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Template, para los anteproyectos de laboratorio eléctrico UCR.

UIT Template Report

Welcome to the MAT320 Homework template on Overleaf — just edit your LaTeX on the left, and we'll compile it for you on the right. (Based on a homework template by Dana Ernst.)

A book on Docker in Portuguese, created using the Legrand Orange Book LaTeX Template from LaTeXTemplates.com. The Legrand Orange Book template was created by Mathias Legrand (legrand.mathias@gmail.com) with modifications by Vel (vel@latextemplates.com) and made available under a CC BY-NC-SA 3.0 license.

A presentation to Faculty of Engineering, University of Ghent, approximating the FirW house style. Voor een presentatie aan de Faculteit Ingenieurswetenschappen kan je de template van Harald Devos gebruiken, die een goede benadering is van de officiële FirW-huisstijl. Mits enige aanpassing is deze stijl ook te gebruiken voor andere faculteiten of aan te passen richting algemene UGent-huisstijl. (Downloaded from LaTeX templates en logo's)

Exemplo de representação da diluição da rede quadrada com o pacote pstricks.

In this project the behavior of the Faraday cage as an insulator against an induced load, either by an effect of nature as lightning or lightning or power surges be considered. As we know the Faraday cage is a conductor of electric current and therefore theoretically there will be inside a magnetic field or electromagnetic wave in the same way there will be no magnetic field.

The differential wave equation can be used to describe electromagnetic waves in a vacuum. In the one dimensional case, this takes the form $\frac{\partial^2\phi}{\partial x^2}-\frac{1}{c^2}\frac{\partial^2\phi}{\partial t^2} = 0$. A general function $f(x,t) = x \pm ct$ will propagate with speed c. To represent the properties of electromagnetic waves, however, the function $\phi(x,t) = \phi _0 sin(kx-\omega t)$ must be used. This gives the Electric and Magnetic field equations to be $E (z,t) = \hat{x} E _0 sin(kz-\omega t)$ and $B (z,t) = \hat{y} B _0 sin(kz-\omega t)$. Using this solution as well as Maxwell's equations the relation $\frac{E_0}{B_0} = c$ can be derived. In addition, the average rate of energy transfer can be found to be $\bar{S} = \frac{E_0 ^2}{2 c \mu _0} \hat{z}$ using the poynting vector of the fields.

This is a modified version of the Tufte Book example, but with the title page and the contents page resembling Tufte's VDQI book, using Kevin Godby's code from this thread.