„Experiments with Polarized Light” változatai közötti eltérés

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(Új oldal, tartalma: „--Investigation of Liquid Crystal Displays-- ---Liquid Crystals--- <wlatex> Liquid crystal (LC) is a state of matter that is intermediate between the crystalline solid…”)
 
19. sor: 19. sor:
 
in general, there are two speeds of propagation. The electric field of the light polarized
 
in general, there are two speeds of propagation. The electric field of the light polarized
 
perpendicular (or parallel) to the optical axis travels with the speed of $v_o = c / n_o$ (or
 
perpendicular (or parallel) to the optical axis travels with the speed of $v_o = c / n_o$ (or
$n_e v = c / n_e$, where $n_e$ is called the extraordinary index of refraction). The birefringence
+
$v_e = c / n_e$, where $n_e$ is called the extraordinary index of refraction). The birefringence
 
(optical anisotropy) is defined as the difference between the extraordinary and the ordinary
 
(optical anisotropy) is defined as the difference between the extraordinary and the ordinary
indices of refraction $\Delta n = n_e − n_o$.
+
indices of refraction $n = n_e − n_o$.
 
</wlatex>
 
</wlatex>

A lap 2017. szeptember 17., 06:36-kori változata

--Investigation of Liquid Crystal Displays--

---Liquid Crystals---


Liquid crystal (LC) is a state of matter that is intermediate between the crystalline solid and the amorphous liquid. The nematic LCs are organic compounds consisting of long-shaped needle-like molecules. The orientation of the molecules can be easily aligned and controlled by applying an electrical field. Uniform or well prescribed orientation of the LC molecules is required in most LC devices. The structure of the LC cell used in this experiment is shown in Fig 1. Rubbing the polyimide film can produce a well-aligned preferred orientation for LC molecules on substrate surfaces, thus due to the molecular interaction the whole slab of LC can achieve uniform molecular orientation. The local molecular orientation is called the director of LC at that point. The LC cell exhibits the so-called double refraction phenomenon with two principal refractive indices. When light propagates along the direction of the director, all polarization components travel with the same speed \setbox0\hbox{$v_o = c / n_o$}% \message{//depth:\the\dp0//}% \box0% , where \setbox0\hbox{$n_o$}% \message{//depth:\the\dp0//}% \box0% is called the ordinary index of refraction. This propagation direction (direction of the director) is called the optical axis of the LC cell. When a light beam propagates in the direction perpendicular to the optical axis, in general, there are two speeds of propagation. The electric field of the light polarized perpendicular (or parallel) to the optical axis travels with the speed of \setbox0\hbox{$v_o = c / n_o$}% \message{//depth:\the\dp0//}% \box0% (or \setbox0\hbox{$v_e = c / n_e$}% \message{//depth:\the\dp0//}% \box0%, where \setbox0\hbox{$n_e$}% \message{//depth:\the\dp0//}% \box0% is called the extraordinary index of refraction). The birefringence (optical anisotropy) is defined as the difference between the extraordinary and the ordinary

indices of refraction LaTex syntax error
\setbox0\hbox{$n = n_e − n_o$}%
\message{//depth:\the\dp0//}%
\box0%
.