A molecular dynamics model of the Bt toxin Cyt1A and its validation by resonance energy transfer

Cyt1A is a cytolytic toxin from Bacillus thuringiensis var. israelensis. A computer model of the toxin in solution was generated and validated by resonance energy transfer (RET). The average distance between the two tryptophans (residues 158 and 161) and the fluorescently labeled cysteine 190 was 2.16 nm, which closely matched the distance predicted in computer simulations, 2.2 nm. The simulation results were able to explain two previous experimental observations: (i) amino-acid sequences of all Cyt toxins contain four blocks of highly conserved residues; and (ii) several single-point mutations drastically abrogated Cyt1A's toxicity. Selective randomization of atomic coordinates in the computer model revealed that the conserved blocks are important for proper folding and stability of the toxin molecule. Replacing lysine 225 with alanine, a mutation that renders the toxin inactive, was shown to result in breaking the hydrogen bonds between K225 and V126, L123, and Y189. Calculated Helmholtz free energy difference of the inactive mutation K225A was higher by 12 kcal/mol and 5 kcal/mol than the values for the benign mutations K118A and K198A, respectively, which indicates that the K225A mutant is significantly destabilized. The normal-mode and principal-component analyses revealed that in the wild-type Cyt1A the region around the residue K225 is quite stationary, due to the hydrogen-bond network around K225. In contrast, pronounced twisting and stretching were observed in the mutant K225A, and the region around the residue K225 becomes unstable. Our results indicate that conformational differences in this mutant spread far away from the site of the mutation, suggesting that the mutant is inactivated due to an overall change in conformation and diminished stability rather than due to a localized alteration of a “binding” or “active” site.     

Tuftsin analogs and their biological activity

Summary In this paper the literature data on the structure-activity relationship for the series of tuftsin analogs are summarized. Among others, the questions of the substitution of particular amino acid residues in different positions of the peptide chain, as well as the questions of shortening and lengthening of the peptide chain of tuftsin, are reviewed. The existing models of the biologically active conformation of tuftsin are also summarized.     

Identification of Binding Sites for Efflux Pump Inhibitors of the AcrAB-TolC Component AcrA

The overexpression of multidrug efflux pumps is an important mechanism of clinical resistance in Gram-negative bacteria. Recently, four small molecules were discovered that inhibit efflux in Escherichia coli and interact with the AcrAB-TolC efflux pump component AcrA. However, the binding site(s) for these molecules was not determined. Here, we combine ensemble docking and molecular dynamics simulations with tryptophan fluorescence spectroscopy, site-directed mutagenesis, and antibiotic susceptibility assays to probe binding sites and effects of binding of these molecules. We conclude that clorobiocin and SLU-258 likely bind at a site located between the lipoyl and β-barrel domains of AcrA.     

Resonance energy transfer study using a rhenium metal-ligand lipid conjugate as the donor in a model membrane.

We measured steady state and time-resolved resonance energy transfer between donors and acceptors in model membranes. The donor was a long lifetime rhenium-lipid complex, which displayed a mean lifetime of 1 microsecond and lifetime components as long as 3 microseconds in the labeled DOPC membranes. The transfer efficiencies were found to be substantially larger than those predicted without consideration of lateral diffusion. The larger transfer efficiencies are consistent with a mutual lateral diffusion coefficient in the membrane near 2 x 10(-8) cm2/s. These results demonstrate that lateral diffusion in membranes can be detected with microsecond lipid probes.     

Distance distributions and anisotropy decays of troponin C and its complex with troponin I

We used frequency domain measurements of fluorescence resonance energy transfer to recover the distribution of distances between Met 25 and Cys 98 in rabbit skeletal troponin C. These residues were labeled with dansylaziridine as energy donor and 5-(iodoacetamido)eosin as acceptor and are located on the N- and C-terminal lobes of the two-domain protein, respectively. We developed a procedure to correct for the fraction of the sample that was incompletely labeled with the acceptor independent of chemical data. At pH 7.5 and in the presence of Mg2+, the mean distance was near 15 A with a half-width of the distribution of 15 A; when Mg2+ was replaced by Ca2+, the mean distance increased to 22 A with a decrease in the half-width by 4 A. Similar but less pronounced differences in the mean distance and half-width between samples containing Mg2+ and Ca2+ were also observed with troponin C complexed to troponin I. The results suggest that the conformation of troponin C is altered by Ca2+ binding to the Ca(2+)-specific sites and displacing bound Mg2+ at the Ca2+/Mg2+ sites. This alteration may play an important role in Ca2+ signaling in muscle. At pH 7.5, the anisotropy decays of the donor-labeled troponin C showed two components, with the long rotational correlation time (12 ns) reflecting the overall motion of the protein. When the pH was lowered from 7.5 to 5.2, the mean distribution distance of apotroponin C increased from 22 to 32 A and the half-width decreased by a factor of 2 from 13 to 7 A. The long correlation time of apotroponin C increased to 19 ns at the acidic pH. These results are discussed in terms of a model in which skeletal troponin C is a dimer at low pH and enable comparison of the solution conformation of the protein at neutral pH with a crystal structure obtained at pH 5.2. While the conformation of the monomeric unit of troponin C dimer at pH 5.2 is extended and consistent with the crystal structure, the conformation at neutral pH is likely more compact than the crystal structure predicts.