Use of 13C conformation-dependent chemical shifts to elucidate the local structure of a large protein with homologous domains in solution and solid state

In order to clarify the difference between solution NMR and X-ray diffraction analyses concerning the presence of alpha-helical structure in protein A, the 13C conformation-dependent chemical shifts of the 13C-labeled carbonyl carbons for selectively labeled protein A were used. In the 13C CP/MAS NMR spectra, the higher-field shifts of the carbonyl carbons of 13C-labeled Thr and Val residues compared with the random coil chemical shifts both in solution and solid state imply the presence of the third helix in the polypeptide chain, in contrast to the crystal structure of Fc-bound B-domain. Thus, a combination of selective isotope labeling and conformation-dependent chemical shifts will be a good Indicator to monitor the local structure of homologous protein in solution and solid state.     

Direct demonstration of the flexibility of the glycosylated proline-threonine linker in the Cellulomonas fimi Xylanase Cex through NMR spectroscopic analysis

The modular xylanase Cex (or CfXyn10A) from Cellulomonas fimi consists of an N-terminal catalytic domain and a C-terminal cellulose-binding domain, joined by a glycosylated proline-threonine (PT) linker. To characterize the conformation and dynamics of the Cex linker and the consequences of its modification, we have used NMR spectroscopy to study full-length Cex in its nonglycosylated ( approximately 47 kDa) and glycosylated ( approximately 51 kDa) forms. The PT linker lacks any predominant structure in either form as indicated by random coil amide chemical shifts. Furthermore, heteronuclear (1)H-(15)N nuclear Overhauser effect relaxation measurements demonstrate that the linker is flexible on the ns-to-ps time scale and that glycosylation partially dampens this flexibility. The catalytic and cellulose-binding domains also exhibit identical amide chemical shifts whether in isolation or in the context of either unmodified or glycosylated full-length Cex. Therefore, there are no noncovalent interactions between the two domains of Cex or between either domain and the linker. This conclusion is supported by the distinct (15)N relaxation properties of the two domains, as well as their differential alignment within a magnetic field by Pf1 phage particles. These data demonstrate that the PT linker is a flexible tether, joining the structurally independent catalytic and cellulose-binding domains of Cex in an ensemble of conformations; however, more extended forms may predominate because of restrictions imparted by the alternating proline residues. This supports the postulate that the binding-domain anchors Cex to the surface of cellulose, whereas the linker provides flexibility for the catalytic domain to hydrolyze nearby hemicellulose (xylan) chains.     

Solution secondary structure of calcium-saturated troponin C monomer determined by multidimensional heteronuclear NMR spectroscopy.

The solution secondary structure of calcium-saturated skeletal troponin C (TnC) in the presence of 15% (v/v) trifluoroethanol (TFE), which has been shown to exist predominantly as a monomer (Slupsky CM, Kay CM, Reinach FC, Smillie LB, Sykes BD, 1995, Biochemistry 34, forthcoming), has been investigated using multidimensional heteronuclear nuclear magnetic resonance spectroscopy. The 1H, 15N, and 13C NMR chemical shift values for TnC in the presence of TFE are very similar to values obtained for calcium-saturated NTnC (residues 1-90 of skeletal TnC), calmodulin, and synthetic peptide homodimers. Moreover, the secondary structure elements of TnC are virtually identical to those obtained for calcium-saturated NTnC, calmodulin, and the synthetic peptide homodimers, suggesting that 15% (v/v) TFE minimally perturbs the secondary and tertiary structure of this stably folded protein. Comparison of the solution structure of calcium-saturated TnC with the X-ray crystal structure of half-saturated TnC reveals differences in the phi/psi angles of residue Glu 41 and in the linker between the two domains. Glu 41 has irregular phi/psi angles in the crystal structure, producing a kink in the B helix, whereas in calcium-saturated TnC, Glu 41 has helical phi/psi angles, resulting in a straight B helix. The linker between the N and C domains of calcium-saturated TnC is flexible in the solution structure.     

Structure of a biologically active fragment of human serum apolipoprotein C-II in the presence of sodium dodecyl sulfate and dodecylphosphocholine

We have studied the three-dimensional structure of a biologically active peptide of apolipoprotein C-II (apoC-II) in the presence of lipid mimetics by CD and NMR spectroscopy. This peptide, corresponding to residues 44-79 of apoC-II, has been shown to reverse the symptoms of genetic apoC-II deficiency in a human subject. A comparison of alpha-proton secondary shifts and CD spectroscopic data indicates that the structure of apoC-II(44-79) is similar in the presence of dodecylphosphocholine and sodium dodecyl sulfate. The three-dimensional structure of apoC-II(44-79) in the presence of sodium dodecyl sulfate, determined by relaxation matrix calculations, contains two amphipathic helical domains formed by residues 50-58 and 67-75, separated by a non-helical linker centered at Tyr63. The C-terminal helix is terminated by a loop formed by residues 76-79. The C-terminal helix is better defined and has a larger hydrophobic face than the N-terminal helix, which leads us to propose that the C-terminal helix together with the non-helical Ile66 constitute the primary lipid binding domain of apoC-II(44-79). Based on our structure we suggest a new mechanism of lipoprotein lipase activation in which both helices of apoC-II(44-79) remain lipid bound, while the seven-residue interhelical linker extends away from the lipid surface in order to project Tyr63 into the apoC-II binding site of lipoprotein lipase.     

Nitrogen-15 chemical shifts in AT (adenine-thymine) and CG (cytosine-guanine) nucleic acid base pairs

This paper presents ab initio (DFT) calculations of the 15N chemical shifts in AT (Adenine-Thymine) and CG (Cytosine-Guanine) nucleic acid base pairs. Calculations were done on 14 AT and 18 CG base pairs using experimental (X-ray) geometries obtained from several DNA decamers. The calculated chemical shifts are compared with the experimental values in the pure bases and subjected to statistical analysis to explore their sensitivity to the local geometry and pair helix parameters. The results indicate that the 15N chemical shifts, isotropic and principal components are quite sensitive to small changes in the geometry of the pairs, but they do not correlate well with the helix pair parameters. From the statistical analysis, several linear correlations between structural parameters and chemical shifts emerge. These relationships may serve as a foundation to extract information on molecular structure from 15N chemical shift measurements.     

Structural and biochemical characterization of neuronal calretinin domain I-II (residues 1-100). Comparison to homologous calbindin D28k domain I-II (residues 1-93).

This study characterizes the calcium-bound CR I-II domain (residues 1-100) of rat calretinin (CR). CR, with six EF-hand motifs, is believed to function as a neuronal intracellular calcium-buffer and/or calcium-sensor. The secondary structure of CR I-II, defined by standard NMR methods on 13C,15N-labeled protein, contains four helices and two short interacting segments of extended structure between the calcium-binding loops. The linker between the two helix-loop-helix, EF-hand motifs is 12 residues long. Limited trypsinolysis at K60 (there are 10 other K/R residues in CR I-II) confirms that the linker of CR I-II is solvent-exposed and that other potential sites are protected by regular secondary structure. 45Ca-overlay of glutathione S-transferase (GST)-CR(1-60) and GST-CR(61-100) fusion proteins confirm that both EF-hands of CR I-II have intrinsic calcium-binding properties. The primary sequence and NMR chemical shifts, including calcium-sensitive glycine residues, also suggest that both EF-hand loops of CR I-II bind calcium. NMR relaxation, analytical ultracentrifugation, chemical cross-linking and NMR translation diffusion measurements indicate that CR I-II exists as a monomer. Calb I-II (the homologous domain of calbindin D28k) has the same EF-hand secondary structures as CR I-II, except that helix B is three residues longer and the linker has only four residues [Klaus, W., Grzesiek, S., Labhardt, A. M., Buckwald, P., Hunziker, W., Gross, M. D. & Kallick, D. A. (1999) Eur. J. Biochem. 262, 933-938]. In contrast, Calb I-II binds one calcium cation per monomeric unit and exists as a dimer. Despite close homology and similar secondary structures, CR I-II and Calb I-II probably have distinct tertiary structure features that suggest different cellular functions for the full-length proteins.     

Secondary structure and dynamics of an intrinsically unstructured linker domain

The transient secondary structure and dynamics of an intrinsically unstructured linker domain from the 70 kDa subunit of human replication protein A was investigated using solution state NMR. Stable secondary structure, inferred from large secondary chemical shifts, was observed for a segment of the intrinsically unstructured linker domain when it is attached to an N-terminal protein interaction domain. Results from NMR relaxation experiments showed the rotational diffusion for this segment of the intrinsically unstructured linker domain to be correlated with the N-terminal protein interaction domain. When the N-terminal domain is removed, the stable secondary structure is lost and faster rotational diffusion is observed. The large secondary chemical shifts were used to calculate phi and psi dihedral angles and these dihedral angles were used to build a backbone structural model. Restrained molecular dynamics were performed on this new structure using the chemical shift based dihedral angles and a single NOE distance as restraints. In the resulting family of structures a large, solvent exposed loop was observed for the segment of the intrinsically unstructured linker domain that had large secondary chemical shifts.     

Helix formation by the phospholipase A2 38–59 fragment: Influence of chain shortening and dimerization monitored by nmr chemical shifts

The solution structure of a peptide fragment corresponding to the 38–59 region of porcine phospholipase A₂ has been investigated using CD, nmr chemical shifts, and nuclear over-hauser effects (NOEs). This isolated fragment of phospholipase forms an α-helix spanning residues 38–55, very similar to the one found in the native protein, except for residues 56–58, which were helical in the crystal but found random in solution. Addition of triflouro-ethanol (TFE) merely increased helix population but it did not redefine helix limits. To investigate how the folding information, in particular that concerning eventual helix start and stop signals, was coded in this particular amino acid sequence, the helices formed by synthetic peptides reproducing sections of this phospholipase 38–59 fragment, namely 40–59, 42–59, 38–50, and 45–57, were characterized using NOEs and helix populations quantitatively evaluated on different peptide chain segments using nmr chemical shifts in two solvents (H₂O and 30% TFE/H₂O). A set of nmr spectra was also recorded and assigned under denaturing conditions (6Murea) to obtain reliable values for the chemical shifts of each peptide in the random state. Based on chemical shift data, it was concluded that the helix formed by the phospholipase 38–59 fragment was not abruptly, but progressively, destabilized all along its length by successive elimination of residues at the N end, while the removal of residues at the C end affected helix stability more locally and to a lesser extent. These results are consistent with the idea that there are not single residues responsible for helix initiation or helix stability, and they also evidence an asymmetry for contributions to helix stability by residues located at the two chain ends. The restriction of molecular mobility caused by linking with a disulphide bridge at Cys 51 two identical 38–59 peptide chains did not increase helix stability. The helix formed by the covalently formed homodimer was very similar in length and population to that formed by the monomer. © 1994 John Wiley & Sons, Inc.     

NMR structure of the N-terminal J domain of murine polyomavirus T antigens. Implications for DnaJ-like domains and for mutations of T antigens

The NMR structure of the N-terminal, DnaJ-like domain of murine polyomavirus tumor antigens (PyJ) has been determined to high precision, with root mean square deviations to the mean structure of 0.38 A for backbone atoms and 0.94 A for all heavy atoms of ordered residues 5-41 and 50-69. PyJ possesses a three-helix fold, in which anti-parallel helices II and III are bridged by helix I, similar to the four-helix fold of the J domains of DnaJ and human DnaJ-1. PyJ differs significantly in the lengths of N terminus, helix I, and helix III. The universally conserved HPD motif appears to form a His-Pro C-cap of helix II. Helix I features a stabilizing Schellman C-cap that is probably conserved universally among J domains. On the helix II surface where positive charges of other J domains have been implicated in binding of hsp70s, PyJ contains glutamine residues. Nonetheless, chimeras that replace the J domain of DnaJ with PyJ function like wild-type DnaJ in promoting growth of Escherichia coli. This activity can be modulated by mutations of at least one of these glutamines. T antigen mutations reported to impair cellular transformation by the virus, presumably via interactions with PP2A, cluster in the hydrophobic folding core and at the extreme N terminus, remote from the HPD loop.     

Recent advances in segmental isotope labeling of proteins: NMR applications to large proteins and glycoproteins

In the last 15 years substantial advances have been made to place isotope labels in native and glycosylated proteins for NMR studies and structure determination. Key developments include segmental isotope labeling using Native Chemical Ligation, Expressed Protein Ligation and Protein Trans-Splicing. These advances are pushing the size limit of NMR spectroscopy further making larger proteins accessible for this technique. It is just emerging that segmental isotope labeling can be used to define inter-domain interactions in NMR structure determination. Labeling of post-translational modified proteins like glycoproteins remains difficult but some promising developments were recently achieved. Key achievements are segmental and site-specific labeling schemes that improve resonance assignment and structure determination of the glycan moiety. We adjusted the focus of this perspective article to concentrate on the NMR applications based on recent developments rather than on labeling methods themselves to illustrate the considerable potential for biomolecular NMR.     

Secondary Structure and Dynamics of an Intrinsically Unstructured Linker Domain

Abstract

The transient secondary structure and dynamics of an intrinsically unstructured linker domain from the 70 kDa subunit of human replication protein A was investigated using solution state NMR. Stable secondary structure, inferred from large secondary chemical shifts, was observed for a segment of the intrinsically unstructured linker domain when it is attached to an N-terminal protein interaction domain. Results from NMR relaxation experiments showed the rotational diffusion for this segment of the intrinsically unstructured linker domain to be correlated with the N-terminal protein interaction domain. When the N-terminal domain is removed, the stable secondary structure is lost and faster rotational diffusion is observed. The large secondary chemical shifts were used to calculate phi and psidihedral angles and these dihedral angles were used to build a backbone structural model. Restrained molecular dynamics were performed on this new structure using the chemical shift based dihedral angles and a single NOE distance as restraints. In the resulting family of structures a large, solvent exposed loop was observed for the segment of the intrinsically unstructured linker domain that had large secondary chemical shifts.     

Native and non-native secondary structure and dynamics in the pH 4 intermediate of apomyoglobin

The partly folded state of apomyoglobin at pH 4 represents an excellent model for an obligatory kinetic folding intermediate. The structure and dynamics of this intermediate state have been extensively examined using NMR spectroscopy. Secondary chemical shifts, (1)H-(1)H NOEs, and amide proton temperature coefficients have been used to probe residual structure in the intermediate state, and NMR relaxation parameters T(1) and T(2) and ?(1)H?-(15)N NOE have been analyzed using spectral densities to correlate motion of the polypeptide chain with these structural observations. A significant amount of helical structure remains in the pH 4 state, indicated by the secondary chemical shifts of the (13)C(alpha), (13)CO, (1)H(alpha), and (13)C(beta) nuclei, and the boundaries of this helical structure are confirmed by the locations of (1)H-(1)H NOEs. Hydrogen bonding in the structured regions is predominantly native-like according to the amide proton chemical shifts and their temperature dependence. The locations of the A, G, and H helix segments and the C-terminal part of the B helix are similar to those in native apomyoglobin, consistent with the early, complete protection of the amides of residues in these helices in quench-flow experiments. These results confirm the similarity of the equilibrium form of apoMb at pH 4 and the kinetic intermediate observed at short times in the quench-flow experiment. Flexibility in this structured core is severely curtailed compared with the remainder of the protein, as indicated by the analysis of the NMR relaxation parameters. Regions with relatively high values of J(0) and low values of J(750) correspond well with the A, B, G, and H helices, an indication that nanosecond time scale backbone fluctuations in these regions of the sequence are restricted. Other parts of the protein show much greater flexibility and much reduced secondary chemical shifts. Nevertheless, several regions show evidence of the beginnings of helical structure, including stretches encompassing the C helix-CD loop, the boundary of the D and E helices, and the C-terminal half of the E helix. These regions are clearly not well-structured in the pH 4 state, unlike the A, B, G, and H helices, which form a native-like structured core. However, the proximity of this structured core most likely influences the region between the B and F helices, inducing at least transient helical structure.     

Multinuclear magnetic resonance studies of Escherichia coli adenylate kinase in free and bound forms. Resonance assignment, secondary structure and ligand binding.

The crystal structure of Escherichia coli adenylate kinase (AKe) revealed three main components: a CORE domain, composed of a five-stranded parallel beta-sheet surrounded by alpha-helices, and two peripheral domains involved in covering the ATP in the active site (LID) and binding of the AMP (NMPbind). We initiated a long-term NMR study aiming to characterize the solution structure, binding mechanism and internal dynamics of the various domains. Using single (15N) and double-labeled (13C and 15N) samples and double- and triple-resonance NMR experiments we assigned 97% of the 1H, 13C and 15N backbone resonances, and proton and 13Cbeta resonances for more than 40% of the side chains in the free protein. Analysis of a 15N-labeled enzyme in complex with the bi-substrate analogue [P1,P5-bis(5'-adenosine)-pentaphosphate] (Ap5A) resulted in the assignment of 90% of the backbone 1H and 15N resonances and 42% of the side chain resonances. Based on short-range NOEs and 1H and 13C secondary chemical shifts, we identified the elements of secondary structure and the topology of the beta-strands in the unliganded form. The alpha-helices and the beta-strands of the parallel beta-sheet in solution have the same limits (+/- 1 residue) as those observed in the crystal. The first helix (alpha1) appears to have a frayed N-terminal side. Significant differences relative to the crystal were noticed in the LID domain, which in solution exhibits four antiparallel beta-strands. The secondary structure of the nucleoside-bound form, as deduced from intramolecular NOEs and the 1Halpha chemical shifts, is similar to that of the free enzyme. The largest chemical shift differences allowed us to map the regions of protein-ligand contacts. 1H/2H exchange experiments performed on free and Ap5A-bound enzymes showed a general decrease of the structural flexibility in the complex which is accompanied by a local increased flexibility on the N-side of the parallel beta-sheet.     

NMR structural and dynamic characterization of the acid-unfolded state of apomyoglobin provides insights into the early events in protein folding

Apomyoglobin forms a denatured state under low-salt conditions at pH 2.3. The conformational propensities and polypeptide backbone dynamics of this state have been characterized by NMR. Nearly complete backbone and some side chain resonance assignments have been obtained, using a triple-resonance assignment strategy tailored to low protein concentration (0.2 mM) and poor chemical shift dispersion. An estimate of the population and location of residual secondary structure has been made by examining deviations of (13)C(alpha), (13)CO, and (1)H(alpha) chemical shifts from random coil values, scalar (3)J(HN,H)(alpha) coupling constants and (1)H-(1)H NOEs. Chemical shifts constitute a highly reliable indicator of secondary structural preferences, provided the appropriate random coil chemical shift references are used, but in the case of acid-unfolded apomyoglobin, (3)J(HN,H)(alpha) coupling constants are poor diagnostics of secondary structure formation. Substantial populations of helical structure, in dynamic equilibrium with unfolded states, are formed in regions corresponding to the A and H helices of the folded protein. In addition, the deviation of the chemical shifts from random coil values indicates the presence of helical structure encompassing the D helix and extending into the first turn of the E helix. The polypeptide backbone dynamics of acid-unfolded apomyoglobin have been investigated using reduced spectral density function analysis of (15)N relaxation data. The spectral density J(omega(N)) is particularly sensitive to variations in backbone fluctuations on the picosecond to nanosecond time scale. The central region of the polypeptide spanning the C-terminal half of the E helix, the EF turn, and the F helix behaves as a free-flight random coil chain, but there is evidence from J(omega(N)) of restricted motions on the picosecond to nanosecond time scale in the A and H helix regions where there is a propensity to populate helical secondary structure in the acid-unfolded state. Backbone fluctuations are also restricted in parts of the B and G helices due to formation of local hydrophobic clusters. Regions of restricted backbone flexibility are generally associated with large buried surface area. A significant increase in J(0) is observed for the NH resonances of some residues located in the A and G helices of the folded protein and is associated with fluctuations on a microsecond to millisecond time scale that probably arise from transient contacts between these distant regions of the polypeptide chain. Our results indicate that the equilibrium unfolded state of apomyoglobin formed at pH 2.3 is an excellent model for the events that are expected to occur in the earliest stages of protein folding, providing insights into the regions of the polypeptide that spontaneously undergo local hydrophobic collapse and sample nativelike secondary structure.     

Structural similarity between ornithine and aspartate transcarbamoylases of Escherichia coli: implications for domain switching.

Each catalytic (c) polypeptide chain of Escherichia coli aspartate transcarbamoylase (ATCase) is composed of two globular domains connected by two interdomain helices. Helix 12, near the C-terminus, extends from the second domain back through the first domain, bringing the two termini close together. This helix is of critical importance for the assembly of a stable enzyme. The trimeric E. coli enzyme ornithine transcarbamoylase (OTCase) is proposed to be similar in tertiary and quaternary structure to the ATCase trimer and has a predicted alpha-helical segment near its C-terminus. In our companion paper, we have shown that this putative helix is essential for OTCase folding and assembly (Murata L, Schachman HK, 1996, Protein Sci 5:709-718). Here, the similarity between OTCase and the ATCase trimer, which are 32% identical in sequence, was tested further by the construction of several chimeras in which various structural elements were switched between the enzymes by genetic techniques. These elements included the two globular domains and regions containing the C-terminal helices. In contrast to results reported previously (Houghton J, O'Donovan G, Wild J, 1989, Nature 338:172-174), none of the chimeric proteins exhibited in vivo activity and all were insoluble when overexpressed. Attempts to make hybrid trimers composed of c chains from ATCase and OTCase were also unsuccessful. These results underscore the complexities of specific intrachain and interchain side-chain interactions required to maintain tertiary and quaternary structures in these enzymes.     

Collagen stabilization at atomic level: crystal structure of designed (GlyProPro)10foldon

In a designed fusion protein the trimeric domain foldon from bacteriophage T4 fibritin was connected to the C terminus of the collagen model peptide (GlyProPro)(10) by a short Gly-Ser linker to facilitate formation of the three-stranded collagen triple helix. Crystal structure analysis at 2.6 A resolution revealed conformational changes within the interface of both domains compared with the structure of the isolated molecules. A striking feature is an angle of 62.5 degrees between the symmetry axis of the foldon trimer and the axis of the triple helix. The melting temperature of (GlyProPro)(10) in the designed fusion protein (GlyProPro)(10)foldon is higher than that of isolated (GlyProPro)(10,) which suggests an entropic stabilization compensating for the destabilization at the interface.     

Structure of the theta subunit of Escherichia coli DNA polymerase III in complex with the epsilon subunit

The catalytic core of Escherichia coli DNA polymerase III contains three tightly associated subunits, the alpha, epsilon, and theta subunits. The theta subunit is the smallest and least understood subunit. The three-dimensional structure of theta in a complex with the unlabeled N-terminal domain of the epsilon subunit, epsilon186, was determined by multidimensional nuclear magnetic resonance spectroscopy. The structure was refined using pseudocontact shifts that resulted from inserting a lanthanide ion (Dy3+, Er3+, or Ho3+) at the active site of epsilon186. The structure determination revealed a three-helix bundle fold that is similar to the solution structures of theta in a methanol-water buffer and of the bacteriophage P1 homolog, HOT, in aqueous buffer. Conserved nuclear Overhauser enhancement (NOE) patterns obtained for free and complexed theta show that most of the structure changes little upon complex formation. Discrepancies with respect to a previously published structure of free theta (Keniry et al., Protein Sci. 9:721-733, 2000) were attributed to errors in the latter structure. The present structure satisfies the pseudocontact shifts better than either the structure of theta in methanol-water buffer or the structure of HOT. satisfies these shifts. The epitope of epsilon186 on theta was mapped by NOE difference spectroscopy and was found to involve helix 1 and the C-terminal part of helix 3. The pseudocontact shifts indicated that the helices of theta are located about 15 A or farther from the lanthanide ion in the active site of epsilon186, in agreement with the extensive biochemical data for the theta-epsilon system.     

Cooperative folding in a multi-domain protein

Most protein domains are found in multi-domain proteins, yet most studies of protein folding have concentrated on small, single-domain proteins or on isolated domains from larger proteins. Spectrin domains are small (106 amino acid residues), independently folding domains consisting of three long alpha-helices. They are found in multi-domain proteins with a number of spectrin domains in tandem array. Structural studies have shown that in these arrays the last helix of one domain forms a continuous helix with the first helix of the following domain. It has been demonstrated that a number of spectrin domains are stabilised by their neighbours. Here we investigate the molecular basis for cooperativity between adjacent spectrin domains 16 and 17 from chicken brain alpha-spectrin (R16 and R17). We show that whereas the proteins unfold as a single cooperative unit at 25 degrees C, cooperativity is lost at higher temperatures and in the presence of stabilising salts. Mutations in the linker region also cause the cooperativity to be lost. However, the cooperativity does not rely on specific interactions in the linker region alone. Most mutations in the R17 domain cause a decrease in cooperativity, whereas proteins with mutations in the R16 domain still fold cooperatively. We propose a mechanism for this behaviour.     

Quantitative comparison of the hydrogen bond network of A-state and native ubiquitin by hydrogen bond scalar couplings

The backbone hydrogen bond (H-bond) network of the partially folded A-state of ubiquitin (60% methanol, 40% water, pH 2) has been characterized quantitatively by (h3)J(NC)(') H-bond scalar couplings between the (15)N nuclei of amino acid H-bond donors and the (13)C carbonyl nuclei of the acceptors. Results on (h3)J(NC)(') couplings and the amide proton ((1)H(N)) chemical shifts for the A-state are compared quantitatively to the native state. The (h3)J(NC)(') correlations of the A-state show intact, nativelike H-bonds of the first beta-hairpin beta1/beta2 and the alpha-helix, albeit at lower strength, whereas the H-bonds in the C-terminal part change from a pure beta-structure to an all alpha-helical H(N)(i)-->O(i-4) connectivity pattern. A residue-specific analysis reveals that the conformations within the conserved secondary structure segments are much more homogeneous in the A-state than in the native state. Thus, the strong asymmetry of (h3)J(NC)(') couplings and (1)H(N) chemical shifts between the interior and exterior sides of the native state alpha-helix vanishes in the A-state. This indicates that the bend of this helix around the native state hydrophobic core is released in the homogeneous solvent environment of the A-state. Similarly, an irregularity in the behavior of H-bond I3-->L15 in hairpin beta1/beta2, which results from strong contacts to strand beta5 in the native state, is absent in the A-state. These findings rationalize the behavior of the (1)H(N) chemical shifts in both states and indicate that the A-state is in many aspects similar to the onset of thermal denaturation of the native state.