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Unit 14: Notation and Summation Convention
It follows from equations (5) and (7) that Notes
x' x
a k i , ...(8)
ki
x i x' k
and from equation (4) that
e i x i e ' j x ' j e , ...(9)
'
k
x' k dx ' k
since x/x = , and from equations (8) and (9) that
k
j
jk
'
e a e , ...(10)
k
ki i
and
'
e a e . ...(11)
i
ki k
Equations (10) and (11) are the transformation rules for base vectors. The nine elements of a are
ij
not all independent, and in general,
a a .
ik
ki
A relation similar to equations (5) and (7),
'
u a u , and u a u ' k ...(12)
ki
k
i
ki
i
'
'
is obtained for a vector u since u e u e , which is similar to equation (4) except that the ui are
k
k
i i
the components of a vector and the x are coordinates of a point.
i
The magnitude |u| = (u u ) of the vector u is independent of the orientation of the coordinate
1/2
i
i
system, that is, it is a scalar invariant; consequently,
'
'
u u = u a a u . ...(13)
k
ki
k
ji
i
i
Eliminating u from equation (12) gives
i
'
'
u a a u ,
k
ki
j
ji
'
'
and since u kj u ,
j
k
a a = . ...(14)
ki ji
kj
Similarly, eliminating u from equation (12) gives
k
a a = . ...(15)
ik jk
ij
It follows from equation (14) or (15) that
{det[a ]} = 1, ...(16)
2
ij
where det [a ] denotes the determinant of a . The negative root of equation (16) is not considered
ij
ij
unless the transformation of axes involves a change of orientation since, for the identity
transformation x = x , a = and det[ ] = 1. Consequently, det[a ] = 1, provided the
'
i
ik
ik
ik
i
ik
transformations involve only right-handed systems (or left-handed systems).
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