Biomedical subjects

Christopher P Jaroniec

Publications and source records attributed to Christopher P Jaroniec.

11 recordsLinked to original sources

PubMed2005

Structure and dynamics of micelle-associated human immunodeficiency virus gp41 fusion domain.

The N-terminal fusion domain of the HIV-1 gp41 envelope glycoprotein is responsible for initiating the fusion of viral and cellular membranes, leading to the subsequent infection of the host cell by HIV-1. We have investigated the backbone structure and dynamics of the 30 N-terminal residues of HIV-1 gp41 in membrane-mimicking environments using NMR spectroscopy and (15)N- and (15)N,(13)C,(2)H-labeled peptides. Similar (15)N-(1)H HSQC spectra were obtained in a variety of detergents, including SDS, DPC, mixed DPC/SDS, and LPPG micelles, indicating that the peptide structure is not strongly influenced by the type of detergent used. Detailed characterization was carried out in SDS micelles, where the long-term sample stability was found to be optimal. In addition to J-coupling and NOE restraints, a nearly complete set of backbone residual dipolar coupling restraints was recorded for the fusion domain-micelle complex aligned with respect to the magnetic field using a stretched polyacrylamide gel. Backbone amide (15)N spin relaxation and amide hydrogen exchange rates with the solvent were also measured. The ensemble of NMR structures reveals an uninterrupted alpha-helix for the least mobile residues (S(2) > 0.65), Ile-4 to Met-19, with transient helical character extending up to Ala-22. A 12-residue (Ile-4 to Ala-15) segment is fully shielded from solvent, with Gly-3 and Gly-16 found at micelle-solvent interfaces. Residues external to the micelle exhibit enhanced picosecond to nanosecond time scale dynamics relative to the residues buried in the micelle, and their mobility increases with the distance from the micelle.

Amino Acid Sequence↗

PubMed2005

Accurate measurement of 15N-13C residual dipolar couplings in nucleic acids.

New 3D HCN quantitative J (QJ) pulse schemes are presented for the precise and accurate measurement of one-bond 15N1/9-13C1', 15N1/9-13C6/8, and 15N1/9-13C2/4 residual dipolar couplings (RDCs) in weakly aligned nucleic acids. The methods employ 1H-13C multiple quantum (MQ) coherence or TROSY-type pulse sequences for optimal resolution and sensitivity. RDCs are obtained from the intensity ratio of H1'-C1'-N1/9 (MQ-HCN-QJ) or H6/8-C6/8-N1/9 (TROSY-HCN-QJ) correlations in two interleaved 3D NMR spectra, with dephasing intervals of zero (reference spectrum) and approximately 1/(2J(NC)) (attenuated spectrum). The different types of 15N-13C couplings can be obtained by using either the 3D MQ-HCN-QJ or TROSY-HCN-QJ pulse scheme, with the appropriate setting of the duration of the constant-time 15N evolution period and the offset of two frequency-selective 13C pulses. The methods are demonstrated for a uniformly 13C, 15N-enriched 24-nucleotide stem-loop RNA sequence, helix-35psi, aligned in the magnetic field using phage Pf1. For measurements of RDCs systematic errors are found to be negligible, and experiments performed on a 1.5 mM helix-35psi sample result in an estimated precision of ca. 0.07 Hz for 1D(NC), indicating the utility of the measured RDCs in structure validation and refinement. Indeed, for a complete set of 15N1/9-13C1', 15N1/9-13C6/8, and 15N1/9-13C2/4 dipolar couplings obtained for the stem nucleotides, the measured RDCs are in excellent agreement with those predicted for an NMR structure of helix-35psi, refined using independently measured observables, including 13C-1H, 13C-13C and 1H-1H dipolar couplings.

Adenine↗

PubMed2004

High-resolution molecular structure of a peptide in an amyloid fibril determined by magic angle spinning NMR spectroscopy.

Amyloid fibrils are self-assembled filamentous structures associated with protein deposition conditions including Alzheimer's disease and the transmissible spongiform encephalopathies. Despite the immense medical importance of amyloid fibrils, no atomic-resolution structures are available for these materials, because the intact fibrils are insoluble and do not form diffraction-quality 3D crystals. Here we report the high-resolution structure of a peptide fragment of the amyloidogenic protein transthyretin, TTR(105-115), in its fibrillar form, determined by magic angle spinning NMR spectroscopy. The structure resolves not only the backbone fold but also the precise conformation of the side chains. Nearly complete (13)C and (15)N resonance assignments for TTR(105-115) formed the basis for the extraction of a set of distance and dihedral angle restraints. A total of 76 self-consistent experimental measurements, including 41 restraints on 19 backbone dihedral angles and 35 (13)C-(15)N distances between 3 and 6 A were obtained from 2D and 3D NMR spectra recorded on three fibril samples uniformly (13)C, (15)N-labeled in consecutive stretches of four amino acids and used to calculate an ensemble of peptide structures. Our results indicate that TTR(105-115) adopts an extended beta-strand conformation in the amyloid fibrils such that both the main- and side-chain torsion angles are close to their optimal values. Moreover, the structure of this peptide in the fibrillar form has a degree of long-range order that is generally associated only with crystalline materials. These findings provide an explanation of the unusual stability and characteristic properties of this form of polypeptide assembly.

Amino Acid Sequence↗

PubMed2004

Quantitative J correlation methods for the accurate measurement of 13C'-13Calpha dipolar couplings in proteins.

Methods are described for the precise and accurate measurement of one-bond dipolar (13)C'-(13)C(alpha) couplings in weakly aligned proteins. The experiments are based on the principle of quantitative J correlation, where (1)J(C'C(alpha)) (or (1)J(C'C(alpha)) + 1D(C'C(alpha)) is measured from the relative intensity of two interleaved 3D TROSY-HN(CO)CA or 3DTROSY-HNCO spectra recorded with dephasing intervals of zero (reference spectrum) and approximately 3/(2(1)J(C'C(alpha)) (attenuated spectrum). In analogy to other quantitative J correlation techniques, the random error in the measured (1)J(C'C(alpha)) value is inversely proportional to the signal-to-noise ratio in the reference spectrum. It is shown that for weakly aligned proteins, with the magnitude of the alignment tensor of D(a)(NH) < or = 10-15 Hz, the systematic errors are typically negligible. The methods are demonstrated for the third IgG-binding domain of protein G (GB3) and a-synuclein in complex with a detergent micelle, where errors in (1)D(C'C(alpha)) of less than 0.1 Hz and ca. 0.2 Hz,respectively, are estimated. Remarkably, the dipolar couplings determined for GB3 are in even better agreement with the recently refined 1.1-angstroms X-ray structure than the input (13)C'-(13)C(alpha) couplings used for the refinement.

Carbon Isotopes↗

PubMed2003

Measurement of multiple psi torsion angles in uniformly 13C,15N-labeled alpha-spectrin SH3 domain using 3D 15N-13C-13C-15N MAS dipolar-chemical shift correlation spectroscopy.

We demonstrate the simultaneous measurement of several backbone torsion angles psi in the uniformly (13)C,(15)N-labeled alpha-Spectrin SH3 domain using two different 3D 15N-13C-13C-15N dipolar-chemical shift magic-angle spinning (MAS) NMR experiments. The first NCCN experiment utilizes double quantum (DQ) spectroscopy combined with the INADEQUATE type 13C-13C chemical shift correlation. The decay of the DQ coherences formed between 13C'(i) and 13C(alphai) spin pairs is determined by the "correlated" dipolar field due to 15N(i)-13C(alphai) and 13C'(i)-15N(i+1) dipolar couplings and is particularly sensitive to variations of the torsion angle in the regime |psi| > 140 degrees. However, the ability of this experiment to constrain multiple psi-torsion angles is limited by the resolution of the 13C(alpha)-(13)CO correlation spectrum. This problem is partially addressed in the second approach described here, which is an NCOCA NCCN experiment. In this case the resolution is enhanced by the superior spectral dispersion of the 15N resonances present in the 15N(i+1)-13C(alphai) part of the NCOCA chemical shift correlation spectrum. For the case of the 62-residue alpha-spectrin SH3 domain, we determined 13 psi angle constraints with the INADEQUATE NCCN experiment and 22 psi constraints were measured in the NCOCA NCCN experiment.

Carbon Isotopes↗

PubMed2002

Molecular conformation of a peptide fragment of transthyretin in an amyloid fibril.

The molecular conformation of peptide fragment 105-115 of transthyretin, TTR(105-115), previously shown to form amyloid fibrils in vitro, has been determined by magic-angle spinning solid-state NMR spectroscopy. 13C and 15N linewidth measurements indicate that TTR(105-115) forms a highly ordered structure with each amino acid in a unique environment. 2D 13C-13C and 15N-13C-13C chemical shift correlation experiments, performed on three fibril samples uniformly 13C,15N-labeled in consecutive stretches of 4 aa, allowed the complete sequence-specific backbone and side-chain 13C and 15N resonance assignments to be obtained for residues 105-114. Analysis of the 15N, 13CO, 13Calpha, and 13Cbeta chemical shifts allowed quantitative predictions to be made for the backbone torsion angles phi and psi. Furthermore, four backbone 13C-15N distances were determined in two selectively 13C,15N-labeled fibril samples by using rotational-echo double-resonance NMR. The results show that TTR(105-115) adopts an extended beta-strand conformation that is similar to that found in the native protein except for substantial differences in the vicinity of the proline residue.

Amino Acid Sequence↗

PubMed2002

Determination of multiple torsion-angle constraints in U-(13)C,(15)N-labeled peptides: 3D (1)H-(15)N-(13)C-(1)H dipolar chemical shift NMR spectroscopy in rotating solids.

We demonstrate constraint of peptide backbone and side-chain conformation with 3D (1)H-(15)N-(13)C-(1)H dipolar chemical shift, magic-angle spinning NMR experiments. In these experiments, polarization is transferred from (15)N[i] by ramped SPECIFIC cross polarization to the (13)C(alpha)[i], (13)C(beta)[i], and (13)C(alpha)[i - 1] resonances and evolves coherently under the correlated (1)H-(15)N and (1)H-(13)C dipolar couplings. The resulting set of frequency-labeled (15)N(1)H-(13)C(1)H dipolar spectra depend strongly upon the molecular torsion angles phi[i], chi1[i], and psi[i - 1]. To interpret the data with high precision, we considered the effects of weakly coupled protons and differential relaxation of proton coherences via an average Liouvillian theory formalism for multispin clusters and employed average Hamiltonian theory to describe the transfer of (15)N polarization to three coupled (13)C spins ((13)C(alpha)[i], (13)C(beta)[i], and (13)C(alpha)[i - 1]). Degeneracies in the conformational solution space were minimized by combining data from multiple (15)N(1)H-(13)C(1)H line shapes and analogous data from other 3D (1)H-(13)C(alpha)-(13)C(beta)-(1)H (chi1), (15)N-(13)C(alpha)-(13)C'-(15)N (psi), and (1)H-(15)N[i]-(15)N[i + 1]-(1)H (phi, psi) experiments. The method is demonstrated here with studies of the uniformly (13)C,(15)N-labeled solid tripeptide N-formyl-Met-Leu-Phe-OH, where the combined data constrains a total of eight torsion angles (three phi, three chi1, and two psi): phi(Met) = -146 degrees, psi(Met) = 159 degrees, chi1(Met) = -85 degrees, phi(Leu) = -90 degrees, psi(Leu) = -40 degrees, chi1(Leu) = -59 degrees, phi(Phe) = -166 degrees, and chi1(Phe) = 56 degrees. The high sensitivity and dynamic range of the 3D experiments and the data analysis methods provided here will permit immediate application to larger peptides and proteins when sufficient resolution is available in the (15)N-(13)C chemical shift correlation spectra.

Carbon Isotopes↗

PubMed2002

3D TEDOR NMR experiments for the simultaneous measurement of multiple carbon-nitrogen distances in uniformly (13)C,(15)N-labeled solids.

We describe three-dimensional magic-angle-spinning NMR experiments for the simultaneous measurement of multiple carbon-nitrogen distances in uniformly (13)C,(15)N-labeled solids. The approaches employ transferred echo double resonance (TEDOR) for (13)C-(15)N coherence transfer and (15)N and (13)C frequency labeling for site-specific resolution, and build on several previous 3D TEDOR techniques. The novel feature of the 3D TEDOR pulse sequences presented here is that they are specifically designed to circumvent the detrimental effects of homonuclear (13)C-(13)C J-couplings on the measurement of weak (13)C-(15)N dipolar couplings. In particular, homonuclear J-couplings lead to two undesirable effects: (i) they generate anti-phase and multiple-quantum (MQ) spin coherences, which lead to spurious cross-peaks and phase-twisted lines in the 2D (15)N-(13)C correlation spectra, and thus degrade the spectral resolution and prohibit the extraction of reliable cross-peak intensities, and (ii) they significantly reduce cross-peak intensities for strongly J-coupled (13)C sites (e.g., CO and C(alpha)). The first experiment employs z-filter periods to suppress the anti-phase and MQ coherences and generates 2D spectra with purely absorptive peaks for all TEDOR mixing times. The second approach uses band-selective (13)C pulses to refocus J-couplings between (13)C spins within the selective pulse bandwidth and (13)C spins outside the bandwidth. The internuclear distances are extracted by using a simple analytical model, which accounts explicitly for multiple spin-spin couplings contributing to cross-peak buildup. The experiments are demonstrated in two U-(13)C,(15)N-labeled peptides, N-acetyl-L-Val-L-Leu (N-ac-VL) and N-formyl-L-Met-L-Leu-L-Phe (N-f-MLF), where 20 and 26 (13)C-(15)N distances up to approximately 5-6 A were measured, respectively. Of the measured distances, 10 in N-ac-VL and 13 in N-f-MLF are greater than 3 A and provide valuable structural constraints.

Carbon Isotopes↗

PubMed2002

De novo determination of peptide structure with solid-state magic-angle spinning NMR spectroscopy.

The three-dimensional structure of the chemotactic peptide N-formyl-l-Met-l-Leu-l-Phe-OH was determined by using solid-state NMR (SSNMR). The set of SSNMR data consisted of 16 (13)C-(15)N distances and 18 torsion angle constraints (on 10 angles), recorded from uniformly (13)C,(15)N- and (15)N-labeled samples. The peptide's structure was calculated by means of simulated annealing and a newly developed protocol that ensures that all of conformational space, consistent with the structural constraints, is searched completely. The result is a high-quality structure of a molecule that has thus far not been amenable to single-crystal diffraction studies. The extensions of the SSNMR techniques and computational methods to larger systems appear promising.

N-Formylmethionine Leucyl-Phenylalanine↗

PubMed2002

Tryptophan interactions in bacteriorhodopsin: a heteronuclear solid-state NMR study.

The bulky and amphiphilic nature of tryptophan residues makes them particularly interesting components of proteins. In bacteriorhodopsin, four of the eight tryptophan residues are in the active site, forming parts of the retinal binding pocket. In this work, we use solid-state NMR to study the interactions of the tryptophan residues in wild-type bacteriorhodopsin, in the resting state, and in critical intermediates of the proton-motive photocycle. The range of the chemical shifts of the indole nitrogens suggests that all eight of them are hydrogen bonded. Using difference spectroscopy, we isolate several changes in these hydrogen bonds in the early and late M states. As found earlier for the peptide backbone, some perturbations found in the early M state relax in the transition to the late M state while new perturbations arise. Interestingly, Rotational Echo DOuble Resonance (REDOR) difference spectroscopy of [20-13C]retinal,[indole-15N]Trp-bR shows that indole of Trp182 is not involved in the significant hydrogen bond perturbations. We also use REDOR to measure dipolar interactions in [20-13C]retinal,[indole-15N]Trp-bR, and thereby determine the distance between the C20 of retinal and the indole nitrogen of Trp182. The internuclear distance changes only slightly from the light-adapted state (3.36 +/- 0.2 A) to the early M state (3.16 +/- 0.4 A).

Bacteriorhodopsins↗

PubMed2002

Chromophore distortions in the bacteriorhodopsin photocycle: evolution of the H-C14-C15-H dihedral angle measured by solid-state NMR.

In recent years, structural information about bacteriorhodopsin has grown substantially with the publication of several crystal structures. However, precise measurements of the chromophore conformation in the various photocycle states are still lacking. This information is critical because twists about the chromophore backbone chain can influence the Schiff base nitrogen position, orientation, and proton affinity. Here, we focus on the C14-C15 bond, using solid-state nuclear magnetic resonance spectroscopy to measure the H-C14-C15-H dihedral angle. In the resting state (bR(568)), we obtain an angle of 164 +/- 4 degrees, indicating a 16 degrees distortion from a planar all-trans chromophore. The dihedral angle is found to decrease to 147 +/- 10 degrees in the early M intermediate (M(o)) and to 150 +/- 4 degrees in the late M intermediate (M(n)). These results demonstrate changes in the chromophore conformation undetected by recent X-ray diffraction studies.

Bacteriorhodopsins↗