The bacterial toxin colicin E9 is secreted by producing Escherichia coli cells with its 9.5 kDa inhibitor protein Im9 bound tightly to its 14.5 kDa C-terminal DNase domain. Double- and triple-resonance NMR spectra of the 24 kDa complex of uniformly 13C and 15N labeled Im9 bound to the unlabeled DNase domain have provided sufficient constraints for the solution structure of the bound Im9 to be determined. For the final ensemble of 20 structures, pairwise RMSDs for residues 3–84 were 0.76 ± 0.14 Å for the backbone atoms and 1.36 ± 0.15 Å for the heavy atoms. Representative solution structures of the free and bound Im9 are highly similar, with backbone and heavy atom RMSDs of 1.63 and 2.44 Å, respectively, for residues 4–83, suggesting that binding does not cause a major conformational change in Im9. The NMR studies have also allowed the DNase contact surface on Im9 to be investigated through changes in backbone chemical shifts and NOEs between the two proteins determined from comparisons of 1H–1H–13C NOESY-HSQC spectra with and without 13C decoupling. The NMR-defined interface agrees well with that determined in a recent X-ray structure analysis with the major difference being that a surface loop of Im9, which is at the interface, has a different conformation in the solution and crystal structures. Tyr54, a key residue on the interface, is shown to exhibit NMR characteristics indicative of slow rotational flipping. A mechanistic description of the influence binding of Im9 has on the dynamic behavior of E9 DNase, which is known to exist in two slowly interchanging conformers in solution, is proposed.

To explore the structure of the pore-forming fragment of colicin E1 in membranes, a series of 23 consecutive single cysteine substitution mutants was prepared in the sequence 402–424. Each mutant was reacted with a sulfhydryl-specific reagent to generate a nitroxide labeled side chain, and the mobility of the side chain and its accessibility to collision with paramagnetic reagents was determined from the electron paramagnetic resonance spectrum. Individual values of these quantities were used to identify tertiary contact sites and the nature of the surrounding solvent, while their periodic dependence on sequence position was used to identify secondary structure. In solution, the data revealed a regular helix of 11 residues in the region 406–416, consistent with helix IV of the crystal structure. Upon binding to negatively charged membranes at pH 4.0, helix IV apparently grows to a length of 19 residues, extending from 402–420. One face of the helix is solvated by the lipid bilayer, and the other by an environment of a polar nature. Surprisingly, a conserved charged pair, D408–R409, is located on the lipid-exposed face. Evidence is presented to suggest a transmembrane orientation of this new helix, although other topographies may exist in equilibrium.