Section 1 Formalism and Rank-2 Tensors
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Working note by Phil (dated 3.11.17) for a document on rotating frames. It contrasts active and passive transformation of rank-2 tensors, with a Dirac bra-ket derivation of (T)'ij. It asks whether the rotation generators Jk transform as passive tensors and tests the hypothesis that they are constant matrices. It applies this to the matrices A and B in an ω calculation and concludes to use A and B without invoking active tensors.
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Section 1 Formalism and Rank-2 Tensors PhL 3.11.17
I want to argue that in the Passive View a rank-2 tensor transforms as follows
(T)' = RTRT (1a)
which is a shorthand for this more precise statement
(T)'ij = RiaTab(RT)bj (1b)
In the Passive View, there is no new tensor (T') as there is in the Active View.
Here is the Dirac version of (2)
(T)'ij = <e'i| T | e'j> = <e'i|en><en| T |em><em| e'j> = Rin(T)nmRjm = [RTRT]ij (2)
It is hard to deny this Dirac derivation of (1b)
Question #1. What then can be said about a new object (T') which is defined as follows
(T') ≡ RTRT (3a)
or
(T')ij = RiaTab(RT)bj (3b)
Comparing the right sides of (1b) and (3b) one would have to conclude that
(T')ij = (T)'ij
If you are free to define (T') as in (3a) due to no name conflicts, then yes, this is the expected result.
Example: Consider T = Jk , one of the rotation generators. Does this transform as a passive rank-2 tensor, yes or no? If yes, we would expect to have
(Jk)' = RJkRT (4a)
(Jk)'ij = Ria(Jk)ab(RT)bj (4b)
If no, we might instead expect to have (Jk)'ij = (Jk)ij . In this case we might vaguely think of Jk as just a matrix of constants which is the same in any Frame. In some sense it is a scalar.
How does one answer the question: which is it? Yes or no? More nubbins questions. One method is to assume one answer and find a contraction. The usual issue is having clean definitions of things. Let's try one of the solutions and see where it leads.
Hypothesis: Jk does not transform as a passive rank-2 tensor. It is just a matrix of constants. Then
(Jk)' = RJkRT not true
(Jk)'ij = Ria(Jk)ab(RT)bj not true
(Jk)'ij = (Jk)ij true
In the context of this hypothesis, we could define a new object as follows
(J'k) ≡ RJkRT
or
(J'k)ij ≡ Ria(Jk)ab(RT)bj // = (R-1)kn(Jn)ij by Theorem 1
This is a matrix whose elements are functions of angles like θ,φ,ψ.
Claim: You could say (as in tensor doc) that the pair of objects { Jk, (J'k)} transform as an active rank-2 tensor. But in the passive view, the object (J'k) does not exist. Only (Jk)' exists. You cannot just define (J'k) ≡ (Jk)' because (J'k) is already defined as RJkRT and this is different from (Jk)' = (J)k.
Fact: Nothing stops you from defining (J'k) ≡ RJkRT if you want to do that. But you cannot make any statement about { Jk, (J'k)} transforming as a passive tensor.
Review of Active and Passive Rank-2 tensors
In the Active View, you have the original tensor T in Frame S and you create a new tensor T' also in Frame S such that (T') = RTRT, The pair {T,T'} transforms as an active rank-2 tensor. There is no Frame S', there is no new basis e'n for Frame S'
In the Passive View, you have the original tensor T in Frame S and there is no tensor T'. You define Frame S' with rotated basis vectors e'n and the rank-2 transformation rule is then (T)' = RTRT .
Application to object A of the ω calculation.
In this calculation I have the following matrix A = aiJi as follows:
A ≡ - [ ( cosψ + sinθsinψ)(iJ1) + ( sinψ - sinθcosψ)(iJ2) + ( + cosθ)(iJ3) ]
The matrix elements are
Aij ≡ - [ ( cosψ + sinθsinψ)(iJ1)ij + ( sinψ - sinθcosψ)(iJ2)ij + ( + cosθ)(iJ3)ij ]
According to the Hypothesis above, since the Jk do NOT transform as passive rank-2 tensors, we must conclude that the object Aij also does NOT transform as a passive rank-2 tensor. Furthermore, since we know that (Jk)'ij = (Jk)ij we also know that (A)'ij = Aij .
We could if we wanted define the object (A') = RTRT . It turns out that when we do the ω calculation we encounter the object B ≡ RTAR so we cannot associate this (A') with B. But suppose we were to give the matrix A a different name like this
A' ≡ - [ ( cosψ + sinθsinψ)(iJ1) + ( sinψ - sinθcosψ)(iJ2) + ( + cosθ)(iJ3) ]
(A')ij ≡ - [ ( cosψ + sinθsinψ)(iJ1)ij + ( sinψ - sinθcosψ)(iJ2)ij + ( + cosθ)(iJ3)ij ]
Then we would end up with
B = RTA'R (A') = RBRT
and in this case we could identify B with A where {A, (A') } form an active rank-2 tensor.
Does this add any clarity to the calculation? I think it does NOT add clarity, because then you have to mention active rank-2 tensor in a passive view world of frames doc. So don't bring this up, and just use A and B!!!
Well, in Frames Doc I do write things like T' = RTRT. Is that active or passive?
OK, I have now made Sections 1.1,2,3 more consistent by always saying (T)' = RTRT . I am trying to be totally consistent. In doing this in a separate file, I found various spelling errors!
Question: What should one make of this development ?
(T')mn ≡ <em| T' |en> = <em| RTR-1 |en> = <R-1em|T |R-1en> = <e'm| T |e'n> = (T)'mn
Well, here I defined a new tensor T' ≡ RTR-1 or (T') ≡ RTR-1 . If you can do this with no naming conflicts, then yes, you will get (T')mn = (T)'mn . Same as what happens with vectors. You have
(V') = RV and if you can define V' ≡ RV with no meaning conflict, you get (V')i = (V)'i.