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We come up with the mirror equation.

Notice that in Mirrors we get a virtual image to the right of the surface. Thus formirrors we say that s i is positive to the left of the mirror. This allows to retain correspondence between s i being negative and an image being virtual.

Again we use the small angle approximation. By inspection of the figure we see that 2 θ i = α + β and θ i = α + γ . Now we multiply the second equation by two and subtract the first equation from itand we get: 2 α + 2 γ α β = 0 or α β = 2 γ . Using the small angle approximation we see that this is h s o + h s i = 2 h r where I have used the fact that s i is negative to the right of the mirror. So I can write the mirror equation as 1 s o + 1 s i = 2 R or 1 s o + 1 s i = 1 f where for a mirror 1 / f = 2 / R

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Source:  OpenStax, Waves and optics. OpenStax CNX. Nov 17, 2005 Download for free at http://cnx.org/content/col10279/1.33
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