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Section 3.2  The Physics of Color  75


                                 from an excited state to a lower energy state. Typical of such lamps is strong
                                 radiation at a small number of wavelengths, which correspond to particular
                                 state transitions. The most common cases are sodium arc lamps and mercury
                                 arc lamps. Sodium arc lamps produce a yellow-orange light extremely effi-
                                 ciently and are quite commonly used for freeway lighting. Mercury arc lamps
                                 produce a blue-white light and are often used for security lighting.

                            Figure 3.5 shows a sample of spectra from different light bulbs.

                                        1
                                                                       Metal halide
                                      0.9                              Standard flourescent
                                                                       Moon white flourescent
                                      0.8                              Daylight flourescent
                                      0.7
                                    energy  0.6


                                    Relative  0.5
                                      0.4

                                      0.3
                                      0.2
                                      0.1

                                        0
                                        350   400    450   500   550   600   650   700    750
                                                            Wavelength in nm
                            FIGURE 3.5: The relative spectral power distribution of four different lamps from the Mit-
                            subishi Electric Corporation. Note the bright, narrow bands that come from the flourescing
                            phosphors in the fluorescent lamp. The figure was plotted from data made available by the
                            Coloring Info Pages at http://www.colorpro.com/info/data/lamps.html;the data was
                            measured by Hiroaki Sugiura.


                                 Black Body Radiators
                                 One useful abstraction is the black body, a body that reflects no light. A heated
                            black body emits electromagnetic radiation. It is a remarkable fact that the spectral
                            power distribution of this radiation depends only on the temperature of the body.
                            If we write T for the temperature of the body in Kelvins, h for Planck’s constant,
                            k for Boltzmann’s constant, c for the speed of light, and λ for the wavelength, we
                            have
                                                          1         1
                                                  E(λ) ∝   5                .
                                                         λ (exp(hc/kλT) − 1)
                            This means that there is one parameter family of light colors corresponding to
                            black body radiators—the parameter being the temperature—and so we can talk
                            about the color temperature of a light source. This is the temperature of the black
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