A thorough investigation is made of the independent point-group symmet
ries and canonical matrix forms that the 2D elastic and hyperelastic t
ensors can have. Particular attention is paid to the concepts relevant
to the proper definition of the independence of a symmetry from anoth
er one. It is shown that the numbers of all independent symmetries for
the 2D elastic and hyperelastic tensors are six and four, respectivel
y. In passing, a symmetry result useful for the homogenization theory
of 2D linear elastic heterogeneous media is derived.