What was Casimir's precise role in describing the center of the universal enveloping algebra of a semisimple Lie algebra?   This question is prompted by a recent MO question on explicit computations of Weyl group invariants for certain exceptional simple Lie algebras:
37602.   Like some others who started graduate study in the 1960s with almost no physics background but with an interest in abstract mathematics, I was  drawn to algebraic Lie theory for mainly esthetic reasons.   I also had no background in differential geometry or Lie groups.  So when I bought a copy of Jacobson's newly-published book on Lie algebras at a bookstore in Ithaca I had no appreciation of the historical connections of the subject. 
The eminent Dutch physicist H.B.G. Casimir was apparently the first to introduce an explicit second degree invariant (unique up to scalars) in the center of $U(\mathfrak{g})$, now called the Casimir element or Casimir invariant.
Roughly speaking, this involves fixing a basis of $\mathfrak{g}$ along with its dual basis under the Killing form, then adding the respective products.  Sometimes it is convenient to recast the answer in terms of PBW monomials for the given ordered basis.    
On the mathematical side, Chevalley and Harish-Chandra determined the full center of $U(\mathfrak{g})$: it is a polynomial algebra in $\ell$(= rank of $\mathfrak{g}$) variables.   Generators can be taken to be homogeneous of uniquely determined degrees.   Moreover, the center is isomorphic in a natural way (but requiring a subtle $\rho$-twist) to the algebra $U(\mathfrak{h})^W$ of invariants of the Weyl group relative to a fixed Cartan subalgebra $\mathfrak{h}$ of $\mathfrak{g}$.   The earlier MO question involved this algebra and its (non-unique) homogeneous generators of degrees $2 = d_1, d_2, \ldots, d_\ell$.   Key papers were those by Harish-Chandra (Trans. AMS 1951) and Chevalley (Amer. J. Math. 1955), the latter generalizing the fundamental theorem on elementary symmetric polynomials for $W=S_n$.      
My question then is: 

What role did Casimir's work play in this mathematical development?    

A related matter is the practice of referring to homogeneous generators of the center of the enveloping algebra as "Casimir operators": how far was Casimir himself involved in this direction beyond his degree 2 invariant?
ADDED: The short article referenced by mathphysicist is illuminating and may be the
best published indication of Casimir's influence on subsequent representation theory.   I was at first hoping to find a more definite paper trail, but this may not exist and would probably reach back before Math Reviews.   What struck me most in browsing through the first volume of Harish-Chandra's collected papers (1944-54) was the abrupt transition around 1948 from his work in physics like Motion of an electron to mathematics like Faithful representations of Lie algebras and of course his foundational 1951 paper I mentioned.   Nowhere along the way do I see any direct citation of Casimir's papers, though the 1950  paper Lie algebras and the Tannaka duality theorem does quote the "Casimir operator" in rank 1 as well known and uses it as a stepping-stone to the general case.   Since Harish-Chandra studied physics with Dirac in his early years, it was probably he who imported Casimir's idea into representation theory.  But Chevalley was at the time also a major influence on Harish-Chandra's thinking, so it's all hard to document.  (They both taught at Columbia for some time.)
 A: Apologies if it isn't customary to answer questions asked and answered so long ago, I'm new here...
In his autobiography Het toeval van de werkelijkheid (1983), Casimir makes a short remark about his operator (there is an English translation, Haphazard reality, but I don't own it so this translation is my own):

My dissertation [...] also describes wat is nowadays often called the Casimir operator. To put this in the proper perspective, I would like to quote something from a witty English book called How to be famous. Concerning Plato, it says: 'His own inaccurate ideas about platonic love are outdated. In his own time, however, they were an improvement on the existing situation, where one had no concept of platonic friendship whatsoever.' Mutatis mutandis, the same could be said about Casimir operators.

This at least tells us he thought he was the first to find the Casimir operator, but he is very modest about his role in the general theory; he doesn't seem to have worked on it besides the case of the rotation group, and I think he says somewhere else that he feels it isn't fair that the operator is named after him.
So I'd agree (and so would Casimir himself): he was the first to find an example, but wasn't involved in the subsequent development.  
A: A while back I was given a hardcopy of Casimir's thesis, and recently scanned it so that I could have an electronic version. The thesis doesn't appear to be readily available online, so thought it would be worth sharing here. You can download it from my public Dropbox here. The quadratic Casimir is introduced in Theorem III on page 93 of the thesis (page 52 of the scan) - the $\mathcal{D}_\mu$ are elements of the Lie algebra, considered as (right-invariant, I think) differential operators on $C^\infty(G)$, and $g^{\lambda\mu}$ is the inverse of the Killing metric with respect to this basis. Casimir actually considered the case of an arbitrary semi-simple Lie group, and not just the rotation group.
EDIT: adding a Scribd link here for those who would prefer not to download the entire 25 meg file.
A: At the first glance it appears that he more or less just gave the first nontrivial example(s) of what was later called the Casimir operators.
His obituary says:
On 1 May 1931 he wrote a letter from The Hague to the famous Gottingen mathematician
Hermann Weyl and announced: ‘While studying the quantum-mechanical properties of the
asymmetic rotator I arrived at some ‘results’ (?) concerning the representation of continuous
groups.’ He then sketched his findings on the matrix elements of the irreducible representations
for the three-dimensional rotation group, and a possible extension for semi-simple groups in
general, where he introduced what was later called the ‘Casimir operator’. This operator turned
out to be a multiple of the unit-operator and may be used to characterize in an elegant way
the irreducible representations of a given continuous group. To Casimir’s question, ‘Whether
the case is worth considering?’, Weyl answered definitely ‘Yes’. Hence the Leiden doctoral
candidate published his mathematical results in a paper, communicated by Ehrenfest to the
meeting of 27 June 1931 of the Amsterdam Academy [7], and he also included them as Chapter
IV of his dissertation, which he defended on 2 November 1931 at the University of Leiden [8].
A: One could say that Casimir “imported his idea into representation theory” himself, jointly with van der Waerden, when they used it to prove complete reducibility in rank $l>1$ (1935; his Festschrift quotes, p. 114, an interesting letter of Pauli to Weyl on how this came about).
But I get that the title question is different. On that, Borel (1998, p. 79) attributes to Racah (1950) the idea of further simplifying the proof by using $l$ independent Casimirs instead of just one. (Both papers have notable reviewers.) He says that Chevalley and Harish-Chandra had totally different motivations. However: H.-C.’s obituary (1985, p. 208) cites a 1951 letter where he “reports on the work of G. Racah on the invariants of the exceptional groups, with its application to the calculation of their Betti numbers”.
(Does the $\mathfrak Z(\mathfrak g) = U(\mathfrak h)^W$ picture allow a simplified proof of complete reducibility?)
