NMR assignments for the insertion domain of bacteriophage Sf6 coat protein

The P22 bacteriophage group is a subgroup of the λ phage supercluster, comprised of the three major sequence types Sf6, P22, and CUS-3, based on their capsid proteins. Our goal is to investigate the extent to which structure–function relationships are conserved for the viral coat proteins and I-domains in this subgroup. Sf6 is a phage that infects the human pathogen Shigella flexneri. The coat protein of Sf6 assembles into a procapsid, which further undergoes maturation during DNA packaging into an infectious virion. The Sf6 coat protein contains a genetically inserted domain, termed the I-domain, similar to the ones present in the P22 and CUS-3 coat proteins. Based on the P22 example, I-domains play important functional roles in capsid assembly, stability, viability, and size-determination. Here we report the ¹H, ¹⁵N, and ¹³C chemical shift assignments for the I-domain of the Sf6 phage coat protein. Chemical shift-based secondary structure prediction and hydrogen-bond patterns from a long-range HNCO experiment indicate that the Sf6 I-domain adopts a 6-stranded β-barrel fold like those of P22 and CUS-3 but with important differences, including the absence of the D-loop that is critical for capsid assembly and the addition of a novel disordered loop region.     

Physiology engages with functional genomics - at last

A report on the XXXV International Congress of Physiological Sciences, held together with Experimental Biology 2005, San Diego, USA, 31 March - 6 April 2005.     

Amyloid accomplices and enforcers

Amyloid-related diseases are often ascribed to protein "misfolding." Yet in the absence of high-resolution structures for mature fibrils or intermediates, the connection between the mechanism of amyloid formation and protein folding remains tenuous. The simplistic view of amyloid fibrillogenesis as a homogeneous self-assembly process is being increasingly challenged by observations that amyloids interact with a variety of cofactors including metals, glycosaminoglycans, glycoproteins such as serum amyloid P and apolipo-protein E, and constituents of basement membranes such as perlecan, laminin, and agrin. These "pathological chaperones" have effects that range from mediating the rate of amyloid fibril formation to increasing the stability of amyloid deposits, and may contribute to amyloid toxicity. An increasing appreciation of the role of accessory molecules in amyloid etiology has paved the way to novel diagnostics and therapeutic strategies.     

Structure and disorder in the ribonuclease S-peptide probed by NMR residual dipolar couplings

NMR residual dipolar couplings for the S-peptide of ribonuclease A aligned in C8E5/n-octanol liquid crystals are consistent with the presence of a native-like alpha-helix structure undergoing dynamic fraying. Residues 3-13, which correspond to the first alpha-helix of ribonuclease A, show couplings that become more negative at low temperature and in the presence of salt, conditions which stabilize alpha-helical structure in the S-peptide. By contrast, dipolar couplings from the N and C termini of the peptide are close to zero and remain nearly invariant with changes in solution conditions. Torsion angle dynamics simulations using a gradient of dihedral restraint bounds that increase from the center to the ends of the peptide reproduce the experimentally observed sequence dependence of dipolar couplings. The magnitudes of residual dipolar couplings depend on the anisotropy of the solute. Native proteins often achieve nearly spherical shapes due to the hydrophobic effect. Embryonic partially folded structures such as the S-peptide alpha-helix have an intrinsically greater potential for anisotropy that can result in sizable residual dipolar couplings in the absence of long-range structure.     

NMR of hydrogen bonding in cold-shock protein A and an analysis of the influence of crystallographic resolution on comparisons of hydrogen bond lengths

Hydrogen bonding in cold-shock protein A of Escherichia coli has been investigated using long-range HNCO spectroscopy. Nearly half of the amide protons involved in hydrogen bonds in solution show no measurable protection from exchange in water, cautioning against a direct correspondence between hydrogen bonding and hydrogen exchange protection. The N to O atom distance across a hydrogen bond, R(NO), is related to the size of the (3h)J(NC') trans hydrogen bond coupling constant and the amide proton chemical shift. Both NMR parameters show poorer agreement with the 2.0-A resolution X-ray structure of the cold-shock protein studied by NMR than with a 1.2-A resolution X-ray structure of a homologous cold-shock protein from the thermophile B. caldolyticus. The influence of crystallographic resolution on comparisons of hydrogen bond lengths was further investigated using a database of 33 X-ray structures of ribonuclease A. For highly similar structures, both hydrogen bond R(NO) distance and Calpha coordinate root mean square deviations (RMSD) show systematic increases as the resolution of the X-ray structure used for comparison decreases. As structures diverge, the effects of coordinate errors on R(NO) distance and Calpha coordinate root mean square deviations become progressively smaller. The results of this study are discussed with regard to the influence of data precision on establishing structure similarity relationships between proteins.     

Nuclear Magnetic Resonance Structure and Dynamics of the Response Regulator Sma0114 from Sinorhizobium meliloti

Receiver domains control intracellular responses triggered by signal transduction in bacterial two-component systems. Here, we report the solution nuclear magnetic resonance structure and dynamics of Sma0114 from the bacterium Sinorhizobium meliloti, the first such characterization of a receiver domain from the HWE-kinase family of two-component systems. The structure of Sma0114 adopts a prototypical α(5)/β(5) Rossman fold but has features that set it apart from other receiver domains. The fourth β-strand of Sma0114 houses a PFxFATGY sequence motif, common to many HWE-kinase-associated receiver domains. This sequence motif in Sma0114 may substitute for the conserved Y-T coupling mechanism, which propagates conformational transitions in the 455 (α4-β5-α5) faces of receiver domains, to prime them for binding downstream effectors once they become activated by phosphorylation. In addition, the fourth α-helix of the consensus 455 face in Sma0114 is replaced with a segment that shows high flexibility on the pico- to nanosecond time scale by (15)N relaxation data. Secondary structure prediction analysis suggests that the absence of helix α4 may be a conserved property of the HWE-kinase-associated family of receiver domains to which Sma0114 belongs. In spite of these differences, Sma0114 has a conserved active site, binds divalent metal ions such as Mg(2+) and Ca(2+) that are required for phosphorylation, and exhibits micro- to millisecond active-site dynamics similar to those of other receiver domains. Taken together, our results suggest that Sma0114 has a conserved active site but differs from typical receiver domains in the structure of the 455 face that is used to effect signal transduction following activation.     

Mechanism of interaction of the double-stranded RNA (dsRNA) binding domain of protein kinase R with short dsRNA sequences

The dsRNA-activated protein kinase (PKR) plays a major role in the cellular response to viral infection. PKR contains an N-terminal dsRNA binding domain (dsRBD) and a C-terminal kinase domain. The dsRBD consists of two tandem copies of a conserved double-stranded RNA binding motif, dsRBM1 and dsRBM2. dsRNA binding is believed to activate PKR by inducing dimerization and subsequent autophosphorylation reactions. We have characterized the function of the dsRBD by assessing the binding of dsRBM1 and dsRBD to a series of dsRNA sequences ranging from 15 to 45 bp. For dsRBM1, the binding stoichiometries agree with an overlapping ligand binding model where the motif binds to multiple faces of the dsRNA duplex and overlaps along the helical axis. Similar behavior is observed for a dsRBD containing both dsRBM1 and dsRBM2 for sequences up to 30 bp; however, the binding affinity is enhanced 30-fold. Longer dsRNA sequences exhibit lower-than-expected stoichiometries, indicating a change in binding mode. NMR spectroscopy was used to define the regions of the dsRBD that interact with dsRNA. dsRNA binding induces exchange broadening of cross-peaks in 1H-15N HSQC spectra. For a 20 bp dsRNA, the resonances most affected map to the known dsRNA binding regions of dsRBM1 as well as the N-terminus of dsRBM2. For a longer 40 bp sequence, additional regions of dsRBM2 exhibit enhanced broadening. These data support a model in which dsRBM1 plays the dominant role in binding short dsRNA sequences and dsRBM2 makes additional interactions with the longer sequences capable of activating PKR.     

Protein yoga: Conformational versatility of the Hemolysin II C‐terminal domain detailed by NMR structures for multiple states

The C‐terminal domain of Bacillus cereus hemolysin II (HlyIIC), stabilizes the trans‐membrane‐pore formed by the HlyII toxin and may aid in target cell recognition. Initial efforts to determine the NMR structure of HlyIIC were hampered by cis/trans isomerization about the single proline at position 405 that leads to doubling of NMR resonances. We used the mutant P405M‐HlyIIC that eliminates the cis proline to determine the NMR structure of the domain, which revealed a novel fold. Here, we extend earlier studies to the NMR structure determination of the cis and trans states of WT‐HlyIIC that exist simultaneously in solution. The primary structural differences between the cis and trans states are in the loop that contains P405, and structurally adjacent loops. Thermodynamic linkage analysis shows that at 25 C the cis proline, which already has a large fraction of 20% in the unfolded protein, increases to 50% in the folded state due to coupling with the global stability of the domain. The P405M or P405A substitutions eliminate heterogeneity due to proline isomerization but lead to the formation of a new dimeric species. The NMR structure of the dimer shows that it is formed through domain‐swapping of strand β5, the last segment of secondary structure following P405. The presence of P405 in WT‐HlyIIC strongly disfavors the dimer compared to the P405M‐HlyIIC or P405A‐HlyIIC mutants. The WT proline may thus act as a “gatekeeper,” warding off aggregative misfolding.     

Antibody VH and VL recombination using phage and ribosome display technologies reveals distinct structural routes to affinity improvements with VH-VL interface residues providing important structural diversity

In vitro selection technologies are an important means of affinity maturing antibodies to generate the optimal therapeutic profile for a particular disease target. Here, we describe the isolation of a parent antibody, KENB061 using phage display and solution phase selections with soluble biotinylated human IL-1R1. KENB061 was affinity matured using phage display and targeted mutagenesis of VH and VL CDR3 using NNS randomization. Affinity matured VHCDR3 and VLCDR3 library blocks were recombined and selected using phage and ribosome display protocol. A direct comparison of the phage and ribosome display antibodies generated was made to determine their functional characteristics.     

Dynamic ��-Helix Structure of Micelle-bound Human Amylin

Amylin is an endocrine hormone that regulates metabolism. In patients afflicted with type 2 diabetes, amylin is found in fibrillar deposits in the pancreas. Membranes are thought to facilitate the aggregation of amylin, and membrane-bound oligomers may be responsible for the islet β-cell toxicity that develops during type 2 diabetes. To better understand the structural basis for the interactions between amylin and membranes, we determined the NMR structure of human amylin bound to SDS micelles. The first four residues in the structure are constrained to form a hairpin loop by the single disulfide bond in amylin. The last nine residues near the C terminus are unfolded. The core of the structure is an α-helix that runs from about residues 5–28. A distortion or kink near residues 18–22 introduces pliancy in the angle between the N- and C-terminal segments of the α-helix. Mobility, as determined by ¹⁵N relaxation experiments, increases from the N to the C terminus and is strongly correlated with the accessibility of the polypeptide to spin probes in the solution phase. The spin probe data suggest that the segment between residues 5 and 17 is positioned within the hydrophobic lipid environment, whereas the amyloidogenic segment between residues 20 and 29 is at the interface between the lipid and solvent. This orientation may direct the aggregation of amylin on membranes, whereas coupling between the two segments may mediate the transition to a toxic structure.Type 2 diabetes affects over 100 million people worldwide (1) and is thought to cost upward of $130 billion dollars a year to treat in the United States alone (2). The endocrine hormone amylin (also known as islet amyloid polypeptide) appears to have key roles in diabetes pathology (3–5). The normal functions of amylin include the inhibition of glucagon secretion, slowing down the emptying of the stomach, and inducing a feeling of satiety through the actions of the hormone on neurons of the hypothalamus in the brain (5). The effects of amylin are exerted in concert with those of insulin and reduce the level of glucose in the blood (3, 5). Circulating amylin levels increase in a number of pathological conditions, including obesity, syndrome X, pancreatic cancer, and renal failure (3). Amylin levels together with insulin are raised initially in type 2 diabetes but fall as the disease progresses to a stage where the pancreatic islets of Langerhans β-cells that synthesize amylin no longer function (3).One of the hallmarks of type 2 diabetes, found in 90% of patients, is the formation of extracellular amyloid aggregates composed of amylin (3–5). The amyloid deposits accumulate in the interstitial fluid between islet cells and are usually juxtaposed with the β-cell membranes (3). Aggregates of amylin are toxic when added to cultures of β-cells, so that the amyloid found in situ may be responsible for β-cell death as type 2 diabetes progresses (6, 7). Genetic evidence that amylin is directly involved in pathology includes a familial S20G mutation that leads to early onset of the disease (8) and produces an amylin variant that aggregates more readily (9).As with all amyloids it is unclear whether fibrillar structures or soluble oligomers are responsible for pathology. A recurrent theme for amyloidogenic proteins is that toxicity appears to be exerted through membrane-bound oligomers that form pores and disrupt ion balance across membranes (4, 10–13). Experimental evidence for such oligomers has been found for the amyloid-β (Aβ)² peptides (14), which cause Alzheimer disease, and for α-synuclein (αS), the protein involved in Parkinson disease (15), a particular interest of our laboratory. The similar toxic effects exerted by these amyloidogenic molecules may have a common structural and physical basis. Detailed structural models are available for Aβ (16) and αS (17) bound to SDS micelle mimetics of membranes. For amylin there are models of peptide fragments 1–19 (18), 20–29 (19), and 17–29 (20) bound to micelles but as of yet no model of the complete hormone. This turns out to be particularly important as the interplay between structure and dynamics in amylin only comes to light when considering the whole molecule.Here we report the solution structure of human amylin bound to SDS micelles. We complement the structure with information on dynamics and on the immersion of amylin into micelles.