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

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322 Chap. 9 • EUCLIDEAN MANIFOLDS<br />

( − )<br />

2 2 1 2 2<br />

⎡a cosh x cos x<br />

0 0 ⎤<br />

⎢<br />

⎥<br />

2 2 1 2 2<br />

⎡<br />

⎣gij( x ) ⎤<br />

⎦ = ⎢ 0 a ( cosh x −cos x ) 0 ⎥<br />

⎢<br />

⎥<br />

2 2 1 2 2<br />

⎢ 0 0 a sinh x sin x ⎥<br />

⎣<br />

⎦<br />

44.7 Elliptical cylindrical coordinates<br />

coordinate system by<br />

1 2 3<br />

( x , x , x ) are defined relative <strong>to</strong> a rectangular Cartesian<br />

z = acosh<br />

x cos x<br />

1 1 2<br />

z = asinh<br />

x sin x<br />

z<br />

2 1 2<br />

= x<br />

3 3<br />

1 2 3<br />

1<br />

where a > 0 . How must ( x , x , x ) be restricted so as <strong>to</strong> make ẑ xˆ<br />

− one-<strong>to</strong>-one?<br />

Discuss the coordinate curves <strong>and</strong> coordinate surfaces. Also, show that<br />

( + )<br />

2 2 1 2 2<br />

⎡a sinh x sin x<br />

0 0⎤<br />

⎢<br />

⎥<br />

2 2 1 2 2<br />

⎡<br />

⎣gij( x ) ⎤<br />

⎦ = ⎢ 0 a ( sinh x + sin x ) 0⎥<br />

⎢<br />

⎥<br />

⎢ 0 0 1⎥<br />

⎣<br />

⎦<br />

44.8 For the cylindrical coordinate system show that<br />

g = (cos x ) i + (sin x ) i<br />

2 2<br />

1 1 2<br />

g =− x (sin x ) i + x (cos x ) i<br />

g<br />

1 2 1 2<br />

2 1 2<br />

= i<br />

3 3<br />

44.9 At a point x in E , the components <strong>of</strong> the position vec<strong>to</strong>r rx ( ) = x−<br />

0 E<br />

with respect <strong>to</strong> the<br />

basis { i ,..., 1<br />

i<br />

N } associated with a rectangular Cartesian coordinate system are<br />

1 N<br />

z ,..., z .<br />

This observation follows, <strong>of</strong> course, from (44.16). Compute the components <strong>of</strong> rx ( ) with<br />

respect <strong>to</strong> the basis { g1( x), g2( x), g3( x )}<br />

for (a) cylindrical coordinates, (b) spherical<br />

coordinates, <strong>and</strong> (c) parabolic coordinates. You should find that

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