1H, 13C,and 15N assignments and secondary structure of the FK506 binding protein when bound to ascomycin

The ¹H, ¹³C, and ¹⁵N resonances of FKBP when bound to the immunosuppressant, ascomycin, were assigned using a computer-aided analysis of heteronuclear double and triple resonance three-dimensional nmr spectra of [U-¹⁵N] FKBP/ascomycin and [U-¹⁵N, ¹³C] FKBP/ascomycin. In addition, from a preliminary analysis of two heteronuclear four-dimensional data sets, ³J coupling constants, amide exchange data, and the differences between the C^α and C^β chemical shifts of FKBP to random coil values, the secondary structure of FKBP when bound to ascomycin was determined. The secondary structure of FKBP when bound to ascomycin in solution closely resembled the x-ray structure of the FKBP/FK506 complex but differed in some aspects from the structure of uncomplexed FKBP in solution. © 1993 John Wiley & Sons, Inc.     

Cross-correlation suppressed T1 and NOE experiments for protein side-chain 13CH2 groups

Relaxation measurements of side-chain ¹³CH₂-groups of uniformly ¹³C labeled human ubiquitin were performed at 600 MHz and 800 MHz magnetic field strength at 30°C. Dipole-dipole cross-correlated relaxation effects in T₁ experiments were suppressed by the combination of radio-frequency pulses and pulsed field gradients during the relaxation delay leading to monoexponential relaxation decays that allow a more accurate extraction of the ¹³C T₁ relaxation times. Heteronuclear ¹H-¹³C NOEs obtained by using different proton saturation schemes indicate that the influence of cross-correlation is small. The experimental T₁ and NOE data were interpreted in a model-free way in terms of a generalized order parameter and an internal correlation time.     

Viability of Cururbita pepo pollen: biophysical and structural data

During ageing of the short-lived pollen grains of Cucurbita pepo L., water loss was examined in relation to viability using biophysical (¹H-nuclear magnetic resonance, NMR) and cytological methods (fluorochromatic reaction test, freezefracture and scanning electron microscopy). A semi-logarithmic representation of the pollen weight loss demonstrated the complexity of the dehydration process. A the study of proton loss using ¹H-NMR indicated that two major releases water of had taken place, each with different flux rates. Pulse ¹H-NMR experiments showed the occurrene of non-exponential signal decay as a function of time, indicating the existence of different fractions of water in a pollen grain sample. These fractions leave the pollen grain at different times during pollen dehydration, and one of them (that of the so-called vital water) can be related to pollen viability. The quantity of protons giving a signal during pulse ¹H-NMR experiments was very low when the pollen grains were judged to be dead according to the fluorochromatic test. Freeze-fracture replicas of these dead pollen grains (less than 25% water content) showed that the plasma membrane had become detached from the intine surface; this ultrastructural feature might therefore be involved in the loss of pollen viability.Abbreviations A initial amplitude of the NMR signal - A₂ quantity of water charcterized by T_2-2 - A₅ quantity of water characterized by T_2–5 - FCR fluorochromatic reaction - NMR nuclear magnetic resonance - T₂ transverse relaxation time - T_2-2 T₂ measured with 2 ms between each pulse of radiofrequency - T_2–5 T₂ measured with 5 ms between each pulse of radiofrequency     

Determination of 13Cα relaxation times in uniformly 13C/15N-enriched proteins

Summary Relaxation times of ¹³C carbons of uniformly ¹³C/¹⁵N-enriched probes have been investigated. The relaxation behaviour was analyzed in terms of a multispin system. Pulse sequences for the determination of T₁, T₂ and the heteronuclear NOE of ¹³C in uniformly ¹³C/¹⁵N-enriched ribonuclease T1 are presented. The experiments performed in order to obtain T₁ and the heteronuclear NOE were similar to those of the corresponding ¹⁵N experiments published previously. The determination of T₂ for the C-carbon in a completely labeled protein is more complicated, since the magnetization transfer during the T₂ evolution period owing to the scalar coupling of C–C must be suppressed. Various different pulse sequences for the T₂ evolution period were simulated in order to optimize the bandwidth for which reliable T₂ relaxation times can be obtained. A proof for the quality of these pulse sequences is given by fitting the intensity decay of individual ¹H–¹³C cross peaks, in a series of (¹H, ¹³C)-ct-HSQC spectra with a modified CPMG sequence as well as a T_1p sequence for the transverse relaxation time, to a single exponential using a simplex algorithm.     

NMR study of 17O from H217O in human erythrocytes

Human erythrocytes were incubated in a Ringer's solution enriched with 10–18% H₂¹⁷O. The longitudinal relaxation time (T₁) of the ¹⁷O was determined separately in samples of red cell suspesions, packed cells, and supernatant. The longitudinal relaxation of ¹⁷O in erythrocyte suspensions was non-exponential, reflecting water exchange across the cell membranes as well as relaxation processes inside and outside the cell.The T₁ of intracellular ¹⁷O is 4–5 times shorter than in the supernatant, similar to the enhancement of proton relaxation by hemoglobin in erythrocytes and free solution at the frequency applied (8.13 MHz). This datum is consistent with the thesis that hemoglobin modifies the NMR relaxation behavior of water inside cells and in free solution in the same way.The rate constant

for water exchange was calculated to be 60 and 107 s⁻¹ at 25 and at 37° C, respectively. The apparent activation energy for

over the temperature range 23–37° C was 8.7±1.0 kcal/mole.     

NMR paramagnetic relaxation enhancements due to manganese in the S0 and S2 states of Photosystem II-enriched membrane fragments and in the detergent-solubilized Photosystem II complex

The NMR paramagnetic relaxation enhancement (NMR-PRE) produced in the solvent proton resonance by manganese in the S₀ and S₂ states of the oxygen evolving center (OEC) has been recorded for three Photosystem II (PS II)-enriched preparations: (1) PS II-enriched thylakoid membrane fragments (TMF-2 particles); (2) salt-washed (2M NaCl) TMF-2 particles; and (3) the octylglucopyranoside (OGP)-solubilized PS II complex. The second and third preparations, but not the first, are depleted of the peripheral 17 and 23 kD polypeptides associated with the OEC. It has been proposed that depletion of these polypeptides increases the exposure of OEC manganese to the aqueous phase. The NMR-PRE response measures the quantity (T_1m+_m)^-1, where T_1m is the spin relaxation time and _m is the mean residence time with respect to chemical exchange reactions of solvent protons in the manganese coordination sphere, and, thus, the NMR-PRE provides a direct measure of the solvent proton chemical exchange rate constant _m ^-1. This study tested whether the 17 and 23 kD polypeptides shield the OEC from the solvent phase and whether their depletion enhances the S₂ and S₀ NMR-PRE signals by removing a kinetic barrier to the solvent proton chemical exchange reaction. The amplitude of the S₂ NMR-PRE signal, measured in its chemical exchange-limited regime (_m>T_1m), is slightly decreased, rather than increased, in preparations (2) and (3) relative to (1), indicating that removal of the 17 and 23 kD polypeptides slightly slows, rather than accelerates, the rate-limiting steps of the solvent proton chemical exchange reactions. In addition, the lifetime of the S₂ state was shortened several-fold in the solubilized PS II complex and in salt-washed TMF-2 membranes relative to untreated TMF-2 control samples. The S₀ NMR-PRE signal, which is present in TMF-2 suspensions, was not detected in suspensions of the solubilized PS II complex, even though these samples contained high concentrations of active manganese centers (approximately double those of the TMF-2 control) and exhibited an S₂ NMR-PRE signal of comparable amplitude to that of the TMF-2 preparation. These results suggest that the 17 and 23 kD extrinsic polypeptides do not shield the NMR-visible water binding site in the OEC from the aqueous phase, although their removal substantially alters the proton relaxation efficiency by shortening T_1m.Abbreviations ADRY acceleration of the deactivation reactions of the water splitting enzyme Y - BBY Photosystem II-enriched membrane fragments prepared by the method of Berthold et al. (1981) - CCCP carbonyl cyanide m-chlorophenyl hydrazone - Chl chlorophyll - DCBQ 2,5-dichlorobenzoquinone - MES morpholinoethanesulfonate - NMR nuclear magnetic resonance - OEC oxygen evolving complex - OGP octylglucopyranoside - PRE paramagnetic relaxation enhancement - PS II Photosystem II - SDS-PAGE sodium dodecyl sulfate polyacrylamide gel electrophoresis - TMF-2 Photosystem II-enriched thylakoid membrane fragments prepared by the method of Radmer et al. (1986) - T₁, T₂ longitudinal and transverse nuclear spin relaxation times     

Unambiguous through-bond sugar-to-base correlations for purines in 13C, 15N-labeled nucleic acids: The HsCsNb,HsCs(N)bCb,and HbNbCb experiments

Summary A set of three 3D (¹H, ¹³C, ¹⁵N) triple-resonance correlation experiments has been designed to provide H1-H8 intraresidue sugar-to-base correlations in purines in an unambiguous and efficient manner. Together, the H_sC_sN_b, H_sC_s(N)_bC_b, and H_bN_bC_b experiments correlate the H1 sugar proton to the H8 proton of the attached base by means of the {H1, C1, N9, C8, H8} heteronuclear scalar coupling network. The assignment strategy presented here allows for unambiguous H1-H8 intraresidue correlations, provided that no two purines have both the same H1 and C1 chemical shifts and the same C8 and N9 chemical shifts. These experiments have yielded H1-H8 intraresidue sugar-to-base correlations for all five guanosines in the [¹³C, ¹⁵N] isotopically labeled RNA duplex r(GGCGCUUGCGUC)₂.     

Conformation of two non-immunosuppressive FK506 analogs when bound to FKBP by isotope-filtered NMR.

The 3D structure of two unlabeled FK506 analogs, (R)- and (S)-[18-OH]ascomycin, when bound to [U-13C,15N]FKBP were determined by isotope-filtered 2D NMR experiments. The structures for the R and S isomers that bind tightly to FKBP but lack immunosuppressive activity are compared to each other and to the conformation of the potent immunosuppressant, ascomycin, when bound to FKBP. The results are interpreted in terms of calcineurin binding to the FKBP/ascomycin complex.     

Concanavalin A interactions with asparagine-linked glycopeptides. The mechanisms of binding of oligomannose,bisected hybrid,and complex type carbohydrates

The affinity of concanavalin A (Con A) for simple saccharides has been known for over 50 years. However, the specificity of binding of Con A with cell-surface related carbohydrates has only recently been examined in detail. Brewer and coworkers [J Biol Chem (1986) 261:7306–10; J Biol Chem (1987) 262:1288–93; J Biol Chem (1987) 262:1294–99] have recently studied the binding interactions of a series of oligomannose and bisected hybrid type glycopeptides and complex type glycopeptides and oligosaccharides with Con A. The relative affinities of the carbohydrates were determined using hemagglutination inhibition measurements, and their modes of binding to the lectin examined by nuclear magnetic relaxation dispersion (NMRD) spectroscopy and quantitative precipitation analyses. The equivalence zones (regions of maximum precipitation) of the precipitin curves of Con A and the carbohydrates indicate that certain oligomannose and bisected hybrid type glycopeptides are bivalent for lectin binding. From the NMRD and precipitation data, two protein binding sites on each glycopeptide have been identified and characterized. Certain bisected complex type oligosaccharides also bind and precipitate Con A, while the corresponding nonbisected analogs bind but do not precipitate the protein. The precipitation data indicate that the bisected complex type oligosaccharides are also bivalent for lectin binding, while the nonbisected analogs are univalent. The NMRD and precipitation data are consistent with different mechanisms of binding of nonbisected and bisected complex type carbohydrates to Con A, including different conformations of the bound saccharides.Abbreviations Con A Concanavalin A with unspecified metal ion content - CMPL Con A with Mn²⁺ and Ca²⁺ at the S1 and S2 sites respectively, in the locked conformation [12]; trisaccharide1, 3,6-di-O-(-d-mannopyranosyl)-d-mannose - -MDM methyl -d-mannopyranoside - NMRD nuclear magnetic relaxation dispersion, the magnetic field dependence of nuclear magnetic relaxation rates, in the present case, the longitudinal relaxation rate, 1/T₁, of solvent protons     

Extending the range of amide proton relaxation dispersion experiments in proteins using a constant-time relaxation-compensated CPMG approach

Relaxation compensated constant-time Carr–Purcell–Meiboom–Gill relaxation dispersion experiments for amide protons are presented that detect s-ms time-scale dynamics of protein backbone amide sites. Because of their ten-fold larger magnetogyric ratio, much shorter 180° pulses can be applied to ¹H than to ¹⁵N spins; therefore, off-resonance effects are reduced and a wider range of effective rf fields can often be used in the case of ¹H experiments. Applications to [¹H-¹⁵N]-ubiquitin and [¹H-¹⁵N]-perdeuterated HIV-1 protease are discussed. In the case of ubiquitin, we present a pulse sequence that reduces artifacts that arise from homonuclear ³J(H_N-H) coupling. In the case of the protease, we show that relaxation dispersion of both ¹H and ¹⁵N spins provides a more comprehensive picture of slow backbone dynamics than does the relaxation dispersion of either spin alone. We also compare the relative merits of ¹H versus ¹⁵N transverse relaxation measurements and note the benefits of using a perdeuterated protein to measure the relaxation dispersion of both spin types.     

Optimized labeling of 13CHD2 methyl isotopomers in perdeuterated proteins: Potential advantages for 13C relaxation studies of methyl dynamics of larger proteins

¹³CHD₂ methyl isotopomers are particularly useful to study methyl dynamics in proteins because, as compared with other methyl isotopomers, the ¹³C relaxation mechanism for this isotopomer is straightforward. However, in the case of proteins, where ()² 1, the refocused INEPT pulse sequence does not completely suppress unwanted ¹³CH₃ signals. The presence of weak ¹³CH₃ peaks is usually not a serious problem for smaller proteins because there are relatively few methyl signals and they are sharp; however, signal overlap becomes more common as the size of the protein increases. We overcome this problem by preparing a protein using a 98% D₂O cell culture medium containing 3-¹³C pyruvic acid, 50–60% deuterated at the 3-position, and 4-¹³C 2-ketobutyric acid, 98% and 62% deuterated at the 3- and 4-positions, respectively. This approach significantly reduces the population of the CH₃ isotopomer while optimizing the production of ¹³CHD₂, the isotopomer desired for ¹³C relaxation measurements. In larger proteins where the deuterium T₂ may be too short to measure accurately, we also suggest the alternative measurement of the proton T₂ of the ¹³CH₂D methyl isotopomer, because these protons are well-isolated from other protons in these highly deuterated samples.     

The State of Water in Muscle Tissue as Determined by Proton Nuclear Magnetic Resonance

The nuclear magnetic resonance (NMR) of water protons in live and glycerinated muscle, suspensions of glycerinated myofibrils, and solutions of several muscle proteins has been studied. T₁ and T₂, measured on partially hydrated proteins by pulsed spin-echo techniques, decreased as the ratio of water to protein decreased, showing that the water which is tightly bound by the protein has short relaxation times. In live muscle fibers the pulse techniques showed that, after either a 180 or a 90° pulse, the relaxation of the magnetization is described by a single exponential. This is direct evidence that a fast exchange of protons occurs among the phases of the intracellular water. The data can be fitted with a model in which the bulk of the muscle water is in a phase which has properties similar to those of a dilute salt solution, while less than 4-5% of the total water is bound to the protein surface and has short relaxation times. Measurements of T₁ and T₂ in protein solutions showed that no change in the proton relaxation times occurred when heavy meromyosin was bound to actin, when myofibrils were contracted with adenosine triphosphate (ATP), or when globular actin was polymerized.     

Magnetic Resonance Water Proton Relaxation in Protein Solutions and Tissue: T1ρ Dispersion Characterization

Background

Image contrast in clinical MRI is often determined by differences in tissue water proton relaxation behavior. However, many aspects of water proton relaxation in complex biological media, such as protein solutions and tissue are not well understood, perhaps due to the limited empirical data.

Principal Findings

Water proton T₁, T₂, and T_1ρ of protein solutions and tissue were measured systematically under multiple conditions. Crosslinking or aggregation of protein decreased T₂ and T_1ρ, but did not change high-field T₁. T_1ρ dispersion profiles were similar for crosslinked protein solutions, myocardial tissue, and cartilage, and exhibited power law behavior with T_1ρ(0) values that closely approximated T₂. The T_1ρ dispersion of mobile protein solutions was flat above 5 kHz, but showed a steep curve below 5 kHz that was sensitive to changes in pH. The T_1ρ dispersion of crosslinked BSA and cartilage in DMSO solvent closely resembled that of water solvent above 5 kHz but showed decreased dispersion below 5 kHz.

Conclusions

Proton exchange is a minor pathway for tissue T₁ and T_1ρ relaxation above 5 kHz. Potential models for relaxation are discussed, however the same molecular mechanism appears to be responsible across 5 decades of frequencies from T_1ρ to T₁.     

Conformation and dynamic structure of poly(inosinic acid) in neutral aqueous solution by 1H-, 2H-, 13C-, and 31P-NMR spectroscopy

The conformation and dynamic structure of single-stranded poly(inosinic acid), poly(I), in aqueous solution at neutral pH have been investigated by nmr of four nuclei at different frequencies: ¹H (90 and 250 MHz), ²H (13.8 MHz), ¹³C (75.4 MHz), and ³¹P (36.4 and 111.6 MHz). Measurements of the proton-proton coupling constants and of the ¹H and ¹³C chemical shifts versus temperature show that the ribose is flexible and that base-base stacking is not very significant for concentrations varying from 0.04 to 0.10M in the monomer unit. On the other hand, the proton T₁ ratios between the sugar protons, T₁ (H₁′)/T₁ (H₃′), indicate a predominance of the anti orientation of the base around the glycosidic bond. The local motions of the ribose and the base were studied at different temperatures by measurements of nuclear Overhauser enhancement (NOE) of protonated carbons, the ratio of the proton relaxation times measured at two frequencies (90 and 250 MHz), and the deuterium quadrupolar transverse relaxation time T₂. For a given temperature between 22 and 62°C, the ¹³C-{¹H} NOE value is practically the same for seven protonated carbons (C₂, C₈, C_1′, C_2′, C_3′, C_4′, C_5′). This is also true for the T₁ ratio of the corresponding protons. Thus, the motion of the ribose–base unit can be considered as isotropic and characterized by a single correlation time, τ_c, for all protons and carbons. The τ_c values determined from either the ¹³C-{¹H} NOE or proton T₁ ratios, T₁(90 MHz)/T₁(250 MHz), and/or deuterium transverse relaxation time T₂ agree well. The molecular motion of the sugar-phosphate backbone (O-P-O) and the chemical-shift anisotropy (CSA) were deduced from T₁ (³¹P) and ³¹P-{¹H} NOE measurements at two frequencies. The CSA contribution to the phosphorus relaxation is about 12% at 36.4 MHz and 72% at 111.6 MHz, corresponding to a value of 118 ppm for the CSA (σ = σ∥ ? σ?). Activation energies of 2–6 kcal/mol for the motion of the ribose–base unit and the sugarphosphate backbone were evaluated from the proton and phosphorus relaxation data.     

Measurement of proton relaxation rates in proteins

Summary Five different types of experiment are described which make it possible to measure various relaxation rates of selected protons in crowded spectra of macromolecules such as proteins: longitudinal spin-lattice relaxation rates =1/T₁, transverse relaxation rates =1/T₂ measured under conditions of free precession, transverse relaxation rates ¹ _LOCK=1/T₁ measured under conditions of spin-locking, and transverse relaxation rates ^DQC=1/T₂ ^DQC and ^ZQC=1/T₂ ^ZQC of double- and zero-quantum coherences. The surprisingly large discrepancy between the transverse rates ^t and ^t is discussed in detail. To separate overlapping proton signals, the experimental schemes involve one or several magnetization transfer steps, using a doubly selective homonuclear Hartmann-Hahn method. Numerous variants of the basic ideas can be conceived, depending on the extent of signal overlap and on the topology of the networks of scalar couplings. Applications are shown to H and H of Tyr²³, to H, H and H of Cys³⁰, and to H and H of Ala²⁴ in bovine pancreatic trypsin inhibitor (BPTI).     

Protein dynamics studied by rotating frame 15N spin relaxation times

Summary Conformational rate processes in aqueous solutions of uniformly ¹⁵N-labeled pancreatic trypsin inhibitor (BPTI) at 36°C were investigated by measuring the rotating frame relaxation times of the backbone ¹⁵N spins as a function of the spin-lock power. Two different intramolecular exchange processes were identified. A first local rate process involved the residues Cys³⁸ and Arg³⁹, had a correlation time of about 1.3 ms, and was related to isomerization of the chirality of the disulfide bond Cys¹⁴-Cys³⁸. A second, faster motional mode was superimposed on the disulfide bond isomerization and was tentatively attributed to local segmental motions in the polypeptide sequence-Cys¹⁴-Ala¹⁵-Lys¹⁶-. The correlation time for the overall rotational tumbling of the protein was found to be 2 ns, using the assumption that relaxation is dominated by dipolar coupling and chemical shift anistropy modulated by isotropic molecular reorientation.Abbreviations BPTI basic pancreatic trypsin inhibitor - 2D two-dimensional - COSY 2D correlation spectroscopy - TOCSY 2D total correlation spectroscopy - RF radio frequency - CW continuous wave - TPPI time-proportional phase incrementation - CSA chemical shift anisotropy - T₁ longitudinal relaxation time - T₂ transverse relaxation time - T₁ relaxation time in the rotating frame , correlation time for overall rotational reorientation of the protein - _ex ^s , _ex ^f , correlation times for two conformational exchange processes (slow and fast).     

Tocopheramines and tocotrienamines as antioxidants: ESR spectroscopy,rapid kinetics and DFT calculations

Tocopheramines (TNH₂) and tocotrienamines (T₃NH₂) are analogues of tocopherols (TOH) and tocotrienols in which phenolic OH is replaced by NH₂. It was shown in previous studies that TNH₂ and T₃NH₂ act as potent antioxidants. In this study we compared the one-electron oxidation of TNH₂/T₃NH₂ by diphenyl picryl hydrazyl (DPPH) and galvinoxyl (GOX) radicals with the one of α-TOH as a reference compound using ESR spectroscopy, stopped flow spectrophotometry and density functional theory (DFT) calculations. ESR spectroscopy revealed the presence of tocopheramine radicals during electrochemical oxidation of α-TNH₂. Kinetic measurements demonstrated that in apolar n-hexane TNH₂/T₃NH₂ derivatives reacted two to three orders of magnitude slower than α-TOH with the model radicals. DFT calculations indicated that this correlates well with the higher bond dissociation energy (BDE) for N–H in TNH₂ than for O–H in α-TOH in pure H-atom transfer (HAT). In the more polar medium ethanol TNH₂/T₃NH₂ derivatives partially reacted faster than α-TOH depending on the reaction partner. DFT calculations suggest that this is due to reaction mechanisms alternative to HAT. According to thermochemistry data sequential proton loss and electron transfer (SPLET) is more favored for α-TOH in ethanol than for TNH₂. Therefore, for TNH₂ a contribution of the alternative mechanism of sequential electron transfer–proton transfer (SET–PT) could be a possible explanation. These data show that the antioxidant reactivity strongly depends on the structure, reaction partners and environment. According to these findings TNH₂/T₃NH₂ should be superior as antioxidants over α-TOH in polar head group regions of membranes but not in the apolar core of lipid bilayers.     

Picosecond Raman spectroscopy of the B830 LH2 complex ofChromatium purpuratum BN 5500

A setup for generating the Stokes Raman lines of benzene (556, 588 and 624 nm, 50 ps) by the use of the second harmonic of a Nd: YLF regenerative amplifier system (527 nm, 70 ps, 1 kHz) has been built. This was then used to detect, for the first time, the picosecond Raman spectrum of a carotenoid bound to an isolated light-harvesting complex of a photosynthetic bacterium. The 527 and 588 nm pulses have been used, respectively, for pumping and probing (delay 0 ps) the S₁ and T₁ states of okenone which is bound to both the isolated B830 LH2 complex and the chromatophores fromChromatium purpuratum BN 5500. Comparison of the above spectra with the S₁ and T₁ Raman spectra of all-trans-okenone, free inn-hexane solution, shows that only the T₁ state is detected with the LH2 complex, and that both the S₁ and T₁ states are detected with the chromatophores. The results indicate that in the chromatophores there are at least two types of S₁ carotenoids with different lifetimes, i.e., one in the LH2 complex which is too short-lived to be detected, most probably due to efficient energy transfer to bacteriochlorophyll, and the other in either the reaction center or the LH1 complex which is long-lived enough to be pumped and probed by 50 70 ps pulses. The results also indicate that at least two of the actively light-harvesting carotenoid molecules are in close connection in the isolated LH2 complex since the T₁ state is generated through singlet homofission within the short S₁ lifetime.