#Equation for polarized light intensity series#

in Waves, Berkeley Physics Course - Vol 3, (McGraw-Hill, NY, 1968), p 434.

605206))Ģ An excellent explanation is given by Frank S. ($65/sheet from Polaroid in 1985, product no. Ours have been cut down to 6' squares and mounted in a wooden frame. A half-wave plate can convert right-handed circularly polarized light into left-handed circularly polarized light and vice versa.ġ Polaroid 140 nm 1/4-wave retarder-the retardation is 1/4 wavelength if the wavelength is 4 × 140 nm = 560 nm (which is green) the wave plate is backed onto 0.030' thick plastic and comes in 12' square sheets. We also have a half-wave and a full-wave plate available. Also, a retardation plate can't convert unpolarized light into polarized light. Note that retardation plates do not influence the state of polarization of incident linearly polarized light, if the light's polarization direction lies along either the slow or the fast axis of the retardation plate. Comments:Ĭircular polarizers are used to reduce annoying reflections, eliminate glare, and enhance contrast for a variety of commercial applications. Use a video camera to look through the circular polarizer and view the reflection of an illuminated foreground object as the angle between the polarizer and wave plate is changed. Propping up the filters with wood blocks will allow for their easy reorientation.Ī mirror with one retarder and one polarizer can also be used.

#Equation for polarized light intensity series#

When the retarders are parallel with each other and at an angle relative to the polaroids, an illuminated object can be viewed through the series of filters using a video camera.

Two quarter-wave retarders are placed between crossed polaroids. Finally, one can substitute a non-reversing mirror (two mirrors mounted together at right angles) to see what happens! Setting it up: The effect is also undone by reversing the order of the polarizer and wave plate. The effect is undone by rotating the linear polarizer with respect to the wave plate. However, it is now polarized perpendicular to the linear polarizing filter's orientation, so it is absorbed and the mirror appears dark 2. The mirror reverses the direction of circular polarization, and the reflected reversed circularly polarized light is converted back into linearly polarized light by the wave plate. The circular polarization produced by the linear polarizer/quarter-wave plate sandwich is also made evident by placing a mirror behind it and looking through the circular polarizer at the mirror reflection. (More generally, if the angle between the wave plate and polarizing filter is not 45°, the two components will differ in intensity and the emerging light will be elliptically polarized.) A second wave plate with the same orientation will result in a 180° phase shift, and the components will now sum to obtain linearly polarized light that has been rotated by 90°. Thus incident unpolarized light emerges as circularly polarized light. Because of the 90° phase shift between the two components after they pass through the retardation plate, the direction of polarization of the light that emerges from the wave plate will rotate in time. The situation dramatically changes when the incident light is polarized.Ī polarizing filter is placed in front of the quarter-wave plate at a relative angle of 45° so that the incident horizontal and vertical components are of equal intensity. Unpolarized light is not affected by this retardation plate (or by any thickness of birefringent material) because the retardation plate only changes the phase of each component of polarization. The quarter-wave retardation plate is a sheet of birefringent (double refracting) material 1 of thickness such that horizontally and vertically polarized light entering in phase will emerge from the retardation plate 1/4 of a wavelength out of phase. Unpolarized light emerges vertically polarized from the polaroid at A a quarter-wave plate at B oriented 45° to the polaroid produces circularly polarized light a second quarter-wave plate at C passes horizontally polarized light, which passes through the polaroid at D.