By Eduardo E Zurek Affiliation: Departamento de Ingeniería de Sistemas, Universidad del Norte, Km. 5 Vía a Puerto Colombia, Barranquilla, Colombia; Wilfrido A Moreno Affiliation: Electrical Engineering Department, University of South Florida, Tampa, FL 336
This paper introduces a brand new software to procedure the results of a diffraction grating and its interplay with different optical and digital parts in a mild wavelength research approach. The model's theoretical historical past is defined. This version is meant for tutorial reasons and it truly is spoke of a miniaturized spectrophotometer. © 2011 Wiley Periodicals, Inc. Comput Appl Eng Educ 22:187-194, 2014; View this article on-line at wileyonlinelibrary.com/journal/cae; DOI 10.1002/cae.20544 Read more...
summary: This paper introduces a brand new software to technique the consequences of a diffraction grating and its interplay with different optical and digital elements in a gentle wavelength research process. The model's theoretical heritage is defined. This version is meant for tutorial reasons and it's observed a miniaturized spectrophotometer. © 2011 Wiley Periodicals, Inc. Comput Appl Eng Educ 22:187-194, 2014; View this text on-line at wileyonlinelibrary.com/journal/cae; DOI 10.1002/cae.20544
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Extra info for A numerical simulation model to facilitate the understanding of the properties of a diffraction grating
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The parameter w is called the spot size of the beam. w depends on the z-coordinate. The intensity profile is Gaussian; hence the beam is called a Gaussian beam. Such a beam maintains its profile as it propagates. The Gaussian beam has a very special place in optics, and is often used for measurement. 11) where A and w0 are constants and ϕ = tan−1 (λz/w02 ). The constant w0 is called the beam waist size and w(z) is called the spot size. We introduce another constant, called the Rayleigh range z0 , which is related to the beam waist size by z0 = πw02 /λ.