How to prove an expression to be a tensor? How to prove that the expression phi, ij:=partial 2phi partial xi partial xj=delta delta phi is a tensor of second order where phi is a scalar? Furthermore, how to prove that a×b:=aibjεijkek is a vector? We can either prove it by definition or use the so-called "tensor recognition theorem" claiming that if p_(i_1 i_2)⋯i_m j_1 j_2⋯j_n q_j1⋯j_n=ri_1⋯i_m, then p must be a tensor of order m+n, where q_j1⋯j_n is a tensor of order n and ri_1⋯i_m a tensor of order m.

bravere4g

bravere4g

Answered question

2022-09-03

How to prove an expression to be a tensor?
How to prove that the expression φ , i j := 2 φ x i x j = φ is a tensor of second order where φ is a scalar? Furthermore, how to prove that q j 1 j n is a vector?
We can either prove it by definition or use the so-called "tensor recognition theorem" claiming that if q j 1 j n , then p must be a tensor of order m+n, where q j 1 j n is a tensor of order n and r i 1 i m a tensor of order m.

Answer & Explanation

Lamar Casey

Lamar Casey

Beginner2022-09-04Added 8 answers

1 ) Suppose that O X 1 X 2 X 3 is the coordinate system corresponding to the given basis e 1 , e 2 , e 3 on E 3 . The gradient of a scalar function φ ( X 1 , X 2 , X 3 ), using this coordinate system, is defined by
O X 1 ~ X 2 ~ X 3 ~
Suppose that O X 1 ~ X 2 ~ X 3 ~ is another orthonormal basis with corresponding cartesian coordinates O X 1 ~ X 2 ~ X 3 ~ given by X ~ i = q i j X j , where Q = ( q i j ) S O ( 3 )
By the chain rule,
X ~ i = q i j X j
Using X ~ i = q i j X j , we have
X k X ~ i = q i k ,
and hence
φ
That is, by definition, φ is a cartesian tensor of order 1. Doing this again, but with φ in place of φ, shows that 2 φ is a cartesian tensor of order 2.
2) a and b are vectors so a i and b j are components of cartesian tensors of order 1, and the alternating tensor ε = ε k l m is a cartesian tensor of order 3.
Taking their product we get that a i b j ε i j m are the components of a cartesian tensor of order 5.
Contracting indices (that is, setting two indices equal and thus effecting a sum) gives that a i b j ε i j m are the components of a cartesian tensor of order 4, and contracting again gives that a i b j ε i j m are the components of a cartesian tensor of order 3.
Hence, a × b is a cartesian tensor of order 3.

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