LGP 
49
do is the diameter
of the objective
in mm. Compares
the light
gathering power
to that of the
human eye
Telescopes are often referred
to by their f-ratio
f
f  ratio  f / 
d
f is the focal length of the
objective and d is its diameter
Magnification is determined
by the focal lengths
When using an eyepiece
M
f primary
f eyepiece
When using a CCD camera,
the image scale determines
the magnification
206.265
 is the size of a single S I 
f primary
pixel in micrometers
The ability of a telescope to
resolve fine detail is given by
the Rayleigh Criterion
sin q  q  1.22

d
 is the wavelength of the light
being used and d is the
diameter of the aperture. q is
the smallest resolvable angle
of the telescope. The angle
will be in radians
Aberrations
Spherical aberration can be
corrected by using parabolic or
hyperbolic surfaces
Coma is worse for parabolic
surfaces than spherical ones.
Correction is to use hyperbolic
surfaces
Astigmatisms are the result of a nonaxially symmetrical lens.
All three of these aberrations
apply to both lenses and mirrors
The Refracting Telescope
Examples of Refractors
Problems With Refractors:
Chromatic Aberration
Achromatic Doublet
Provides some color correction but doesn’t
completely remove all chromatic aberration.
Apochromatic Design
The best apochromats use a three element design
with low dispersion glass to reduce chromatic
aberration to a minimum. Of course, the more glass
the light goes through, the greater the loss.
Newtonian Reflector
Still a popular design among amateurs
but not widely used by professionals. The
focal plane is not large and there are lots
of off-axis distortions.
Examples of Newtonian Reflectors
Invented by Isaac Newton in 1668
Cassegrain Reflector
Invented by Laurent Cassegrain in 1672
Classic Cassegrain…Parabolic Mirrors
Ritchey-Chretien (RC)…Hyperbolic Mirrors
Examples of Cassegrain’s
Keck 1
Most professional telescopes
use a Cassegrain focus with
hyperbolic mirrors: an RC
Gemini North
Schmidt-Cassegrain Design
Primary mirror is spherical instead of parabolic. The
“correcting lens” corrects for spherical aberrations.
Examples of Schmidt-Cassegrain
telescopes
Maksutov-Cassegrain Design
The correcting lens is a meniscus shape. The
Maksutov-Newtonian is also a popular design
Examples of Maksutov Telescopes
Mounts
Alt-Az Mounts
The Dobsonian Mount is an
Alt-Az mount
Equatorial Mounts
German Equatorial Mount
Fork Equatorial Mounts
Other Types of Equatorial Mounts
Cross-Axis Equatorial
English Yoke Equatorial
Example of a Yoke mount
Hooker Telescope
Mount Wilson, CA
Eyepieces come in a variety of
different optical designs
The
magnification
of a telescope
is just the ratio
of the focal
length of the
objective to the
focal length of
the eyepiece
mag 
f objective
f eyepiece Since the light is passing through glass,
eyepieces suffer from chromatic aberration
My personal favorites are
Tele Vue eyepieces
Field of View depends on the
eyepiece
fov 
foveyepiece
mag

foveyepiece
f objective
f eyepiece
60 ° fov
68 ° fov

f eyepiece foveyepiece
f objective
82 ° fov