Rate of Molecular Transfer of Allyl Alcohol across an AOT Surfactant Layer Using Muon Spin Spectroscopy.

The transfer rate of a probe molecule across the interfacial layer of a water-in-oil (w/o) microemulsion was investigated using a combination of transverse field muon spin rotation (TF-µSR), avoided level crossing muon spin resonance (ALC-µSR), and Monte Carlo simulations. Reverse microemulsions consist of nanometer-sized water droplets dispersed in an apolar solvent separated by a surfactant monolayer. Although the thermodynamic, static model of these systems has been well described, our understanding of their dynamics is currently incomplete. For example, what is the rate of solute transfer between the aqueous and apolar solvents, and how this is influenced by the structure of the interface? With an appropriate choice of system and probe molecule, µSR offers a unique opportunity to directly probe these interfacial transfer dynamics. Here, we have employed a well characterized w/o microemulsion stabilized by bis(2-ethylhexyl) sodium sulfosuccinate (Aerosol OT), with allyl alcohol (CH2═CH-CH2-OH, AA) as the probe. Resonances due to both muoniated radicals, CMuH2-C*H-CH2-OH and C*H2-CHMu-CH2-OH, were observed with the former being the dominant species. All resonances displayed solvent dependence, with those in the microemulsion observed as a single resonance located at intermediate magnetic fields to those present in either of the pure solvents. Observation of a single resonance is strong evidence for interfacial transfer being in the fast exchange limit. Monte Carlo calculations of the ΔM = 0 ALC resonances are consistent with the experimental data, indicating exchange rates greater than 10(9) s(-1), placing the rate of interfacial transfer at the diffusion limit.

Spin evolution in a radio frequency field studied through muon spin resonance.

The application of composite inversion pulses to a novel area of magnetic resonance, namely muon spin resonance, is demonstrated. Results confirm that efficient spin inversion can readily be achieved using this technique, despite the challenging experimental setup required for beamline measurements and the short lifetime (≈2.2µs) associated with the positive muon probe. Intriguingly, because the muon spin polarisation is detected by positron emission, the muon magnetisation can be monitored during the radio-frequency (RF) pulse to provide a unique insight into the effect of the RF field on the spin polarisation. This technique is used to explore the application of RF inversion sequences under the non-ideal conditions typically encountered when setting up pulsed muon resonance experiments.

NMR characterisation of the relationship between frustration and the excited state of Im7.

Previous work shows that Im9 folds in a two-state transition while its homologue Im7 folds in a three-state transition via an on-pathway kinetic intermediate state (KIS), with this difference being related to frustration in the structure of Im7. We have used NMR spectroscopy to study conformational dynamics connected to the frustration. A combination of equilibrium peptide N(1)H/N(2)H exchange, model-free analyses of backbone NH relaxation data and relaxation dispersion (RD)-NMR shows that the native state of Im7 is in equilibrium with an intermediate state that is lowly populated [equilibrium intermediate state (EIS)]. Comparison of kinetic and thermodynamic parameters describing the EIS native-state equilibrium obtained by RD-NMR with previously reported parameters describing the KIS native-state equilibrium obtained from stopped-flow fluorescence studies of refolding His-tagged Im7 shows that the KIS and the EIS are the same species. (15)N chemical shifts of the EIS obtained from the RD-NMR analysis show that residues forming helix III in the native state are unstructured in the EIS while other residues experiencing frustration in the native state are in structured regions of the EIS. We show that binding of Im7 and its L53A/I54A variant (which resembles the EIS as shown in previous work) to the cognate partner for Im7, the DNase domain of colicin E7, causes the dynamic processes associated with the frustration to be dampened.

Alpha-zirconium phosphonates: versatile supports for N-heterocyclic carbenes.

alpha-Zirconium phosphonates derivatised with N-heterocyclic carbenes provide a versatile platform for organocatalysis and metal-catalysed transformations, including the ring-opening polymerisation of cyclic esters, and olefin metathesis and hydroformylations by surface-bound ruthenium, rhodium and iridium complexes.

Muon spin relaxation study of Zr(H2PO4)(PO4).2H2O.

Muon spin relaxation has been used to study the muon dynamics in the layered zirconium phosphate Zr(H(2)PO(4))(PO(4)).2H(2)O as a function of temperature. Radiofrequency decoupling was used to establish the origin of the local dipolar field as coupling with (1)H spins. Muons were trapped at two sites, one identified as HMuO and the other consistent with PO-Mu on the basis of their zero-field second moments. Although a small decrease in the local nuclear dipolar field was seen with temperature, the muons remained essentially static over the temperature range 20-300 K.

Clusters in an intrinsically disordered protein create a protein-binding site: the TolB-binding region of colicin E9.

The 61-kDa colicin E9 protein toxin enters the cytoplasm of susceptible cells by interacting with outer membrane and periplasmic helper proteins and kills them by hydrolyzing their DNA. The membrane translocation function is located in the N-terminal domain of the colicin, with a key signal sequence being a pentapeptide region that governs the interaction with the helper protein TolB (the TolB box). Previous NMR studies [Collins et al. (2002) J. Mol. Biol. 318, 787-904; MacDonald et al. (2004), J. Biomol. NMR 30, 81-96] have shown that the N-terminal 83 residues of colicin E9, which includes the TolB box, is intrinsically disordered and contains clusters of interacting side chains. To further define the properties of this region of colicin E9, we have investigated the effects on the dynamical and TolB-binding properties of three mutations of colicin E9 that inactivate it as a toxin. The mutations were contained in a fusion protein consisting of residues 1-61 of colicin E9 connected to the N terminus of the E9 DNase by an eight-residue linking sequence. The NMR data reveals that the mutations cause major alterations to the properties of some of the clusters, consistent with some form of association between them and other more distant parts of the amino acid sequence, particularly toward the N terminus of the protein. However, (15)N T(2) measurements indicates that residues 5-13 of the fusion protein bound to the 43-kDa TolB remain as flexible as they are in the free protein. The NMR data point to considerable dynamic ordering within the intrinsically disordered translocation domain of the colicin that is important for creating the TolB-binding site. Furthermore, amino acid sequence considerations suggest that the clusters of amino acids occur because of the size and polarities of the side chains forming them influenced by the propensities of the residues within the clusters and those immediately surrounding them in sequence space to form beta turns.

Characterisation of a mobile protein-binding epitope in the translocation domain of colicin E9.

The 61 kDa colicin E9 protein toxin enters the cytoplasm of susceptible cells by interacting with outer membrane and periplasmic helper proteins, and kills them by hydrolysing their DNA. The membrane translocation function is located in the N-terminal domain of the colicin, with a key signal sequence being a pentapeptide region that governs the interaction with the helper protein TolB (the TolB box). Previous NMR studies (Collins et al., 2002 J. Mol. Biol. 318, 787-804) have shown that the N-terminal 83 residues of colicin E9, which includes the TolB box, is largely unstructured and highly flexible. In order to further define the properties of this region we have studied a fusion protein containing residues 1-61 of colicin E9 connected to the N-terminus of the E9 DNase by an eight-residue linking sequence. 53 of the expected 58 backbone NH resonances for the first 61 residues and all of the expected 7 backbone NH resonances of the linking sequence were assigned with 3D (1)H-(13)C-(15)N NMR experiments, and the backbone dynamics of these regions investigated through measurement of (1)H-(15)N relaxation properties. Reduced spectral density mapping, extended Lipari-Szabo modelling, and fitting backbone R(2) relaxation rates to a polymer dynamics model identifies three clusters of interacting residues, each containing a tryptophan. Each of these clusters is perturbed by TolB binding to the intact colicin, showing that the significant region for TolB binding extends beyond the recognized five amino acids of the TolB box and demonstrating that the binding epitope for TolB involves a considerable degree of order within an otherwise disordered and flexible domain. Abbreviations : Im9, the immunity protein for colicin E9; E9 DNase, the endonuclease domain of colicin E9; HSQC, heteronuclear single quantum coherence; ppm, parts per million; DSS, 2,2-(dimethylsilyl)propanesulfonic acid; TSP, sodium 3-trimethylsilypropionate; T(1 - 61)-DNase fusion protein, residues 1-61 of colicin E9 connected to the N-terminus of the E9 DNase by an eight residue thrombin cleavage sequence.

Structural dynamics of the receptor-binding domain of colicin E9.

Colicin E9 is a 61 kDa antibacterial protein secreted by E. coli. In order for it to enter the cytoplasm of susceptible bacteria and kill them by hydrolysing their DNA, the colicin must first interact with an outer membrane receptor on the target cell, BtuB, and a translocation pathway involving Tol proteins. The receptor binding, translocation and DNase functions of colicin E9 are housed in discrete structural domains, which have been independently expressed and characterized. The minimal receptor-binding domain is a 76 amino acid protein (min-R). X-ray structure determination of a related colicin shows its receptor-binding-domain to have a helical hairpin structure (S. Soelaiman, K. Jakes, N. Wu, C. Li and M. Shoham, Molecular Cell. 2001, 8, 1053). Our solution NMR studies of min-R have confirmed it has a helical hairpin structure, and shown it has multiple slowly interchanging conformers and a flexible inter-helix loop. A plausible interpretation of these data is that in solution the helical hairpin can adopt a variety of structures differing in the spatial relationship of the two helices. A possible biological role for this involves the hairpin opening during translocation into bacteria.

Structural dynamics of the membrane translocation domain of colicin E9 and its interaction with TolB.

In order for the 61 kDa colicin E9 protein toxin to enter the cytoplasm of susceptible cells and kill them by hydrolysing their DNA, the colicin must interact with the outer membrane BtuB receptor and Tol translocation pathway of target cells. The translocation function is located in the N-terminal domain of the colicin molecule. (1)H, (1)H-(1)H-(15)N and (1)H-(13)C-(15)N NMR studies of intact colicin E9, its DNase domain, minimal receptor-binding domain and two N-terminal constructs containing the translocation domain showed that the region of the translocation domain that governs the interaction of colicin E9 with TolB is largely unstructured and highly flexible. Of the expected 80 backbone NH resonances of the first 83 residues of intact colicin E9, 61 were identified, with 43 of them being assigned specifically. The absence of secondary structure for these was shown through chemical shift analyses and the lack of long-range NOEs in (1)H-(1)H-(15)N NOESY spectra (tau(m)=200 ms). The enhanced flexibility of the region of the translocation domain containing the TolB box compared to the overall tumbling rate of the protein was identified from the relatively large values of backbone and tryptophan indole (15)N spin-spin relaxation times, and from the negative (1)H-(15)N NOEs of the backbone NH resonances. Variable flexibility of the N-terminal region was revealed by the (15)N T(1)/T(2) ratios, which showed that the C-terminal end of the TolB box and the region immediately following it was motionally constrained compared to other parts of the N terminus. This, together with the observation of inter-residue NOEs involving Ile54, indicated that there was some structural ordering, resulting most probably from the interactions of side-chains. Conformational heterogeneity of parts of the translocation domain was evident from a multiplicity of signals for some of the residues. Im9 binding to colicin E9 had no effect on the chemical shifts or other NMR characteristics of the region of colicin E9 containing the TolB recognition sequence, though the interaction of TolB with intact colicin E9 bound to Im9 did affect resonances from this region. The flexibility of the translocation domain of colicin E9 may be connected with its need to recognise protein partners that assist it in crossing the outer membrane and in the translocation event itself.