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

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318 Chap. 9 • EUCLIDEAN MANIFOLDS<br />

Based upon (44.44), the curvilinear coordinate system is orthogonal if g<br />

ij<br />

= 0 when i ≠ j. The<br />

symbol g denotes a scalar field on U defined by<br />

g( x) = det ⎡<br />

⎣g ij<br />

( x ) ⎤<br />

⎦<br />

(44.45)<br />

for all<br />

x ∈U .<br />

At the point<br />

x ∈U , the differential element <strong>of</strong> arc ds is defined by<br />

2<br />

ds = d ⋅ d<br />

x x (44.46)<br />

<strong>and</strong>, by (44.8), (44.33), <strong>and</strong> (44.39),<br />

∂x<br />

∂x<br />

ˆ<br />

∂x<br />

∂x<br />

i j<br />

= g ( x)<br />

dx dx<br />

2<br />

i j<br />

ds = ( x( x)) ⋅ ( x( x))<br />

dx dx<br />

i<br />

j<br />

ij<br />

ˆ<br />

(44.47)<br />

If ( U , x ) <strong>and</strong> ( , y )<br />

1 ˆ<br />

U are charts where U1∩U 2<br />

≠∅, then at x ∈U1∩<br />

U<br />

2<br />

2<br />

ˆ<br />

h ( x) = h ( x) ⋅h ( x)<br />

ij i j<br />

∂x<br />

∂x<br />

= ∂ y<br />

∂ y<br />

k<br />

l<br />

1 N<br />

1 N<br />

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

( x)<br />

i<br />

j<br />

(44.48)<br />

Equation (44.48) is helpful for actual calculations <strong>of</strong> the quantities g ( x ) . For example, for<br />

the transformation (44.23), (44.48) can be arranged <strong>to</strong> yield<br />

ij<br />

k<br />

k<br />

∂z<br />

1 N ∂z<br />

1 N<br />

gij( x ) = ( x ,..., x ) ( x ,..., x )<br />

(44.49)<br />

∂<br />

i j<br />

x ∂ x<br />

since k l kl<br />

⋅ =δ i i . For the cylindrical coordinate system defined by (44.25) a simple calculation<br />

based upon (44.49) yields

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