Solution Conformation and Dynamics of the HIV-1 Integrase Core Domain

The human immunodeficiency virus type 1 (HIV-1) integrase (IN) is a critical enzyme involved in infection. It catalyzes two reactions to integrate the viral cDNA into the host genome, 3′ processing and strand transfer, but the dynamic behavior of the active site during catalysis of these two processes remains poorly characterized. NMR spectroscopy can reveal important structural details about enzyme mechanisms, but to date the IN catalytic core domain has proven resistant to such an analysis. Here, we present the first NMR studies of a soluble variant of the catalytic core domain. The NMR chemical shifts are found to corroborate structures observed in crystals, and confirm prior studies suggesting that the α4 helix extends toward the active site. We also observe a dramatic improvement in NMR spectra with increasing MgCl₂ concentration. This improvement suggests a structural transition not only near the active site residues but also throughout the entire molecule as IN binds Mg²⁺. In particular, the stability of the core domain is linked to the conformation of its C-terminal helix, which has implications for relative domain orientation in the full-length enzyme. ¹⁵N relaxation experiments further show that, although conformationally flexible, the catalytic loop of IN is not fully disordered in the absence of DNA. Indeed, automated chemical shift-based modeling of the active site loop reveals several stable clusters that show striking similarity to a recent crystal structure of prototype foamy virus IN bound to DNA.     

Conformation and dynamics changes of bacteriorhodopsin and its D85N mutant in the absence of 2D crystalline lattice as revealed by site-directed C NMR

¹³C NMR spectra of [3-¹³C]Ala- and [1-¹³C]Val-labeled D85N mutant of bacteriorhodopsin (bR) reconstituted in egg PC or DMPC bilayers were recorded to gain insight into their secondary structures and dynamics. They were substantially suppressed as compared with those of 2D crystals, especially at the loops and several transmembrane α_II-helices. Surprisingly, the ¹³C NMR spectra of [3-¹³C]Ala-D85N turned out to be very similar to those of [3-¹³C]Ala-bR in lipid bilayers, in spite of the presence of globular conformational and dynamics changes in the former as found from 2D crystalline preparations. No further spectral change was also noted between the ground (pH 7) and M-like state (pH 10) as far as D85N in lipid bilayers was examined, in spite of their distinct changes in the 2D crystalline state. This is mainly caused by that the resulting ¹³C NMR peaks which are sensitive to conformation and dynamics changes in the loops and several transmembrane α_II-helices of the M-like state are suppressed already by fluctuation motions in the order of 10⁴-10⁵ Hz interfered with frequencies of magic angle spinning or proton decoupling. However, ¹³C NMR signal from the cytoplasmic α-helix protruding from the membrane surface is not strongly influenced by 2D crystal or monomer. Deceptively simplified carbonyl ¹³C NMR signals of the loop and transmembrane α-helices followed by Pro residues in [1-¹³C]Val-labeled bR and D85N in 2D crystal are split into two peaks for reconstituted preparations in the absence of 2D crystalline lattice. Fortunately, ¹³C NMR spectral feature of reconstituted [1-¹³C]Val and [3-¹³C]Ala-labeled bR and D85N was recovered to yield characteristic feature of 2D crystalline form in gel-forming lipids achieved at lowered temperatures.     

Assignment Strategies for Large Proteins by Magic-Angle Spinning NMR: The 21-kDa Disulfide-Bond-Forming Enzyme DsbA

We present strategies for chemical shift assignments of large proteins by magic-angle spinning solid-state NMR, using the 21-kDa disulfide-bond-forming enzyme DsbA as prototype. Previous studies have demonstrated that complete de novo assignments are possible for proteins up to  ∼ 17 kDa, and partial assignments have been performed for several larger proteins. Here we show that combinations of isotopic labeling strategies, high field correlation spectroscopy, and three-dimensional (3D) and four-dimensional (4D) backbone correlation experiments yield highly confident assignments for more than 90% of backbone resonances in DsbA. Samples were prepared as nanocrystalline precipitates by a dialysis procedure, resulting in heterogeneous linewidths below 0.2 ppm. Thus, high magnetic fields, selective decoupling pulse sequences, and sparse isotopic labeling all improved spectral resolution. Assignments by amino acid type were facilitated by particular combinations of pulse sequences and isotopic labeling; for example, transferred echo double resonance experiments enhanced sensitivity for Pro and Gly residues; [2-¹³C]glycerol labeling clarified Val, Ile, and Leu assignments; in-phase anti-phase correlation spectra enabled interpretation of otherwise crowded Glx/Asx side-chain regions; and 3D NCACX experiments on [2-¹³C]glycerol samples provided unique sets of aromatic (Phe, Tyr, and Trp) correlations. Together with high-sensitivity CANCOCA 4D experiments and CANCOCX 3D experiments, unambiguous backbone walks could be performed throughout the majority of the sequence. At 189 residues, DsbA represents the largest monomeric unit for which essentially complete solid-state NMR assignments have so far been achieved. These results will facilitate studies of nanocrystalline DsbA structure and dynamics and will enable analysis of its 41-kDa covalent complex with the membrane protein DsbB, for which we demonstrate a high-resolution two-dimensional ¹³C-¹³C spectrum.     

4D Non-uniformly sampled C,C-NOESY experiment for sequential assignment of 13C,15N-labeled RNAs

¹³C spin diluted protein samples can be produced using [1-¹³C] and [2-¹³C]-glucose (Glc) carbon sources in the bacterial growth medium. The ¹³C spin dilution results in favorable ¹³C spectral resolution and polarization transfer behavior. We recently reported the combined use of [1-¹³C]- and [2-¹³C]-Glc labeling to facilitate the structural analysis of insoluble and non-crystalline biological systems by solid-state NMR (ssNMR), including sequential assignment, detection of long-range contacts and structure determination of macromolecular assemblies. In solution NMR the beneficial properties of sparsely labeled samples using [2-¹³C]-glycerol (¹³C labeled Cα sites on a ¹²C diluted background) have recently been exploited to provide a bi-directional assignment method (Takeuchi et al. in J Biomol NMR 49(1):17–26, 2011 ). Inspired by this approach and our own recent results using [2-¹³C]-Glc as carbon sources for the simplification of ssNMR spectra, we present a strategy for a bi-directional sequential assignment of solid-state NMR resonances and additionally the detection of long-range contacts using the combination of ¹³C spin dilution and 3D NMR spectroscopy. We illustrate our results with the sequential assignment and the collection of distance restraints on an insoluble and non-crystalline supramolecular assembly, the Salmonella typhimurium type III secretion system needle.     

Differences in the Structure and Dynamics of the Apo- and Palmitate-ligated Forms of Aedes aegypti Sterol Carrier Protein 2 (AeSCP-2)

Sterol carrier protein-2 (SCP-2) is a nonspecific lipid-binding protein expressed ubiquitously in most organisms. Knockdown of SCP-2 expression in mosquitoes has been shown to result in high mortality in developing adults and significantly lowered fertility. Thus, it is of interest to determine the structure of mosquito SCP-2 and to identify its mechanism of lipid binding. We report here high quality three-dimensional solution structures of SCP-2 from Aedes aegypti determined by NMR spectroscopy in its ligand-free state (AeSCP-2) and in complex with palmitate. Both structures have a similar mixed α/β fold consisting of a five-stranded β-sheet and four α-helices arranged on one side of the β-sheet. Ligand-free AeSCP-2 exhibited regions of structural heterogeneity, as evidenced by multiple two-dimensional ¹⁵N heteronuclear single-quantum coherence peaks for certain amino acids; this heterogeneity disappeared upon complex formation with palmitate. The binding of palmitate to AeSCP-2 was found to decrease the backbone mobility of the protein but not to alter its secondary structure. Complex formation is accompanied by chemical shift differences and a loss of mobility for residues in the loop between helix αI and strand βA. The structural differences between the αI and βA of the mosquito and the vertebrate SCP-2s may explain the differential specificity (insect versus vertebrate) of chemical inhibitors of the mosquito SCP-2.     

Backbone dynamics of membrane proteins in lipid bilayers: the effect of two-dimensional array formation as revealed by site-directed solid-state C NMR studies on [3-C]Ala- and [1-C]Val-labeled bacteriorhodopsin

We have recorded site-directed solid-state ¹³C NMR spectra of [3-¹³C]Ala- and [1-¹³C]Val-labeled bacteriorhodopsin (bR) as a typical membrane protein in lipid bilayers, to examine the effect of formation of two-dimensional (2D) lattice or array of the proteins toward backbone dynamics, to search the optimum condition to be able to record full ¹³C NMR signals from whole area of proteins. Well-resolved ¹³C NMR signals were recorded for monomeric [3-¹³C]Ala-bR in egg phosphatidylcholine (PC) bilayer at ambient temperature, although several ¹³C NMR signals from the loops and transmembrane α-helices were still suppressed. This is because monomeric bR reconstituted into egg PC, dimyristoylphosphatidylcholine (DMPC) or dipalmytoylphosphatidylcholine (DPPC) bilayers undergoes conformational fluctuations with frequency in the order of 10⁴-10⁵ Hz at ambient temperature, which is interfered with frequency of magic angle spinning or proton decoupling. It turned out, however, that the ¹³C NMR signals of purple membrane (PM) were almost fully recovered in gel phase lipids of DMPC or DPPC bilayers at around 0 °C. This finding is interpreted in terms of aggregation of bR in DMPC or DPPC bilayers to 2D hexagonal array in the presence of endogenous lipids at low temperature, resulting in favorable backbone dynamics for ¹³C NMR observation. It is therefore concluded that [3-¹³C]Ala-bR reconstituted in egg PC, DMPC or DPPC bilayers at ambient temperature, or [3-¹³C]Ala- and [1-¹³C]Val-bR at low temperature gave rise to well-resolved ¹³C NMR signals, although they are not always completely the same as those of 2D hexagonal lattice from PM.     

Functional insights by comparison of modeled structures of 18kDa small heat shock protein and its mutant in Mycobacterium leprae

In this work we are proposing Homology modeled structures of Mycobacterium leprae 18kDa heat shock protein and its mutant. The more closely related structure of the small heat shock protein (sHSP) belonging to the eukaryotic species from wheat sHSP16.9 and 16.3kDa ACR1 protein from Mycobacterium tuberculosis were used as template structures. Each model contains an N-terminal domain, alpha-crystalline domain and a C-terminal tail. The models showed that a single point mutation from serine to proline at 52^nd position causes structural changes. The structural changes are observed in N-terminal region and alpha-crystalline domains. Serine in 52^nd position is observed in β4 strand and Proline in 52^nd position is observed in loop. The number of residues contributing α helix at N-terminal region varies in both models. In 18S more number of residues is present in α helix when compared to 18P. The loop regions between β3 and β4 strands of both models vary in number of residues present in it. Number of residues contributing β4 strand in both models vary. β6 strand is absent in both models. Major functional peptide region of alpha crystalline domains of both models varies. These differences observed in secondary structures support their distinct functional roles. It also emphasizes that a point mutation can cause structural variation.     

Secondary structural analysis of proteins based on 13C chemical shift assignments in unresolved solid-state NMR spectra enhanced by fragmented structure database

Magic-angle-spinning solid-state ¹³C NMR spectroscopy is useful for structural analysis of non-crystalline proteins. However, the signal assignments and structural analysis are often hampered by the signal overlaps primarily due to minor structural heterogeneities, especially for uniformly-¹³C,¹⁵N labeled samples. To overcome this problem, we present a method for assigning ¹³C chemical shifts and secondary structures from unresolved two-dimensional ¹³C–¹³C MAS NMR spectra by spectral fitting, named reconstruction of spectra using protein local structures (RESPLS). The spectral fitting was conducted using databases of protein fragmented structures related to ¹³C^α, ¹³C^β, and ¹³C′ chemical shifts and cross-peak intensities. The experimental ¹³C–¹³C inter- and intra-residue correlation spectra of uniformly isotope-labeled ubiquitin in the lyophilized state had a few broad peaks. The fitting analysis for these spectra provided sequence-specific C^α, C^β, and C′ chemical shifts with an accuracy of about 1.5 ppm, which enabled the assignment of the secondary structures with an accuracy of 79 %. The structural heterogeneity of the lyophilized ubiquitin is revealed from the results. Test of RESPLS analysis for simulated spectra of five different types of proteins indicated that the method allowed the secondary structure determination with accuracy of about 80 % for the 50–200 residue proteins. These results demonstrate that the RESPLS approach expands the applicability of the NMR to non-crystalline proteins exhibiting unresolved ¹³C NMR spectra, such as lyophilized proteins, amyloids, membrane proteins and proteins in living cells.     

Diversity of Channels Generated by Different Combinations of Epithelial Sodium Channel Subunits

The epithelial sodium channel is a multimeric protein formed by three homologous subunits: α, β, and γ; each subunit contains only two transmembrane domains. The level of expression of each of the subunits is markedly different in various Na⁺ absorbing epithelia raising the possibility that channels with different subunit composition can function in vivo. We have examined the functional properties of channels formed by the association of α with β and of α with γ in the Xenopus oocyte expression system using two-microelectrode voltage clamp and patch-clamp techniques. We found that αβ channels differ from αγ channels in the following functional properties: (a) αβ channels expressed larger Na⁺ than Li⁺ currents (I_Na+/I_Li+ 1.2) whereas αγ channels expressed smaller Na⁺ than Li⁺ currents (I_Na+/I_Li+ 0.55); (b) the Michaelis Menten constants (K _m) of activation of current by increasing concentrations of external Na⁺ and Li⁺ of αβ channels were larger (K _m > 180 mM) than those of αγ channels (K _m of 35 and 50 mM, respectively); (c) single channel conductances of αβ channels (5.1 pS for Na⁺ and 4.2 pS for Li⁺) were smaller than those of αγ channels (6.5 pS for Na⁺ and 10.8 pS for Li⁺); (d) the half-inhibition constant (K _i) of amiloride was 20-fold larger for αβ channels than for αγ channels whereas the K _i of guanidinium was equal for both αβ and αγ. To identify the domains in the channel subunits involved in amiloride binding, we constructed several chimeras that contained the amino terminus of the γ subunit and the carboxy terminus of the β subunit. A stretch of 15 amino acids, immediately before the second transmembrane domain of the β subunit, was identified as the domain conferring lower amiloride affinity to the αβ channels. We provide evidence for the existence of two distinct binding sites for the amiloride molecule: one for the guanidium moiety and another for the pyrazine ring. At least two subunits α with β or γ contribute to these binding sites. Finally, we show that the most likely stoichiometry of αβ and αγ channels is 1α:1β and 1α:1γ, respectively.     

C, N CP MAS and high resolution multinuclear NMR study of methyl

MAX8, a designer peptide known to undergo self-assembly following changes in temperature, pH, and ionic strength, has demonstrated usefulness for tissue engineering and drug delivery. It is hypothesized that the self-assembled MAX8 nanofiber structure consists of closed β-hairpins aligned into antiparallel β-sheets. Here, we report evidence from solid-state NMR spectroscopy that supports the presence of the hypothesized β-hairpin conformation within the nanofiber structure. Specifically, our ¹³C-¹³C two-dimensional exchange data indicate spatial proximity between V3 and K17, and ¹³C-¹³C dipolar coupling measurements reveal proximity between the V3 and V18 backbone carbonyls. Moreover, isotopic dilution of labeled MAX8 nanofibers did not result in a loss of the ¹³C-¹³C dipolar couplings, showing that these couplings are primarily intramolecular. NMR spectra also indicate the existence of a minor conformation, which is discussed in terms of previously hypothesized nanofiber physical cross-linking and possible nanofiber polymorphism.     

Solid-State NMR Evidence for β-Hairpin Structure within MAX8 Designer Peptide Nanofibers

MAX8, a designer peptide known to undergo self-assembly following changes in temperature, pH, and ionic strength, has demonstrated usefulness for tissue engineering and drug delivery. It is hypothesized that the self-assembled MAX8 nanofiber structure consists of closed β-hairpins aligned into antiparallel β-sheets. Here, we report evidence from solid-state NMR spectroscopy that supports the presence of the hypothesized β-hairpin conformation within the nanofiber structure. Specifically, our ¹³C-¹³C two-dimensional exchange data indicate spatial proximity between V3 and K17, and ¹³C-¹³C dipolar coupling measurements reveal proximity between the V3 and V18 backbone carbonyls. Moreover, isotopic dilution of labeled MAX8 nanofibers did not result in a loss of the ¹³C-¹³C dipolar couplings, showing that these couplings are primarily intramolecular. NMR spectra also indicate the existence of a minor conformation, which is discussed in terms of previously hypothesized nanofiber physical cross-linking and possible nanofiber polymorphism.     

Residue-specific millisecond to microsecond fluctuations in bacteriorhodopsin induced by disrupted or disorganized two-dimensional crystalline lattice, through modified lipid-helix and helix-helix interactions, as revealed by C NMR

We have recorded ¹³C NMR spectra of [3-¹³C]-, [1-¹³C]Ala-, and [1-¹³C]Val-labeled bacteriorhodopsin (bR), W80L and W12L mutants and bacterio-opsin (bO) from retinal-deficient E1001 strain, in order to examine the possibility of their millisecond to microsecond local fluctuations with correlation time in the order of 10⁻⁴ to 10⁻⁵ s, induced or prevented by disruption or assembly of two-dimensional (2D) crystalline lattice, respectively, at ambient temperature. The presence of disrupted or disorganized 2D lattice for W12L, W80L and bO from E1001 strain was readily visualized by increased relative proportions of surrounding lipids per protein, together with their broadened ¹³C NMR signals of transmembrane α-helices and loops in [3-¹³C]Ala-labeled proteins, with reference to those of wild-type. In contrast, ¹³C CP-MAS NMR spectra of [1-¹³C]Ala- and Val-labeled these mutants were almost completely suppressed, owing to the presence of fluctuations with time scale of 10⁻⁴ s interfered with magic angle spinning. In particular, ¹³C NMR signals of [1-¹³C]Ala-labeled transmembrane α-helices of wild-type were almost completely suppressed at the interface between the surface and inner part (up to 8.7 Å deep from the surface) with reference to those of the similarly suppressed peaks by Mn²⁺-induced accelerated spin-spin relaxation rate. Such fluctuation-induced suppression of ¹³C NMR peaks from the interfacial regions, however, was less significant for [1-¹³C]Val-labeled proteins, because fluctuation motions in Val residues with bulky side-chains at the C_α moiety were modified to those of longer correlation time (>10⁻⁴ s), if any, by residue-specific manner. To support this view, we found that such suppressed ¹³C NMR signals of [1-¹³C]Ala-labeled peaks in the wild-type were recovered for D85N and bO in which correlation times of fluctuations were shifted to the order of 10⁻⁵ s due to modified helix-helix interactions as previously pointed out [Biochemistry, 39 (2000) 14472; J. Biochem. (Tokyo) 127 (2000) 861].     

Increasing the Amphiphilicity of an Amyloidogenic Peptide Changes the β-Sheet Structure in the Fibrils from Antiparallel to Parallel

Solid-state NMR measurements have been reported for four peptides derived from β-amyloid peptide Aβ(1–42): Aβ(1–40), Aβ(10–35), Aβ(16–22), and Aβ(34–42). Of these, the first two are predicted to be amphiphilic and were reported to form parallel β-sheets, whereas the latter two peptides appear nonamphiphilic and adopt an antiparallel β-sheet organization. These results suggest that amphiphilicity may be significant in determining fibril structure. Here, we demonstrate that acylation of Aβ(16–22) with octanoic acid increases its amphiphilicity and changes the organization of fibrillar β-sheet from antiparallel to parallel. Electron microscopy, Congo Red binding, and one-dimensional ¹³C NMR measurements demonstrate that octanoyl-Aβ(16–22) forms typical amyloid fibrils. Based on the stability of monolayers at the air-water interface, octanoyl-Aβ(16–22) is more amphiphilic than Aβ(16–22). Measurements of ¹³C-¹³C and ¹⁵N-¹³C nuclear magnetic dipole-dipole couplings in isotopically labeled fibril samples, using the constant-time finite-pulse radiofrequency-driven recoupling (fpRFDR-CT) and rotational echo double resonance (REDOR) solid-state NMR techniques, demonstrate that octanoyl-Aβ(16–22) fibrils are composed of parallel β-sheets, whereas Aβ(16–22) fibrils are composed of antiparallel β-sheets. These data demonstrate that amphiphilicity is critical in determining the structural organization of β-sheets in the amyloid fibril. This work also shows that all amyloid fibrils do not share a common supramolecular structure, and suggests a method for controlling the structure of amyloid fibrils.     

Electrophysiological Characterization of the Rat Epithelial Na+ Channel (rENaC) Expressed in MDCK Cells : Effects of Na+ and Ca2+

The epithelial Na⁺ channel (ENaC), composed of three subunits (α, β, and γ), is expressed in several epithelia and plays a critical role in salt and water balance and in the regulation of blood pressure. Little is known, however, about the electrophysiological properties of this cloned channel when expressed in epithelial cells. Using whole-cell and single channel current recording techniques, we have now characterized the rat αβγENaC (rENaC) stably transfected and expressed in Madin-Darby canine kidney (MDCK) cells. Under whole-cell patch-clamp configuration, the αβγrENaC-expressing MDCK cells exhibited greater whole cell Na⁺ current at −143 mV (−1,466.2 ± 297.5 pA) than did untransfected cells (−47.6 ± 10.7 pA). This conductance was completely and reversibly inhibited by 10 μM amiloride, with a Ki of 20 nM at a membrane potential of −103 mV; the amiloride inhibition was slightly voltage dependent. Amiloride-sensitive whole-cell current of MDCK cells expressing αβ or αγ subunits alone was −115.2 ± 41.4 pA and −52.1 ± 24.5 pA at −143 mV, respectively, similar to the whole-cell Na⁺ current of untransfected cells. Relaxation analysis of the amiloride-sensitive current after voltage steps suggested that the channels were activated by membrane hyperpolarization. Ion selectivity sequence of the Na⁺ conductance was Li⁺ > Na⁺ >> K⁺ = N-methyl-d-glucamine⁺ (NMDG⁺). Using excised outside-out patches, amiloride-sensitive single channel conductance, likely responsible for the macroscopic Na⁺ channel current, was found to be ∼5 and 8 pS when Na⁺ and Li⁺ were used as a charge carrier, respectively. K⁺ conductance through the channel was undetectable. The channel activity, defined as a product of the number of active channel (n) and open probability (P _o), was increased by membrane hyperpolarization. Both whole-cell Na⁺ current and conductance were saturated with increased extracellular Na⁺ concentrations, which likely resulted from saturation of the single channel conductance. The channel activity (nP _o) was significantly decreased when cytosolic Na⁺ concentration was increased from 0 to 50 mM in inside-out patches. Whole-cell Na⁺ conductance (with Li⁺ as a charge carrier) was inhibited by the addition of ionomycin (1 μM) and Ca²⁺ (1 mM) to the bath. Dialysis of the cells with a pipette solution containing 1 μM Ca²⁺ caused a biphasic inhibition, with time constants of 1.7 ± 0.3 min (n = 3) and 128.4 ± 33.4 min (n = 3). An increase in cytosolic Ca²⁺ concentration from <1 nM to 1 μM was accompanied by a decrease in channel activity. Increasing cytosolic Ca²⁺ to 10 μM exhibited a pronounced inhibitory effect. Single channel conductance, however, was unchanged by increasing free Ca²⁺ concentrations from <1 nM to 10 μM. Collectively, these results provide the first characterization of rENaC heterologously expressed in a mammalian epithelial cell line, and provide evidence for channel regulation by cytosolic Na⁺ and Ca²⁺.     

The core of Ure2p prion fibrils is formed by the N-terminal segment in a parallel cross-β structure: evidence from solid-state NMR

Intracellular fibril formation by Ure2p produces the non-Mendelian genetic element [URE3] in Saccharomyces cerevisiae, making Ure2p a prion protein. We show that solid-state NMR spectra of full-length Ure2p fibrils, seeded with infectious prions from a specific [URE3] strain and labeled with uniformly ¹⁵N-¹³C-enriched Ile, include strong, sharp signals from Ile residues in the globular C-terminal domain (CTD) with both helical and nonhelical ¹³C chemical shifts. Treatment with proteinase K eliminates these CTD signals, leaving only nonhelical signals from the Gln-rich and Asn-rich N-terminal segment, which are also observed in the solid-state NMR spectra of Ile-labeled fibrils formed by residues 1-89 of Ure2p. Thus, the N-terminal segment, or “prion domain” (PD), forms the fibril core, while CTD units are located outside the core. We additionally show that, after proteinase K treatment, Ile-labeled Ure2p fibrils formed without prion seeding exhibit a broader set of solid-state NMR signals than do prion-seeded fibrils, consistent with the idea that structural variations within the PD core account for prion strains. Measurements of ¹³C-¹³C magnetic dipole-dipole couplings among ¹³C-labeled Ile carbonyl sites in full-length Ure2p fibrils support an in-register parallel β-sheet structure for the PD core of Ure2p fibrils. Finally, we show that a model in which CTD units are attached rigidly to the parallel β-sheet core is consistent with steric constraints.     

Gentisic acid conjugates of Medicago truncatula roots

Three phenolic glycosides 5-O-{[5′′-O-E-(4′′′-O-threo-guaiacylglycerol)-feruloyl]-β-apiofuranosyl-(1→2)-β-xylopyranosyl} gentisic acid, 5-O-[(5′′-O-vanilloyl)-β-apiofuranosyl-(1→2)-β-xylopyranosyl] gentisic acid and 1-O-[E-(4′′′-O-threo-guaiacylglycerol)-feruloyl]-3-O-β-galacturonopyranosyl glycerol were isolated and identified from the roots of Medicago truncatula together with four known 5-O-β-xylopyranosyl gentisic acid, vicenin-2, hovetrichoside C and pterosupin identified for the first time in this species. Structural elucidation was carried out on the basis of UV, mass, ¹H and ¹³C NMR spectral data.     

Hydrogen exchange of monomeric alpha-synuclein shows unfolded structure persists at physiological temperature and is independent of molecular crowding in Escherichia coli

Amide proton NMR signals from the N-terminal domain of monomeric α-synuclein (αS) are lost when the sample temperature is raised from 10°C to 35°C at pH 7.4. Although the temperature-induced effects have been attributed to conformational exchange caused by an increase in α-helix structure, we show that the loss of signals is due to fast amide proton exchange. At low ionic strength, hydrogen exchange rates are faster for the N-terminal segment of αS than for the acidic C-terminal domain. When the salt concentration is raised to 300 mM, exchange rates increase throughout the protein and become similar for the N- and C-terminal domains. This indicates that the enhanced protection of amide protons from the C-terminal domain at low salt is electrostatic in nature. Cα chemical shift data point to <10% residual α-helix structure at 10°C and 35°C. Conformational exchange contributions to R2 are negligible at both temperatures. In contrast to the situation in vitro, the majority of amide protons are observed at 37°C in ¹H-¹⁵N HSQC spectra of αS encapsulated within living Escherichia coli cells. Our finding that temperature effects on αS NMR spectra can be explained by hydrogen exchange obviates the need to invoke special cellular factors. The retention of signals is likely due to slowed hydrogen exchange caused by the lowered intracellular pH of high-density E. coli cultures. Taken together, our results emphasize that αS remains predominantly unfolded at physiological temperature and pH—an important conclusion for mechanistic models of the association of αS with membranes and fibrils.