9 research outputs found

    Stretching-Induced Conformational Transition of [3-<sup>13</sup>C]Ser- and [3-<sup>13</sup>C]Tyr-Antheraea yamamai Silk Fibroin before Spinning Investigated with <sup>13</sup>C Solid-State NMR Spectroscopy

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    The conformational transition of [3-13C]Ser- and [3-13C]Tyr-Antheraea yamamai silk fibroin before spinning induced by stretching was investigated with 13C CP/MAS NMR spectroscopy. The Ī±-helix content of the silk fibroin before stretching was found to be 31.6% based on the Ala and Ser peaks. With increasing stretching ratio, the Ī±-helix and the random coil Ala CĪ² peaks decreased gradually, while the Ī²-sheet peak was observed at a stretching ratio of Ɨ5 and increased rapidly upon further stretching. For Ser residue, the Ī±-helix peak decreased monotonically with increasing stretching ratio, but the random coil peak increased slightly till the stretching ratio of Ɨ5 and then decreased. A small Ī²-sheet peak was observed before stretching and then increased rapidly starting from the stretching ratio of Ɨ7. In contrast, a gradual decrease of random coil peak and an increase of Ī²-sheet peak were observed for the Tyr residue. The results of this investigation may be helpful for further studies of fiber formation mechanism in A. yamamai and in the future design of artificial silk materials

    Determination of Local Structure of <sup>13</sup>C Selectively Labeled 47-mer Peptides as a Model for Gly-Rich Region of <i>Nephila clavipes</i> Dragline Silk Using a Combination of <sup>13</sup>C Solid-State NMR and MD Simulation

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    For the first time, we elucidate the complex structure of the Gly-rich regions in <i>Nephila clavipes</i> dragline silk through synergistic experimental and theoretical studies. First, the <sup>13</sup>C selectively labeled 47-mer peptides selected from the glycine (Gly)-rich region of <i>N. clavipes</i> dragline silk were synthesized. The <sup>13</sup>C CP/MAS NMR spectra were analyzed to determine the fractions of the conformations of individual Gly and Ala residues through <sup>13</sup>C conformation-dependent chemical shifts and peak deconvolution. By comparing the <sup>13</sup>C solid-state NMR spectra of several simple model peptides, the presence of 3<sub>1</sub> helix in the 47-mer peptides was disproved, and the (Ala)<sub>6</sub> regions were shown to form Ī²-sheet structure in the staggered arrangement. Although the fraction of Ī²-sheet components tended to increase and the fraction of random coil component decrease toward both chain ends, significant change in the fractions was observed depending on the amino acid position. These results were successfully rationalized through molecular dynamics simulation

    Unusual Dynamics of Alanine Residues in Polyalanine Regions with Staggered Packing Structure of Samia cynthia ricini Silk Fiber in Dry and Hydrated States Studied by <sup>13</sup>C Solid-State NMR and Molecular Dynamics Simulation

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    Recently, the wild silkworm and spider dragline silks have been paid considerable attention as potentially valuable biomedical materials. Samia cynthia ricini is one of the wild silkworms and the primary structure of the silk fibroin (SF) consists of tandemly repeated polyalanine (poly-A:(A)<sub>12,13</sub>). Here, we report the unusual dynamical character observed in Ala CĪ² groups in the poly-A region which forms an antiparallel-Ī²-sheet structure with a staggered packing arrangement. The <sup>13</sup>C spinā€“lattice relaxation (<i>T</i><sub>1</sub>ā€™s) and spinā€“spin relaxation times (<i>T</i><sub>2</sub>ā€™s) of Ala CĪ² peaks in S. c. ricini SF fibers were observed in dry and hydrated states. The lowest field peak in Ala CĪ² of the poly-A region showed 2 times longer <i>T</i><sub>1</sub> value and shorter correlation time than the other Ala CĪ² peaks of the staggered packing structure, suggesting unusually fast hopping in methyl groups. Molecular dynamics simulations indicated that two of the Ala CĪ² carbons out of eight existing in the unit cell of the staggered packing structure exhibited the fastest hopping motion in spite of the shortest CĪ²ā€“CĪ² distance, indicating a geared hopping motion. <i>T</i><sub>2</sub> values of the hydrated and dry Ala CĪ² peaks showed a similar value, indicating that the backbone motion of S. c. ricini SF fiber is not significantly affected by hydration

    Packing Arrangements and Intersheet Interaction of Alanine Oligopeptides As Revealed by Relaxation Parameters Obtained from High-Resolution <sup>13</sup>C Solid-State NMR

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    Alanine oligopeptides provide a key structure of the crystalline domains of the silks from spiders and wild silkworm and also the sequences included in proteins such as antifreeze proteins and amyloids. In this paper, the local dynamics of alanine oligopeptides, (Ala)<sub>3</sub>, (Ala)<sub>4</sub>, and (Ala)<sub>6</sub> were examined by high-resolution <sup>13</sup>C solid-state NMR. The <sup>13</sup>C spinā€“lattice relaxation times (<i>T</i><sub>1</sub>ā€™s) for the CĪ²4 carbons of antiparallel (AP)-Ī²-sheet (Ala)<sub>4</sub> significantly prolonged and the correlation time was estimated as 3.6 Ɨ 10<sup>ā€“11</sup> s which was shorter than those of other carbons in the AP-Ī²-sheet (Ala)<sub>4</sub> (2.8 Ɨ 10<sup>ā€“10</sup> s). The <i>T</i><sub>1</sub> values for the CĪ² carbons of (Ala)<sub>6</sub> showed significantly longer correlation time (8.8 Ɨ 10<sup>ā€“9</sup> s) than those of AP-Ī²-sheet (Ala)<sub>4</sub>. It is thus revealed that AP-Ī²-sheet (Ala)<sub>6</sub> exhibited stronger intersheet interaction than those of AP-Ī²-sheet (Ala)<sub>4</sub>. The <sup>13</sup>C spinā€“spin relaxation times (<i>T</i><sub>2</sub>ā€™s) for the CĪ²4 carbons showed longer than those of the other CĪ²1ā€“3 carbons of AP-Ī²-sheet (Ala)<sub>4</sub>. <i>T</i><sub>2</sub> values of CĪ² carbons reflect the slow time-scale (āˆ¼70 kHz) backbone motions. The C-terminal forms strong hydrogen bonds with water molecules and thus the backbone motion is slower than āˆ¼70 kHz, while the central backbone motions are faster than āˆ¼70 kHz in the AP-Ī²-sheet (Ala)<sub>4</sub>

    Effect of Water on the Structure and Dynamics of Regenerated [3-<sup>13</sup>C] Ser, [3-<sup>13</sup>C] , and [3-<sup>13</sup>C] Ala-<i>Bombyx mori</i> Silk Fibroin Studied with <sup>13</sup>C Solid-State Nuclear Magnetic Resonance

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    The effects of water on the structure and dynamics of natural and regenerated silk fibroin (SF) samples were studied using <sup>13</sup>C solid-state nuclear magnetic resonance (NMR) spectroscopy. We prepared different types of SF materials, sponges, and fibers with different preparation methods and compared their NMR spectra in the dry and hydrated states. Three kinds of <sup>13</sup>C NMR techniques, r-INEPT, CP/MAS, and DD/MAS, coupled with <sup>13</sup>C isotope labeling of Ser, Tyr, and Ala residues were used. In the hydrated sponges, several conformations, that is, Silk I* and two kinds of Ī²-sheets, A and B, random coil, and highly mobile hydrated random coil were observed, and the fractions were determined. The fractions were remarkably different among the three sponges but with only small differences among the regenerated and native fibers. The increase in the fraction of Ī²-sheet B might be one of the structural factors for preparing stronger regenerated SF fiber

    Mixture of Rectangular and Staggered Packing Arrangements of Polyalanine Region in Spider Dragline Silk in Dry and Hydrated States As Revealed by <sup>13</sup>C NMR and Xā€‘ray Diffraction

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    For the first time, we determined the relative percentages of ā€œrectangularā€ and ā€œstaggeredā€ packing arrangements in the crystalline polyalanine regions with antiparallel Ī²-sheet structure within spider dragline silk fiber from <i>Nephila clavata</i> (NCF) and recombinant silk protein (RSP). The methods used included X-ray diffraction and <sup>13</sup>C NMR coupled with selective <sup>13</sup>C isotope labeling of the Ala CĪ² carbons. From deconvolution analyses of the Ala CĪ² peaks in the <sup>13</sup>C CP/MAS NMR spectra, the relative percentages of the rectangular arrangements in [3-<sup>13</sup>C]Ā­Ala-NCF were determined to be 49 Ā± 8% and 40 Ā± 7% in the dry and hydrated states, respectively, and in [3-<sup>13</sup>C]Ā­Ala-RSP 62 Ā± 11% and 81 Ā± 5% in the dry and hydrated states, respectively. Thus, the packing structure changed significantly between the two spider silks and also between the two physical states. The use of NMR was critical in this analysis; from X-ray diffraction patterns alone it would have been difficult to obtain these quantitative data

    NMR Investigation about Heterogeneous Structure and Dynamics of Recombinant Spider Silk in the Dry and Hydrated States

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    Spider silks continue to attract researchers because of their excellent mechanical properties and supercontraction behavior. In this paper, the structure and dynamics of recombinant spider silk protein (RSP) were characterized using <sup>13</sup>C CP/MAS, <sup>13</sup>C DD/MAS, and <sup>13</sup>C refocused-INEPT NMR spectroscopies in the dry and hydrated states. The fractions of several structures of RSP with helical, random coil, and Ī²-sheet polyalanine sequences were determined from the CP/MAS NMR spectra in the dry state. The CP/MAS NMR spectra changed to very simple one with dominant Ī²-sheet Ala peaks by hydration due to a significant loss in CP signals of the other mobile carbons. On the contrary, only sharp mobile peaks, and both mobile and immobile peaks could be observed in the refocused-INEPT and DD/MAS NMR spectra, respectively. The cis/trans proportion of the Glyā€“Pro bond was also determined. Our measurements provide new insight into understanding the supercontraction phenomenon of spider silks
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