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Overzicht van definities en stellingen bij vectorvelden, naar

Kowalsky

Citation for published version (APA):

Meiden, van der, W. (1975). Overzicht van definities en stellingen bij vectorvelden, naar Kowalsky. (Eindhoven University of Technology : Dept of Mathematics : memorandum; Vol. 7501). Technische Hogeschool Eindhoven.

Document status and date: Gepubliceerd: 01/01/1975 Document Version:

Uitgevers PDF, ook bekend als Version of Record Please check the document version of this publication:

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• The final author version and the galley proof are versions of the publication after peer review.

• The final published version features the final layout of the paper including the volume, issue and page numbers.

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(2)

TECHNISCHE HOGESCHOOL EINDHOVEN Onderafdeling der Wiskunde.

Memorandum 1975-01 j anuari 1975

Overzicht van definities en stellingen bij vectorvelden, naar Kowalsky

door

W. van der Meiden

Technische Hogeschool Onderafdeling der Wiskunde PO Box 513, Eindhoven Nederland

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Overzicht van definities en stellingen bij vectorvelden, naar Kowalsky Deformatie. A: J

~

CI(D,X) met J E N(O)

in~,

DC'X

=

~n,

en A(O)

=

IdID.

Lineaire deformatie. D = X en A (J) C £ (X,X).

Divergentie van een lineaire deformatie. div A :=

~

det A(t) I 0'"

dt t:=

1. div A

=

spoo~ A(O).

2. Als A E £ (X,X) 'zijn er een a E £ (X,X) en een T E £ (X,X) ZQ dat

i) T is orthogonaal.

ii) a is positief definiet (en symmetrisch). iii) A

=

T 0 a,

en deze decompositie is eenduidig.

Het geval van een positief definiete lineaire deformatie a. 3. ~(t) is symmetrisch.

4. (CI (t), ••• 'Cn (t)) := spec a (t), {~1 (t), ••• '~n (t)} is de bijbehorende or-thonormale basis van eigenvectoren; dan

i)

v.

C.

(0) E spec ~ (0) •

1 1

ii) Voor rijen t. ~ 0 met e. * = lime.(t.) is e. * eigenvector bij

J -1 j-+oo -J J 1 6" (0) •

Het geval van een orthogonale lineaire deformatie T •. , 5. t(t) is scheefsymmetrisch.

6. Zij T(t.)a(t.)

=

a(t.), t. ~ 0 en a(t.) ~ a*; dan is t(O)_a*

=

£.

1 - 1 - 1 1 - 1

-c.

(0) van

1

7. Zij M. (t) := M[e! (t) ,e'~ (t) ] een invariante deelruimte van T (t) met

J - J - J

{e! (t) ,e'! (t)} als orthonormale basis en T (t) I M. (t)

=

D (t) ,

-J -J J Cij e

~k)

:= lim e

~k)

(t) (k = 1,2); dan -J t~ -J i) ii) lim Ci. (t) t~O J a. (0)2 is J

=

o.

e.w. bij _teO) 0 teO)

Het algemene geval A(t)

=

T(t) 0 a(t).

8. T(O)

=

a(O)

=

Id.

met e. v.

9. 20(0) =

~(O)

+

~(O)T,

2t(0) =

~(O)

-

~(O)T.

Rotatie van een lineaire deformatie. rot A =

2a(0)~;

X =

~3;

hierin is (zie 7ii)

.=. :=.=.'

x e" met &(0) ~ O.

(4)

2

-. Ret geval van strorrring: q): D x J -+ JRll, met D C JRn: J c lR en cp

(~,O)

=

11. [DICP(~,t)J is een lineaire deformatie.

12. (D2CP(~,t)J is de snelheidsverdeling van de stroming.

13. Iedere ~: lRn -+lRn is snelheidsverdeling van een stroming, bijv.

cp(~,t) := ~ + t~(~)

Divergentie van een stroming. div cp

:=

Ix

div

D1CP(~tt).

Divergentie van een vectorveld. div ~ := div cpo n

14. div

~

=

I

L

D.~.(e).

A. i= 1 1. 1.

, 3 ~

Rotatie van eenlR -stroming. n

=

3 en rot cP

:=

I~rot DICP(~,t).

Rotatie van eenlR3-vectorveld. rot

~ :=

rot cpo

15. rot

~

:=

leVX~(~).

n

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