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Schematic representation of Brewster’s Law. The dots correspond to the electric vector perpendicular to the page, whereas the double-headed arrows represent the electric vector in the plane of the page. An unpolarized, or arbitrarily plane-polarized, incident ray (upper right quadrant), strikes a surface at an angle of incidence, θ B , corresponding to the Brewster’s angle, or the angle of polariza- 

Schematic representation of Brewster’s Law. The dots correspond to the electric vector perpendicular to the page, whereas the double-headed arrows represent the electric vector in the plane of the page. An unpolarized, or arbitrarily plane-polarized, incident ray (upper right quadrant), strikes a surface at an angle of incidence, θ B , corresponding to the Brewster’s angle, or the angle of polariza- 

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Affirming Kirchhoff’s Law of thermal emission, Max Planck conferred upon his own equation and its constants, h and k, universal significance. All arbitrary cavities were said to behave as blackbodies. They were thought to contain black, or normal radiation, which depended only upon temperature and frequency of observation, irrespective of the natur...

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... result was stunning. Max Planck had determined that the reflectivities of all arbitrary media were equal. Yet, he attempted to dismiss such a conclusion by stating relative to Eq. 20 [5, Eq. 40]: “ The first of these two relations, which states that holtz. ” Planck provided for the element of the bounding surface two separate coe ffi cients of reflection. These must, in fact, correspond to those of the media utilized. Planck has already stated in § 35 that “ . . . let all quantities referring to the second substance be indicated by the addition of an accent. ” Consequently, ρ and ρ ′ can only take meaning with respect to the media under consideration. Thus, how did Planck possi- bly reach the conclusion that these values must be equal? At the onset in Eq. 19 [5, § 35], Planck sought to force ρ ν = ρ ′ ν , in general, by first making ρ ν = ρ ′ ν = 0, in particular. To accomplish this feat, he considered rays that were, “ polarized at right angles to the plane of inci- gle of polarization ” [5, § 37]. Again, such rays could never exist in the context of heat radiation [23, p. 450]. The “plane of incidence” is that containing the unit normal vector from the surface of incidence and the direction of the incident ray. There are two natural ways by which the orientation of an electromagnetic wave can be fixed; by the electric vector E or the magnetic vector B . Contemporary convention is to use the electric vector E [24, § 1.4.2]. Planck used the erstwhile magnetic vector convention. The “angle of polarization” is Brewster’s angle [23, p. 450]. The angle between reflected and refracted rays resulting from a given incident ray is then 90 o . The reflected wave is entirely plane-polarized ∗ , as shown in Figure 3, Planck’s medium 2 has a Brewster’s angle complementary to the Brewster’s angle of his medium 1 ( θ B + θ ′ B = 90 o ). Brewster’s angle is defined in terms of a reflected and a refracted beam. Unpolarized light, and plane-polarized light that is not “ at right angles to the plane of incidence ”, produce reflected and refracted beams, in accordance with Brewster’s Law. Planck invoked Brewster’s Law [23, p. 450] with the special condition that incident rays are orthogonal to the plane of incidence. In this case, there could be no reflection, but only refraction, in accordance with Snell’s Law. He simulta- neously applied these same restricted conditions to medium 2. “ Now in the special case when the rays are ...
Context 2
... 1: Expansion of Figure 3 in “The Theory of Heat Radiation” [5] depicting the full complement of rays involved in treating the interaction between two media separated by a “bounding surface” which contained a hypothetical element of interest, d σ . Planck considered the reflective nature of d σ to ascertain whether its reflection coe ffi cients were identical depending on whether the incident ray originated from medium 1, (A), or medium 2, (B). A) Schematic representation of the incident specific intensity, K ν (plain arrow), at an angle θ , contained in the conical section, d Ω , of the first medium (upper right quadrant) which is reflected by the bounding surface into the conical section d Ω in the upper left quadrant and refracted into the conical section d Ω ′ of the second medium, at an angle θ ′ , in the lower left quadrant. Note that in order to preserve the proper specific intensities, K ν , in the upper left quadrant, Planck must sum the reflected portion of the incident specific intensity of medium 1, ρ ν K ν , with the refracted portion of the incident specific intensity of medium 2, (1 − α ′ ν − ρ ν ′ ) K ′ ν , depicted in B. This fact is represented by the feathered arrow. However, he neglected to include that part of the specific intensity in the upper left quadrant was being produced by emission in that direction, η ν , by d σ . B) Schematic representation of the incident specific intensity, K ′ ν (plain arrow), at an angle θ ′ ,contained in the conical section, d Ω ′ , of the second medium (lower right quadrant) which  ...

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