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![Formulario Segundo Parcial Fenomenos de transporte 3](https://writelatex.s3.amazonaws.com/published_ver/7189.jpeg?X-Amz-Expires=14400&X-Amz-Date=20240630T192451Z&X-Amz-Algorithm=AWS4-HMAC-SHA256&X-Amz-Credential=AKIAWJBOALPNFPV7PVH5/20240630/us-east-1/s3/aws4_request&X-Amz-SignedHeaders=host&X-Amz-Signature=ede74b32dda8145ba7bc356302b782b9b2ee5c69e09637f6051b518d4cb2a4b5)
Formulario Segundo Parcial Fenomenos de transporte 3
Detalles de formulas utilizadas parcial segundo fenomenos de tranporte 3 FCQ-UNA
Oscar Daniel Rivas Villar
![Ritabh Ranjan's CV](https://writelatex.s3.amazonaws.com/published_ver/5738.jpeg?X-Amz-Expires=14400&X-Amz-Date=20240630T192451Z&X-Amz-Algorithm=AWS4-HMAC-SHA256&X-Amz-Credential=AKIAWJBOALPNFPV7PVH5/20240630/us-east-1/s3/aws4_request&X-Amz-SignedHeaders=host&X-Amz-Signature=bb0fba81555dbebcd5007c2aca3a7789fc97e0f50a8bdae0e9b26d0f0fb35bff)
Ritabh Ranjan's CV
Ritabh Ranjan's CV
Ritabh Ranjan
![My Final Proof Journal](https://writelatex.s3.amazonaws.com/published_ver/3785.jpeg?X-Amz-Expires=14400&X-Amz-Date=20240630T192451Z&X-Amz-Algorithm=AWS4-HMAC-SHA256&X-Amz-Credential=AKIAWJBOALPNFPV7PVH5/20240630/us-east-1/s3/aws4_request&X-Amz-SignedHeaders=host&X-Amz-Signature=225a75afa77eae7d61f87d7d8a6f9052880d6d7a84d2aae2b5cf7892a9482b78)
My Final Proof Journal
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This is all preamble stuff that you don't have to worry about.
Head down to where it says "Start here"
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Chesyti Brown
![Docker: O fim do "na minha máquina funciona"](https://writelatex.s3.amazonaws.com/published_ver/2121.jpeg?X-Amz-Expires=14400&X-Amz-Date=20240630T192451Z&X-Amz-Algorithm=AWS4-HMAC-SHA256&X-Amz-Credential=AKIAWJBOALPNFPV7PVH5/20240630/us-east-1/s3/aws4_request&X-Amz-SignedHeaders=host&X-Amz-Signature=d91e2d3738247fcf31c7e8825f8699db40449d147f26ee74d084691f3f14f5bf)
Docker: O fim do "na minha máquina funciona"
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.
Rafael Gomes
![A Última Palavra de Jesus na Cruz](https://writelatex.s3.amazonaws.com/published_ver/2191.jpeg?X-Amz-Expires=14400&X-Amz-Date=20240630T192451Z&X-Amz-Algorithm=AWS4-HMAC-SHA256&X-Amz-Credential=AKIAWJBOALPNFPV7PVH5/20240630/us-east-1/s3/aws4_request&X-Amz-SignedHeaders=host&X-Amz-Signature=dfe64bbbf65436920539491386aa2e3c7355c9145582b4bfadd92ee0fed54b6c)
A Última Palavra de Jesus na Cruz
Pregação baseada no Sermão pregado na noite de Domingo, 9 de Junho de 1889; Por Charles Haddon Spurgeon; No Tabernáculo Metropolitano, Newington, Londres. E selecionado para leitura em 4 de junho de 1893
Egmon
![Técnicas experimentales, Experimento 1](https://writelatex.s3.amazonaws.com/published_ver/2181.jpeg?X-Amz-Expires=14400&X-Amz-Date=20240630T192451Z&X-Amz-Algorithm=AWS4-HMAC-SHA256&X-Amz-Credential=AKIAWJBOALPNFPV7PVH5/20240630/us-east-1/s3/aws4_request&X-Amz-SignedHeaders=host&X-Amz-Signature=ed5e6de45d1194fee02845d18e735fd07cfbf42332000b44775d004084b9091e)
Técnicas experimentales, Experimento 1
En ésta páctica medimos y cuantificamos algunas de las propiedades de diferentes rocas, como la densidad y la masa, utilizando los equipos necesarios y comparándolas entre ellas para saber como es el comportamiento de las rocas que recolectamos. Al finalizar de hacer experimentos con las diferentes rocas, se compararon los resultados con los de otro equipo y se observ ́o que ambos resultados eran similares, lo que indica que cada tipo de roca tiene características diferentes de las demás, como su porosidad o densidad, independientemente de su masa o volumen.
EmilianoPadilla
![Finding Bounds on Ehrhart Quasi-Polynomials](https://writelatex.s3.amazonaws.com/published_ver/3810.jpeg?X-Amz-Expires=14400&X-Amz-Date=20240630T192451Z&X-Amz-Algorithm=AWS4-HMAC-SHA256&X-Amz-Credential=AKIAWJBOALPNFPV7PVH5/20240630/us-east-1/s3/aws4_request&X-Amz-SignedHeaders=host&X-Amz-Signature=f79e58b4f587344edbac51d16322bd8db4bc8e1cc39052028e4ff6e9f678d6e9)
Finding Bounds on Ehrhart Quasi-Polynomials
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)
Harald Devos (uploaded by LianTze Lim)
![Proyecto: Jaula de Faraday](https://writelatex.s3.amazonaws.com/published_ver/4330.jpeg?X-Amz-Expires=14400&X-Amz-Date=20240630T192451Z&X-Amz-Algorithm=AWS4-HMAC-SHA256&X-Amz-Credential=AKIAWJBOALPNFPV7PVH5/20240630/us-east-1/s3/aws4_request&X-Amz-SignedHeaders=host&X-Amz-Signature=15d4a4efd0d98ef9b16968148069c443d31dd9913731b6393a7b75b89dc1a16e)
Proyecto: Jaula de Faraday
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.
Eduardo
![Using the One Dimensional Wave Equation to Represent Electromagnetic Waves in a Vacuum](https://writelatex.s3.amazonaws.com/published_ver/3805.jpeg?X-Amz-Expires=14400&X-Amz-Date=20240630T192451Z&X-Amz-Algorithm=AWS4-HMAC-SHA256&X-Amz-Credential=AKIAWJBOALPNFPV7PVH5/20240630/us-east-1/s3/aws4_request&X-Amz-SignedHeaders=host&X-Amz-Signature=a3c37e8d681c12203120f3259e1cc8de991b2aa07c2c2b1fb3eacd764f866113)
Using the One Dimensional Wave Equation to Represent Electromagnetic Waves in a Vacuum
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.
Eric Minor