Influence of D and L amino-acid residues on the conformation of peptides in solution: A carbon-13 nuclear magnetic resonance study of cyclo(prolyl-leucyl)

The ¹³C chemical shifts and spin-lattice relaxation times are reported for cyclo(L -Pro-L -Leu) and cyclo(L -Pro-D -Leu). The chemical shifts of the D and L leucyl residues in the cyclic peptides differ from each other by 1.8 and 3.6 parts per million for the α and β carbons, respectively. The α-carbons of the prolyl residues differ by 1.0 ppm as a consequence of proximity to a D or an L leucyl residue. The ¹³C spin-lattic relaxation time(T₁) of the prolyl residues, but not the leucyl residues, in both compounds are indicative of difference in conformational equilibria within the pyrrolidine ring in the L -L isomer as compared to the L -D isomer. Anisotropic overall molecular reorientation is not responsible for the differences observed in the T₁ values. The differences in T₁ values and chemical shifts between cyclo(L -Pro-L -Leu) and cyclo(L -Pro-D -Leu) appear to result from a difference in conformations of the two diketopiperazine rings.     

Molecular mobility of polypeptides containing proline as determined by 13C magnetic resonance

The molecular conformations and dynamics of poly(L -prolyl), poly(hydroxyl-L -prolyl), poly(L -prolyl-glycyl), poly(hydroxyl-L -prolyl), and poly(glycyl-glycyl-L -prolyl-glycyl), in aqueous solution, have been studied using ¹³C pulse Fourier transform nmr spectroscopy. From a measurement of the intensities of major and minor resonances in the spectra of the copolypeptides, it was determined that 15–20% of the glycyl-prolyl and glycyl-hydroxyprolyl peptide bonds are cis. Effective rotational correlation times (τ_eff), obtained from measurements of spin-lattice relaxation times (T₁) of individual backbone and side-chain carbons, demonstrated that backbone reorientation is approximately isotropic for the five polypeptides and is characterized by correlation times of ca. 0.3–0.6 nanoseconds as a result of rapid segmental motion. In a given polypeptide glycyl and pyrrolidine residues were found to have the same backbone correlation times, but backbone carbon τ_eff values did decrease as the glycyl content of the peptides increased. A semi-quantitative analysis of C^β, C^γ, and C^δ correlation times suggests that rapid ring motion in both prolyl and hydroxyprolyl involves primarily C^γ and C^β, with the prolyl ring being more mobile than the hydroxyprolyl ring.     

A 13C spin-lattice relaxation study of dipeptides containing glycine and proline: mobility of the cyclic proline side chain.

Molecular dynamics of the cyclic dipeptides cyclo(Gly-L -Pro), cyclo-(L-Pro-L -Pro), and cyclo(L-Pro-D-Pro) and the linear dipeptides L-Pro-Gly and cis and trans Gly-L -Pro were studied in neutral aqueous solution by ¹³C nuclear magnetic resonance. Spinlattice relaxation times (T₁) were determined for each individual carbon atom. The correlation times, τ, were derived from a semiquantitative analysis of the T₁ data. The correlation times of the proline ring carbons, β, γ, and δ suggest that the cyclic dipeptides have more restriction of conformational freedom in the proline ring than the linear dipeptides. This effect is most pronounced on the γ carbon.     

Conformation of the common purine (β) ribosides in solution: further evidence for a correlation between N-S state of the ribose moiety and syn-anti equilibrium

The solution conformations of adenosine, guanosine and inosine in liquid ND₃ have been determined by NMR. Comparison of the Karplus analysis of the proton HR spectra of the ribose moiety obtained in this solvent with the data from aqueous solutions of A and I proves that the conformations of the nucleosides are very similar in both liquids. From the analysis of the vicinal coupling constants of the ring protons it has been deduced that the S state C(2′)-endo is slightly preferred. The mole fraction in S approximates 0.6 for all three nucleosides. C-13 relaxation measurements have been applied in the determination of the correlation times for rotational diffusion. Only at temperatures below −40‡ C is the pseudorotation of the furanoside ring slowed down sufficiently for it not to contribute to the measured relaxation rates. From NOE studies and T¹ measurements on the individual protons it is derived that the N, C(3′)-endo, form of the ribose is correlated with an anti conformation of the base (Y≈210‡ to 220‡) and the S, C(2′)-endo, form of the ribose with a syn conformation of the base (Y≈30‡ to 50‡). The glycosyl torsion angles derived for the two conformations of A, G, and I are equal within the limits of accuracy.     

Proton and phosphorus-31 magnetic relaxation studies on the interaction of polyriboadenylic acid with Mn2+

Proton and phosphorus-31 nuclear spin–lattice relaxation times T₁ and spin–spin relaxation times T₂ have been measured on the single-stranded polyriboadenylic acid [poly(A)]–Mn²⁺ system in a neutral D₂O solution in the temperature range 10°–90°C at 100 and 40.5 MHz, respectively, with the Fourier transform nmr method. Minimum values of T₁ have been found for all these nuclei, which have enabled the exact estimation of apparent distances from Mn²⁺ to H₂, H₈, H_1′, and the phosphorus nucleus to be 4.7, 4.1, 5.2, and 3.0 Å, respectively. The electron spin of Mn²⁺ penetrates into the phosphorus nucleus, giving ³¹P hyperfine coupling of more than 10⁶ Hz. Evidence of penetration of the electron spin into H₈ and H₂ is also obtained, suggesting direct coordination of nitrogen atoms of the adenine ring to the Mn²⁺ Ion. Combined with the result from proton relaxation enhancement of water, it is concluded that every Mn²⁺ ion added is bound directly to two phosphate groups with a Mn²⁺–phosphorus distance of 3.3 Å, while a part of the Mn²⁺ ions are simultaneouly bound to the adenine ring. It is estimated that 39 ± 13% and 13 ± 5% of Mn²⁺ are coordinated by N₇ and N₃ (or N₁), respectively. The motional freedom of poly(A) in the environment of the Mn²⁺ binding site has been found to be quenched to the extent that the rotational motion becomes several times slower than that of the corresponding Mn²⁺–free poly(A). The activation energies for the molecular motion are, however, practically unchanged from those for Mn²⁺–free poly(A), and are found to be 8.3, 8.5, 6.1, and 8.7 kcal/mol for H₈, H₂, H_1′, and phosphorus, respectively. T₂ of phosphorus is determined by the dissociation rate (k_?1) of Mn²⁺ from the phosphate group for the whole temperature range studied with activation enthalpy of 6.5 kcal/mol. The dissociation rates of Mn²⁺ from the adenine ring are also estimated from proton T₂ values below 50°C.     

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.     

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.     

High resolution <Superscript>13</Superscript>C-detected solid-state NMR spectroscopy of a deuterated protein

High resolution ¹³C-detected solid-state NMR spectra of the deuterated beta-1 immunoglobulin binding domain of the protein G (GB1) have been collected to show that all ¹⁵N, ¹³C′, ¹³Cα and ¹³Cβ sites are resolved in ¹³C–¹³C and ¹⁵N–¹³C spectra, with significant improvement in T ₂ relaxation times and resolution at high magnetic field (750 MHz). The comparison of echo T ₂ values between deuterated and protonated GB1 at various spinning rates and under different decoupling schemes indicates that ¹³Cα T ₂′ times increase by almost a factor of two upon deuteration at all spinning rates and under moderate decoupling strength, and thus the deuteration enables application of scalar-based correlation experiments that are challenging from the standpoint of transverse relaxation, with moderate proton decoupling. Additionally, deuteration in large proteins is a useful strategy to selectively detect polar residues that are often important for protein function and protein–protein interactions.     

An investigation of the dynamics of spermine bound to duplex and quadruplex DNA by <Superscript>13</Superscript>C NMR spectroscopy

A detailed analysis of the ¹³C relaxation of ¹³C-labelled spermine bound to duplex and quadruplex DNA is presented. T₁, T₂ and heteronuclear NOE data were collected at four ¹³C frequencies (75.4, 125.7, 150.9 and 201.2 MHz). The data were analyzed in terms of a frequency-dependent order parameter, S ²(ω), to estimate the generalized order parameter and the contributions to the relaxation from different motional frequencies in the picosecond–nanosecond timescale and from any exchange processes that may be occurring on the microsecond–millisecond timescale. The relaxation data was surprisingly similar for spermine bound to two different duplexes and a linear parallel quadruplex. Analysis of the relaxation data from these complexes confirmed the conclusions of previous studies that the dominant motion of spermine is independent of the macroscopic tumbling of the DNA and has an effective correlation time of ∼50 ps. In contrast, spermine bound to a folded antiparallel quadruplex had faster relaxation rates, especially R ₂. As with the other complexes, a fast internal motion of the order of 50 ps makes a substantial contribution to the relaxation. The generalized order parameter for spermine bound to duplex DNA and the linear quadruplex is small but is larger for spermine bound to the folded quadruplex. In the latter case, there is evidence for exchange between at least two populations of spermine occurring on the microsecond–millisecond timescale. Electronic supplementary material The online version of this article (doi:) contains supplementary material, which is available to authorized users.     

The conformation of oxytocin in dimethylsulfoxide as revealed by carbon-13 spin-lattice relaxation times

Information was obtained on rates of overall molecular reorientation and segmental motion of amino acid sidechains of oxytocin in dimethylsulfoxide by determination of spin-lattice relaxation times (T₁) at 25 MHz for carbon-13 in natural abundance in the hormone. The T₁ values of the α-carbons of amino acid residues located in the 20-membered ring of oxytocin are all about 50 msec. The overall correlation time for the hormone backbone was estimated to be 8.8 × 10^?10 sec. The sidechains of Tyr, Ile and Gln undergo segmental motion with respect to the backbone of the ring. The T₁ value of the α-carbon of the Leu residue is greater than for any α-carbon in the ring, indicating an increased mobility of the backbone of the C-terminal acyclic peptide as compared to the ring. The β- and γ-carbons of the Pro residue undergo an exo-endo interconversion with regard to the plane formed by α-carbon, δ-carbon and N atom of the Pro pyrollidine ring. These data are discussed in light of results from other experimental and theoretical studies, including carbon-13 spin-lattice relaxation times for oxytocin in aqueous solution.     

A novel strategy for the assignment of side-chain resonances in completely deuterated large proteins using 13C spectroscopy

The assignment of the aliphatic ¹³C resonances of trimeric Bacillus Subtilis chorismate mutase, a protein with a molecular mass of 44 kDa, consisting of three 127-residue monomers is presented by use of two-dimensional (2D) ¹³C-start and ¹³C-observe NMR experiments. These experiments start with ¹³C excitation and end with ¹³C observation while relying on the long transverse relaxation times of ¹³C spins in uniformly deuterated and ¹³C,¹⁵N-labeled large proteins. Gains in sensitivity are achieved by the use of a paramagnetic relaxation enhancement agent to reduce ¹³C T ₁ relaxation times with little effect on ¹³C T ₂ relaxation times. Such 2D ¹³C-only NMR experiments circumvent problems associated with the application of conventional experiments for side-chain assignment to proteins of larger sizes, for instance, the absence or low concentration of the side-chain ¹H spins, the transfer of the side-chain spin polarization to the ¹H^N spins for signal acquisition, or the necessity of a quantitative reprotonation of the methyl moieties in the otherwise fully deuterated side-chains. We demonstrate that having obtained a nearly complete assignment of the side-chain aliphatic ¹³C resonances, the side-chain ¹H chemical shifts can be assigned in a semiautomatic fashion using 3D ¹⁵N-resolved and ¹³C-resolved NOESY experiments measured with a randomly partially protonated protein sample. We also discuss perspectives for structure determination of larger proteins by using novel strategies which are based on the ¹H,¹H NOEs in combination with multiple residual dipolar couplings between adjacent ¹³C spins determined with 2D ¹³C-only experiments.     

Synthesis and conformation of the cyclic octapeptides cyclo(Phe-Pro)4, cyclo(Leu-Pro)4, and cyclo[Lys(Z)-Pro]4

Cyclic octapeptides, cyclo(X-Pro)₄, where X represents Phe, Leu, or Lys(Z), were synthesized and their conformations investigated. A C₂-symmetric conformer containing two cis peptide bonds was found in all of these cyclic octapeptides. The numbers of available conformations due to the cis–trans isomerization of Pro peptide bonds depended on the nature of the solvent and X residue: they decreased in the following order: cyclo[Lys(Z)-Pro]₄ > cyclo(Leu-Pro)₄ > cyclo(Phe-Pro)₄ in CDCl₃. ¹³C spin-lattice relaxation times (T₁) of these cyclic octapeptides were measured, and the contribution of segmental mobility to T₁ was found to vary with the nature of the X residue.     

Residue Specific Ribose and Nucleobase Dynamics of the cUUCGg RNA Tetraloop Motif by MNMR 13C Relaxation

The dynamics of the nucleobase and the ribose moieties in a 14-nt RNA cUUCGg hairpin-loop uniformly labeled with ¹³C and ¹⁵N were studied by ¹³C spin relaxation experiments. R₁, R_1ρ and the ¹³C-{¹H} steady-state NOE of C₆ and C_1′ in pyrimidine and C₈ and C_1′ in purine residues were obtained at 298 K. The relaxation data were analyzed by the model-free formalism to yield dynamic information on timescales of pico-, nano- and milli-seconds. An axially symmetric diffusion tensor with an overall rotational correlation time τ_c of 2.31±0.13 ns and an axial ratio of 1.35±0.02 were determined. Both findings are in agreement with hydrodynamic calculations. For the nucleobase carbons, the validity of different reported ¹³C chemical shift anisotropy values (Stueber, D. and Grant, D. M., 2002 J. Am. Chem. Soc. 124, 10539–10551; Fiala et al., 2000 J. Biomol. NMR 16, 291–302; Sitkoff, D. and Case, D. A., 1998 Prog. NMR Spectroscopy 32, 165–190) is discussed. The resulting dynamics are in agreement with the structural features of the cUUCGg motif in that all residues are mostly rigid (0.82 < S² < 0.96) in both the nucleobase and the ribose moiety except for the nucleobase of U7, which is protruding into solution (S² = 0.76). In general, ribose mobility follows nucleobase dynamics, but is less pronounced. Nucleobase dynamics resulting from the analysis of ¹³C relaxation rates were found to be in agreement with ¹⁵N relaxation data derived dynamic information (Akke et al., 1997 RNA 3, 702–709). Electronic supplementary material Electronic supplementary material is available for this article at and accessible for authorised users.     

Molecular mobilities of soluble components in the aqueous phase of chromaffin granules

NMR relaxation times have been used to characterize molecular motion and intermolecular complexes in the aqueous phase of bovine chromaffin granules. Partially relaxed ¹³C and proton spectra have been obtained at 3 and 25°C. T₁ measurements of five protonated carbons on epinephrine (C₂, C₅, C₆ CHOH and NCH₃) give a correlation time of 0.15 (10^?9) s at 25°C for the catechol ring and methine carbon, while the effective correlation time for the NCH₃ group is somewhat shorter due to its internal degree of rotational freedom. Resonances of protonated carbons on the soluble protein chromogranin give very similar corerlation times: 0.20 (10^?9) s for the peptide α-carbon and 0.2 (10^?9) s for the methylene sidechain carbons of glutamic acid. The correlation time (τ_R) of ATP was not measured direrctly using ¹³C T₁ data due to the weakness of its spectrum, but its reorinetation appears to be substantially slower than that of epinephrine or chromogranin. This conclusion is based on three observations: (1) the qualitative temperature dependence of T₁ for H₂ and H₈ on the adenine ring places τ_R for ATP to the right of the T₁ minimum, or τ_R ? 1.0 (10^?9) s; (2) ¹³C resonances of ATP have anomalously low amplitudes compared with epinphrine resonances, a fact that is readily explained only if ATP undergoes substantially slower reorientation; and (3) a comparision of the T₁ data on H₈ on chromaffin granules and in a dilute aqueous solution, where ρ_R for ATP cam be measured directly, indicates that τ_R ～ 1.0 (10^?9 s at 25°C in the granules. The relaxation data are consistent with the concept of a storage complex based on electrostatic interaction between a polyion (chromogranin) and its counterious (ATP and epinephrine), in which ATP cross-links cationic sidechains of the protein.     

Multi-conformational peptide dynamics derived from NMR data: A new search algorithm and its application to antamanide

Summary A search algorithm, called MEDUSA, is presented which allows the determination of multiple conformations of biomolecules in solution with exchange rate constants typically between 10³ and 10⁷ s^–1 on the basis of experimental high-resolution NMR data. Multiples of structures are generated which are consistent as ensembles with NMR cross-relaxation rates (NOESY, ROESY), scalar J-coupling constants, and T_1p measurements. The algorithm is applied to the cyclic decapeptide antamanide dissolved in chloroform. The characteristic radio-frequency field dependence of the T_1p relaxation rates found for the NH protons of Val¹ and Phe⁶ can be explained by a dynamical exchange between two structures.     

Proton and phosphorus magnetic relaxation studies on the dynamic structure of single-stranded polyriboadenylic acid

Proton and phosphorus-31 nuclear spin-lattice relaxation times (T₁) have been measured with the Fourier-transform method at 100 and 40.5 MHz, respectively, on single-stranded polyriboadenylic acid (poly(A)) in a neutral D₂O solution in the temperature range of 14–82°C. T₁ minimum is observed around 35–45°C for H(8), H(1′), and phosphorus resonances. Rotational correlation times have been deduced from the T₁ data, which indicate that the sugar–phosphate backbone as well as the base–sugar segment is undergoing rapid internal motion of 10^?8–10^?10 sec range. The molecular motion of the sugar–phosphate backbone as deduced from the phosphorus relaxation is well-characterized by a single activation enthalpy of 8.1 kal/mole for the whole temperature range of 14–82°C. Activation enthalpies of similar magnitude have been obtained for the motion of the adenine–ribose moiety from H(8) and H(1′) relaxation. The relative magnitude of T₁ for H(8) and H(1′) infers that the poly(A) nucleotide exists on the average as anti in the single-stranded form. The phosphorus T₁ value is consistent with a conformation such that both C(4′)–C(5′) and C(4′)–C(3′) bonds are nearly trans to their connected O–P bonds.     

Alternate-site isotopic labeling of ribonucleotides for NMR studies of ribose conformational dynamics in RNA

Heteronuclear NMR spin relaxation studies of conformational dynamics are coming into increasing use to help understand the functions of ribozymes and other RNAs. Due to strong magnetic interactions within the ribose ring, however, these studies have thus far largely been limited to ¹³C and ¹⁵N resonances on the nucleotide base side chains. We report here the application of the alternate-site ¹³C isotopic labeling scheme, pioneered by LeMaster for relaxation studies of amino acid side chains, to nucleic acid systems. We have used different strains of E. coli to prepare mononucleotides containing ¹³C label in one of two patterns: Either C1′ or C2′ in addition to C4′, termed (1′/2′,4′) labeling, or nearly complete labeling at the C2′ and C4′ sites only, termed (2′,4′) labeling. These patterns provide isolated H spin systems on the labeled carbon atoms and thus allow spin relaxation studies without interference from scalar or dipolar coupling. Using relaxation studies of AMP dissolved in glycerol at varying temperature to produce systems with correlation times characteristic of different size RNAs, we demonstrate the removal of errors due to interaction in T ₁ measurements of larger nucleic acids and in T _1ρ measurements in RNA molecules. By extending the applicability of spin relaxation measurements to backbone ribose groups, this technology should greatly improve the flexibility and completeness of NMR analyses of conformational dynamics in RNA.     

Effects of temperature and field strength on the NMR relaxation times of Na in frog striated muscle

Pulsed NMR techniques have been applied to the study of the relaxation parameters characterizing ²³Na within frog striated muscle. Experiments were performed at 3°C, 22–24°C and 39°C at a Larmor frequency of 15.7 MHz; at 22–24°C, measurements were obtained both at 15.7 MHz and at 7.85 MHz.As previously reported, only a single spine-lattice relaxation time (T₁) was observed, but both slow (T₂)_I and fast (T₂)_II components of the spin-spin relaxation time were measured. The effect of temperature (θ) upon (1/T₁) was qualitatively similar to that reported for ²³Na in free solution; (θ) did not significantly affect (1/T₂) over the range of temperatures studied. (1/T₂)_I, and to a lesser degreee, (1/T₁) exhibited a modest inverse dependence of doubtful significance on the Larmor frequency.The data are examined within the framework of a simple specific model; a conservative values in assumed for the quadrupolar coupling constant characterizing immobilized intracellular Na⁺. Within this framework, the results suggest that the fraction of bound ions whose molecular tumbling is severely restricted does not exceed some few percent of the total sodium population.     

Dynamic aspects of extracellular loop region as a proton release pathway of bacteriorhodopsin studied by relaxation time measurements by solid state NMR

Local dynamics of interhelical loops in bacteriorhodopsin (bR), the extracellular BC, DE and FG, and cytoplasmic AB and CD loops, and helix B were determined on the basis of a variety of relaxation parameters for the resolved ¹³C and ¹⁵N signals of [1-¹³C]Tyr-, [¹⁵N]Pro- and [1-¹³C]Val-, [¹⁵N]Pro-labeled bR. Rotational echo double resonance (REDOR) filter experiments were used to assign [1-¹³C]Val-, [¹⁵N]Pro signals to the specific residues in bR. The previous assignments of [1-¹³C]Val-labeled peaks, 172.9 or 171.1 ppm, to Val69 were revised: the assignment of peak, 172.1 ppm, to Val69 was made in view of the additional information of conformation-dependent ¹⁵N chemical shifts of Pro bonded to Val in the presence of ¹³C-¹⁵N correlation, although no assignment of peak is feasible for ¹³C nuclei not bonded to Pro. ¹³C or ¹⁵N spin-lattice relaxation times (T₁), spin-spin relaxation times under the condition of CP-MAS (T₂), and cross relaxation times (T_CH and T_NH) for ¹³C and ¹⁵N nuclei and carbon or nitrogen-resolved, ¹H spin-lattice relaxation times in the rotating flame (¹H T_1ρ) for the assigned signals were measured in [1-¹³C]Val-, [¹⁵N]Pro-bR. It turned out that V69-P70 in the BC loop in the extracellular side has a rigid β-sheet in spite of longer loop and possesses large amplitude motions as revealed from ¹³C and ¹⁵N conformation-dependent chemical shifts and T₁, T₂, ¹H T_1ρ and cross relaxation times. In addition, breakage of the β-sheet structure in the BC loop was seen in bacterio-opsin (bO) in the absence of retinal.