Though the structures presented in crystallographic models of macromolecules appear to possess rock-like solidity, real proteins and nucleic acids are not particularly rigid. Most structural work to date has centred upon the native state of macromolecules, the most probable macromolecular form. But the native state of a molecule is merely its most abundant form, certainly not its only form. Thermodynamics requires that all other possible structural forms, however improbable, must also exist, albeit with representation corresponding to the factor exp( — Gi/RT) for each state of free energy Gi (see Moelwyn-Hughes, 1961), and one appreciates that each molecule within a population of molecules will in time explore the vast ensemble of possible structural states.

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The NMR resonances from the hydrogen-bonded guanine and thymine imino protons of base pairs in the four separate complexes forming the arms of a stable DNA four-arm junction have been assigned by using sequential nuclear Overhauser effects connecting protons in adjacent pairs. Comparison of the spectra of these individual duplex arms with that of the intact four-stranded junction suggests that base pairing occurs at the site of branching. The presence of new resonances in the spectrum of the junction can be inferred from comparison of the junction spectrum with the simulated spectra of the four individual arms. In addition, upfield shifts of the ring protons in the base pairs at the penultimate positions in the complex are observed, consistent with a change in the structure at the site of branching. These studies represent the first stage of a detailed analysis of the structure and dynamics of a DNA junction.

Nearly complete assignments of the proton nuclear magnetic resonance (NMR) spectrum of the polypeptide toxin III from the sea anemone Radianthus paumotensis (RP) are presented. The secondary structures of the related toxins RP II and RP III are described and are compared with each other and with another related toxin ATX Ia from Anemonia sulcata [Widmer, H., Wagner, G., Schweitz, H., Lazdunski, M., & Wüthrich, K. (1988) Eur. J. Biochem. 171, 177-192]. All of these proteins contain a highly twisted four-strand antiparallel beta-sheet core connected by loops of irregular structure. From the work done with AP-A from Anthopleura xanthogrammica [Gooley, P. R., & Norton, R. S. (1986) Biochemistry 25, 2349-2356], it is clear that this homologous toxin also has the same basic core. Some small differences are seen in the structures of these toxins, particularly in the position of the N-terminal residues that form one of the outside strands of the beta-sheet. In addition, the R. paumotensis toxins are two residues longer, extending the third strand of sheet containing the C-terminal residues. A comparison of chemical shifts for assigned residues is also presented, in general supporting the similarity of structure among these proteins.