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Introductory Physics Volume Two

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168 Geometric Optics 8.6<br />

In the diagram we are able to draw the three rays that are bolded,<br />

because they are, (top ray) parallel to the optical axis, (middle ray)<br />

through the center, and (bottom ray) through the focal point. These<br />

three rays are called the principle rays. From the three principle rays<br />

(we only needed two really) the location of the focus is determined.<br />

After the location of the focus is determined, the other faint rays are<br />

drawn so that they go through the focus.<br />

Notice that the rays of light actually do pass through the focus. If<br />

we place a piece of paper at that point the paper would be illuminated.<br />

This type of image is called a real image.<br />

x o<br />

x i<br />

y o<br />

y i<br />

f<br />

f<br />

The location and size of the image can be computed from the<br />

location and size of the object.<br />

Theorem: Thin Lens Equations<br />

With the dimensions as shown in the figure above,<br />

1<br />

x o<br />

+ 1 x i<br />

= 1 f<br />

Theorem: Magnification Equations<br />

With the dimensions as shown in the figure above,<br />

= − x i<br />

y o y i<br />

where y is negative if below the optical axis.<br />

x o

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