# Nonlinear finite elements/Functions

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There are certain terms involving relationships between functions that you will often encounter in papers dealing with finite elements and continuum mechanics. We list some of the basic terms that you will see. More details can be found in books on advanced calculus and functional analysis.

## Functions edit

Let and be two sets. A function is a rule that assigns to each an element of . A function is usually denoted by

Sometimes, one also writes

For example, if the function is , then we may write .

## Domain and Range edit

For a function , the set is called the* domain* of . See Figure 1.

The *range* of is the set

Therefore, .

## One-to-one mapping (injection) edit

A function is called *one-to-one* (or an *injection*) if no two distinct elements of are mapped to the same element of .

## Onto mapping (surjection) edit

A function is called *onto* if for every
there is an such that .

If that case, .

## One-to-one and onto mapping (bijection) edit

When a mapping is both one-to-one and onto it is called a *bijection*. For example, if and with

the map is one-to-one and onto.

On the other hand, if

the map is one-to-one but not onto.

If we choose

the map is neither one-to-one nor onto.

## Image, pre-image, and inverse functions edit

Suppose we have a function . Let be a subset of (see Figure~1). Let us define

Then, is called the *image* of .

On the other hand, if is a subset of and we define

Then, is called the *inverse image* or* pre-image* of .

If is *one-to-one and onto*, then there is a unique function such that

The function is called an* inverse function* of .

## Identity map edit

The map such that for all is called the* identity map*. This map is one-to-one and onto.

## Composition edit

A notation that you will commonly see in papers on nonlinear solid mechanics is the* composition* of two functions. See Figure 2.

Let and be two functions such that and
. The* composition* is defined as

Let us consider a stretch ( ) followed by a translation ( ). Then we can write and .

The composition is given by

The inverse composition is given by

## Isomorphism and Homeomorphism edit

You will also come across the terms* isomorphism* and *homeomorphism* in the literature on nonlinear solid mechanics.

* Isomorphism* is a very general concept that appears in several areas of mathematics. The word means, roughly, "equal shapes". It usually refers to one-to-one and onto maps that preserve relations among elements.

A *homeomorphism* is a continuous transformation between two geometric figures that is continuous in both directions. The map has to be one-to-one to be homeomorphic. It also has to satisfy the requirements on an equivalence relation.

## Continuously differentiable functions edit

A function

is said to be * -times continuous differentiable* or *of class * if its derivatives of order (where ) exist and are continuous functions.

Figure 3 shows three functions ( , , ) and their derivatives.

### C^{-1} Functions
edit

The function is called the* Heaviside step function* (usually written ) which is defined as

The derivative of the Heaviside function is the* Dirac delta function* (written ) which has the defining property that

for any function and any constant . The delta function is singular and discontinuous. Hence, the Heaviside function is not continuously differentiable. Sometimes the Heaviside function is said to belong to the class of functions.

### C^{0} Functions
edit

The function in Figure 3 (also called a* hat *function) is continuous but has discontinuous derivatives. In this particular case, the function has the form

Such functions that are differentiable only once are called functions.

### C^{∞} Functions
edit

The function in Figure 3 is infinitely differentiable and has continuous derivatives every time it is differentiable. Such functions are called functions. Since the function can be differentiated once to give a continuous derivative, it also falls into the category of functions.

## Sobolev spaces of functions edit

You will find Sobolev spaces being mentioned when you read the finite element literature. A clear understanding of these function spaces needs a knowledge of functional analysis. The book *Introduction to Functional Analysis with Applications to Boundary Value Problems and Finite Elements* by B. Daya Reddy is a good starting point that is just right for engineers. We will not get into the details here.

Of particular interest in finite element analysis are Sobolev spaces of functions such as

where

The function space is the space of **square integrable functions**.

Of interest to us is an outcome of Sobolev's* theorem* which says that if a function is of class then it is actually a bounded function. If we choose our basis functions from the set of square integrable functions with continuous derivatives, certain singularities are automatically precluded.