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

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324 Chap. 9 • EUCLIDEAN MANIFOLDS<br />

Section 45. Transformation Rules for Vec<strong>to</strong>rs <strong>and</strong> Tensor Fields<br />

In this section, we shall formalize certain ideas regarding fields on E <strong>and</strong> then investigate<br />

the transformation rules for vec<strong>to</strong>rs <strong>and</strong> tensor fields. Let U be an open subset <strong>of</strong> E ; we shall<br />

denote by F ∞ ( U ) the set <strong>of</strong> C ∞ functions f : U →R. First we shall study the algebraic structure<br />

<strong>of</strong> F ∞ ( U ) . If f <strong>and</strong> 1<br />

f<br />

2<br />

are in F ∞ ( U ) , then their sum f1+ f2<br />

is an element <strong>of</strong> F ∞ ( U ) defined by<br />

( f + f )( x) = f ( x) + f ( x )<br />

(45.1)<br />

1 2 1 2<br />

<strong>and</strong> their produce f1f 2<br />

is also an element <strong>of</strong> F ∞ ( U ) defined by<br />

( ff)( x) = f( x) f( x )<br />

(45.2)<br />

1 2 1 2<br />

for all<br />

x ∈U . For any real number λ ∈R the constant function is defined by<br />

λ( x ) = λ<br />

(45.3)<br />

for all x ∈U . For simplicity, the function <strong>and</strong> the value in (45.3) are indicated by the same<br />

symbol. Thus, the zero function in F ∞ ( U ) is denoted simply by 0 <strong>and</strong> for every f ∈ F ∞ ( U )<br />

f<br />

+ 0= f<br />

(45.4)<br />

It is also apparent that<br />

1f<br />

= f<br />

(45.5)<br />

In addition, we define<br />

− f = ( − 1) f<br />

(45.6)

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