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# Fundamentals of FEM

## Chapter 1

Intro to 1 Degree of Freedom Second Order PDE

Appendix 4.I.1

Equivalence of Strong and Weak Forms

Global and Local Coordinates

Method of Weighted Residuals&#x20;

Chapter 2

Heat Transfer&#x20;

Elastostatics

FE Pseudocode

### Linear Space&#x20;

Vectors will appear in the problems, so it is important to note that they are distinct from scalars that most people are used to. Rather than a single value, they are list of multiple scalars collected into a single object and reside in a space, $$\mathcal{L}$$. Vectors obey addition and multiplication rules, though differently traditional scalars.&#x20;

#### Vector Addition

$$
\begin{align}
{\bf u}+{\bf v}&=\left(u\_{1}, u\_{2}, u\_{3}, \ldots u\_{n}\right)+\left(v\_{1}, v\_{2}, v\_{3}, \ldots v\_{n}\right)\\
&=\left(u\_{1}+v\_{1}, u\_{2}+v\_{2}, u\_{3}+v\_{3}, \ldots u\_{n}+v\_{n}\right)
\end{align}
$$

Note that subraction works the same as addition using negative vectors, just like how subtraction of scalars is addition using a negative number.

#### Vector Multiplcation

Multiplication of a vector by a scalar is communitive, just like two scalars.&#x20;

### Inner Product


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