NMR study of silk I structure of Bombyx mori silk fibroin with 15N- and 13C-NMR chemical shift contour plots

The metastable state silk I structures of Bombyx mori silk fibroin in the solid state were studied on the basis of ¹⁵N- and ¹³C-nmr chemical shifts of Ala, Ser, and Gly residues. The ¹⁵N cross-polarization magic angle spinning (CP/MAS) nmr spectra of the precipitated fraction after chymotrypsin hydrolysis of B. mori silk fibroin with the silk I and silk II forms were measured to determine the ¹⁵N chemical shifts of Gly, Ala, and Ser residues. For comparison, ¹⁵N CP/MAS nmr chemical shifts of Ala were measured for [¹⁵N] Ala Philosamia cynthia ricini silk fibroin with antiparallel β-sheet and α-helix forms. The ¹³C CP/MAS nmr chemical shifts of Ala, Ser, and Gly residues of B. mori silk fibroin with the silk I and silk II forms, as well as ¹³C CP/MAS nmr chemical shifts of Ala residue of P. c. ricini silk fibroin with β-sheet and α-helix forms, are used for the examination of the silk I structure. Both silk I and α-helix peaks are shifted to a lower field than silk II (β-sheet) for the Cα carbons of the Ala residues, while both Cβ carbon peaks are shifted to higher field. However, the silk I peak of the ¹⁵N nucleus of the Ala residue is shifted to lower field than the silk II peak, but the α-helix peak is shifted to high field. Thus, the difference in the structure between the silk I and α-helix is reflected in a different manner between the ¹³C and ¹⁵N chemical shifts. The Cα and Cβ chemical shift contour plots for Ala and Ser residues, and the Cα plot for the Gly residue, were prepared from the Protein Data Bank data obtained for 12 proteins and used for discussing the silk I structure quantitatively from the conformation-dependent chemical shifts. The plots reported by Le and Oldfield for ¹⁵N chemical shifts were also used for the purpose. All these chemical shift data support Fossey's model (Ala: ϕ = −80°, φ = 150°, Gly: ϕ = −150°, φ = 80°) and do not support Lotz and Keith's model (Ala: ϕ = −104.6°, φ = 112.2°, Gly: ϕ = 79.8°, φ = 49.7° or Ala: ϕ = −124.5°, φ = 88.2°, Gly: ϕ = −49.8°, φ = −76.1°) as the silk I structure. © 1997 John Wiley & Sons, Inc.     

Comparative structure analysis of tyrosine and valine residues in unprocessed silk fibroin (silk I) and in the processed silk fiber (silk II) from Bombyx mori using solid-state (13)C,(15)N, and (2)H NMR

The solid-state (13)C CP-MAS NMR spectra of biosynthetically labeled [(13)C(alpha)]Tyr, [(13)C(beta)]Tyr, and [(13)C(alpha)]Val silk fibroin samples of Bombyx mori, in silk I (the solid-state structure before spinning) and silk II (the solid-state structure after spinning) forms, have been examined to gain insight into the conformational preferences of the semicrystalline regions. To establish the relationship between the primary structure of B. mori silk fibroin and the "local" structure, the conformation-dependent (13)C chemical shift contour plots for Tyr C(alpha), Tyr C(beta), and Val C(alpha) carbons were generated from the atomic coordinates of high-resolution crystal structures of 40 proteins and their characteristic (13)C isotropic NMR chemical shifts. From comparison of the observed Tyr C(alpha) and Tyr C(beta) chemical shifts with those predicted by the contour plots, there is strong evidence in favor of an antiparallel beta-sheet structure of the Tyr residues in the silk fibroin fibers. On the other hand, Tyr residues take a random coil conformation in the fibroin film with a silk I form. The Val residues are likely to assume a structure similar to those of Tyr residues in silk fiber and film. Solid-state (2)H NMR measurements of [3,3-(2)H(2)]Tyr-labeled B. mori silk fibroin indicate that the local mobility of the backbone and the C(alpha)-C(beta) bond is essentially "static" in both silk I and silk II forms. The orientation-dependent (i.e., parallel and perpendicular to the magnetic field) solid-state (15)N NMR spectra of biosynthetically labeled [(15)N]Tyr and [(15)N]Val silk fibers reveal the presence of highly oriented semicrystalline regions.     

Possible implications of serine and tyrosine residues and intermolecular interactions on the appearance of silk I structure of Bombyx mori silk fibroin-derived synthetic peptides: high-resolution 13C cross-polarization/magic-angle spinning NMR study

Bombyx mori silk fibroin molecule is known to exist in two distinct structural forms: silk I (unprocessed silk fibroin) and silk II (processed silk fibroin). Using synthetic peptides, we attempt to explore the structural role played by Ser and Tyr residues on the appearance of silk I structural form of the fibroin. Twelve selected peptides (1-12) incorporating Ser and Tyr residues in the (Ala-Gly)(n) copolypeptide, that is, the sequences mimicking the primary structure of B. mori silk fibroin molecule, have been investigated under the silk I state, employing high-resolution (13)C cross-polarization/magic-angle spinning (CP/MAS) NMR spectroscopy. To acquire the silk I structural form, all the peptides were dissolved in 9 M LiBr and then dialyzed extensively against water, as established previously for the synthetic (Ala-Gly)(15) copolypeptide and B. mori silk fibroin. The diagnostic line shape of the Ala C(beta) peaks and the conformation-dependent (13)C chemical shifts of Ala and Gly resonances are presented to analyze and characterize the structural features. The results indicate that the incorporation of one Ser and/or one Tyr residue(s) at selected position in the basic (Ala-Gly)(15) sequence tend to retain predominantly the silk I structure. Conversely, the repeat pentameric and octameric Ala-Gly-Ser-Gly-Ala-Gly sequences, for example, (Ala-Gly-Ser-Gly-Ala-Gly)(5) or (Ala-Gly-Ser-Gly-Ala-Gly)(8), preferred predominantly the silk II form. The peptide sequences incorporating Ser and Tyr residue(s) into repeat Ala-Gly-Ser-Gly-Ala-Gly sequences, however, adopted the silk II structure with certain content structural heterogeneity or randomness, more pronounced for specific peptides studied. Interestingly, the crystalline Cp fraction of B. mori silk fibroin, when mixed with (Ala-Gly-Ser-Gly-Ala-Gly)(5) sequence in a 5:1 molar ratio, dissolved in 9 M LiBr, and dialyzed against distilled water, favor the silk I form. The finding tends to suggest that the less stable silk I form in (Ala-Gly-Ser-Gly-Ala-Gly)(n) sequences is likely to be induced and facilitated via intermolecular interactions with the Cp fraction, which predominantly prefers the silk I form under similar conditions; however, the hydrogen-bond formation involving O(gamma)H groups of the Ser residues may have some implications.     

Design, expression and solid-state NMR characterization of silk-like materials constructed from sequences of spider silk, Samia cynthia ricini and Bombyx mori silk fibroins

Silk has a long history of use in medicine as sutures. To address the requirements of a mechanically robust and biocompatible material, basic research to clarify the role of repeated sequences in silk fibroin in its structures and properties seems important as well as the development of a processing technique suitable for the preparation of fibers with excellent mechanical properties. In this study, three silk-like protein analogs were constructed from two regions selected from among the crystalline region of Bombyx mori silk fibroin, (GAGSGA)(2), the crystalline region of Samia cynthia ricini silk fibroin, (Ala)(12), the crystalline region of spider dragline silk fibroin, (Ala)(6), and the Gly-rich region of spider silk fibroin, (GGA)(4). The silk-like protein analog constructed from the crystalline regions of the spider dragline silk and B. mori silk fibroins, (A(6)SCS)(8), that constructed from the crystalline regions of the S. c.ricini and B. mori silk fibroins, (A(12)SGS)(4), that constructed from and the crystalline region of S. c.ricini silk fibroin and the glycine-rich region of spider dragline silk fibroin, (A(12)SGS)(4),were expressed their molecular weights being about 36.0 kDa, 17.0 kDa and 17.5 kDa, respectively in E. coli by means of genetic engineering technologies. (A(12)SCS)(4) and (A(12)SGS)(4 )undergo a structural transition from alpha-helix to beta-sheet on a change in the solvent treatment from trifluoroacetic acid (TFA) to formic acid (FA). However, (A(6)SCS)(8) takes on the beta-sheet structure predominantly on TFA treatment and FA treatment. Structural analysis was performed on model peptides selected from spider dragline and S. c.ricini silks by means of (13)C CP/MAS NMR.     

13C CP/MAS NMR study on structural heterogeneity in Bombyx mori silk fiber and their generation by stretching

It is important to resolve the structure of Bombyx mori silk fibroin before spinning (silk I) and after spinning (silk II), and the mechanism of the structural transition during fiber formation in developing new silk-like fiber. The silk I structure has been recently resolved by (13)C solid-state NMR as a "repeated beta-turn type II structure." Here, we used (13)C solid-state NMR to clarify the heterogeneous structure of the natural fiber from Bombyx mori silk fibroin in the silk II form. Interestingly, the (13)C CP/MAS NMR revealed a broad and asymmetric peak for the Ala Cbeta carbon. The relative proportions of the various heterogeneous components were determined from their relative peak intensities after line shape deconvolution. Namely, for 56% crystalline fraction (mainly repeated Ala-Gly-Ser-Gly-Ala-Gly sequences), 18% distorted beta-turn, 13% beta-sheet (parallel Ala residues), and 25% beta-sheet (alternating Ala residues). The remaining fraction of 44% amorphous Tyr-rich region, 22% in both distorted beta-turn and distorted beta-sheet. Such a heterogeneous structure including distorted beta-turn can be observed for the peptides (AG)(n) (n > 9 ). The structural change from silk I to silk II occurs exclusively for the sequence (Ala-Gly-Ser-Gly-Ala-Gly)(n) in B. mori silk fibroin. The generation of the heterogeneous structure can be studied by change in the Ala Cbeta peak of (13)C CP/MAS NMR spectra of the silk fibroin samples with different stretching ratios.     

Tightly winding structure of sequential model peptide for repeated helical region in Samia cynthia ricini silk fibroin studied with solid-state NMR

There are many kinds of silks from silkworms and spiders with different structures and properties, and thus, silks are suitable to study the structure-property relationship of fibrous proteins. Silk fibroin from a wild silkworm, Samia cynthia ricini, mainly consists of the repeated similar sequences by about 100 times where there are alternative appearances of the polyalanine (Ala)(12-13) region and the Gly-rich region. In this paper, a sequential model peptide, GGAGGGYGGDGG(A)(12)GGAGDGYGAG, which is a typical sequence of the silk fibroin, was synthesized, and the atomic-level conformations of Gly residues at the N- and C-terminal ends of the polyalanine region were determined as well as that of the central Ala residue using (13)C 2D spin diffusion solid-state nuclear magnetic resonance (NMR) under off-magic angle spinning. In the model peptide with alpha-helical conformation, the torsion angle of the central Ala residue, the 19th Ala, was determined to be (phi, psi) = (-60 degrees, -50 degrees ), which was a typical alpha-helical structure, but the torsion angles of two Gly residues, the 12th and 25th Gly residues, which are located at the N- and C-terminal ends of the polyalanine region, were determined to be (phi, psi) = (-70 degrees, -30 degrees ) and (phi, psi) = (-70 degrees, -20 degrees ), respectively. Thus, it was observed that the turns at both ends of polyalanine with alpha-helix conformation in the model peptide are tightly wound.     

Position dependence of the 13C chemical shifts of alpha-helical model peptides. Fingerprint of the 20 naturally occurring amino acids

The position dependence of the (13)C chemical shifts was investigated at the density functional level for alpha-helical model peptides represented by the sequence Ac-(Ala)(i)-X-(Ala)(j)-NH(2), where X represents any of the 20 naturally occurring amino acids, with 0 < or = i < or = 8 and i + j = 8. Adoption of the locally dense basis approach for the quantum chemical calculations enabled us to reduce the length of the chemical-shift calculations while maintaining good accuracy of the results. For the 20 naturally occurring amino acids in alpha-helices, there is (1) significant variability of the computed (13)C shielding as a function of both the guest residue (X) and the position along the sequence; for example, at the N terminus, the (13)C(alpha) and (13)C(beta) shieldings exhibit a uniform pattern of variation with respect to both the central or the C-terminal positions; (2) good agreement between computed and observed (13)C(alpha) and (13)C(beta) chemical shifts in the interior of the helix, with correlation coefficients of 0.98 and 0.99, respectively; for (13)C(alpha) chemical shifts, computed in the middle of the helix, only five residues, namely Asn, Asp, Ser, Thr, and Leu, exhibit chemical shifts beyond the observed standard deviation; and (3) better agreement for four of these residues (Asn, Asp, Ser, and Thr) only for the computed values of the (13)C(alpha) chemical shifts at the N terminus. The results indicate that (13)C(beta), but not (13)C(beta), chemical shifts are sensitive enough to reflect the propensities of some amino acids for specific positions within an alpha-helix, relative to the N and C termini of peptides and proteins.     

Distinctive influence of two hexafluoro solvents on the structural stabilization of Bombyx mori silk fibroin protein and its derived peptides: 13C NMR and CD studies

Employing high-resolution (13)C solution NMR and circular dichroism (CD) spectroscopic techniques, the distinctive influence of two intimately related hexafluoro solvents, 1,1,1,3,3,3-hexafluoro-2-propanol (HFIP) and hexafluoroacetone trihydrate (HFA), on the structural characteristics of Bombyx mori (B. mori) silk fibroin, the chymotrypsin precipitate (C(p)) fraction, and two synthetic peptides, (AGSGAG)(5) and (AG)(15), is described. The observed (13)C solution NMR and CD spectra of these polypeptides in HFIP and HFA revealed a distinctive influence on their conformational characteristics. The (13)C NMR spectra, as analyzed from the unique chemical shifts of C(alpha) and C(beta) resonances of constituent residues revealed that fibroin largely assumes helical conformation(s) in both solvents. However, the peak shifts were greater for the samples in HFIP, indicating that the types of helical structure(s) may be different from the one populated in HFA. Similar structural tendencies of these polypeptides were reflected in CD spectra. The observed CD patterns, i.e., a strong positive band at approximately 190 nm and negative bands at approximately 206 and 222 nm, have been attributed to the preponderance of helical structures. Of the two prevalent helical structures, alpha-helix and 3(10)-helix, the evidence emerged for the fibroin protein in favor of 3(10)-helical structure stabilization in HFIP and its significant disruption in HFA, as deduced from the characteristic R1 (=[theta](190)/[theta](202)) and R2 (=[theta](222)/[theta](206)) ratios, determined from the CD data. Conversely, the native polypeptides and synthetic peptide fragments derived from highly crystalline regions of the silk fibroin protein sustained predominantly an unordered structure in HFA solvent.     

Solid-state NMR investigation of major and minor ampullate spider silk in the native and hydrated states

Silks spun from the major (Ma) and minor (Mi) ampullate glands by the spider Nephila clavipes respond to water differently. Specifically, Ma silk supercontracts (shrinks 40-50% in length) while Mi silk does not contract at all when hydrated with water. In the present study, 1H --> 13C cross polarization magic angle spinning (CP-MAS), 13C MAS NMR collected with dipolar decoupling, and two-dimensional wide-line separation spectra are presented on Mi silk in its native and hydrated state and comparisons are made to Ma silk. This combination of NMR data demonstrates that water plasticizes Mi and Ma silk similarly, with an increase in chain dynamics observed in regions containing Gly, Glu, Ser, Tyr, Leu, and a fraction of Ala when the Mi silk is hydrated. Resonances that correspond to the poly(Ala) and poly(Gly Ala) motifs of Ma and Mi silk are predominately rigid indicating that water does not penetrate these beta-sheet domains.     

A high-resolution 13C-nmr study of collagenlike polypeptides and collagen fibrils in solid state studied by the cross-polarization–magic angle-spinning method. Manifestation of conformation-dependent 13C chemical shifts and application to conformational characterization

We have recorded high-resolution ¹³C-nmr spectra of collagen fibrils in the solid state by the cross-polarization–magic-angle-spinning(CP–MAS)method and analyzed the spectra with reference to those of collagenlike polypeptides. We used two kinds of model polypeptides to obtain reference ¹³C chemical shifts of major amino acid residues of collagen (Gly, Pro, Ala, and Hyp): the 3₁-helical polypeptides [(Gly)_nII, (Pro)_nII, (Hyp)_n, and (Ala? Gly? Gly)_nII], and the triple-helical polypeptides [(Pro? Gly? Pro)_n and (Pro? Ala? Gly)_n]. Examination of the ¹³C chemical shifts of these polypeptides, together with our previous data, showed that the ¹³C chemical shifts of individual amino acid residues are the same, within experimental error (±0.5 ppm), among different polypeptides with different primary sequences, if the conformations are the same. We found that the ¹³C chemical shifts of Ala residues of the 3₁-helical (Ala? Gly? Gly)_n and triple-helical (Pro? Ala? Gly)_n are significantly displaced, compared with those of the α-helix, β-sheet, and silk I form, and can be utilized as excellent probes to examine conformational features of collagen-like polypeptides. Further, the ¹³C chemical shifts of Gly and Pro residues in the triple-helical polypeptides are substantially displaced from those found in (Gly)_nII and (Pro)_nII of the 3₁-helix, reflecting further conformational change from the 3₁-helix to the supercoiled triple helix. In particular, the ¹³C chemical shifts of Gly C ? O carbons of the triple-helical polypeptides are substantially displaced upfield (4.1–5.1 ppm), with respect to those of the 3₁-helical polypeptides. These displacements are interpreted by that Gly C ? O of the former is not involved in NH …? O ? C hydrogen bonds, while this carbon of the latter is linked by these kinds of hydrogen bonds. On the basis of these ¹³C chemical shifts, as reference data for the collagenlike structure, we were able to assign the ¹³C-nmr peaks of Gly, Ala, Pro, and Hyp residues of collagen fibrils, which are in good agreement with the values expected from the model polypeptides mentioned above. We also discuss a plausible conformational change of collagen fibrils during denaturation.     

Structure and dynamics of the HIV-1 Vpu transmembrane domain revealed by solid-state NMR with magic-angle spinning

We report solid-state nuclear magnetic resonance (NMR) measurements on the peptide Vpu(1-40), comprising residues 1-40 of the 81-residue type 1 integral membrane protein Vpu encoded by the HIV-1 genome. On the basis of a combination of 13C and 15N NMR chemical shifts under magic-angle spinning (MAS), effects of local mobility on NMR signal intensities, site-specific MAS NMR line widths, and NMR-detected hydrogen-deuterium exchange, we develop a model for the structure and dynamics of the Vpu(1-40) monomer in phospholipid bilayer membranes. Our data are largely consistent with earlier structural studies of Vpu peptides by Opella and co-workers, in which solution NMR and solid-state NMR without MAS were used, but our data provide new information about local variations in the degree of mobility and structural order. In addition, our data indicate that the transmembrane alpha-helix of Vpu(1-40) extends beyond the hydrophobic core of the bilayer. We find no evidence for heterogeneity in the conformation and intermolecular contacts of the transmembrane alpha-helix, with the exception of two distinct chemical shifts observed for the C alpha and C beta atoms of A18 that may reflect distinct modes of helix-helix interaction. These results have possible implications for the supramolecular structure of Vpu oligomers that form cation-selective ion channels.     

Heterogeneous exchange behavior of Samia cynthia ricini silk fibroin during helix-coil transition studied with (13)C NMR

The structure and structural transition of the glycine residue adjacent to the N-terminal alanine residue of the poly(L-alanine), (Ala)(12-13), region in Samia cynthia ricini silk fibroin was studied using (13)C nuclear magnetic resonance (NMR). Most of the glycine carbonyl peaks in the (13)C solution NMR spectrum of [1-(13)C]glycine-silk fibroin could be assigned to the primary structure from the comparison of the (13)C chemical shifts of seven glycine-containing tripeptides. The slow exchange between helix and coil forms in the NMR time scale was observed with increasing temperature exclusively for the underlined glycine residue in the Gly-Gly-(Ala)(12-13) sequence during fast helix-coil transition of the (Ala)(12-13) region.     

Structures of Bombyx mori and Samia cynthia ricini silk fibroins studied with solid-state NMR

There are many kinds of silks spun by silkworms and spiders, which are suitable to study the structure-property relationship for molecular design of fibers with high strength and high elasticity. In this review, we mainly focus on the structural determination of two well-known silk fibroin proteins that are from the domesticated silkworm, Bombyx mori, and the wild silkworm, Samia cynthia ricini, respectively. The structures of B. mori silk fibroin before and after spinning were determined by using an appropriate model peptide, (AG)(15), with several solid-state NMR methods; (13)C two-dimensional spin-diffusion solid-state NMR and rotational echo double resonance (REDOR) NMR techniques along with the quantitative use of the conformation-dependent (13)C CP/MAS chemical shifts. The structure of S. c. ricini silk fibroin before spinning was also determined by using a model peptide, GGAGGGYGGDGG(A)(12)GGAGDGYGAG, which is a typical repeated sequence of the silk fibroin, with the solid-state NMR methods. The transition from the structure of B. mori silk fibroin before spinning to the structure after spinning was studied with molecular dynamics calculation by taking into account several external forces applied to the silk fibroin in the silkworm.     

Structure of model peptides based on Nephila clavipes dragline silk spidroin (MaSp1) studied by 13C cross polarization/magic angle spinning NMR

To obtain detailed structural information for spider dragline spidroin (MaSp1), we prepared three versions of the consensus peptide GGLGGQGAGAAAAAAGGAGQGGYGGLGSQGAGR labeled with 13C at six different sites. The 13C CP/MAS NMR spectra were observed after treating the peptides with different reagents known to alter silk protein conformations. The conformation-dependent 13C NMR chemical shifts and peak deconvolution were used to determine the local structure and the fractional compositions of the conformations, respectively. After trifluoroacetic acid (solvent)/diethyl ether (coagulant) treatment, the N-terminal region of poly-Ala (PLA) sequence, Ala8 and Ala10, adopted predominantly the alpha-helix with a substantial amount of beta-sheet. The central region, Ala15, Ala18, and Leu26, and C-terminal region, Ala31, of the peptide were dominated by either 3(1)-helix or alpha-helix. There was no indication of beta-sheet, although peak broadening indicates that the torsion angle distribution is relatively large. After 9 M LiBr/dialysis treatment, three kinds of conformation, beta-sheet, random coil, and 3(1)-helix, appeared, in almost equal amounts of beta-sheet and random coil conformations for Ala8 and Ala10 residues and distorted 3(1)-helix at the central region of the peptide. In contrast, after formic acid/methanol and 8 M urea/acetonitrile treatments, all of the local structure tends to beta-sheet, although small amounts of random coil are also observed. The peak pattern of the Ala Cbeta carbon after 8 M urea/acetonitrile treatment is similar to the corresponding patterns of silk fiber from Bombyx mori and Samia cynthia ricini. We also synthesized a longer 13C-labeled peptide containing two PLA blocks and three Gly-rich blocks. After 8 M urea/acetonitrile treatment, the conformation pattern was closely similar to that of the shorter peptide.     

Use of 13C conformation-dependent chemical shifts to elucidate the local structure of a large protein with homologous domains in solution and solid state

In order to clarify the difference between solution NMR and X-ray diffraction analyses concerning the presence of alpha-helical structure in protein A, the 13C conformation-dependent chemical shifts of the 13C-labeled carbonyl carbons for selectively labeled protein A were used. In the 13C CP/MAS NMR spectra, the higher-field shifts of the carbonyl carbons of 13C-labeled Thr and Val residues compared with the random coil chemical shifts both in solution and solid state imply the presence of the third helix in the polypeptide chain, in contrast to the crystal structure of Fc-bound B-domain. Thus, a combination of selective isotope labeling and conformation-dependent chemical shifts will be a good Indicator to monitor the local structure of homologous protein in solution and solid state.     

Structure of Bombyx mori silk fibroin before spinning in solid state studied with wide angle x-ray scattering and (13)C cross-polarization/magic angle spinning NMR

The structure of a crystalline form of Bombyx mori silk fibroin, commonly found before the spinning process (known as silk I), has been proposed as a repeated beta-turn type II-like structure by combining data obtained from solid-state two dimensional spin-diffusion nuclear magnetic resonance and rotational-echo double-resonance (T. Asakura et al., J Mol Biol, in press). In this paper, the WAXS pattern of alanine-glycine alternating copolypeptide, (Ala-Gly)(15) with silk I form which was used for a silk I model of B. mori silk fibroin was observed. The pattern calculated with the silk I model proposed by us is well reproduced the observed one, indicating the validity of the proposed silk I model. In addition, two peptides of the other repeated sequences which contain Tyr or Val residues in the silk fibroin,23 were synthesized; (Ala-Gly-Tyr-Gly-Ala-Gly)(5) and (X-Gly)(15) where X is Tyr for the 7th, 15th and 23th residues, and Val for the 11th residue and Ala for other residues. There are no sharp peaks in the WAXS patterns, and therefore both samples are in the non-crystalline state. This is in agreement with the (13)C CP/MAS NMR result, where the conformation is mainly random coil.     

Synthesis and characterization of chimeric silkworm silk

A synthetic gene encoding a chimeric silklike protein was constructed that combined a polyalanine encoding region (Ala)(18), a sequence slightly longer than the (Ala)(12-13) found in the silk fibroin from the wild silkworm Samia cynthia ricini, and a sequence encoding GVGAGYGAGAGYGVGAGYGAGVGYGAGAGY, found in the silk fibroin from the silkworm Bombyx mori. A tetramer of the chimeric repeat sequence encoding a approximately 29 kDa protein was expressed as a fusion protein in Escherichia coli. In comparison to S. c. ricini silk, the chimeric protein demonstrated improved solubility because it could be dissolved in 8 M urea. The purified protein assumed an alpha-helical structure based on solid-state (13)C CP/MAS NMR and was less prone to conformational transition to a beta-sheet, unlike native silk proteins from S. c. ricini. Model peptides representing the crystalline region of S. c. ricini silk fibroin, (Ala)(12) and (Ala)(18), formed beta-sheet structures. Therefore, the solubility and structural transitions of the chimeric protein were significantly altered through the formation of this chimeric silk. This experimental strategy to the study of silk structure and function can be used to develop an improved understanding of the contributions of protein domains in repetitive silkworm and spider silk sequences to structure development and structural transitions.     

酪氨酸酶催化氧化对丝素蛋白结构与性能的影响

采用酪氨酸酶对丝素蛋白催化氧化,考察了酶促氧化反应对丝素蛋白结构及丝素膜性能的影响。研究结果表明,酪氨酸酶可催化氧化丝素蛋白中酪氨酸残基生成多巴和多巴醌结构衍生物,并且两者含量随催化反应时间延长呈波动性变化;酶促反应后丝素蛋白中游离氨基含量下降,丝素风干膜断裂强度增加,表明酶促氧化中丝素大分子间发生自交联。XRD结果表明酪氨酸酶催化氧化对丝素蛋白二级结构有一定影响;SEM显示酶促改性可能影响丝素蛋白冷冻干燥膜多孔形态结构。     

The role of irregular unit,GAAS, on the secondary structure of Bombyx mori silk fibroin studied with 13C CP/MAS NMR and wide-angle X-ray scattering

Bombyx mori silk fibroin is a fibrous protein whose fiber is extremely strong and tough, although it is produced by the silkworm at room temperature and from an aqueous solution. The primary structure is mainly Ala-Gly alternative copolypeptide, but Gly-Ala-Ala-Ser units appear frequently and periodically. Thus, this study aims at elucidating the role of such Gly-Ala-Ala-Ser units on the secondary structure. The sequential model peptides containing Gly-Ala-Ala-Ser units selected from the primary structure of B. mori silk fibroin were synthesized, and their secondary structure was studied with (13)C CP/MAS NMR and wide-angle X-ray scattering. The (13)C isotope labeling of the peptides and the (13)C conformation-dependent chemical shifts were used for the purpose. The Ala-Ala units take antiparallel beta-sheet structure locally, and the introduction of one Ala-Ala unit in (Ala-Gly)(15) chain promotes dramatical structural changes from silk I (repeated beta-turn type II structure) to silk II (antiparallel beta-sheet structure). Thus, the presence of Ala-Ala units in B. mori silk fibroin chain will be one of the inducing factors of the structural transition for silk fiber formation. The role of Tyr residue in the peptide chain was also studied and clarified to induce "locally nonordered structure."     

13C NMR of Nephila clavipes major ampullate silk gland.

The major ampullate glands of the spider Nephila clavipes contain approximately 0.2 microliter each of a highly concentrated (approximately 50%) solution of silk fibroin. Therefore, the reservoir of silk in these glands presents an ideal opportunity to observe prefolded conformations of a protein in its native state. To this end, the structure and conformation of major ampullate gland silk fibroin within the glands of the spider N. clavipes were examined by 13C NMR spectroscopy. These results were compared to those from silk protein first drawn from the spinneret and then denatured. The 13C NMR chemical shifts, along with infrared and circular dichroism data, suggest that the silk fibroin in the glands exists in dynamically averaged helical conformations. Furthermore, there is no evidence of proline residues in U-(13)C-D-glucose-labeled silk. This transient prefolded "molten fibril" state may correspond to the silk I form found in Bombyx mori silk. There is no evidence of the final beta-sheet structure in the ampullate gland silk fibroin before final silk processing. However, the conformation of silk in the glands appears to be in a highly metastable state, as plasticization with water produces the beta-sheet structure. Therefore, the ducts connecting the ampullate glands to the spinnerets play a larger role in silk processing than previously thought.