Backbone dynamics of an oncogenic mutant of Cdc42Hs shows increased flexibility at the nucleotide-binding site

Cdc42Hs, a member of the Ras superfamily of GTP-binding signal transduction proteins, binds guanine nucleotides, and acts as a molecular-timing switch in multiple signal transduction pathways. The structure of the wild-type protein has been solved (Feltham et al. (1997) Biochemistry 36, 8755-8766), and the backbone dynamics have been characterized by NMR spectroscopy (Loh et al. (1999) Biochemistry 38, 12547-12557). The F28L mutation of Cdc42Hs is characterized by an increased rate of cycling between the GTP and GDP-bound forms leading to cell transformation (Lin et al. (1997) Curr. Biol. 7, 794-797). Here, we describe the backbone dynamics of Cdc42Hs(F28L)-GDP using 1H-15N NMR measurements of T1, T1rho, and steady-state NOE at two magnetic field strengths. Residue-specific values of the generalized order parameters (Ss2 and Sf2), local correlation time (tau(e)), and exchange rate (R(ex)) were obtained using the Lipari-Szabo formalism. Chemical-shift perturbation analysis suggested that very little structural change was evident outside of the nucleotide-binding site. However, residues comprising the nucleotide-binding site, as well as the nucleotide itself, exhibit increased dynamics over a wide range of time scales in Cdc42Hs(F28L) relative to the wild type. In addition to changes in dynamics measured by relaxation methods, hydrogen-deuterium exchange indicated a substantial disruption of the hydrogen-bonding network within the nucleotide-binding site. Thus, local dynamic changes introduced by a single-point mutation can affect important aspects of signaling processes without disrupting the conformation of the whole protein.     

Backbone dynamics of the oligomerization domain of p53 determined from 15N NMR relaxation measurements.

The backbone dynamics of the tetrameric p53 oligomerization domain (residues 319-360) have been investigated by two-dimensional inverse detected heteronuclear 1H-15N NMR spectroscopy at 500 and 600 MHz. 15N T1, T2, and heteronuclear NOEs were measured for 39 of 40 non-proline backbone NH vectors at both field strengths. The overall correlation time for the tetramer, calculated from the T1/T2 ratios, was found to be 14.8 ns at 35 degrees C. The correlation times and amplitudes of the internal motions were extracted from the relaxation data using the model-free formalism (Lipari G, Szabo A, 1982, J Am Chem Soc 104:4546-4559). The internal dynamics of the structural core of the p53 oligomerization domain are uniform and fairly rigid, with residues 327-354 exhibiting an average generalized order parameter (S2) of 0.88 +/- 0.08. The N- and C-termini exhibit substantial mobility and are unstructured in the solution structure of p53. Residues located at the N- and C-termini, in the beta-sheet, in the turn between the alpha-helix and beta-sheet, and at the C-terminal end of the alpha-helix display two distinct internal motions that are faster than the overall correlation time. Fast internal motions (< or = 20 ps) are within the extreme narrowing limit and are of uniform amplitude. The slower motions (0.6-2.2 ns) are outside the extreme narrowing limit and vary in amplitude.(ABSTRACT TRUNCATED AT 250 WORDS)     

Backbone dynamics of barstar: a (15)N NMR relaxation study

Backbone dynamics of uniformly (15)N-labeled barstar have been studied at 32 degrees C, pH 6.7, by using (15)N relaxation data obtained from proton-detected 2D (1)H-(15)N NMR spectroscopy. (15)N spin-lattice relaxation rate constants (R(1)), spin-spin relaxation rate constants (R(2)), and steady-state heteronuclear (1)H-(15)N NOEs have been determined for 69 of the 86 (excluding two prolines and the N-terminal residue) backbone amide (15)N at a magnetic field strength of 14.1 Tesla. The primary relaxation data have been analyzed by using the model-free formalism of molecular dynamics, using both isotropic and axially symmetric diffusion of the molecule, to determine the overall rotational correlation time (tau(m)), the generalized order parameter (S(2)), the effective correlation time for internal motions (tau(e)), and NH exchange broadening contributions (R(ex)) for each residue. As per the axially symmetric diffusion, the ratio of diffusion rates about the unique and perpendicular axes (D( parallel)/D( perpendicular)) is 0.82 +/- 0.03. The two results have only marginal differences. The relaxation data have also been used to map reduced spectral densities for the NH vectors of these residues at three frequencies: 0, omega(H), and omega(N), where omega(H),(N) are proton and nitrogen Larmor frequencies. The value of tau(m) obtained from model-free analysis of the relaxation data is 5.2 ns. The reduced spectral density analysis, however, yields a value of 5.7 ns. The tau(m) determined here is different from that calculated previously from time-resolved fluorescence data (4.1 ns). The order parameter ranges from 0.68 to 0.98, with an average value of 0.85 +/- 0.02. A comparison of the order parameters with the X-ray B-factors for the backbone nitrogens of wild-type barstar does not show any considerable correlation. Model-free analysis of the relaxation data for seven residues required the inclusion of an exchange broadening term, the magnitude of which ranges from 2 to 9.1 s(-1), indicating the presence of conformational averaging motions only for a small subset of residues.     

Backbone dynamics of the Bacillus subtilis glucose permease IIA domain determined from 15N NMR relaxation measurements.

The backbone dynamics of the uniformly 15N-labeled IIA domain of the glucose permease of Bacillus subtilis have been characterized using inverse-detected two-dimensional 1H-15N NMR spectroscopy. Longitudinal (T1) and transverse (T2) 15N relaxation time constants and steady-state (1H)-15N NOEs were measured, at a spectrometer proton frequency of 500 MHz, for 137 (91%) of the 151 protonated backbone nitrogens. These data were analyzed by using a model-free dynamics formalism to determine the generalized order parameter (S2), the effective correlation time for internal motions (tau e), and 15N exchange broadening contributions (Rex) for each residue, as well as the overall molecular rotational correlation time (tau m). The T1 and T2 values for most residues were in the ranges 0.45-0.55 and 0.11-0.15 s, respectively; however, a small number of residues exhibited significantly slower relaxation. Similarly, (1H)-15N NOE values for most residues were in the range 0.72-0.80, but a few residues had much smaller positive NOEs and some exhibited negative NOEs. The molecular rotational correlation time was 6.24 +/- 0.01 ns; most residues had order parameters in the range 0.75-0.90 and tau e values of less than ca. 25 ps. Residues found to be more mobile than the average were concentrated in three areas: the N-terminal residues (1-13), which were observed to be highly disordered; the loop from P25 to D41, the apex of which is situated adjacent to the active site and may have a role in binding to other proteins; and the region from A146 to S149. All mobile residues occurred in regions close to termini, in loops, or in irregular secondary structure.     

Backbone dynamics of the ribonuclease binase active site area using multinuclear ((15)N and (13)CO) NMR relaxation and computational molecular dynamics

The nano-pico second backbone dynamics of the ribonuclease binase, homologous to barnase, is investigated with (15)N, (13)C NMR relaxation at 11.74 and 18.78 T and with a 1.1 ns molecular dynamics simulation. The data are compared with the temperature factors reported for the X-ray structure of this enzyme. The molecular dynamics and X-ray data correspond well and predict motions in the loops 56-61 and 99-104 that contain residues that specifically recognize substrate and are catalytic (His101), respectively. In contrast, the (15)N relaxation data indicate that these loops are mostly ordered at the nano-pico second time scale. Nano-pico second motions in the recognition loop 56-61 are evident from (13)CO-(13)C cross relaxation data, but the mobility of the catalytic loop 99-104 is not detected by (13)CO cross relaxation either. From the results of this and previous work [Wang, L., Pang, Y., Holder, T., Brender, J. R., Kurochkin, A., and Zuiderweg, E. R. P. (2001) Proc. Natl. Acad. Sci. U.S.A., 98, 7684-7689], the following dynamical characterization of the active site area of binase emerges: a beta sheet, rigid at all probed time scales, supports the catalytic residue Glu 72. Both substrate-encapsulating loops are mobile on both fast and slow time scales, but the fast motions of the loop which contains the other catalytic residue, His 101, as predicted by B-factors and computational molecular dynamics is not detected by NMR relaxation. This work strongly argues for the use of several measures in the study of protein dynamics.     

Backbone dynamics of the cytotoxic ribonuclease alpha-sarcin by 15N NMR relaxation methods

The cytotoxic ribonuclease -sarcin is a 150-residue protein that inactivates ribosomes by selectively cleaving a single phosphodiester bond in a strictly conserved rRNA loop. In order to gain insights on the molecular basis of its highly specific activity, we have previously determined its solution structure and studied its electrostatics properties. Here, we complement those studies by analysing the backbone dynamics of -sarcin through measurement of longitudinal relaxation rates R₁, off resonance rotating frame relaxation rates R₁, and the ¹⁵N¹HNOE of the backbone amide ¹⁵N nuclei at two different magnetic field strengths (11.7 and 17.6 T). The two sets of relaxation parameters have been analysed in terms of the reduced spectral density mapping formalism, as well as by the model-free approach. -Sarcin behaves as an axial symmetric rotor of the prolate type (D/D=1.16 ± 0.02) which tumbles with a correlation time _m of 7.54 ± 0.02 ns. The rotational diffusion properties have been also independently evaluated by hydrodynamic calculations and are in good agreement with the experimental results. The analysis of the internal dynamics reveals that -sarcin is composed of a rigid hydrophobic core and some exposed segments which undergo fast (ps to ns) internal motions. Slower motions in the s to ms time scale are less abundant and in some cases can be assigned to specific motional processes. All dynamic data are discussed in relation to the role of some particular residues of -sarcin in the process of recognition of its ribosomal target.     

Concerted motion of a protein-peptide complex: backbone dynamics studies of an (15)N-labeled peptide derived from P(21)-activated kinase bound to Cdc42Hs.GMPPCP.

Cdc42Hs is a member of the Ras superfamily of GTPases which, when active, initiates a cascade beginning with the activation of several kinases, including P(21)-activated kinase (PAK). We previously determined the structure of a complex between a 46 amino acid fragment peptide derived from the PAK binding domain (PBD46) and Cdc42Hs.GMPPCP (Gizachew, D., Guo, W., Chohan, K. K., Sutcliffe, M. J., and Oswald, R. E. (2000) Biochemistry 39, 3963-3971). Previous studies (Loh, A. P., Guo, W., Nicholson, L. K., and Oswald, R. E. (1999) Biochemistry 38, 12547-12557) suggest that the regions of Cdc42Hs that bind effectors and regulators have distinct dynamic properties from the remainder of the protein. Here, we describe the backbone dynamics of PBD46 bound to Cdc42Hs.GMPPCP. T(1), T(2), T(1)(rho), and steady-state nuclear Overhauser effects were measured at 500 and 600 MHz. An extension of the Lipari-Szabo model-free analysis was used to determine the order parameters (S(2)) and local correlation times (tau(e)) of the N-H bond vectors within PBD46. Both Cdc42Hs and PBD46 exhibit increased mobility in the free versus the bound state, suggesting that protein flexibility may be required for high-affinity PBD46 binding and, presumably, the activation of PAK. Different backbone dynamics were observed in different regions of the peptide. The beta-strand region of bound PBD46, which makes contacts with beta2 of Cdc42Hs, exhibits low mobility on the pico- to nanosecond timescale. However, the part of PBD46 that interacts with Switch I of Cdc42Hs exhibits greater mobility. Thus, PBD46 and Cdc42Hs form a tight complex that exhibits concerted dynamics.     

A comparison of 15N NMR relaxation measurements with a molecular dynamics simulation: Backbone dynamics of the glucocorticoid receptor DNA-binding domain

The rapid motions of the backbone of the DNA-binding domain of the glucocorticoid receptor (GR DBD) have been investigated using proton-detected heteronuclear NMR experiments on ¹⁵N-labeled protein at pH 6.0 and with a 200 psec molecular dynamics simulation of hydrated GR DBD. The experimental data were interpreted in terms of a generalized order parameter (S²) and an effective correlation time (τ_e) for the internal motion of each amide bond. A back calculation, using the same model, yielded the {¹H}-¹⁵N nuclear Overhauser effects (NOEs) and the ¹⁵N spin-lattice relaxation times (T₁) from the simulated data. The rapid motions of the backbone turned out to be rather limited and uniform throughout the protein, with a somewhat reduced mobility in the two major α-helical regions and a slightly enhanced flexibility for some residues in the first zinc coordinating region. The agreement between the experimental and simulated S²-values was as good as quantitative for most of the residues, except for some residues that were subject to a more large-scale, and in the simulation thus poorly sampled, motion. Examples of such motions that were found in the simulation include jumps of the amide bond of Ile-487 between the charged oxygens of the side chain of Asp-485 and less distinct large scale motions for some of the residues in the extended regions, that were shown to give rise to noisy and/or fast decaying internal reorientational correlation functions. For these residues large differences in the simulated and experimental τ_e-values were found, indicating that motions on different time scales were dominating in the experimental and simulated values. The lower (<0.7) experimental NOEs for these residues could not be reproduced in the simulation and were shown to be a consequence of the lower τ_e-values estimated in the simulation. By combining information from the simulation and the experiment a more complete picture of the motions for these residues can be obtained as is illustrated with an estimation of the jump angle and jump frequency for the amide bond of Ile-487. © 1993 Wiley-Liss, Inc.     

Backbone dynamics of escherichia coli adenylate kinase at the extreme stages of the catalytic cycle studied by (15)N NMR relaxation

Adenylate kinase from Escherichia coli (AKeco), consisting of a single 23.6 kDa polypeptide chain folded into domains CORE, AMPbd, and LID, catalyzes the reaction AMP + ATP --> 2ADP. Domains LID and AMPbd execute large-scale movements during catalysis. Backbone dynamics of ligand-free and AP(5)A-inhibitor-bound AKeco were studied comparatively with (15)N NMR relaxation methods. Overall diffusion with correlation times of 15.05 (11.42) ns and anisotropy D(parallel)/D(perp) = 1.25 (1.10), and fast internal motions with correlation times up to 100 ps (50 ps), were determined for AKeco (AKecoAP(5)A). Fast internal motions affect 93% of the AKeco sites, with pronounced preference for domains AMPbd and LID, and 47% of the AKecoAP(5)A sites, with limited variability along the chain. The mean squared generalized order parameters, , of secondary structure elements and loops are affected by ligand binding differentially and in a domain-specific manner. Nanosecond motions predominate within AMPbd. Prominent exchange contributions, associated in particular with residue G10 of the nucleotide-binding P-loop motif, are interpreted to reflect hydrogen-bond dynamics at the inhibitor-binding site. The hypothesis of energetic counter balancing of substrate binding based on crystallographic data is strongly supported by the solution NMR results. Correlations between backbone dynamics and domain displacement are established.     

Backbone dynamics of the channel-forming antibiotic zervamicin IIB studied by 15N NMR relaxation

The backbone dynamics of the channel-forming peptide antibiotic zervamicin IIB (Zrv-IIB) in methanol were studied by 15N nuclear magnetic resonance relaxation measurements at 11.7, 14.1 and 18.8 T magnetic fields. The anisotropic overall rotation of the peptide was characterized based on 15N relaxation data and by hydrodynamic calculations. 'Model-free' analysis of the relaxation data showed that the peptide is fairly rigid on a sub-nanosecond time-scale. The residues from the polar side of Zrv-IIB helix are involved in micro-millisecond time-scale conformational exchange. The conformational exchange observed might indicate intramolecular processes or specific intermolecular interactions of potential relevance to Zrv-IIB ion channel formation.     

Backbone dynamics of a biologically active human FGF-1 monomer, complexed to a hexasaccharide heparin-analogue, by 15N NMR relaxation methods

The binding site and backbone dynamics of a bioactive complex formed by the acidic fibroblast growth factor (FGF-1) and a specifically designed heparin hexasaccharide has been investigated by HSQC and relaxation NMR methods. The comparison of the relaxation data for the free and bound states has allowed showing that the complex is monomeric, and still induces mutagenesis, and that the protein backbone presents reduced motion in different timescale in its bound state, except in certain points that are involved in the interaction with the fibroblast growth factor receptor (FGFR).Angeles Canales-Mayordomo and Rosa Fayos have contributed equally to this research.     

Comparison of backbone dynamics of oxidized and reduced putidaredoxin by 15N NMR relaxation measurements.

The backbone dynamics of uniformly 15N-labeled reduced and oxidized putidaredoxin (Pdx) have been studied by 2D 15N NMR relaxation measurements. 15N T1 and T2 values and 1H-15N NOEs have been measured for the diamagnetic region of the protein. These data were analyzed by using a model-free dynamics formalism to determine the generalized order parameters (S2), the effective correlation time for internal motions (tau e), and the 15N exchange broadening contributions (Rex) for each residue, as well as the overall correlation time (tau(m)). Order parameters for the reduced Pdx are generally higher than for the oxidized Pdx, and there is increased mobility on the microsecond to millisecond time scale for the oxidized Pdx, in comparison with the reduced Pdx. These results clearly indicate that the oxidized protein exhibits higher mobility than the reduced one, which is in agreement with the recently published redox-dependent dynamics studied by amide proton exchange. In addition, we observed very high T1/T2 ratios for residues 33 and 34, giving rise to a large Rex contribution. Residue 34 is believed to be involved in the binding of Pdx to cytochrome P450cam (CYP101). The differences in the backbone dynamics are discussed in relation to the oxidation states of Pdx, and their impact on electron transfer. The entropy change occurring on oxidation of reduced Pdx has been calculated from the order parameters of the two forms.     

Backbone dynamics of the calcium-signaling protein apo-S100B as determined by 15N NMR relaxation

Backbone dynamics of homodimeric apo-S100B were studied by (15)N nuclear magnetic resonance relaxation at 9.4 and 14.1 T. Longitudinal relaxation (T(1)), transverse relaxation (T(2)), and the (15)N-[(1)H] NOE were measured for 80 of 91 backbone amide groups. Internal motional parameters were determined from the relaxation data using the model-free formalism while accounting for diffusion anisotropy. Rotational diffusion of the symmetric homodimer has moderate but statistically significant prolate axial anisotropy (D( parallel)/D( perpendicular) = 1.15 +/- 0.02), a global correlation time of tau(m) = 7.80 +/- 0.03 ns, and a unique axis in the plane normal to the molecular symmetry axis. Of 29 residues at the dimer interface (helices 1 and 4), only one has measurable internal motion (Q71), and the order parameters of the remaining 28 were the highest in the protein (S(2) = 0.80 to 0.91). Order parameters in the typical EF hand calcium-binding loop (S(2) = 0.73 to 0.87) were slightly lower than in the pseudo-EF hand (S(2) = 0.75 to 0.89), and effective internal correlation times, tau(e), distinct from global tumbling, were detected in the calcium-binding loops. Helix 3, which undergoes a large, calcium-induced conformational change necessary for target-protein binding, does not show evidence of interchanging between the apo and Ca(2+)-bound orientations in the absence of calcium but has rapid motion in several residues throughout the helix (S(2) = 0.78 to 0.88; 10 < or = tau(e) < or = 30 ps). The lowest order parameters were found in the C-terminal tail (S(2) = 0.62 to 0.83). Large values for chemical exchange also occur in this loop and in regions nearby in space to the highly mobile C-terminal loop, consistent with exchange broadening effects observed.     

Rotational motions in myoglobin assessed by carbon 13 relaxation measurements at two magnetic field strengths.

Proton-decoupled Fourier transform nuclear magnetic resonance spectroscopy of natural abundance 13C was used to obtain spectra of cyanoferrimyoglobin of sperm whale (Physeter catadon) at 14.1 and 23.5 kG. Comparison of the spin lattice relaxation times at these two field strengths allowed the unambiguous assignment of a rotational correlation time of 22 plus or minus 5 ns for the alpha carbon resonances. The spin lattice relaxation time value for a major band attributable to aromatic carbon atoms also corresponded to a single correlation time, attributable to over-all tumbling of the molecule. Certain narrower resonances reflect other modes of rotational motion in addition to the over-all tumbling. Observations of nuclear Overhauser enhancement and line widths accord with these conslusions.     

Backbone dynamics of free barnase and its complex with barstar determined by 15N NMR relaxation study

Backbone dynamics of uniformly ¹⁵N-labeled free barnase and its complex with unlabelled barstar have been studied at 40°C, pH 6.6, using ¹⁵N relaxation data obtained from proton-detected 2D {¹H}-¹⁵N NMR spectroscopy. ¹⁵N spin-lattice relaxation rate constants (R₁), spin-spin relaxation rate constants (R₂), and steady-state heteronuclear {¹H}-¹⁵N NOEs have been measured at a magnetic field strength of 14.1 Tesla for 91 residues of free barnase and for 90 residues out of a total of 106 in the complex (excluding three prolines and the N-terminal residue) backbone amide ¹⁵N sites of barnase. The primary relaxation data for both the cases have been analyzed in the framework of the model-free formalism using both isotropic and axially symmetric models of the rotational diffusion tensor. As per the latter, the overall rotational correlation times (_m) are 5.0 and 9.5 ns for the free and complexed barnase, respectively. The average order parameter is found to be 0.80 for free barnase and 0.86 for the complex. However, the changes are not uniform along the backbone and for about 5 residues near the binding interface there is actually a significant decrease in the order parameters on complex formation. These residues are not involved in the actual binding. For the residues where the order parameter increases, the magnitudes vary significantly. It is observed that the complex has much less internal mobility, compared to free barnase. From the changes in the order parameters, the entropic contribution of NH bond vector motion to the free energy of complex formation has been calculated. It is apparent that these motions cause significant unfavorable contributions and therefore must be compensated by many other favorable contributions to effect tight complex formation. The observed variations in the motion and their different locations with regard to the binding interface may have important implications for remote effects and regulation of the enzyme action.     

Sampling of protein dynamics in nanosecond time scale by 15N NMR relaxation and self-diffusion measurements.

This paper presents a procedure for detection of intermediate nanosecond internal dynamics in globular proteins. The procedure uses 1H-15N relaxation measurements at several spectrometer frequencies and hydrodynamic calculations based on experimental self-diffusion coefficients. New heteronuclear experiments, using pulse field gradients, are introduced for the measurement of translation diffusion coefficients of 15N labeled proteins. An advanced interpretation of recently published (Luginbühl et al., Biochemistry, 36, 7305-7312 (1997)) backbone amide 15N relaxation data, measured at two spectrometers (400 and 750 MHz for 1H) for N-terminal DNA-binding domain (1-63) of 434 repressor, is presented. Non-applicability of commonly used fast (picosecond) dynamics model (FD) was justified by (i) poor fit of relaxation data by the FD model-free spectral density function both for isotropic and anisotropic models of the overall molecular tumbling; (ii) specific dependence of the overall rotation correlation times calculated from T1/T2 ratio on the spectrometer frequency; (iii) mismatch of the ratio of longitudinal 15N relaxation times T1, measured at different spectrometer frequencies, in comparison with that anticipated for the FD model; (iv) significantly underestimated overall rotation correlation time provided by the FD model (5.50+/-0.15 and 5.80+/-0.15 ns for 750 and 400 MHz spectrometer frequency respectively) in comparison with correlation time obtained from hydrodynamics. On the other hand, all relaxation and hydrodynamics data are in good correspondence with the model of intermediate (nanoseconds) dynamics. Overall rotation correlation time of 7.5+/-0.7 ns was calculated from experimental translation self-diffusion rate using hydrodynamics formalism (Garcia de la Torre, J. and Bloomfield, V.A. Quart. Rev. Biophys., 14, 81-139 (1981)). The statistical analysis of 15N relaxation data along with the hydrodynamic consideration clearly revealed that most of the residues in 434(1-63) repressor are involved in the nanosecond internal dynamics characterized by the the mean order parameters of 0.59+/-0.06 and the correlation times of ca. 5 ns.     

Backbone dynamics of the human MIA protein studied by (15)N NMR relaxation: implications for extended interactions of SH3 domains

The melanoma inhibitory activity (MIA) protein is a clinically valuable marker in patients with malignant melanoma as enhanced values diagnose metastatic melanoma stages III and IV. Here, we report the backbone dynamics of human MIA studied by (15)N NMR relaxation experiments. The folded core of human MIA is found to be rigid, but several loops connecting beta-sheets, such as the RT-loop for example, display increased mobility on picosecond to nanosecond time scales. One of the most important dynamic features is the pronounced flexibility of the distal loop, comprising residues Asp 68 to Ala 75, where motions on time scales up to milliseconds occur. Further, significant exchange contributions are observed for residues of the canonical binding site of SH3 domains including the RT-loop, the n-Src loop, for the loop comprising residues 13 to 19, which we refer to as the"disulfide loop", in part for the distal loop, and the carboxyl terminus of human MIA. The functional importance of this dynamic behavior is discussed with respect to the biological activity of several point mutations of human MIA. The results of this study suggest that the MIA protein and the recently identified highly homologous fibrocyte-derived protein (FDP)/MIA-like (MIAL) constitute a new family of secreted proteins that adopt an SH3 domain-like fold in solution with expanded ligand interactions.     

Backbone dynamics of detergent-solubilized alamethicin from amide hydrogen exchange measurements.

Alamethicin is a 20 amino acid antibiotic peptide produced by the soil fungus Trichoderma viride. The peptide inserts into bacterial membranes and self-associates to form ion channels, but the details of this process are unknown. Residue-specific acid- and base-catalyzed exchange data were obtained for 16 of 18 backbone amides of alamethicin dissolved in sodium dodecyl sulfate micelles using high-resolution 2-dimensional heteronuclear nuclear magnetic resonance spectroscopy. To facilitate interpretation of the exchange data, we synthesized N-acetyl-alpha-aminoisobutyric acid-N'-methyl and N-acetyl-alanine-N'-methyl and measured the pD dependence of their hydrogen-deuterium exchange rates to determine the sequence-dependent inductive and steric effects of the alpha-aminoisobutyric acid residue. Intramolecular H-bonding in alamethicin was monitored through the exchange parameters kmin (minimum exchange rate) which indicate that the backbone is significantly more stable than the backbones of alanine-based helical peptides. Rapid exchange at Gly-11 suggests a highly local conformational flexibility in the middle of the peptide. Interactions with the detergent micelle were revealed by the exchange parameters pDmin (pD of minimum exchange) which suggest that the N-terminus of alamethicin interacts more strongly with the detergent micelle than does the C-terminus. A periodicity in pDmin difference data reveals that one surface of the helix interacts more strongly with the micelle. The surface consists of residues 1, 5, 9, 13, 16, and 20. The opposite face of the helix contains several polar residues (two glutamines and a glycine), suggesting that, on average, this face of the helix is directed toward the solvent. These results serve as a model for the interaction of the peptide with membranes containing anionic lipid. In combination with published molecular dynamics simulations [Gibbs et al. (1997) Biophys. J. 72, 2490-2495], the present results also offer insight into the mechanisms of hydrogen-deuterium exchange in helical peptides.     

Anisotropic rotational diffusion of perdeuterated HIV protease from 15N NMR relaxation measurements at two magnetic fields

Summary ¹⁵N NMR relaxation times in perdeuterated HIV-1 protease, complexed with the sub-nanomolar inhibitor DMP323, have been measured at 600 and 360 MHz ¹H frequency. The relative magnitudes of the principal components of the inertia tensor, calculated from the X-ray coordinates of the protein-drug complex, are 1.0:0.85:0.44. The relation between the T₁/T₂ ratios observed for the individual backbone amides and their N-H orientation within the 3D structure of the protease dimer yields a rotational diffusion tensor oriented nearly collinear to the inertia tensor. The relative magnitudes of its principal components (1.00:1.11:1.42) are also in good agreement with hydrodynamic modeling results. The orientation and magnitude of the diffusion tensors derived from relaxation data obtained at 360 and 600 MHz are nearly identical. The anisotropic nature of the rotational diffusion has little influence on the order parameters derived from the ¹⁵N T₁ and T₂ relaxation times; however, if anisotropy is ignored, this can result in erroneous identification of either exchange broadening or internal motions on a nanosecond time scale. The average ratio of the T₁ values measured at 360 and 600 MHz is 0.50±0.015, which is slightly larger than the value of 0.466 expected for an isotropic rigid rotor with _c = 10.7 ns. The average ratio of the T₂ values measured at 360 and 600 MHz is 1.14±0.04, which is also slightly larger than the expected ratio of 1.11. This magnetic field dependence of the T₁ and T₂ relaxation times suggests that the spectral density contribution from fast internal motions is not negligible, and that the chemical shift anisotropy of peptide backbone amides, on average, is larger than the 160 ppm value commonly used in ¹⁵N relaxation studies of proteins.