Jahn-Teller effects are grouped into two categories. The first arises from incomplete shells of degenerate orbitals. It includes the first-order Jahn-Teller effect, and the pseudo Jahn-Teller effect. The second arises from filled and empty molecular orbitals that are close in energy, and is the second-order Jahn-Teller effect. The two categories have quite different physical bases. As a result, geometric distortions produced by the first are quite small and normally lead to dynamic effects only. In favorable cases, the second-order Jahn-Teller effect produces very large distortions, including complete dissociation of a molecule. This can occur even when the relevant molecular orbitals are separated in energy by as much as 4 eV.An examination of the recent literature shows a rapidly increasing number of phenomena that are explained by invoking a Jahn-Teller effect. The examples come from many areas of physics and chemistry, including biochemistry.The effects invoked are those arising from orbitally degenerate states (Jahn-Teller effect proper), and from states which are nondegenerate but close in energy (pseudo, or secondorder Jahn-Teller effect).One attitude has been to lump these several effects together and to blur any distinction between them (1, 2). Another has been a reasonable belief that nondegenerate states must be very close in energy, less than 1 eV separation, before any distortion of molecular shape could be expected, and that second-order effects are very small (3-5). The purpose of this note is to point out that the nature of the first-order effect (FOJT) is such that distortions are inevitably very small, leading to the dynamic Jahn-Teller situation as a rule. Paradoxically, the second-order effect (SOJT) has a physical basis that can lead to very large distortions of molecular geometry, or even to complete dissociation.Following Jahn and Teller and Bader (6, 7), the potential energy, in terms of small displacements, Q, from an initial nuclear configuration, is given byEo -Ek The FOJT proper comes from the term linear in Q. For small displacements there is a complex mixing of electronic and vibrational states. This mixing is not under discussion here, but rather the possibility of a large distortion, which permanently affects the geometry of the molecule (static effect). Eq.[I] will not be valid for large distortions, but it still can be used to derive the symmetry constraints on the nuclear motions. The SOJT effect comes from the terms in [1] that are quadratic in Q. The Renner-Teller effect is a special second-order distortion which is important for linear molecules, but which will not be discussed further (8).Eq [1] is written in terms of state wave functions. It is necessary to interpret these in terms of molecular orbital (MO) theory to proceed further. The FOJT effect arises from incompletely filled shells. These shells are doubly and triply degenerate MO's which by their nature are not only of the same symmetry, but of the same kind. Examples are d orbitals in inorganic chemistry an...