Abstract.It is known that some results for spinors, and in particular for superenergy spinors, are much less transparent and require a lot more effort to establish, when considered from the tensor viewpoint. In this paper we demonstrate how the use of dimensionally dependent tensor identities enables us to derive a number of 4-dimensional identities by straightforward tensor methods in a signature independent manner. In particular, we consider the quadratic identity for the Bel-Robinson tensor T abcx T abcy = δ y x T abcd T abcd /4 and also the new conservation laws for the Chevreton tensor, both of which have been obtained by spinor means; both of these results are rederived by tensor means for 4-dimensional spaces of any signature, using dimensionally dependent identities, and also we are able to conclude that there are no direct higher dimensional analogues. In addition we demonstrate a simple way to show non-existense of such identities via counter examples; in particular we show that there is no non-trivial Bel tensor analogue of this simple Bel-Robinson tensor quadratic identity. On the other hand, as a sample of the power of generalising dimensionally dependent tensor identities from four to higher dimensions, we show that the symmetry structure, trace-free and divergence-free nature of the four dimensional Bel-Robinson tensor does have an analogue for a class of tensors in higher dimensions. It is reassuring to know that certain important but perhaps unexpected properties -disguised in the complexities of the tensor formalism -become more transparent in the spinor formalism; but the parallel and more transparent spinor investigations are restricted to 4-dimensional spacetimes with Lorentz signature, and so this assistance is not available in higher dimensions nor in four dimensional spaces with other signatures. Deser [6] has emphasised the significance of the Bel-Robinson tensor in higher dimensions, and one of the important features of Senovilla's method of construction of superenergy tensors [3] is that it is applicable to arbitrary fields in any dimension; and so, for higher dimensions, it becomes an obvious concern whether there could be unexpected properties for superenergy tensors -disguised in the even deeper complexities of tensor formalism in higher dimensions -analogous to those properties revealed by spinor formalism in four dimensions. Deeper investigations into the interaction between dimension and tensor identities have been instrumental in illustrating the uniqueness of some of the Bel-Robinson tensor's properties in four dimensions [6], explaining