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Snell law of refraction

Once the ray encounters the new surface Snells law of refraction is applied if it is a transparent surface (real index of refraction) or if it is a reflective surface... [Pg.38]

In some physical circumstances, we can derive familiar elements of the less fundamental theory from the more fundamental by straightforward limiting inferences. Thus if ordinary cases of refraction and reflection are what is being considered, we may simply derive a geometrical law of reflection or a Snell law of refraction from wave optics and Huygens principle, with, perhaps, applications of the method of going to the limit where wavelengths are small relative to macroscopic relevant features of the experimental setup. [Pg.238]

At point A in Figure 2.2, a ray of white light enters the medium and its velocity diminishes, with the result that its path is bent towards the normal at this point. Snell s law of refraction states that the relation between the angles of incidence (i) and refraction (r) is given by Equation 2.1, where n is the ratio of refractive indices of the medium and air. [Pg.82]

Snell s law of refraction may be solved graphically using slowness surfaces. It may be expressed as the requirement that the tangential component of the k-vector be conserved across a refracting interface. This is illustrated for waves in water incident on an (001) GaAs surface in Fig. 11.3. The slowness surfaces... [Pg.233]

The law of geometrical optics anticipated by Hero of Alexandria was formulated by Fermat (1601-1655) as a principle of least time, consistent with Snell s law of refraction (1621). The time for phase transmission from point P to point Q along a path x(r) is given by... [Pg.4]

Thus, an electromagnetic wave reflected at an interface between media of different refractive indices undergoes a phase shift of it radians when it is refracted, it suffers no phase shift. The fifth condition above is Snell s law of refraction ... [Pg.79]

FIGURE 5.4. (a) Snell s Law of Refraction, (b) total internal reflection, and (c) dispersion (the refractive index for violet light is greater than that for red light, therefore the deviation 62 is greater for red light). [Pg.148]

When a monochromatic ray of light passes from one isotropic medium (A) to another (B), it changes its wave velocity and direction. The change in direction is called refraction and the relationship between the angle of incidence and the angle of refraction is given by Snell s law of refraction, namely... [Pg.1336]

Figure 16.17 ( ) Snell s law of refraction, (b) Total internal reflection, (c) Light rays from point source enter at many angles. Rays that impinge at an angle that is less than the critical angle are guided down the optical waveguide by total internal reflection. Figure 16.17 ( ) Snell s law of refraction, (b) Total internal reflection, (c) Light rays from point source enter at many angles. Rays that impinge at an angle that is less than the critical angle are guided down the optical waveguide by total internal reflection.
This result, sometimes called Snell s law of refraction, shows that the sines of the angles of incidence and refraction must be proportional to the velocity of the light in the two given media in order that the light may pass from one point to the other in the shortest possible interval of time. Experiment justifies Fermat s guess. The ratio of the sines of the two angles, therefore, is constant for the same two media. The constant is usually denoted by the symbol p, and called the index of refraction. [Pg.165]

Around 1621, the Dutch scientist Wihibrod Snell discovered the correct law of refraction, which both Ptolemy and Alhazen were unable to deduce. By applying heuristic momentum conservation arguments in terms of sines, Rene Descartes independently derived the law in his 1637 philosophical and mathematical treatise. Discourse on Method. Descartes was able to solve several optical problems with the aid of this law. [Pg.37]

The expression P = (1 + cos 20)/2 is called the polarization factor. For a partially polarized primary beam, the expectation values < cos fi > and < sin fi > are different from 1/2.20 is the angle between Sq and s, i.e. between the direction of the primary beam and that of the scattered beam or the direction of observation. It must be noted that the scattered beams are partially polarized. When the angle 20 = 90°, the polarization is total. This corresponds to Brewsters Law the reflection from a mirror is totally polarized if the refracted and reflected beams are perpendicular. According to Snell s law of refraction, half of the angle between the incident and reflected beams is given by cot 6 = n where n is the index of refraction. For X-rays, n=i and hence 20 = 90°. Any reflection of light from... [Pg.101]

Figure 3 Graphic illustration of Snell s law of refraction. (A) Refracted and reflected light beam at the refractive index boundary for n, > ri2. (B) The refraction of the plane wave. Reflected wave is not shown. Figure 3 Graphic illustration of Snell s law of refraction. (A) Refracted and reflected light beam at the refractive index boundary for n, > ri2. (B) The refraction of the plane wave. Reflected wave is not shown.
Snell s law n. Snell s law of refraction states that if i is the angle of incidence through a transparent medium, r is the angle of refraction, the index of refraction n, then... [Pg.896]

Viner etal. found that Snell s law of refraction can be applied to quasi-two-dimensional fronts [109]. They prepared mixtures of a triacrylate with kaolin clay and peroxide and spread them into slabs. Figure 4.17 shows fronts propagating in such slabs. The upper slab contained less peroxide and so it propagated more slowly. [Pg.59]

D., and Gross, L. (2007) Snell s law of refraction observed in thermal frontal polymerization. Chaos, 17, 033125. [Pg.67]

Pojman etal developed a system for studying Snell s Law of refraction in FP. Using trimethylolpropane triacrylate with 47% by mass kaolin clay (Polygloss 90), they created a formulation with the consistency of a putty, which could be molded into desired shapes. Viner et a used fillers that were inert but melted, so-called phase change materials, in an attempt to lower the front temperature without significantly reducing the front velocity. [Pg.973]

The interference fit specimens were placed on a vee block within the scanning tank and the transducer height set to scan the sleeve/shaft interface. The ultrasonic wave is refracted at the water/steel interface. The height of the transducer required to focus the wave on the interference interface was calculated using Snell s law of refraction (see Figure 5). [Pg.452]


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