Fermat's (biography on pp. $352-353$ ) principle in optics states that light traveling from one point to another follows that path for which the total travel time is minimum. In a uniform medium, the paths of "minimum time" and "shortest distance" turn out to be the same, so that light, if unobstructed, travels along a straight line. Assume that we have a light source, a flat mirror, and an observer in a uniform medium. If a light ray leaves the source, bounces off the mirror, and travels on to the observer, then its path will consist of two line segments, as shown in Figure Ex-61. According to Fermat's principle, the path will be such that the total travel time $t$ is minimum or, since the medium is uniform. the path will be such that the total distance traveled from $A$ to $P$ to $B$ is as small as possible. Assuming the minimum occurs when $d t / d x=0,$ show that the light ray will strike the mirror at the point $P$ where the "angle of incidence" $\theta_{1}$ equals the "angle of reflection" $\theta_{2}$
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