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4 5 Consider inΩ⊂Rna symmetric, covariant tensor of second ordergij, which is supposed to be invertible with inverse (gij

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Ubungen zu Analysis III¨ Blatt 3

1 Consider the functionf :R2→R2

f(x, y) =

(xy(x2−y2)

x2+y2 , (x, y)6= (0,0), 0, (x, y) = (0,0).

and prove that the second partial derivatives off exist in the origin, but that they are

neither continuous nor symmetric there. 4

2 LetA∈L(E, F), thenA∈C(E, F) andD2A≡0. 4

3 Prove the relation in (7.5.86). 4

4 Leta∈Lk(E1, . . . Ek;F), thena∈C(Qk

i=1Ei, F) andDk+1a≡0.

Note: Give a simple and elegant proof. 4

5 Consider inΩ⊂Rna symmetric, covariant tensor of second ordergij, which is supposed to be invertible with inverse (gij) = (gij)−1. A covariant tensor of this kind is said to be ametric.

Prove that

(i) The inversegij is a contravariant tensor of second order. 3 (ii) Relative to a fixed metricgij define thedivergenceof a contravariant vector field

ξ= (ξi) by

divξ= 1 p|g|

∂xi

p|g|ξi ,

whereg= det(gij), and therotationof a covariant vector fieldλ= (λi) by rotλ= (λi,j−λj,i).

The comma indicates an ordinary partial derivative λi,j= ∂λi

∂xj.

Prove that divξis a function and rotλa covariant tensor of order two. 6

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