A simple working telescope requires
nothing more than a pair of lenses mounted in a tube. The lens in front, known
as the objective lens, focuses an image; the lens in back, known
as the eyepiece lens, magnifies that image. Although it may seem
like a crude device, a simple telescope nicely illustrates the basic working
principles of more powerful astronomical instruments.
Light normally moves in straight lines,
but there are situations in which this is not true. You are already familiar
with some: for example, the distortions you see looking through the surface of
the ocean occur because light bends as it passes from the water into the air.
Long before we understood why light bends as it passes from one
transparent material to another, people had used this effect to create lenses:
optical devices which can gather light together or spread it apart.
In order to understand how a lens
works, you need to know a little about how light behaves in passing from one
material to another. Imagine a tank of water on the table in front of you; the
surface of the water should be perfectly flat and horizontal. If you shine a
ray of light straight down from above, it will pass through the surface
of the water without bending. But if you shine the light in at an angle, it
will bend as it passes through the surface. The diagram below illustrates two
important facts about this effect. First, in passing from air to water, the
light always bends into the water. Second, the smaller the angle between
the light ray and the surface, the more it bends in passing through. The same
rules would also apply if the tank of water was replaced with a block of glass.
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Light
rays passing from air into water. If the ray strikes the surface at a 90°
angle it does not bend (left). But if the angle is less than 90° the light
does bend (middle); reducing the angle between the light and the surface
increases the bend (right). |
What if you shine the light up
through the water into the air? The answer is very simple; light follows the same
path no matter which way it's going! To illustrate this on the diagram above,
all you'd need to do is draw upward-pointing arrows at the other end of each
light ray.
To create a lens which can focus many
parallel rays of light to a single point, the idea is to curve the surface of
the glass so that all these rays, after passing through, come together at the
same place. It's a bit tricky to do this right, but we don't need to worry
about the details. The simplest kind of lens is a `plano-convex'
lens; one side is flat, while the other bulges out at the middle. Below is a
diagram showing how such a lens focuses light. The optical axis
of the lens is the thick line which passes right through the middle of the
lens; a ray of light traveling along the optical axis is not bent at all. Rays
which pass through the top of the lens are bent downward, while rays which pass
through the bottom of the lens are bent upward. Thus all these light rays are
bent toward the optical axis. If the lens is well-made, all rays meet at the
same focal point. The distance between the lens and the focal
point, measured along the optical axis, is called the focal length.
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A
simple lens in operation. Parallel light rays come from the right, pass
through the lens, and meet at the focal point on the left. The thick line
through the middle of the lens is the optical axis; the
distance F is the focal length. |
A lens which could only focus
light rays striking the glass head-on (as in the illustration above) would be
fairly useless for astronomy. Fortunately, most lenses can also accept rays
which come in at a slight angle to the optical axis, and bring them to a focus
as well. This focal point is not the same as the focal point for rays
which are parallel to the optical axis; depending on the angle of the incoming
rays, their focus lies on one side or the other of the optical axis, as shown
in the diagram below. But if the lens is well-made, all these focal points will
lie on a plane which is parallel to the face of the lens; this is called the focal
plane.
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A
simple lens forming an image. The red rays arrive with an
downward slant, and come to a focus below the optical axis, while the blue
rays arrive with a upward slant, and come to a focus above the optical axis.
The vertical dotted line at left represents the focal plane. |
There's one slightly subtle consequence
of this image-formation process: the image is upside-down! The next diagram
shows why: rays from the lower part of the subject (on the right) come together
at the upper part of the image (left), and vice versa. This is also true
of any camera you may own; of course, you turn the prints right way up when you
get them from the photo store, so you're probably not aware of the orientation
of the image inside your camera.
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The
image formed by a simple lens is upside-down with respect to the subject.
Here the subject (right) is an arrow with a red tip pointing upward; its
image (left, at the focal plane) points down. |
Your simple telescope kit includes a
large objective lens which you will use to study image formation. Take the
large lens and mount it at one end of the larger cardboard tube; slide the
smaller tube into the other end of the larger one, and use a rubber band to
hold a sheet of tracing paper over the open end of the smaller tube. Now point
the tubes at the subject we've set up in the lab, and slide the smaller tube in
and out until you focus a sharp image of the subject on the tracing paper.
Record your observations
and measurements in your lab notebook. Include a sketch the image.
Most of the time, professional
astronomers use telescopes to take pictures of astronomical objects. The
instrument you've just built is a crude model of a professional photographic
telescope; if the tracing paper was replaced by a piece of photographic film,
you could use this equipment to take a picture in much the same way the pros
do.
To make a telescope you can actually look
through, you'll need to add another lens. This eyepiece lens magnifies the
image formed by the large objective lens and directs the light to your eye.
Basically, the eyepiece works a lot like a magnifying glass; it enables your
eye to focus much more closely than you normally can. The eyepiece on a typical
telescope allows you to inspect the image formed by the objective lens from a
distance of an inch or less. The diagram below shows how the objective lens and
eyepiece work together in a simple telescope.
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Diagram
of a simple telescope. Parallel light rays enter from the left, pass through
the objective lens, come to a focus at the focal plane, and exit through the
eyepiece lens. The focal length of the objective is F, and the focal
length of the eyepiece is f. |
Before installing the eyepiece lens in
your telescope kit, you should first measure its focal length, f. Remove
the lens from its foam mounting and hold it by the edges. Point the flat side
of the lens toward a distant light-source and hold a sheet of paper behind the
lens and parallel to its face. Move the paper closer or further from the lens
until you see a sharp image of the light-source, and measure the distance from
the curved face of the lens to the paper. (This really requires three hands;
get your lab partner to help!) Record the focal length f in your lab
notebook.
You're now ready to put the telescope kit
together. Replace the eyepiece lens in its foam mounting. Remove the tracing
paper, and insert the foam mounting in the smaller tube. Point the telescope at
a distant target and slide the tube in and out until you get a good focus.
Which way is the image oriented?
Compared to the image in your binoculars
or a real telescope, the image you'll see with this simple telescope is
probably a bit fuzzy; you may also notice bands of color around bright objects.
These effects are due to the limitations of the simple lenses used in this
telescope kit. You can make the image sharper by installing the paper washer in
front of the objective lens, but this will also make the image dimmer since the
telescope will gather less light.
The magnification of a telescope can be
easily calculated once you know the focal lengths F and f of the
objective lens and eyepiece, respectively. The formula for the magnification M
is
M = F ÷ f .
Here you can use any units for F and f, as long as you use
the same units for both. For example, if you measure F in
millimeters, you should also measure f in millimeters. Using the values
for F and f you measured above, calculate the expected
magnification of your telescope.
So that you can measure the magnification
of your telescope directly, we will set up a target - basically a meter stick
with marks a unit distance apart. From the other end of the room, focus your
telescope on the meter stick. Now look through the telescope while keeping both
eyes open; you should see a double image of the meter stick, where one image is
magnified and the other is not. Compare the two images; how many of the
unmagnified units fit within one magnified unit? The answer is a direct
measurement of your telescope's magnification; record it in your notebook and
compare it to the magnification you calculated above.
Do the experiments described in the
sections on IMAGE FORMATION and EYEPIECES AND MAGNIFICATION, and write a report
on your work. This report should include, in order,
In more detail, here are several things
you should be sure to do in your lab report: