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On Differential Forms

Original post is here eklausmeier.goip.de/blog/2015/03-15-on-differential-forms-2.


Abstract. This article will give a very simple definition of k-forms or differential forms. It just requires basic knowledge about matrices and determinants. Furthermore a very simple proof will be given for the proposition that the double outer differentiation of k-forms vanishes.

MSC 2010: 58A10

1. Basic definitions

We denote the submatrix of A=(aij)Rm×n consisting of the rows i1,,ik and the columns j1,,jk with

[A]j1i1jkik:=(ai1j1ai1jkaikj1aikjk)
and its determinant with
Aj1i1jkik:=det[A]j1i1jkik.

For example

A=(a11a12a13a21a22a23),A1,21,3=a11a23a21a13.

Suppose

HRn×(n+1)

and let

f,g:URnR,U open,

be two functions which are two-times continuously differentiable. Then we call for a fixed k the expression

fHα1k,α=(i1,,ik){1,,n}k,

a basic k-form or basic differential form of order k. It's a real function of n+k2 variables. For k>n the expression is defined to be zero. If f also depends on α then

1i1<<iknfi1ikH1i1kik

is called a k-form. It's a real function of n+kn variables which is k-linear in the k column-vectors of H.

For example for f:RR and HR1×1 we have f(x),H. This is a linear function in H and a possibly non-linear function in x.

2. Differentiation of k-forms

For the differential form

ω=fHα1k,α=(i1,,ik),

we define

dω:=ν=1nfxνHν,α1k+1

as the outer differentiation of ω. This is a (k+1)-form. It's a function of n+(k+1)n variables.

The 0-form

ω=f,|α|=k=0

yields

(1)dw=ν=1nfxνHν1,

which corresponds to f=gradf.

In the special case k=|α|=1 we get for

ω=i=1nfiHi1

the result

(2)dω=i=1nj=1nfixjHj,i1,2=i<j(fixjfjxi)Hj,i1,2.

This corresponds to rotf.

Let hat (^) mean exclusion from the index list. The case k=n1 for

ω=i=1n(1)i1fiH1ı^n1n1

delivers

dw=i=1nν=1n(1)i1fixνHν,1ı^n1n=i=1nfixνH1n1n=(i=1nfixi)detH.

This corresponds to divf.

Theorem. For ω=fHα1k we have

ddω=0.

Proof: With

dω=ν=1nfxνHν,α1k+1

we get

ddω=ν=1nμ=1n2fxνxμHμ,ν,α1k+2

and this is zero, because

Hμ,μ,α1k+2=0,Hμ,ν,α1k+2=Hν,μ,α1k+2,

and

2fxνxμ=2fxμxν.

Application of this theorem to an 0-form with an f:URnR and a 1-form with an a:URn reading (1) and then (2) yields

rotgradf=0,divrota=0.

The second equation is only true for n=3 because

(n2)=n(nN)n=3.

Definition. Suppose

ϕ:DERn,DRk,

is differentiable, its derivative denoted by ϕ, and

f:ER.

For the differential form ω=fHα1k we define the back-transportation as

ϕω:=(fϕ)(ϕ)α1k

and the integral over k-forms as

ϕω:=Dϕω.

For example the case k=1,

ω=i=1nfiHi1

gives

ϕω=i=1n(fiϕ)(ϕ)i1.

3. The outer product of differential forms

Suppose

HRn×(n+1),k+mn.

For the two differential forms

ω=1i1<<iknfi1ikH1i1kik

and

λ=1j1<<jmngj1jmHk+1j1k+mjm

the outer product is defined as

wλ:=1i1<<ikn1j1<<jmnfi1ikgj1jmH1i1kikk+1j1k+mjm.

This is a differential form of order k+m. It's a function in n+(k+m)n variables.

Theorem.

d(ωλ)=dωλ+(1)kωdλ

Proof: With

ω=αfαHα1k,λ=βgβHβ1m

then

d(ωλ)=α,βν=1n(fαxνgβ+fβgβxν)Hν,α,β1k+m+1=α,βν=1nfαxνgβHν,α,β1k+m+1+α,βν=1nfαgβxνHν,α,β1k+m+1=dωλ+(1)kωdλ,

due to

Hν,α,β1k+m+1=(1)kHν,β,α1k+m+1

and

dλ=βν=1ngβxνHν,β1m+1.

An alternative definition for the differentiation of k-forms could be given.

Theorem. Suppose

ω=fHα1k,0|α|k,

and

H=(h1,,hn,hn+1)Rn×(n+1)

with α=(i1,,ik) we have

dω=det(col(f,[Idn]α1n)[H]1n1k+1)=ν=1nfxνHν,α1k+1,

where col just stacks matrices one above another and Idn is the identity matrix in Rn.

Proof:

dω=|f,h1f,hkf,hk+1ei1,h1ei1,hkei1,hk+1eik,h1eik,hkeik,hk+1|
=ν=1nfxν|h1,νh1,i1h1,ikhk,νhk,i1hk,ikhk+1,νhk+1,i1hk+1,ik|

since

f,h1=ν=1nfxνh1,ν,
f,hk+1=ν=1nfxνhk+1,ν.

REFERENCES.

  1. Walter Rudin, Principles of Mathematical Analysis, Second Edition, McGraw-Hill, New York, 1964

  2. Otto Forster, Analysis 3: Integralrechnung im Rn mit Anwendungen, Third Edition, Friedrich Vieweg & Sohn, Braunschweig/Wiesbaden, 1984