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Physics · Ch 6 — Optics

Fizeau's Method to Determine Speed of Light

6.3.1

Fizeau's Method to Determine Speed of Light

Fizeau's apparatus for measuring the speed of light in air used a light source SS, a partially silvered glass plate GG tilted at 45°45° to send light out towards a rotating toothed wheel with NN teeth and NN equal-width cuts (gaps), and a distant fixed mirror MM placed a known distance dd (about 8 km) away. Light passing through one gap in the wheel travels to MM, reflects back, and (if the wheel had not rotated in the meantime) would pass back through the same gap to reach the observer looking through GG. As the wheel's angular speed ω\omega was increased from zero, at some speed the returning light became completely blocked by the tooth adjacent to that gap -- the light vanished for the first time. At that instant, the wheel had rotated through the angle θ\theta between one tooth and the next slot (θ=2π/2N=π/N\theta=2\pi/2N=\pi/N) in the light's round-trip travel time t=2d/vt=2d/v; combining ω=θ/t\omega=\theta/t with v=2d/tv=2d/t gives v=2dωNπv=\dfrac{2d\omega N}{\pi}. Increasing ω\omega further, the light reappears at 2ω2\omega and vanishes again at …

Figure 6.13Speed of light by Fizeau's method

What this figure shows. Light from a source S reflects off a partially silvered glass plate G tilted at 45 degrees, passes outward through a gap between two teeth of a rotating toothed wheel, travels a long known distance d to a fixed distant mirror M, and returns along the same path back through the wheel to an observer looking through G. As the wheel's rotation speed is increased from rest, the returning light is eventually completely blocked by the tooth immediately next to the gap it went out through, at which instant the observer sees the light vanish for the first time -- the angular speed at which this first happens is what the formula v = 2dNomega/pi is built from, using the geometry of exactly how far the wheel must turn (the …