Carbonyl carbon transverse relaxation dispersion measurements and ms-μs timescale motion in a protein hydrogen bond network

A constant-time, Carr-Purcell-Meiboom-Gill (CPMG) transverse relaxation, R(2), dispersion experiment for carbonyl carbons was designed and executed to detect micros-ms time-scale dynamics of protein backbone carbonyl sites. Because of the large (ca. 55 Hz) C(alpha)-C' J-coupling, the carbonyl signal intensity is strongly modulated as the spacing between CPMG pulses is varied, in uniformly (13)C enriched proteins, unless care is taken to minimize the perturbation of the C(alpha) magnetization by the CPMG pulses. CPMG pulse trains consisting of either a band-selective pulse, such as RE-BURP, or rectangular (with an excitation null in the C(alpha) region of the spectrum) pulses were employed in order to minimize C' signal modulation by C(alpha)-C' J-coupling. The performance of these types of CPMG refocusing pulses was assessed by computer simulation, and by comparing dispersion profiles measured for (1) uniformly [(13)C,(15)N, (2)H] ((2)H at non-labile hydrogen sites) labeled, and (2) uniformly (15)N/selectively-(13)C' labeled samples of HIV-1 protease bound to a potent inhibitor, DMP323. In addition, because the uniformly (13)C/(15)N/(2)H labeled sample was well suited to measure (15)N and (1)H R(2) dispersion as well as (13)C' dispersion, conformational exchange in the inter subunit beta-sheet hydrogen-bond network of the inhibitor-bound protease was elucidated using relaxation dispersion data of all three types of nuclei.     

Characterization of millisecond time-scale dynamics in the molten globule state of alpha-lactalbumin by NMR

The motional dynamics of the molten globule (MG) state of alpha-lactalbumin have been characterized using (15)N transverse relaxation rates (R2). A modified version of the Carr-Purcell-Meiboom-Gill (CPMG) R2 pulse sequence is proposed in order to overcome the loss of sensitivity that arises from extreme line broadening due to complex dynamics on the millisecond time-scale. Using this pulse sequence, chemical exchange rates were extracted by examining the (15)N transverse relaxation rates as a function of CPMG delay values. The results clearly illustrate that pervasive conformational exchange of 0.2-0.5 ms in the (15)N backbone resonances of the molten globule state of alpha-lactalbumin. The temperature dependence of the conformational exchange rates display standard Arrhenius kinetic behavior between 10 and 30 degrees C. Estimates of the activation energies range from 0.8 to 4. 4 kcal/mol, indicating a low energetic barrier to conformational fluctuations relative to native state proteins. The fluctuations and low energetic barriers may be critical for directing the search for contacts that will result in the transition from the MG state to the native state.     

Measurement of 15N relaxation in deuterated amide groups in proteins using direct nitrogen detection

15N chemical shielding tensors contain useful structural information, and their knowledge is essential for accurate analysis of protein backbone dynamics. The anisotropic component (CSA) of 15N chemical shielding can be obtained from 15N relaxation measurements in solution. However, the predominant contribution to nitrogen relaxation from 15N-(1)H dipolar coupling in amide groups limits the sensitivity of these measurements to the actual CSA values. Here we present nitrogen-detected NMR experiments for measuring 15N relaxation in deuterated amide groups in proteins, where the dipolar contribution to 15N relaxation is significantly reduced by the deuteration. Under these conditions nitrogen spin relaxation becomes a sensitive probe for variations in 15N chemical shielding tensors. Using the nitrogen direct-detection experiments we measured the rates of longitudinal and transverse 15N relaxation for backbone amides in protein G in D(2)O at 11.7 T. The measured relaxation rates are validated by comparing the overall rotational diffusion tensor obtained from these data with that from the conventional 15N relaxation measurements in H(2)O. This analysis revealed a 17-24 degree angle between the NH-bond and the unique axis of the 15N chemical shielding tensor.     

Conformational flexibility of a human immunoglobulin light chain variable domain by relaxation dispersion nuclear magnetic resonance spectroscopy: implications for protein misfolding and amyloid assembly

The conformational flexibility of a human immunoglobulin κIV light-chain variable domain, LEN, which can undergo conversion to amyloid under destabilizing conditions, was investigated at physiological and acidic pH on a residue-specific basis by multidimensional solution-state nuclear magnetic resonance (NMR) methods. Measurements of backbone chemical shifts and amide (15)N longitudinal and transverse spin relaxation rates and steady-state nuclear Overhauser enhancements indicate that, on the whole, LEN retains its native three-dimensional fold and dimeric state at pH 2 and that the protein backbone exhibits limited fast motions on the picosecond to nanosecond time scale. On the other hand, (15)N Carr--Purcell--Meiboom--Gill (CPMG) relaxation dispersion NMR data show that LEN experiences considerable slower, millisecond time scale dynamics, confined primarily to three contiguous segments of about 5-20 residues and encompassing the N-terminal β-strand and complementarity determining loop regions 2 and 3 in the vicinity of the dimer interface. Quantitative analysis of the CPMG relaxation dispersion data reveals that at physiological pH these slow backbone motions are associated with relatively low excited-state protein conformer populations, in the ~2-4% range. Upon acidification, the minor conformer populations increase significantly, to ~10-15%, with most residues involved in stabilizing interactions across the dimer interface displaying increased flexibility. These findings provide molecular-level insights about partial protein unfolding at low pH and point to the LEN dimer dissociation, initiated by increased conformational flexibility in several well-defined regions, as being one of the important early events leading to amyloid assembly.     

The effects of the extracellular manganese concentration and variation of the interpulse delay time in the CPMG sequence on water exchange time across erythrocyte membranes

There has been broad disagreement in the literature regarding the dependence of water exchange times (Te) across erythrocyte membranes studied by the 1H-NMR Carr-Purcell-Meiboom-Gill (CPMG) pulse sequence on extracellular Mn2+ concentration. While some workers saw no change in Te with Mn2+, others reported a 35-50% decrease in Te with this extracellular paramagnetic relaxation agent. We present 1H-NMR evidence that a 30-50% change in Te can be produced by interdependence of the interpulse delay time of the CPMG pulse sequence and the external Mn2+ concentration. Such a large dependency is interpreted in terms of the diffusional effect as a major source. However, it is shown experimentally that if a large number of refocusing pi pulses are used, the observed transverse relaxation times are unaffected by Mn2+. Under these conditions excellent agreement of Te obtained in our study (13.0 +/- 0.64 ms (N = 36) at 21 degrees C) and that of 12.8 +/- 3.6 ms at 20-23 degrees C reported by the radiotracer method was found. Our findings suggest new and important implications for evaluating the previous reports of the 1H-NMR CPMG method concerning the [Mn2+] effect in the decrease of Te, and provide conditions where studies of water transport across erythrocyte membranes using this magnetic resonance method can be used with confidence.     

Backbone dynamics of (1–71)- and (1–36)bacterioopsin studied by two-dimensional 1H-15N NMR spectroscopy

Summary The backbone dynamics of uniformly ¹⁵N-labelled fragments (residues 1–71 and 1–36) of bacterioopsin, solubilized in two media (methanol-chloroform (1:1), 0.1 M ²HCO₂NH₄, or SDS micelles) have been investigated using 2D proton-detected heteronuclear ¹H-¹⁵N NMR spectroscopy at two spectrometer frequencies, 600 and 400 MHz. Contributions of the conformational exchange to the transverse relaxation rates of individual nitrogens were elucidated using a set of different rates of the CPMG spin-lock pulse train and were essentially suppressed by the high-frequency CPMG spin-lock. We found that most of the backbone amide groups of (1–71)bacterioopsin in SDS micelles are involved in the conformational exchange process over a rate range of 10³ to 10⁴ s^-1. This conformational exchange is supposed to be due to an interaction between two -helixes of (1–71)bacterioopsin, since the hydrolysis of the peptide bond in the loop region results in the disappearance of exchange line broadening. ¹⁵N relaxation rates and ¹H-¹⁵N NOE values were interpreted using the model-free approach of Lipari and Szabo [Lipari, G. and Szabo, A. (1982) J. Am. Chem. Soc., 104, 4546–4559]. In addition to overall rotation of the molecule, the backbone N-H vectors of the peptides are involved in two types of internal motions: fast, on a time scale <20 ps, and intermediate, on a time scale close to 1 ns. The intermediate dynamics in the -helical stretches was mostly attributed to bending motions. A decrease in the order parameter of intermediate motions was also observed for residues next to Pro⁵⁰, indicating an anisotropy of the overall rotational diffusion of the molecule. Distinctly mobile regions are identified by a large decrease in the order parameter of intermediate motions and correspond to the N- and C-termini, and to a loop connecting the -helixes of (1–71)bacterioopsin. The internal dynamics of the -helixes on the millisecond and nanosecond time scales should be taken into account in the development of a model of the functioning bacteriorhodopsin.Abbreviations BO bacterioopsin - 2D two-dimensional - CPMG Carr-Purcell-Meiboom-Gill (Carr and Purcell, 1954) - SDS sodium dodecyl(²H₂₅) sulfate - R(S_x), R(S_z) ¹⁵N transverse and longitudinal relaxation rates, respectively     

Conformational dynamics and molecular recognition: backbone dynamics of the estrogen receptor DNA-binding domain.

We examined the internal mobility of the estrogen receptor DNA-binding domain (ER DBD) using NMR15N relaxation measurements and compared it to that of the glucocorticoid receptor DNA-binding domain (GR DBD). The studied protein fragments consist of residues Arg183-His267 of the human ER and residues Lys438-Gln520 of the rat GR. The15N longitudinal (R1) and transverse (R2) relaxation rates and steady state {1H}-15N nuclear Overhauser enhancements (NOEs) were measured at 30 degrees C at1H NMR frequencies of 500 and 600 MHz. The NOE versus sequence profile and calculated order parameters for ER DBD backbone motions indicate enhanced internal dynamics on pico- to nanosecond time-scales in two regions of the core DBD. These are the extended strand which links the DNA recognition helix to the second zinc domain and the larger loop region of the second zinc domain. The mobility of the corresponding regions of the GR DBD, in particular that of the second zinc domain, is more limited. In addition, we find large differences between the ER and GR DBDs in the extent of conformational exchange mobility on micro- to millisecond time-scales. Based on measurements of R2as a function of the15N refocusing (CPMG) delay and quantitative (Lipari-Szabo-type) analysis, we conclude that conformational exchange occurs in the loop of the first zinc domain and throughout most of the second zinc domain of the ER DBD. The conformational exchange dynamics in GR DBD is less extensive and localized to two sites in the second zinc domain. The different dynamical features seen in the two proteins is consistent with previous studies of the free state structures in which the second zinc domain in the ER DBD was concluded to be disordered whereas the corresponding region of the GR DBD adopts a stable fold. Moreover, the regions of the ER DBD that undergo conformational dynamics on the micro- to millisecond time-scales in the free state are involved in intermolecular protein-DNA and protein-protein interactions in the dimeric bound state. Based on the present data and the previously published dynamical and DNA binding properties of a GR DBD triple mutant which recognize an ER binding site on DNA, we argue that the free state dynamical properties of the nuclear receptor DBDs is an important element in molecular recognition upon DNA binding.     

Measurement of ¹⁵N relaxation rates in perdeuterated proteins by TROSY-based methods

While extracting dynamics parameters from backbone (15)N relaxation measurements in proteins has become routine over the past two decades, it is increasingly recognized that accurate quantitative analysis can remain limited by the potential presence of systematic errors associated with the measurement of (15)N R(1) and R(2) or R(1ρ) relaxation rates as well as heteronuclear (15)N-{(1)H} NOE values. We show that systematic errors in such measurements can be far larger than the statistical error derived from either the observed signal-to-noise ratio, or from the reproducibility of the measurement. Unless special precautions are taken, the problem of systematic errors is shown to be particularly acute in perdeuterated systems, and even more so when TROSY instead of HSQC elements are used to read out the (15)N magnetization through the NMR-sensitive (1)H nucleus. A discussion of the most common sources of systematic errors is presented, as well as TROSY-based pulse schemes that appear free of systematic errors to the level of <1 %. Application to the small perdeuterated protein GB3, which yields exceptionally high S/N and therefore is an ideal test molecule for detection of systematic errors, yields relaxation rates that show considerably less residue by residue variation than previous measurements. Measured R(2)'/R(1)' ratios fit an axially symmetric diffusion tensor with a Pearson's correlation coefficient of 0.97, comparable to fits obtained for backbone amide RDCs to the Saupe matrix.     

Phosphorus-31 Transverse Relaxation Rate Measurements by NMR Spectroscopy: Insight into Conformational Exchange Along the Nucleic Acid Backbone

Phosphorus ((31)P) NMR spectroscopy can provide important information about the dynamics of nucleic acids. In this communication, we propose an inversely detected (31)P transverse relaxation rate ( R (2)) measurement experiment. This experiment enables fast measurement of accurate (31)P transverse relaxation rates and provides the possibility to detect slow motions mapped by the phosphorus nuclei along the nucleic acid backbone. Dispersion curves show some (31)P nuclei experiencing chemical exchange in the millisecond time scale. Under the assumption of a two-state exchange process, the reduced lifetimes of the exchanging sites (tau(ex)) obtained are in accordance with base pair lifetime estimates deduced from imino proton exchange measurements.     

Off-resonance effects in 15N T2 CPMG measurements

The systematic difference between T ₂ values obtained from CPMG and T ₁ experiments was observed for backbone ¹⁵N nuclei of bacterial ribonuclease barnase. Theoretical consideration suggests that the observed difference is caused by off-resonance effects of 180° pulses of the CPMG pulse train. Namely, at off-resonance conditions T ₁-dependent secondary echo coherence pathways considerably contribute to the signal decay in the CPMG experiment and result in systematic (up to 10%) offset-dependent overestimation of ¹⁵N T ₂ measured by the CPMG technique. Under certain circumstances off-resonance effects result in dependence of ¹⁵N T ₂ on CPMG frequency, which might be erroneously interpreted as conformational exchange on the millisecond time-scale. A procedure for numerical correction of ¹⁵N T ₂ (CPMG) data is proposed.     

Separating the contributions to 15N transverse relaxation in a fibronectin type III domain

In proteins, dynamic mobility is an important feature of structure, stability, and biomolecular recognition. Uniquely sensitive to motion throughout the milli- to picosecond range, rates of transverse relaxation, R2, are commonly obtained for the characterization of chemical exchange, and the construction of motional models that attempt to separate overall and internal mobility. We have performed an in-depth study of transverse relaxation rates of backbone 15N nuclei in TNfn31–90, the third fibronectin type III domain from human tenascin. By combining the results of spin-echo (CPMG) and off-resonance T1 experiments, we present R2 rates at effective field strengths of 2 to 40 krad/s, obtaining a full spectrum of 16 independent R2 data points for most residues. Collecting such a large number of replicate measurements provides insight into intrinsic uncertainties. The median standard deviation in R2 for non-exchanging residues is 0.31, indicating that isolated measurements may not be sufficiently accurate for a precise interpretation of motional models. Chemical exchange events on a timescale of 570 s were observed in a cluster of residues at the C terminus. Rates of exchange for five other residues were faster than the sampled range of frequencies and could not be determined. Averaged 'exchange free' transverse relaxation rates, R20, were used to calculate the diffusion tensor for rotational motion. Despite a highly asymmetric moment of inertia, the narrow angular dispersion of N-H vectors within the sandwich proves insufficient to define deviations from isotropic rotation. Loop residues provide exclusive evidence for axially symmetric diffusion (Dpar/Dper=1.55).     

Chemical exchange effects during refocusing pulses in constant-time CPMG relaxation dispersion experiments

In the analysis of the constant-time Carr-Purcell-Meiboom-Gill (CT-CPMG) relaxation dispersion experiment, chemical exchange parameters, such as rate of exchange and population of the exchanging species, are typically optimized using equations that predict experimental relaxation rates recorded as a function of effective field strength. In this process, the effect of chemical exchange during the CPMG pulses is typically assumed to be the same as during the free-precession. This approximation may introduce systematic errors into the analysis of data because the number of CPMG pulses is incremented during the constant-time relaxation period, and the total pulse duration therefore varies as a function of the effective field strength. In order to estimate the size of such errors, we simulate the time-dependence of magnetization during the entire constant time period, explicitly taking into account the effect of the CPMG pulses on the spin relaxation rate. We show that in general the difference in the relaxation dispersion profile calculated using a practical pulse width from that calculated using an extremely short pulse width is small, but under certain circumstances can exceed 1 s^?1. The difference increases significantly when CPMG pulses are miscalibrated.     

Backbone dynamics of the C-terminal SH2 domain of the p85alpha subunit of phosphoinositide 3-kinase: effect of phosphotyrosine-peptide binding and characterization of slow conformational exchange processes

The backbone dynamics of the C-terminal SH2 domain from the regulatory subunit p85alpha (p85alpha C-SH2) of phosphoinositide 3-kinase has been investigated in the absence of, and in complex with, a high-affinity phosphotyrosine-containing peptide ligand derived from the platelet-derived growth-factor receptor. (15)N R(1) and R(2) relaxation rates and steady-state [(1)H]-(15)N NOE values were measured by means of (1)H-(15)N correlated two-dimensional methods and were analyzed within the framework of the model-free formalism. Several residues in the BC loop and in the neighbouring secondary structural elements display fast local dynamics in the absence of phosphotyrosine peptide ligand as evidenced by below-average [(1)H]-(15)N NOE values. Furthermore, residue Gln41 (BC3) displays conformational exchange phenomena as indicated by an above-average R(2) relaxation rate. Upon binding of the phosphotyrosine peptide, the NOE values increase to values observed for regular secondary structure and the exchange contribution to the R(2) relaxation rate for Gln41 (BC3) vanishes. These observations indicate a loss of backbone flexibility upon ligand binding. Substantial exchange contributions for His56 (betaD4) and Cys57 (betaD5), which are known to make important interactions with the ligand, are attenuated upon ligand binding. Several residues in the betaD'-FB region and the BG loop, which contribute to the ligand binding surface of the protein, exhibit exchange terms which are reduced or vanish when the ligand is bound. Together, these observations suggest that ligand binding is accompanied by a loss of conformational flexibility on the ligand binding face of the protein. However, comparison with other SH2 domains reveals an apparent lack of consensus in the changes in dynamics induced by ligand binding. Exchange rates for individual residues were quantified in peptide-complexed p85alpha C-SH2 from the dependence of the exchange contributions on the CPMG delay in an R(2) series and show that peptide-complexed p85alpha C-SH2 is affected by multiple conformational exchange processes with exchange rate constants from 10(2) s(-1) to 7.10(3) s(-1). Mapping of the exchange-rate constants on the protein surface show a clustering of residues with similar exchange-rate constants and suggests that clustered residues are affected by a common predominant exchange process.     

(15)N backbone dynamics of ferricytochrome b(562): comparison with the reduced protein and the R98C variant.

The backbone dynamics of ferricytochrome b(562), a four-helix bundle protein from Escherichia coli, have been studied by NMR spectroscopy. The consequences of the introduction of a c-type thioether linkage between the heme and protein and the reduction to the ferrous cytochrome have also been analyzed. (15)N relaxation rates R(1) and R(2) and (1)H-(15)N NOEs were measured at proton Larmor frequencies of 500 and 600 MHz for the oxidized and reduced protein as well as for the oxidized R98C variant. In the latter protein, an "artificial" thioether covalent bond has been introduced between the heme group and the protein frame [Arnesano, F., Banci, L., Bertini, I., Ciofi-Baffoni, S., de Lumley Woodyear, T., Johnson, C. M., and Barker, P. D. (2000) Biochemistry 39, 1499-1514]. The (15)N relaxation data were analyzed with the ModelFree protocol, and the mobility parameters on the picosecond to nanosecond time scale were compared for the three species. The three forms are rather rigid as a whole, with average generalized order parameters values of 0.87 +/- 0.08 (oxidized cytochrome b(562)), 0.84 +/- 0.07 (reduced cytochrome b(562)), and 0.85 +/- 0.07 (oxidized R98C cytochrome b(562)), indicating similar mobility for each system. Lower order parameters (S(2)) are found for residues belonging to loops 1 and 2. Higher mobility, as indicated by lower order parameters, is found for heme binding helices alpha 1 and alpha 4 in the R98C variant with respect to the wild-type protein. The analysis requires a relatively long rotational correlation time (tau(m) = 9.6 ns) whose value is accounted for on the basis of the anisotropy of the molecular shape and the high phosphate concentration needed to ensure the occurrence of monomer species. A parallel study of motions in the millisecond to microsecond time scale has also been performed on oxidized wild-type and R98C cytochrome b(562). In a CPMG experiment, decay rates were analyzed in the presence of spin-echo pulse trains of variable spacing. The dynamic behavior on this time scale is similar to that observed on the sub-nanosecond time scale, showing an increased mobility in the residues connected to the heme ligands in the R98C variant. It appears that the increased protein stability of the variant, established previously, is not correlated with an increase in rigidity.     

Heteronuclear relaxation in time-dependent spin systems: 15N-T1ρ dispersion during adiabatic fast passage

A novel NMR experiment comprising adiabatic fast passage techniques for the measurement of heteronuclear self-relaxation rates in fully 15N-enriched proteins is described. Heteronuclear self-relaxation is monitored by performing adiabatic fast passage (AFP) experiments at variable adiabaticity (e.g., variation of RF spin-lock field intensity). The experiment encompasses gradient- selection and sensitivity-enhancement. It is shown that transverse relaxation rates derived with this method are in good agreement with the ones measured by the classical Carr–Purcell–Meiboom–Gill (CPMG) sequences. An application of this method to the study of the carboxyl-terminal LIM domain of quail cysteine and glycine-rich protein qCRP2(LIM2) is presented.     

Backbone dynamics of apocytochrome b5 in its native, partially folded state

The backbone dynamics in the native state of apocytochrome b5 were studied using 15N nuclear magnetic spin relaxation measurements. The field (11.7 and 14.1 T) and temperature (10-25 degrees C) dependence of the relaxation parameters (R1, R2, and R1rho) and the 1H-15N NOE established that the protein undergoes multiple time scale internal motions related to the secondary structure. The relaxation data were analyzed with the reduced spectral density mapping approach and within the extended model-free framework. The apoprotein was confirmed to contain a disordered heme-binding loop of approximately 30 residues with dynamics on the sub-nanosecond time scale (0.6 < S2 < 0.7, 100 ps < taue < 500 ps). This loop is attached to a structured hydrophobic core, rigid on the picosecond time scale (S2 > 0.75, taue < 50 ps). The inability to fit the data for several residues with the model-free protocol revealed the presence of correlated motion. An exchange contribution was detected in the transverse relaxation rate (R2) of all residues. The differential temperature response of R2 along the backbone supported slower exchange rates for residues in the loop (tauex > 300 micros) than for the folded polypeptide chain (tauex < 150 micros). The distribution of the reduced spectral densities at the 1H and 15N frequencies followed the dynamic trend and predicted the slowing of the internal motions at 10 degrees C. Comparison of the dynamics with those of the holoprotein [Dangi, B., Sarma, S., Yan, C., Banville, D. L., and Guiles, R. D. (1998) Biochemistry 37, 8289-8302] demonstrated that binding of the heme alters the time scale of motions both in the heme-binding loop and in the structured hydrophobic core.     

Measurement of the signs of methyl 13C chemical shift differences between interconverting ground and excited protein states by R 1ρ : an application to αB-crystallin

Carr-Purcell-Meiboom-Gill relaxation dispersion (CPMG RD) NMR spectroscopy has emerged as a powerful tool for quantifying the kinetics and thermodynamics of millisecond time-scale exchange processes involving the interconversion between a visible ground state and one or more minor, sparsely populated invisible 'excited' conformational states. Recently it has also become possible to determine atomic resolution structural models of excited states using a wide array of CPMG RD approaches. Analysis of CPMG RD datasets provides the magnitudes of the chemical shift differences between the ground and excited states, Δ?, but not the sign. In order to obtain detailed structural insights from, for example, excited state chemical shifts and residual dipolar coupling measurements, these signs are required. Here we present an NMR experiment for obtaining signs of (13)C chemical shift differences of (13)CH(3) methyl groups using weak field off-resonance R(1ρ) relaxation measurements. The accuracy of the method is established by using an exchanging system where the invisible, excited state can be converted to the visible, ground state by altering sample conditions so that the signs of Δ? values obtained from the spin-lock approach can be validated against those measured directly. Further, the spin-lock experiments are compared with the established H(S/M)QC approach for measuring signs of chemical shift differences and the relative strengths of each method are discussed. In the case of the 650 kDa human αB-crystallin complex where there are large transverse relaxation differences between ground and excited state spins the R(1ρ) method is shown to be superior to more 'traditional' experiments for sign determination.     

NMR investigation of the dynamics of tryptophan side-chains in hemoglobins

NMR relaxation measurements of 15N spin-lattice relaxation rate (R(1)), spin-spin relaxation rate (R(2)), and heteronuclear nuclear Overhauser effect (NOE) have been carried out at 11.7T and 14.1T as a function of temperature for the side-chains of the tryptophan residues of 15N-labeled and/or (2H,15N)-labeled recombinant human normal adult hemoglobin (Hb A) and three recombinant mutant hemoglobins, rHb Kempsey (betaD99N), rHb (alphaY42D/betaD99N), and rHb (alphaV96W), in the carbonmonoxy and the deoxy forms as well as in the presence and in the absence of an allosteric effector, inositol hexaphosphate (IHP). There are three Trp residues (alpha14, beta15, and beta37) in Hb A for each alphabeta dimer. These Trp residues are located in important regions of the Hb molecule, i.e. alpha14Trp and beta15Trp are located in the alpha(1)beta(1) subunit interface and beta37Trp is located in the alpha(1)beta(2) subunit interface. The relaxation experiments show that amino acid substitutions in the alpha(1)beta(2) subunit interface can alter the dynamics of beta37Trp. The transverse relaxation rate (R(2)) for beta37Trp can serve as a marker for the dynamics of the alpha(1)beta(2) subunit interface. The relaxation parameters of deoxy-rHb Kemspey (betaD99N), which is a naturally occurring abnormal human hemoglobin with high oxygen affinity and very low cooperativity, are quite different from those of deoxy-Hb A, even in the presence of IHP. The relaxation parameters for rHb (alphaY42D/betaD99N), which is a compensatory mutant of rHb Kempsey, are more similar to those of Hb A. In addition, TROSY-CPMG experiments have been used to investigate conformational exchange in the Trp residues of Hb A and the three mutant rHbs. Experimental results indicate that the side-chain of beta37Trp is involved in a relatively slow conformational exchange on the micro- to millisecond time-scale under certain experimental conditions. The present results provide new dynamic insights into the structure-function relationship in hemoglobin.     

Enhanced accuracy of kinetic information from CT-CPMG experiments by transverse rotating-frame spectroscopy

Micro-to-millisecond motions of proteins transmit pivotal signals for protein function. A powerful technique for the measurement of these motions is nuclear magnetic resonance spectroscopy. One of the most widely used methodologies for this purpose is the constant-time Carr–Purcell–Meiboom–Gill (CT-CPMG) relaxation dispersion experiment where kinetic and structural information can be obtained at atomic resolution. Extraction of accurate kinetics determined from CT-CPMG data requires refocusing frequencies that are much larger than the nuclei’s exchange rate between states. We investigated the effect when fast processes are probed by CT-CPMG experiments via simulation and show that if the intrinsic relaxation rate $ \left( {R_{2,0}^{CT - CPMG} } \right) $ ( R 2 , 0 CT ? CPMG ) is not known a priori the extraction of accurate kinetics is hindered. Errors on the order of 50 % in the exchange rate are attained when processes become fast, but are minimized to 5 % with a priori $ R_{2,0}^{CT - CPMG} $ R 2 , 0 CT ? CPMG information. To alleviate this shortcoming, we developed an experimental scheme probing $ R_{2,0}^{CT - CPMG} $ R 2 , 0 CT ? CPMG with large amplitude spin-lock fields, which specifically contains the intrinsic proton longitudinal Eigenrelaxation rate. Our approach was validated with ubiquitin and the Oscillatoria agardhii agglutinin (OAA). For OAA, an underestimation of 66 % in the kinetic rates was observed if $ R_{2,0}^{CT - CPMG}\, $ R 2 , 0 CT ? CPMG is not included during the analysis of CT-CPMG data and result in incorrect kinetics and imprecise amplitude information. This was overcome by combining CT-CPMG with $ R_{2,0}^{CT - CPMG} $ R 2 , 0 CT ? CPMG measured with a high power R_1ρ experiment. In addition, the measurement of $ R_{2,0}^{CT - CPMG} $ R 2 , 0 CT ? CPMG removes the ambiguities in choosing between different models that describe CT-CPMG data.