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mathematical_physics_2007_10.pdf, Study Guides, Projects, Research of Mathematical Physics

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bg1
VECTOR
OPERATIONS
13
Now let’s repeat
this
derivation using the subscriptlsummation notation. Equa-
tion
l
.40
allows us to write
_-
A.
A
=
AiAi
(1.60)
(1.61)
A
.A
=
A:A:.
Notice how we have been careful to use different subscripts for the two sums in
Equations 1.60 and 1.61. This ensures the
sums
will remain independent as they
are manipulated in the following steps. The primed components can be expressed in
terms
of
the unprimed components as
-1 -1
A,!
=
R..A
‘I
I
.,
(1.62)
where
Rij
is the
ijth
component of the rotation matrix
R[4].
Inserting this expression
into Equation 1.61 gives
(1.63)
A
*A
=
R,A,R,,A,,
where again, we have been careful to use
the
two different subscripts
u
and
v.
This
equation has three implicit sums, over the subscripts
r,
u,
and
u.
In
subscript notation, unlike matrix notation, the ordering
of
the terms is not
important,
so
we rearrange Equation 1.63 to read
--I --I
(1.64)
A *A
=
A,A,R,R,,.
Next concentrate on the sum over
r,
which only involves the
[R]
matrix elements,
in the product
R,R,,.
What exactly does
this
product mean? Let’s compare it to an
operation we discussed earlier. In Equation 1.12, we pointed out the subscripted ex-
pression
MijNjk
represented the regular matrix product
[M][N],
because the summed
subscript
j
is in the second position
of
the
[MI
matrix and the first position of the
[N]
matrix. The expression
R,R,,,
however, has a contraction over the first index
of
both
matrices. In order to make sense
of
this product, we write the first instance
of
[R]
using the transpose:
--I
--I
RruRru
+
[Rlt [Rl-
(1.65)
Consequently, from Equation 1.57,
R,R,,
=
&,.
(1.66)
Substituting this
result
into Equation 1.64 gives
(1.67)
Admittedly, this example is too easy. It
does
not demonstrate any significant
advantage of using the subscriptlsummation notation over matrices. It does, how-
ever, highlight the equivalence
of
the two approaches. In our next example, the
subscriptlsummation notation will prove to
be
almost indispensable.
pf3

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VECTOR OPERATIONS 13

Now let’s repeat this derivation using the subscriptlsummation notation. Equa- tion l .40 allows us to write

_ -

A. A = AiAi (1.60)

A. A = A:A:. (1.61)

Notice how we have been careful to use different subscripts for the two sums in Equations 1.60 and 1.61. This ensures the sums will remain independent as they are manipulated in the following steps. The primed components can be expressed in terms of the unprimed components as

-1 - 1

A,! = R.. A‘I I ., (1.62)

where Rij is the ijth component of the rotation matrix R [ 4 ]. Inserting this expression into Equation 1.61 gives

A * A = R,A,R,,A,, (1.63)

where again, we have been careful to use the two different subscripts u and v. This equation has three implicit sums, over the subscripts r , u, and u. In subscript notation, unlike matrix notation, the ordering of the terms is not important, so we rearrange Equation 1.63 to read

--I --I

A * A = A,A,R,R,,. (1.64)

Next concentrate on the sum over r , which only involves the [ R ] matrix elements, in the product R,R,,. What exactly does this product mean? Let’s compare it to an operation we discussed earlier. In Equation 1.12, we pointed out the subscripted ex- pression MijNjk represented the regular matrix product [ M ] [ N ] , because the summed

subscript j is in the second position of the [MI matrix and the first position of the

[ N ] matrix. The expression R,R,,, however, has a contraction over the first index of both matrices. In order to make sense of this product, we write the first instance of [R] using the transpose:

--I --I

RruRru + [Rlt [Rl- (1.65)

Consequently, from Equation 1.57,

R,R,, = &,. (1.66)

Substituting this result into Equation 1.64 gives

(1.67)

Admittedly, this example is too easy. It does not demonstrate any significant advantage of using the subscriptlsummation notation over matrices. It does, how- ever, highlight the equivalence of the two approaches. In our next example, the subscriptlsummation notation will prove to be almost indispensable.

14 A REVIEW OF VECTOR AND MATRIX ALGEBRA

 ### Example 1. 2 The subscript/summation notation allows the derivation of vector identities that seem almost impossibleusing any other approach.The exampleworked out here is the derivation of an identity for the double cross product between three ## vectors, X (B X 0. This one example essentially demonstrates all the common operations that occur in these types of manipulations. Other examples are suggested in the problems listed at the end of this chapter. ## The expression A X (B X c) is written in vector notation and is valid in any ### coordinate system. To derive our identity, we will convert this expression into sub- ### script/summationnotation in a Cartesian coordinate system. In the end, however, we will return our answer to vector notation to obtain a result that does not depend upon any coordinatesystem. In this example, we will need to use the subscripted form for a vector - ## v = Vi&, (1.68) for a dot product between two vectors ## _ _ ### A * B = AiBi, (1.69) and for a cross product To begin, let - ### D = B X C , (1.71) which, written using the Levi-Civita symbol, is = BiCj&€ijk. (1.72) ## SubstitutingEquation 1.71 into the expressionx X ( B X c), and using the Levi-Civita expression again, gives ## A x (Bx C) = A x D = A ~ D ~ ~ + ~ E ,. , ~. (1.73) ## The sth component of D is obtained by dot multiplying both sides of Equation 1. ### by ii, as follows: Substituting the result of Equation 1.74 into Equation 1.73 gives