Focal lengths and focal points
Lenses can focus light and make images in a very similar way to mirrors. Lenses are either converging (convex on both sides, or concave on one side but more strongly convex on the other --- i.e., thicker in the center than at the edges) or diverging (concave on both sides, or concave on one side more strongly than convex on the other --- i.e., thinner in the center than at the edges). Both concave and convex lenses are used in a variety of optical instruments that will be studied in the next lecture.
As in the case of mirrors, there are three prototypical cases. The principal example is the camera lens -- a converging lens used to form a real image of an object that is farther away from the lens than the focal point. Equivalent examples are the lens in a slide or movie projector, which forms a real image on the screen; or a magnifying glass being used to form a real image of the sun on dry twigs to start a fire. In this case, like the real-image case for the mirror, the equation
1/di + 1/do = 1/f
has di, do, and f all positive. The magnification
M = -di / do
is therefore negative, so the real image is inverted.A second prototypical case is the magnifying glass used in the classic Sherlock Holmes style: a converging lens used to form a virtual image of an object that is held closer to the lens than the focal point. Here f is still positive (converging lens), but di is negative. Hence the magnification M is positive, so the virtual image is not inverted.
The third prototypical case is the peep-hole lens, a diverging lens used to make a virtual image that is smaller than the object. Here f is negative (diverging lens) and M is positive so the image is not inverted.
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