Energetic space

In mathematics, more precisely in functional analysis, an energetic space is, intuitively, a subspace of a given real Hilbert space equipped with a new "energetic" inner product. The motivation for the name comes from physics, as in many physical problems the energy of a system can be expressed in terms of the energetic inner product. An example of this will be given later in the article.

Energetic space

Formally, consider a real Hilbert space $X$ with the inner product $(\cdot|\cdot)$ and the norm $\|\cdot\|$ . Let $Y$ be a linear subspace of $X$ and $B:Y\to X$ be a strongly monotone symmetric linear operator, that is, a linear operator satisfying

$(Bu|v)=(u|Bv)\,$ for all $u, v$ in $Y$
$(Bu|u) \ge c\|u\|^2$ for some constant $c>0$ and all $u$ in $Y.$

The energetic inner product is defined as

: $(u|v)_E =(Bu|v)\,$ for all $u,v$ in $Y$

and the energetic norm{{anchor|energetic norm}} is

: $\|u\|_E=(u|u)^\frac{1}{2}_E \,$ for all $u$ in $Y.$

The set $Y$ together with the energetic inner product is a pre-Hilbert space. The energetic space $X_E$ is defined as the completion of $Y$ in the energetic norm. $X_E$ can be considered a subset of the original Hilbert space $X,$ since any Cauchy sequence in the energetic norm is also Cauchy in the norm of $X$ (this follows from the strong monotonicity property of $B$ ).

The energetic inner product is extended from $Y$ to $X_E$ by

: $(u|v)_E = \lim_{n\to\infty} (u_n|v_n)_E$

where $(u_n)$ and $(v_n)$ are sequences in Y that converge to points in $X_E$ in the energetic norm.

Energetic extension

The operator $B$ admits an energetic extension $B_E$

: $B_E:X_E\to X^*_E$

defined on $X_E$ with values in the dual space $X^*_E$ that is given by the formula

: $\langle B_E u | v \rangle_E = (u|v)_E$ for all $u,v$ in $X_E.$

Here, $\langle \cdot |\cdot \rangle_E$ denotes the duality bracket between $X^*_E$ and $X_E,$ so $\langle B_E u | v \rangle_E$ actually denotes $(B_E u)(v).$

If $u$ and $v$ are elements in the original subspace $Y,$ then

by the definition of the energetic inner product. If one views $Bu,$ which is an element in $X,$ as an element in the dual $X^*$ via the Riesz representation theorem, then $Bu$ will also be in the dual $X_E^*$ (by the strong monotonicity property of $B$ ). Via these identifications, it follows from the above formula that $B_E u= Bu.$ In different words, the original operator $B:Y\to X$ can be viewed as an operator $B:Y\to X_E^*,$ and then $B_E:X_E\to X^*_E$ is simply the function extension of $B$ from $Y$ to $X_E.$

An example from physics

File:String illust.svg

Consider a string whose endpoints are fixed at two points $a on the real line (here viewed as a horizontal line). Let the vertical outer force density at each point x (a\le x \le b) on the string be f(x)\mathbf{e}, where \mathbf{e} is a unit vector pointing vertically and f:[a, b]\to \mathbb R. Let u(x) be the deflection of the string at the point x under the influence of the force. Assuming that the deflection is small, the elastic energy of the string is$

: $\frac{1}{2} \int_a^b\! u'(x)^2\, dx$

and the total potential energy of the string is

: $F(u) = \frac{1}{2} \int_a^b\! u'(x)^2\,dx - \int_a^b\! u(x)f(x)\,dx.$

The deflection $u(x)$ minimizing the potential energy will satisfy the differential equation

: $-u''=f\,$

with boundary conditions

: $u(a)=u(b)=0.\,$

To study this equation, consider the space $X=L^2(a, b),$ that is, the Lp space of all square-integrable functions $u:[a, b]\to \mathbb R$ in respect to the Lebesgue measure. This space is Hilbert in respect to the inner product

: $(u|v)=\int_a^b\! u(x)v(x)\,dx,$

with the norm being given by

: $\|u\|=\sqrt{(u|u)}.$

Let $Y$ be the set of all twice continuously differentiable functions $u:[a, b]\to \mathbb R$ with the boundary conditions $u(a)=u(b)=0.$ Then $Y$ is a linear subspace of $X.$

Consider the operator $B:Y\to X$ given by the formula

: $Bu = -u'',\,$

so the deflection satisfies the equation $Bu=f.$ Using integration by parts and the boundary conditions, one can see that

: $(Bu|v)=-\int_a^b\! u''(x)v(x)\, dx=\int_a^b u'(x)v'(x) = (u|Bv)$

for any $u$ and $v$ in $Y.$ Therefore, $B$ is a symmetric linear operator.

$B$ is also strongly monotone, since, by the Friedrichs's inequality

: $\|u\|^2 = \int_a^b u^2(x)\, dx \le C \int_a^b u'(x)^2\, dx = C\,(Bu|u)$

for some $C>0.$

The energetic space in respect to the operator $B$ is then the Sobolev space $H^1_0(a, b).$ We see that the elastic energy of the string which motivated this study is

: $\frac{1}{2} \int_a^b\! u'(x)^2\, dx = \frac{1}{2} (u|u)_E,$

so it is half of the energetic inner product of $u$ with itself.

To calculate the deflection $u$ minimizing the total potential energy $F(u)$ of the string, one writes this problem in the form

: $(u|v)_E=(f|v)\,$ for all $v$ in $X_E$ .

Next, one usually approximates $u$ by some $u_h$ , a function in a finite-dimensional subspace of the true solution space. For example, one might let $u_h$ be a continuous piecewise linear function in the energetic space, which gives the finite element method. The approximation $u_h$ can be computed by solving a system of linear equations.

The energetic norm turns out to be the natural norm in which to measure the error between $u$ and $u_h$ , see Céa's lemma.

References

{{cite book

| last = Zeidler

| first = Eberhard

| title = Applied functional analysis: applications to mathematical physics

| publisher = New York: Springer-Verlag

| date = 1995

| pages =

| isbn = 0-387-94442-7

| url = https://books.google.com/books?id=bFqRaovfY4MC&q=%22energetic+space%22

}}

{{cite book

| last = Johnson

| first = Claes

| title = Numerical solution of partial differential equations by the finite element method

| publisher = Cambridge University Press

| date = 1987

| pages =

| isbn = 0-521-34514-6

}}

Category:Functional analysis

Category:Hilbert spaces

Energetic space

Energetic space

Energetic extension

An example from physics

See also

References