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Introduction to Vectors and Tensors Vol 2 (Bowen 246). - Index of

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312 Chap. 9 • EUCLIDEAN MANIFOLDS<br />

3<br />

z<br />

3<br />

z<br />

i<br />

3<br />

r<br />

r<br />

3<br />

i<br />

1<br />

z<br />

i<br />

1<br />

0 E<br />

i<br />

2<br />

2<br />

z<br />

1<br />

z<br />

1<br />

i<br />

0 E<br />

2<br />

i<br />

2<br />

z<br />

Figure 8<br />

1 N<br />

Given any rectangular coordinate system ( zˆ<br />

,..., z ˆ ) , we can characterize a general or a<br />

curvilinear coordinate system as follows: Let ( , xˆ<br />

)<br />

U be a chart. Then it can be specified by the<br />

coordinate transformation from ẑ <strong>to</strong> ˆx as described earlier, since in this case the overlap <strong>of</strong> the<br />

coordinate neighborhood is U = E ∩U . Thus we have<br />

z z = zˆ<br />

xˆ<br />

x x<br />

1 N<br />

−1 1 N<br />

( ,..., ) ( ,..., )<br />

x x = xˆ<br />

zˆ<br />

z z<br />

1 N<br />

−1 1 N<br />

( ,..., ) ( ,..., )<br />

(44.23)<br />

−1<br />

where zˆ xˆ<br />

: xˆ( U) → zˆ( U)<br />

<strong>and</strong><br />

<strong>of</strong> (44.23) are<br />

ˆ ˆ : ˆ( ) → ˆ( U)<br />

are diffeomorphisms. Equivalent versions<br />

−1<br />

x z zU<br />

x<br />

z = z x x = z x<br />

j j 1 N j k<br />

( ,..., ) ( )<br />

x = x z z = x z<br />

j j 1 N j k<br />

( ,..., ) ( )<br />

(44.24)

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