In the last 65 years the properties of Tutton salts containing Cu 2+ cations have been interpreted on the basis of elongated complexes induced by a static Jahn−Teller effect (JTE). Through the analysis of experimental data and the results of first-principles calculations, we show here that such an idea, though widely followed, is not correct. By contrast, this work proves that the local geometry of Cu(H 2 O) 6 2+ units in Tutton salts actually arises from a compressed octahedron although hidden by an additional orthorhombic instability fully unrelated to the JTE. For understanding this conclusion, it is crucial to consider the effects of the internal electric field, E R (r), created by the rest of the lattice ions on the electrons localized in the Cu(H 2 O) 6 2+ unit. Indeed, the E R (r) field in Tutton salts opens a gap between ∼x 2 −y 2 and ∼3z 2 −r 2 antibonding molecular orbitals that favors a hole in ∼3z 2 −r 2 and triggers an orthorhombic distortion in the XY plane that reasonably explains available experimental data. The conditions responsible for the orthorhombic instability are discussed pointing out the singularity of Cu 2+ complexes in the realm of 3d divalent cations. For the sake of completeness the properties of Cu(H 2 O) 6 2+ units in trigonal lattices, where a JTE is clearly observed, are analyzed in detail and compared to results of Cu 2+ cations in cubic lattices. In the trigonal compounds, the force constant of the Jahn−Teller mode is shown to be smaller than that for hard ligands like O 2− or F − but comparable to the softer ligand Cl −. This fact helps to promote the orthorhombic instability in the Cu(H 2 O) 6 2+ complex when the hole is no longer in the ∼x 2 −y 2 orbital but in ∼3z 2 −r 2 .