ASTR 1230 (O'Connell) Lecture Notes
2. INTRODUCTION TO TELESCOPES
Summit of Mauna Kea, Hawaii, world's
largest astronomical observing complex
The telescope is the single most important invention for astronomy.
Without it, we would have little of the profound understanding we
have obtained over the last few hundred years about the physical
nature of the universe and its history.
This lecture describes the main features of the design and operating
principles of optical-band telescopes.
A. THE ELECTROMAGNETIC SPECTRUM
Maxwell (1865) discovered that electric and magnetic forces can
propagate through space at the speed of light. The
immediate inference was that light is an electromagnetic
disturbance. The propagating disturbance moves through space like
a wave through water and is called an electromagnetic ("EM")
EM waves are characterized by their wavelengths, or distance
between peaks where the EM forces are strongest. All wavelengths from
zero to infinity are possible for EM waves, and this total range is
called the EM spectrum. From longest to shortest
wavelengths, the EM spectrum includes: Radio, microwaves,
infrared, optical light, ultraviolet light, X-rays, and gamma rays.
The human eye is directly sensitive only to a very small
range of wavelengths in the EM spectrum. This is called the
visible or optical region (see figure below). Within
this region, the wavelength of the light determines the sensation of
color produced in our eyes. Shorter wavelengths correspond
to bluer colors.
Full EM Spectrum with the Optical/Visible Band Enlarged
- Wavelengths of optical light are
conventionally measured in units of "Ångstroms" (where 1 Å
= 10-8 cm).
- The optical band extends roughly from
wavelengths of 4000 Å in the deep violet to 7000 Å in the
deep red. Green light has a wavelength around 5000 Å, or about
0.0005 mm---far smaller than sizes encountered in everyday life.
Because the wavelength of optical light is so small, we are not
conscious of light's wavelike character.
are microns. 1 micron = 10-4cm = 10,000 Å)
The Earth's atmosphere is opaque to most wavelengths in the EM
spectrum. This is good for lifeforms on Earth's surface, because the
more energetic types of EM radiation are harmful. But, obviously, it
is not convenient for astronomers who want to monitor the universe
across the full EM spectrum. (This is the main motivation for space
astronomy.) The chart below shows the ability of different wavelengths
to penetrate the atmosphere. The two main "atmospheric windows,"
where cosmic EM radiation can easily reach Earth's surface, are in the
radio and optical bands. (Click for enlargement.)
The rest of this lecture describes telescopes designed to work in the
optical band. Telescopes in adjacent regions of the EM spectrum
(the infrared and ultraviolet) are quite similar. But "telescopes" for
the radio, X-ray, or gamma-ray bands are very different in design./p>
B. TELESCOPES: GENERAL
The telescope is a beautiful example of interplay between technology
(fabrication of quality glass, polishing techniques, large mechanical
structures, computers) and basic science.
- Invented: 1608 (Lipperhey, Holland). [Note: microscope invented
1654, also in Holland.]
- First astronomical use: 1609, by
Italy). Even though his telescopes were small (only 1-2 inch lenses) and
crude by modern standards, they utterly transformed astronomy.
- Galileo discovered, for instance, that there were thousands of
stars too faint to be seen with the naked eye.
In honor of the 400th anniversary of Galileo's introduction of the telescope
to astronomy, 2009 was designated the International Year of Astronomy.
Click on the logo below for more information.
- Collect more light from source
This is the most important attribute of an astronomical telescope (because most astronomical
sources are so faint)
- Magnify source
"Magnify" means to make the source appear larger in angular size; this is the most
important attribute of a terrestrial telescope
- Resolve more detail in source
"Resolution" is distinct from magnification. A higher resolution image looks
more sharp, less blurry, regardless of how large it is.
- An objective or primary optical element forms
an image (i.e. an accurate representation of original scene)
at a usable focus, where it can be studied by eye, recorded
by film or other detectors (as in a camera), or fed into yet other
Objectives: Two Types
Reflection of Light by a Figured Mirror
- Lens: A lens is a piece transparent glass
or plastic shaped to refract (or bend) light rays to a focus.
The image at the left below shows how a flat glass surface bends light
rays (in this case, two flat surfaces at an angle combine to make a
prism). The shorter the wavelength (e.g. blue light), the
stronger the bending. The image at the right shows how a glass
surface can be continuously curved to bring all the light rays
passing through it from a distant object to a common focal
point. Each element of the lens acts like a small prism.
Refraction of Light By a Prism
(click for descriptive animation)
Shaped Convex Lens
- Note that light rays travel in straight lines through
empty space or through any medium (air, glass, water, etc) that has
uniform properties. It will only be at the boundaries
between two uniform media that light rays can be deflected or "bent."
The optical elements of a telescope therefore only change the
directions of light rays at their surfaces (which represent glass/air
- Mirror: A mirror is a shaped piece of glass which
reflects light rays off its front surface to a common focus.
A mirror shaped like a parabola will focus all rays that are
parallel to its optical axis to a single point. See picture below.
Applet. Here is a Java applet illustrating the
differences between refraction, reflection, and diffraction.
- Note: Because the primary optical element is the most important
element of a telescope, the "size" of a telescope is characterized by
the diameter of its primary. The length of a telescope is
not in direct proportion to its primary diameter but rather depends
on the optical design.
Thus, the "26-in"
McCormick refracting telescope has a primary lens that is 26 inches in
diameter. The "200-in" Palomar telescope has a primary mirror that is
200 inches in diameter.
- For distant objects (including all astronomical objects), the
incoming rays from each point on the source are parallel to each
other. In this case, the image is formed at a position which is one
focal length from the objective.
- For nearer objects, the
image is formed at a larger distance from the objective. Click on
the button below for a Java applet illustrating image formation.
- Note that the image is inverted with respect to the
original, as in the drawing below:
- In order to look through a telescope, a small lens called an
eyepiece is used to magnify the image at the focal point and
make the rays parallel again. This allows the eye to form a sharp
image of it.
(Although the lens of your eye is partially adjustable and can adjust
to focus on nearby or distant objects, the light beam from the
objective of a telescope is converging or diverging too strongly to
correct in the absence of an eyepiece.)
C. CELESTRON TELESCOPES USED IN ASTR 1230
The telescopes you will use in this class are Celestron 8-in Schmidt-Cassegrain
reflectors and use an equatorial fork-mount.
This terminology is explained in the rest of the lecture.
A more complete description and full details on operation of the
Celestrons are given in Chapter 3 of the ASTR 1230 Laboratory
D. TELESCOPE PERFORMANCE CHARACTERISTICS
Focal ratio (or "f/ number")
Magnification or "power"
- f/ = (Objective Focal Length)/(Objective Diameter).
- The smaller is the focal ratio, the more
concentrated is the light in the focal plane and the
easier it is to see faint extended objects like nebulae.
[Same as for the aperture setting on a camera---the smaller
the f/ number, the higher is the brightness in the focal plane.]
- Typical small telescopes have f/ numbers in the range 5-20. The Celestron
8-in telescopes are f/10 with focal lengths of 2032 mm.
Field of View
- Defined to be the fractional increase in the apparent angular
size (measured, e.g., in degrees) of the image. With a "10x" or
"10 power" telescope, a scene viewed through the telescope will appear
to be 10 times larger in angular size than when viewed without the
- Mag = (Apparent Image Size in Degrees) / (Object Size Without Scope in Degrees).
- For a given telescope, magnification is inversely proportional to the
focal length of the eyepiece:
Mag = (Focal Length Telescope) / (Focal Length Eyepiece)
For the Celestron 8-in scopes: Mag = 2032 mm/FLE. Thus:
Note: high powers (> 150x) are not necessarily better, except
for specialized applications (e.g. planets). High magnification is
susceptible to image blurring by atmosphere, telescope vibration.
- A 40 mm eyepiece yields 50 power
- A 20 mm eyepiece yields 100 power
Light Gathering Power
- Defined to be the original angular diameter
of the maximal region viewable through the telescope. Field of view
decreases as magnification increases.
- E.g. with a 20 mm eyepiece, the Celestron 8-in scopes produce
a field which is 20 minutes of arc in diameter. This is smaller than
the angular diameter of the full Moon, which is 30 min of arc diameter. So
you could not view the entire Moon through the telescope with a 20 mm
eyepiece. However, you could do so with a 40 mm eyepiece.
Resolution: Optical Figuring Tolerance
- Most important attribute of a telescope
- Light collected is proportional to the area of the objective;
think of the telescope as a "light bucket."
The area of the objective is proportional to its diameter2.
- Comparing the capability of the 8-in Celestron scope to the human
- Assume pupil diameter of dark-adapted eye is 5 mm. Celestron
objective is 203.2 mm.
- Light gathering capability of the
Celestron is therefore (203/5)2 = (40)2 = 1600x larger than
- Therefore, with the telescope, you can see objects which are 1600x fainter
than with your naked eye. If your eye can detect magnitude 5 stars,
the Celestron will detect stars of 13th magnitude.
There are over 5,000,000 of these, compared to the
2,000 or so visible with the naked eye!
- For more information on the human eye as an astronomical
detector, see this page.
Resolution: Diffraction of Light Waves
- Resolution is quantitatively defined to be the smallest
measurable detail in an image and is quoted in seconds of arc. In
practice, this depends on your telescope's optics, the wave nature of light,
and the Earth's atmosphere.
- To produce a good image, telescope optics must be fabricated to
match their designed surface shape within a minimum tolerance of about
1/4 of a wavelength of light in their operating band. For optical
telescopes, this is 10-5 cm. Very small! but relatively
easy to achieve with current technology.
- Good polishing/test techniques were not developed until the 19th
century. To overcome limitations in optical technology, early
astronomers favored telescopes with very long focal lengths (click here for an
example), which reduced chromatic and spherical aberrations.
- A fundamental limit to the resolution of any optical system is set by
the physics of light: since it is a wave phenomenon, light
spreads out or diffracts.
The picture above shows how light waves diffract when passing through a
narrow aperture, such as the objective lens of a telescope.
Because of the interference of light waves from different parts of the
aperture, the larger the aperture, the more concentrated the
emerging beam, implying better resolution.
- The resolution is proportional to (Wavelength/Objective Diameter).
The larger the telescope, the better the resolution.
picture illustrates the effects of telescope diameter on the size
of the image of a binary star.
(Note that all stars are so distant that they appear as
point sources in smaller telescopes. You cannot
actually detect any detail on star surfaces except in the largest telescopes).
- A 10-in diameter telescope with perfect optics will produce a 1
arc-sec diameter image of a star (assuming a perfectly stable
The Earth's atmosphere also refracts light, and
because it is constantly moving, there is always a blurring and
jittering of images in a scope. Astronomers call this "seeing."
Quantitatively, seeing is defined
to be the diameter of a star image
(in seconds of arc) caused by atmospheric turbulence.
Expect typical seeing of 2-4
seconds of arc at the Student Observatory. Seeing can be measured by
observing a double star of known separation (see writeup for Lab 3).
dominates diffraction in most cases, so having a better telescope often
does not improve performance. Instead, you may need a better observing site.
Below is an enlarged image of the bright star Betelgeuse taken with a
large telescope. It is a large blob, broken up into smaller near
point-like units by seeing effects in the Earth's atmosphere. (The
small "speckles" represent the image size you could see in the absence
of atmospheric effects.) Click on the image for a video of the seeing effects.
for illustrations of seeing effects on observations of planets and the
"Seeing" Produced by Earth's Atmosphere
E. TELESCOPE TYPES
Three basic types of telescope optics:
great variety! Here are four common types of
- Refracting: objective is a lens; bends rays.
Examples: Galileo's telescopes; the McCormick 26-in.
- Reflecting: objective is a mirror; reflects rays. Invented
by Gregory; improved by Newton. All large telescopes are reflectors.
- Catadioptric: combines lenses and mirrors, e.g. to produce
a larger well defined field of view. Most famous: Schmidt wide field
survey telescopes. These use a spherical primary mirror
surface, which by itself would produce serious blurring but add a
specially-shaped correcting lens at the front of the telescope
that eliminates the blur.
Note that in three of the designs shown, a "secondary" mirror at the
top of the telescope tube is used to redirect the light beam. Although
the secondary does block part of the primary, this has only a small
effect on the net image quality. In particular, it does not
produce a "hole" in the center of the image. In the Cassegrain design,
a hole is actually made in the primary itself.
The Celestrons you will use are catadioptric systems. They
combine a spherical mirror and Schmidt corrector plate
with a Cassegrain through-the-primary light beam design. See diagram
Mounting designs: again, a great variety.
Two primary types:
Why are all large telescopes reflectors?
- Altitude-Azimuth (Alt/Az) mount: one vertical axis and
one horizontal axis. Easier to engineer, and therefore lower cost.
But these require computer control for accurate tracking
since the telescope must be moved in two axes simultaneously to follow
- Equatorial mount: two axes, but polar axis is tilted
to parallel the Earth's rotation axis. See this
illustration. Motion around this one axis then tracks the stars as they
move across the sky.
Harder to engineer, easier to operate. Most telescopes use equatorial
mounts but the largest ones are Alt-Az. Your Celestron 8-inch telescopes are
- Lenses produce chromatic aberration (see above). Since
light of only a small range of wavelengths is in good focus, this is a
particular difficulty for using modern broad-band electronic
- Mirrors need be figured only on one side
- Mirrors are easy to support accurately from behind; lenses require
support at edges, tend to sag.
- It is harder to support a heavy lens mechanically at the top of
a telescope tube than a mirror at the bottom.
- The folding action of primary and secondary mirrors
means that reflector tubes are much shorter than in a "straight
through" refracting design.
- For all these and other reasons, large reflectors are easier to
design and cheaper to build than refractors and offer better
performance in most applications. You can find more discussion at this
Glass mirror blank
for one of the two 8.4-m diameter
mirrors of the Large Binocular
F. TELESCOPE MILESTONES
A binocular is simply a pair of two small, co-aligned refracting
telescopes mounted together in such a way that each eye can look
through one of telescopes.
- Additional optics (prisms---see at right) are used so that the
view is "right side up."
- The view for nearby objects is 3-dimensional; special optics may
be used to increase the separation of the objective lenses for better
- Astronomical objects are so distant that there can be
no 3-D effect. However, views with binoculars can be especially vivid
because simultaneous use of both eyes produces less eye strain, and the
optics of binoculars usually allow for easy centering of the eyes on
the emergent beam. It is much easier to find your target with binoculars
than with a telescope (assuming it's bright enough).
- Binocular optics are usually classified in the form "7 x 35".
Here, the first number is the net magnification of the
binoculars, and the second is the diameter of the primary
lenses in millimeters. Good types for general astronomical
observations are 7x35 or 8x50. Binoculars higher than 10 power require
tripods for stability. The field of view is also often marked on
the binoculars, typically given as the diameter in feet for objects
at a distance of 1000 yards.
- Binoculars produce some of the best views of the Moon, rich star
fields, comets, and the Milky Way.
Sunset over the William Herschel
Telescope (La Palma, Spain)
- Download, print, and read the notes for Lecture 2.
- Take Review Quiz--Week 3 on the Collab site.
- Read Appendix C in the Manual on "Telescope Basics"
Lab 1 (Constellations) at either of the next two observing
- Begin Labs 2 (Introduction to Binoculars) and 3 (Introduction to
Small Telescopes) as soon as possible after Lab 1. You do not have to complete
Lab 2 before beginning Lab 3.
Prepare for the Labs by carefully reading the writeups in
Read Appendices D and E on preparing lab reports and filling
out observing forms.
September 2011 by rwo
Text copyright © 1998-2011 Robert W. O'Connell. All rights
reserved. Some images copyright © by Prentice-Hall and by the
University of Tennessee at Knoxville. WHT image copyright © by N.
Szymanek. These notes are intended for the private, noncommercial use
of students enrolled in Astronomy 1230 at the University of Virginia.