In the ray model of Section 34.1 we noted that light within a medium can be scattered or absorbed. As we’ve now seen, the absorption of light can be wavelength dependent and can create color in objects. What are the effects of scattering?
Light can scatter from small particles that are suspended in a medium. If the particles are large compared to the wavelengths of light—even though they may be microscopic and not readily visible to the naked eye—the light essentially reflects off the particles. The law of reflection doesn’t depend on wavelength, so all colors are scattered equally. White light scattered from many small particles makes the medium appear cloudy and white. Two well-known examples are clouds, where micrometer-size water droplets scatter the light, and milk, which is a colloidal suspension of microscopic droplets of fats and proteins.
A more interesting aspect of scattering occurs at the atomic level. The atoms and molecules of a transparent medium are much smaller than the wavelengths of light, so they can’t scatter light simply by reflection. Instead, the oscillating electric field of the light wave interacts with the electrons in each atom in such a way that the light is scattered. This atomic-level scattering is called Rayleigh scattering.
Sunsets are red because all the blue light has scattered as the sunlight passes through the atmosphere.
Unlike the scattering by small particles, Rayleigh scattering from atoms and molecules does depend on the wavelength. A detailed analysis shows that the intensity of scattered light depends inversely on the fourth power of the wavelength: . This wavelength dependence explains why the sky is blue and sunsets are red.
As sunlight travels through the atmosphere, the dependence of Rayleigh scattering causes the shorter wavelengths to be preferentially scattered. If we take 650 nm as a typical wavelength for red light and 450 nm for blue light, the intensity of scattered blue light relative to scattered red light is
Four times more blue light is scattered toward us than red light and thus, as FIGURE 35.22 shows, the sky appears blue.
Sunlight has to travel much farther through the atmosphere when we see it at sunrise or sunset than it does during the midday hours. In fact, the path length through the atmosphere at sunset is so long that essentially all the short wavelengths have been lost due to Rayleigh scattering. Only the longer wavelengths remain—orange and red—and they make the colors of the sunset.