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Schaum's Outline to Tensor Calculus ― chapter 1, example 1.5 ―――

If $y_i = a_{ij}x_j$, express the quadratic form $Q = g_{ij}y_iy_j$ in terms of the $x$-variables.

Solution: I can't substitute $y_i$ directly because it contains $j$ and there's already a $j$ in the given quadratic form. So $y_i = a_{i \huge{j}}x_{\huge{j}} = a_{i \huge{r}}x_{\huge{r}}$.
This implies $ y_{\huge{j}} = a_{{\huge{j}}r}x_r.$ But I already used $r$ (in the sentence before the previous) so need to replace $r$ ――― $ y_j = a_{j \huge{r}}x_{\huge{r}} = a_{j \huge{s}}x_{\huge{s}}.$ Therefore, by substitution, $Q = g_{ij}(a_{ir}x_r)(a_{js}x_s)$ $$ = g_{ij}a_{ir}a_{js}x_rx_s. \tag{1}$$ $$= h_{rs}x_rx_s, \text{ where } h_{rs} = g_{ij}a_{ir}a_{js}. \tag{2}$$

Equation ($1$): Why can they commute $a_{js}$ and $x_r$? How are any of the terms commutative?

Equation ($2$): How does $rs$ get to be the subscript of $h$? Why did they define $h_{rs}$?

3 Answers3

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It's easiest to see what's going on if you put the implied summation symbols back in. Right before your equations (1) and (2), you have:

$$Q = \sum_{i,j} g_{ij} \sum_r a_{ir} x_r \sum_s a_{js} x_s$$

Now pull all the summations out to the front. Then all the terms in the summation symbol are numbers, so they commute, and we get $$Q= \sum_{i,j} \sum_{r} \sum_s g_{ij} a_{ir}x_r a_{js}x_s = \sum_{i,j,r,s} g_{ij} a_{ir} \color{green}{x_r a_{js}}x_s = \sum_{i,j,r,s} g_{ij} a_{ir} \color{green}{a_{js} x_r} x_s.$$

This is your equation (1). Now bring the $r$ and $s$ summations back in: $$Q = \sum_{i,j} g_{ij} a_{ir} a_{js} \sum_{r,s} x_r x_s.$$

This is your equation (2).

Ted
  • 33,788
  • Before commuting any term, why does $$\large{\sum_{i,j} g_{ij} \sum_{r}a_{ir}x_r \sum_s a_{js}x_s = \sum_{i,j,r,s} g_{ij}a_{ir}x_ra_{js}x_s}$$ $${\LARGE{\text{BUT NOT }}} \large{\sum_{i,j} \sum_{r} \sum_s g_{ij} a_{ir}x_r a_{js}x_s?}$$ – Dwayne E. Pouiller Jul 07 '13 at 11:11
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    @DePouiller All those expressions are equal. It doesn't matter whether you write $\sum_{i,j,r,s}$ versus $\sum_{i,j} \sum_r \sum_s$. What does this have to do with your question? – Ted Jul 07 '13 at 21:21
  • Thanks - I just want to clarify that step in your question. Without expanding or induction - how can you intuit or see that all three expressions are equal? – Dwayne E. Pouiller Jul 15 '13 at 05:33
  • @DePouiller If you have a $\sum_i$, then you can move any factor not depending on $i$ in or out of the sum. This is just the distributive property. Writing something like $\sum_{i,j,r,s}$ versus multiple summations $\sum_{i,j} \sum_r \sum_s$ is the commutative and associative laws of addition. I don't know why you want to avoid expanding and induction. That's how you prove these rules I've stated rigorously. – Ted Jul 15 '13 at 05:47
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The name of repeated indices is non important; in expressions like

$$y_i=a_{ij}x_j$$

you can change $j$ to any other index different from $i$, as it is repeated. In other words

$$y_i=a_{ij}x_j=a_{ik}x_k=a_{il}x_l=\dots$$

are all represeantations of the same object, i.e. $y_i$. Let us consider the quadratic form $Q=g_{ij}y_iy_j$. It is defined using the indices $i$ and $j$. In the definitions of $y_i$ and $y_j$ we must choose other repeated indices, to avoid confusion with the sum over $i$ and $j$. Let us do it by choosing $k$ and $l$ s.t.

$$y_i=a_{ik}x_k, $$ $$y_j=a_{jl}x_l. $$

We arrive at the expression

$$Q=g_{ij}y_iy_j=Q=g_{ij}a_{ik}x_ka_{jl}x_l=(a_{\bullet\bullet}\text{ are just scalars!Scalars commute})=g_{ij}a_{ik}a_{jl}x_kx_l,$$

or

$$Q=\sum_{i,j,k,l}g_{ij}a_{ik}a_{jl}x_kx_l, $$

which is quadratic in the $x_{\bullet}$'s, as claimed. I hope this helps with the first question of yours.

In your second question you introduce the quantity $h$ through the components

$$h_{rs}:=g_{ij}a_{ir}a_{js}.$$

The question is: why is the definition of $h_{rs}$ well posed? Let us have a better look at the definition of the $h_{rs}$; the $h_{rs}$ are equivalent to

$$h_{rs}=\sum_{i,j}g_{ij}a_{ir}a_{js},$$

as the repeated indices are $i$ and $j$. This is really the definition of the Einstein notation, no hidden trick here. The free indices in

$$g_{ij}a_{ir}a_{js} $$

are $r$ and $s$. The quantity "$h$" is then defined for each pair of $(r,s)$. In other words, it is a matrix whose components are just the $h_{rs}$'s. I hope it helps.

Avitus
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In equation (1) $a_{js}$ and $x_r$ commute because these are just regular (reals or complex) numbers using standard multiplication which is commutative.

Equation (2) $h_{rs}$ is defined to save space more than anything, it's the coefficients of the polynomial in $x_i$.