Gallery Items tagged Math
Recent

Notions principales de la thermodynamique
Chapitre 1, Peip1, Polytech'Nice Sophia
Rémy Collie

Generational Economics Assignment 4 (Part A)
Deze ding
Georges de Boeck

Time-Frequency Analysis and the Wavelet Transform
A brief (lets not kid ourselves its long) introduction to the continuous and discrete wavelet transforms. Comments on implementations on the computer using MATLAB and other software is also included.
ryanplestid

Bayes' Theorem in Baseball
A basic understanding on Bayes' theorem and how to apply it to baseball statistics.
Christopher Amici

SU MAT320 Homework Template (Bryant)
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.)
Lance Bryant

Formulario Segundo Parcial Fenomenos de transporte 3
Detalles de formulas utilizadas parcial segundo fenomenos de tranporte 3 FCQ-UNA
Oscar Daniel Rivas Villar

My Final Proof Journal
--------------------------------------------------------------
This is all preamble stuff that you don't have to worry about.
Head down to where it says "Start here"
--------------------------------------------------------------
Chesyti Brown

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

Midtvejsrapportskabelon - Førsteårsprojekt i matematik (MatProjekt)
Skabelon til midtvejsrapporten for kurset Førsteårsprojekt i matematik ved Institut for Matematiske Fag, Københavns Universitet
Astrid Steen Rasmussen & Abrahim Borgi