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PHYSICS 220/230
Lab 8: Lenses and Mirrors
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You have studied lenses and mirrors and the equations, sign conventions, and ray tracing
techniques that allow you to find images in geometrical optics. We want to look at these phenomena
computationally and experimentally. The following reference link provides the relevant
equations: Geometric Optics
The applet below allows you to simulate standard optical elements (lenses, mirrors, sources, and
objects) and observe the ways that light rays propagate through these elements. You should
conduct a simulation with this applet immediately before each of your real experiments to visualize
how the principal rays converge and form the image that you will observe.
I. Converging Lenses
- Place a lens on the simulation screen by clicking the lens button and then clicking a position
on the principal axis. Now put an object on the screen by clicking the object button and
then selecting a position on the screen. You can reposition the lens or the object by
clicking and dragging. When the lens is selected, you can also click and drag the focal
point to adjust the focal length of the lens. Play with these parameters and describe how
the image position and size depend on the position of the object.
- Now place the light source, the thin converging lens, and the screen in holders along the
experimental optical bench. Adjust their heights to be about the same. Fix the position of the
source and lens, and then adjust the position of the screen until a sharply defined image is
formed on it. For an image that is enlarged, record all the positions as well as the size of
the object and the image. Then, make the required calculations to complete the data in the
following tables.
CONVERGING LENS: Power = + 6 Diopters
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Trial l |
| (1) source position |
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| (2) lens position |
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| (3) screen position |
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| (4) object size: h |
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| (5) image size: h' |
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| (6) source distance: p |
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| (7) image distance: q |
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| (8) f (from lens formula) |
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| (9) f (from 1/P) |
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| (10) compare (8) and (9) |
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| (11) m = h' / h |
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| (12) m = -q/ p |
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| (13) compare (11) and (12) |
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- Repeat this set of measurements and computations for the thicker positive lens. In this case
make the image a diminished one. Incorporate that data into the following table.
CONVERGING LENS
Power = + 20 Diopters
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Trial 2 |
| (1) source position |
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| (2) lens position |
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| (3) screen position |
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| (4) object size: h |
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| (5) image size: h' |
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| (6) source distance: p |
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| (7) image distance: q |
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| (8) f (from lens formula) |
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| (9) f (from 1/P) |
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| (10) compare (8) and (9) |
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| (11) m = h' / h |
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| (12) m = -q/ p |
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| (13) compare (11) and (12) |
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II. Concave Mirror
- Clear the simulation screen (click Clear All) and add a mirror and an object. Observe
and record how the image position and size depend on the object position.
- Repeat experimental measurements, similar to those in part I, for the concave mirror. Note
that in these measurements the source and screen both face the mirror and both are on the same
side of the mirror. Hence, the heights of the screen and mirror must necessarily be slightly
different so the rays from the source can focus on the screen. Do two trials, one with a
magnified image and one with a diminished image.

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Trial l |
Trial 2 |
| (1) source position |
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| (2) mirror position |
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| (3) screen position |
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| (4) object size: h |
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| (5) image size: h' |
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| (6) source distance: p |
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| (7) image distance: q |
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| (8) f (from mirror formula) |
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| (9) m = h' / h |
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| (10) m = -q/p |
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| (11) compare (9) and (10) |
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III. Diverging Lens
- Simulate a concave lens by adding a lens and then
dragging the focal point through the lens. Place an object on the
screen and describe the image that is formed. How could you view this
image? On a screen? With your eye? Now add a converging lens between the object and the diverging
lens. Can you configure this combination to produce an image that
could be viewed on a screen? How can you do this?
- Since negative or diverging lenses do not form REAL images of REAL objects, use the thin
converging lens to set up an experimental VIRTUAL OBJECT for the diverging lens. Your setup
should be as follows:

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DIVERGING LENS: Power = -2 Diopters |
Trial l |
| (1) source position |
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| (2) converging lens position |
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| (3) screen position without lens 2 |
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| (4) diverging lens position |
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| (5) screen position with lens 2 |
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| (6) source distance: p2 |
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| (7) image distance: q2 |
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| (8) f2 (from lens formula) |
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| (9) f2 (from 1 / P2) |
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| (10) compare (8) and (9) |
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IV. Convex Mirror
- Simulate a convex mirror by adding a mirror and
then dragging the focal point through the mirror. Add an object and describe the image. Now add a
converging lens and observe how the trajectories of the optical rays change
as you vary the positions of the lens and object. Why do multiple
images appear and how are they numbered?
- Experimentally determine the focal length of the convex mirror by using it in conjunction with
the thinner converging lens. First obtain a REAL image of the source using the lens alone.
Interpose the mirror between the lens and the original image. Next, turn the screen around and
move it between the lens and the mirror. Adjust the heights of the source, lens, and screen so
the top of the screen covers the lower half of the lens and the REAL image can be seen on the
screen. Move the screen and/or mirror to observe a sharp image on the screen. Record the data
and calculations as before.

CONVEX MIRROR
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Trial l |
| (1) virtual object position |
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| (2) mirror position |
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| (3) final screen position |
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| (4) source distance p |
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| (5)image distance q |
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| (6) f (from mirror formula) |
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