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.     

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.     

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.     

Determination of the torsion angles of alanine and glycine residues of model compounds of spider silk (AGG)(10) using solid-state NMR methods

Spiders synthesize several kinds of silk fibers. In the primary structure of spider silk, one of the major ampullate (dragline, frame) silks, spidroin 1, and flagelliform silk (core fibers of adhesive spiral), there are common repeated X-Gly-Gly (X = Ala, Leu, Pro, Tyr, Glu, and Arg) sequences, which are considered to be related to the elastic character of these fibers. In this paper, two dimensional spin diffusion solid-state NMR under off magic angle spinning (OMAS), ¹³C chemical shift contour plots, and Rotational Echo DOuble Resonance (REDOR) were applied to determine the torsion angles of one Ala and two kinds of Gly residues in the Ala-Gly-Gly sequence of ¹³C=O isotope-labeled (Ala-Gly-Gly)₁₀. The torsion angles were determined to be (, ) = (–90°, 150° ) within an experimental error of ±10° for each residue. This conformation is characterized as 3₁ helix which is in agreement with the structure proposed from the X-ray powder diffraction pattern of poly(Ala-Gly-Gly). The 3₁ helix of (Ala-Gly-Gly)₁₀ does not change by formic acid treatment although (Ala-Gly)₁₅ easily changes from the silk I conformation (the structure of Bombyx mori silk fibroin before spinning in the solid state) to silk II conformation (the structure of the silk fiber after spinning) by such treatment. Thus, the 3₁ helix conformation of (Ala-Gly-Gly)₁₀ is considered very stable. Furthermore, the torsion angles of the 16th Leu residue of (Leu-Gly-Gly)₁₀ were also determined as (, ) = (–90°, 150° ) and this peptide is also considered to take 3₁ helix conformation.     

Structure of the model peptides of Bombyx mori silk-elastin like protein studied with solid state NMR

The peptides (AG)(6)(VPGVG)(AG)(7) and (AG)(5)(VPGVG)(2)(AG)(5) are models for a new type of protein with both composition and properties such as Bombyx mori silk and elastin. In this paper, we report the solid-state NMR results for these samples and related peptides; the structures after dialysis of the 9 M LiBr aqueous solution and after treatment with formic acid were determined and compared. The detailed structural analyses were performed using deconvolution subroutines assuming Gaussian line shapes for the Ala Cbeta peaks of the (AG)(n) sequences in these peptides. The peptide (AG)(6)(VPGVG)(AG)(7) took the silk II structure after the dialysis, which is in contrast to the silk I form of (AG)(15) after the same treatment. However, a drastic structural change of the (AG)(n) sequences was observed for (AG)(5)(VPGVG)(2)(AG)(5); the fraction of distorted beta-turn was 81% after the dialysis, but the distorted beta-sheet became dominant (84%) after treatment with formic acid. The local structures of the Gly residue of the VG units in the elastin-like subunits, (VPGVG) and (VPGVG)(2), were the distorted structures with a distribution of the torsion angles, which was derived from the 2D spin diffusion NMR spectral pattern of (AG)(5)VPG[1-(13)C]V[1-(13)C]GVPGVG(AG)(5). Observation of this distribution of the Gly residue was independent of the treatment, dialysis or formic acid.     

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.     

NMR analysis of the fibronectin cell-adhesive sequence, Arg-Gly-Asp, in a recombinant silk-like protein and a model peptide

It is well established that by introducing the cell-adhesive sequence Arg-Gly-Asp (RGD) from fibronectin into Bombyx mori silk fibroin by covalent coupling or bioengineering techniques, excellent biomaterials have been developed with the modified silk fibroin. However, there is no report about the structure and dynamics of the RGD moiety in the silk fibroin. To clarify the origin of such a high cell adhesion character and to design new recombinant silk protein with higher cell adhesion ability, it is necessary to characterize the structure and dynamics of the RGD moiety introduced into silk fibroin. In this study, the structure and dynamics of the RGD moiety in a recombinant silk-like protein, SLPF(10), consisting of the repeated silk fibroin sequence (AGSGAG)(3) and the sequence ASTGRGDSPA including the RGD moiety, were studied using solution NMR. The (1)H, (15)N, and (13)C chemical shifts indicate that the RGD moiety, as well as the silk fibroin sequence, takes a random coil form with high mobility in aqueous solution. Next, a (13)C solid-state NMR study was performed on a (13)C selectively labeled model peptide, AGSGAG[3-(13)C]A(7)GSGAGAGSGGT[2-(13)C]G(19)R[1-(13)C]G(21)DSPAGGGAGAGSGAG. After formic acid treatment, an increase in the β-sheet fraction for the AGSGAG sequence and peak narrowing of the residues around the RGD moiety were observed in the dry state. The latter indicates a decrease in the chemical shift distribution although the RGD moiety is still in random coil. A decrease in the peak intensities of the RGD moiety in the swollen state after immersing it in distilled water was observed, indicating high mobility of the RGD sequence in the peptide in the swollen state. Thus, the random coil state of the RGD moiety in the recombinant silk-like protein is maintained in aqueous solution and also in both dry and swollen state. This is similar to the case of the RGD moiety in fibronectin. The presence of the linker ASTG at the N-terminus and SPAGG at the C-terminus seems important to maintain the random coil form and the flexible state of the RGD sequence in order to permit access for binding to various integrins.     

Conformation transition in silk protein films monitored by time-resolved Fourier transform infrared spectroscopy: effect of potassium ions on Nephila spidroin films

We used time-resolved Fourier transform infrared spectroscopy (FTIR) to follow a conformation transition in Nephila spidroin film from random coil and/or helical structures to beta-sheet induced by the addition of KCl from 0.01 to 1.0 mol/L in D(2)O. Time series difference spectra showed parallel increases in absorption at 1620 and 1691 cm(-)(1), indicating formation of beta-sheet, together with a coincident loss of intensity of approximately 1650 cm(-)(1), indicating decrease of random coil and/or helical structures. Increase in KCl concentration produced an increased rate of the conformation transition that may attributable to weakening of hydrogen bonds within spidroin macromolecules. The conformation transition was a biphasic process with [KCl] > or = 0.3 mol/L but monophasic with [KCl] < or = 0.1 mol/L. This suggests that, at high KCl concentrations, segments of the molecular chain are adjusted first and then the whole molecule undergoes rearrangement. We discuss the possible significance of these findings to an understanding of the way that spiders spin silk.     

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.     

Vibrational 13C-cross-polarization/magic angle spinning NMR spectroscopic and thermal characterization of poly(alanine-glycine) as model for silk I Bombyx mori fibroin

This study focuses on the conformational characterization of poly(alanine-glycine) II (pAG II) as a model for a Bombyx mori fibroin silk I structure. Raman, IR, and 13C-cross-polarization/magic angle spinning NMR spectra of pAG II are discussed in comparison with those of the crystalline fraction of B. mori silk fibroin (chymotryptic precipitate, Cp) with a silk I (silk I-Cp) structure. The spectral data give evidence that silk I-Cp and the synthetic copolypeptide pAG II have similar conformations. Moreover, the spectral findings reveal that silk I-Cp is more crystalline than pAG II; consequently, the latter contains a larger amount of the random coil conformation. Differential scanning calorimetry measurements confirm this result. N-Deuteration experiments on pAG II allow us to attribute the Raman component at 1320 cm(-1) to the amide III mode of a beta-turn type II conformation, thus confirming the results of those who propose a repeated beta-turn type II structure for silk I. The analysis of the Raman spectra in the nuNH region confirms that the silk I structure is characterized by the presence of different types of H-bonding arrangements, in agreement with the above model.     

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.     

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.     

Effects of pH and calcium ions on the conformational transitions in silk fibroin using 2D Raman correlation spectroscopy and 13C solid-state NMR

Silk fibroin exists in a number of different states, such as silk I and silk II, with different properties largely defined by differences in secondary structure composition. Numerous attempts have been made to control the transitions from silk I to silk II in vitro to produce high-performance materials. Of all the factors influencing the structural compositions, pH and some metal ions play important roles. This paper focuses on the influence of pH and Ca(2+) ions on the conformational transition from silk I to silk II in regenerated (redissolved) Bombyx mori fibroin. One- and two-dimensional correlation Raman spectroscopy was used to describe qualitatively the transitions in secondary structure in silk I, silk II, and their intermediates as pH and Ca(2+) ion concentration were changed, while (13)C cross polarization magic angle spinning (CP/MAS) solid-state NMR was used to quantify these changes. We showed that conditions (low pH, pH 5.2; a defined range of Ca(2+) ion concentrations; gradual water removal) that mimic natural silk spinning promote the formations of beta-sheet and distorted beta-sheet characteristic of silk II or silk II-related intermediate. In contrast, higher pH (pH 6.9-8.0) and higher Ca(2+) ion concentrations maintain "random coil" conformations typical of silk I or silk I-related intermediate. These results help to explain why the natural silk spinning process is attended by a reduction in pH from 6.9 to 4.8 and a change in the Ca(2+) ion concentration in the gland lumen as fibroin passes from the posterior division through the secretory pathway to the anterior division.     

The structural properties of the transmembrane segment of the integral membrane protein phospholamban utilizing (13)C CPMAS, (2)H, and REDOR solid-state NMR spectroscopy

Solid-state NMR spectroscopic techniques were used to investigate the secondary structure of the transmembrane peptide phospholamban (TM-PLB), a sarcoplasmic Ca(2+) regulator. (13)C cross-polarization magic angle spinning spectra of (13)C carbonyl-labeled Leu39 of TM-PLB exhibited two peaks in a pure 1-palmitoyl-2-oleoyl-phosphocholine (POPC) bilayer, each due to a different structural conformation of phospholamban as characterized by the corresponding (13)C chemical shift. The addition of a negatively charged phospholipid (1-palmitoyl-2-oleoylphosphatidylglycerol (POPG)) to the POPC bilayer stabilized TM-PLB to an alpha-helical conformation as monitored by an enhancement of the alpha-helical carbonyl (13)C resonance in the corresponding NMR spectrum. (13)C-(15)N REDOR solid-state NMR spectroscopic experiments revealed the distance between the (13)C carbonyl carbon of Leu39 and the (15)N amide nitrogen of Leu42 to be 4.2+/-0.2A indicating an alpha-helical conformation of TM-PLB with a slight deviation from an ideal 3.6 amino acid per turn helix. Finally, the quadrupolar splittings of three (2)H labeled leucines (Leu28, Leu39, and Leu51) incorporated in mechanically aligned DOPE/DOPC bilayers yielded an 11 degrees +/-5 degrees tilt of TM-PLB with respect to the bilayer normal. In addition to elucidating valuable TM-PLB secondary structure information, the solid-state NMR spectroscopic data indicates that the type of phospholipids and the water content play a crucial role in the secondary structure and folding of TM-PLB in a phospholipid bilayer.     

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.     

Conformational transitions and fibrillation mechanism of human calcitonin as studied by high-resolution solid-state 13C NMR

Conformational transitions of human calcitonin (hCT) during fibril formation in the acidic and neutral conditions were investigated by high-resolution solid-state 13C NMR spectroscopy. In aqueous acetic acid solution (pH 3.3), a local alpha-helical form is present around Gly10 whereas a random coil form is dominant as viewed from Phe22, Ala26, and Ala31 in the monomer form on the basis of the 13C chemical shifts. On the other hand, a local beta-sheet form as viewed from Gly10 and Phe22, and both beta-sheet and random coil as viewed from Ala26 and Ala31 were detected in the fibril at pH 3.3. The results indicate that conformational transitions from alpha-helix to beta-sheet, and from random coil to beta-sheet forms occurred in the central and C-terminus regions, respectively, during the fibril formation. The increased 13C resonance intensities of fibrils after a certain delay time suggests that the fibrillation can be explained by a two-step reaction mechanism in which the first step is a homogeneous association to form a nucleus, and the second step is an autocatalytic heterogeneous fibrillation. In contrast to the fibril at pH 3.3, the fibril at pH 7.5 formed a local beta-sheet conformation at the central region and exhibited a random coil at the C-terminus region. Not only a hydrophobic interaction among the amphiphilic alpha-helices, but also an electrostatic interaction between charged side chains can play an important role for the fibril formation at pH 7.5 and 3.3 acting as electrostatically favorable and unfavorable interactions, respectively. These results suggest that hCT fibrils are formed by stacking antiparallel beta-sheets at pH 7.5 and a mixture of antiparallel and parallel beta-sheets at pH 3.3.     

The natural silk spinning process. A nucleation-dependent aggregation mechanism?

The spinning mechanism of natural silk has been an open issue. In this study, both the conformation transition from random coil to beta sheet and the beta sheet aggregation growth of silk fibroin are identified in the B. mori regenerated silk fibroin aqueous solution by circular dichroism (CD) spectroscopy. A nucleation-dependent aggregation mechanism, similar to that found in prion protein, amyloid beta (Abeta) protein, and alpha-synuclein protein with the conformation transition from a soluble protein to a neurotoxic, insoluble beta sheet containing aggregate, is a novel suggestion for the silk spinning process. We present evidence that two steps are involved in this mechanism: (a) nucleation, a rate-limiting step involving the conversion of the soluble random coil to insoluble beta sheet and subsequently a series of thermodynamically unfavorable association of beta sheet unit, i.e. the formation of a nucleus or seed; (b) once the nucleus forms, further growth of the beta sheet unit becomes thermodynamically favorable, resulting a rapid extension of beta sheet aggregation. The aggregation growth follows a first order kinetic process with respect to the random coil fibroin concentration. The increase of temperature accelerates the beta sheet aggregation growth if the beta sheet seed is introduced into the random coil fibroin solution. This work enhances our understanding of the natural silk spinning process in vivo.     

Conformational study of silklike peptides modified by the addition of the calcium-binding sequence from the shell nacreous matrix protein MSI60 using 13C CP/MAS NMR spectroscopy

The calcium-binding site of the pearl oyster (Pinctada fucata) nacreous layer matrix protein MSI60 was introduced between different Ala-Gly repeating regions derived from the primary sequences of several silk fibroins. Several different organic solvents whose effect on the repetitive domains of silk peptides is well-understood were used to modify the secondary structure of the flanking Ala-Gly repeating regions. The local conformations of the flanking Ala-Gly repeating regions as well as the calcium-binding motif, MSI60, were determined by 13C CP/MAS NMR spectroscopy. The secondary structures of the polyalanine, poly(Ala), domains were modified by the solvent treatments in a predictable fashion, suggesting that only the solvent treatment and not the conformation of the MSI60 domain affected the conformation of poly(Ala) regions. Ala-Gly domains behaved differently, taking random coil conformation regardless of the choice of solvent, indicating that their secondary structure is affected by the central MSI60 domain. The conformation of the MSI60 domain is not altered by the solvent treatments, suggesting that it may retain its ability to bind calcium ions. This was confirmed using a calcium-binding assay. The assay further showed that the calcium-binding capability of MSI60 in the synthetic peptides was most effective when the flanking domain was in the beta-sheet structure.     

The Alzheimer beta-peptide shows temperature-dependent transitions between left-handed 3-helix, beta-strand and random coil secondary structures

The temperature-induced structural transitions of the full length Alzheimer amyloid beta-peptide [A(beta)(1-40) peptide] and fragments of it were studied using CD and 1H NMR spectroscopy. The full length peptide undergoes an overall transition from a state with a prominent population of left-handed 3(1) (polyproline II; PII)-helix at 0 degrees C to a random coil state at 60 degrees C, with an average DeltaH of 6.8 +/- 1.4 kJ.mol(-1) per residue, obtained by fitting a Zimm-Bragg model to the CD data. The transition is noncooperative for the shortest N-terminal fragment A(beta)(1-9) and weakly cooperative for A(beta)(1-40) and the longer fragments. By analysing the temperature-dependent 3J(HNH(alpha)) couplings and hydrodynamic radii obtained by NMR for A(beta)(1-9) and A(beta)(12-28), we found that the structure transition includes more than two states. The N-terminal hydrophilic A(beta)(1-9) populates PII-like conformations at 0 degrees C, then when the temperature increases, conformations with dihedral angles moving towards beta-strand at 20 degrees C, and approaches random coil at 60 degrees C. The residues in the central hydrophobic (18-28) segment show varying behaviour, but there is a significant contribution of beta-strand-like conformations at all temperatures below 20 degrees C. The C-terminal (29-40) segment was not studied by NMR, but from CD difference spectra we concluded that it is mainly in a random coil conformation at all studied temperatures. These results on structural preferences and transitions of the segments in the monomeric form of A(beta) may be related to the processes leading to the aggregation and formation of fibrils in the Alzheimer plaques.     

Structural analysis of silk with 13C NMR chemical shift contour plots.

The polymorphic structures of silk fibroins in the solid state were examined on the basis of a quantitative relationship between the 13C chemical shift and local structure in proteins. To determine this relationship, 13C chemical shift contour plots for C alpha and C beta carbons of Ala and Ser residues, and the C alpha chemical shift plot for Gly residues were prepared using atomic co-ordinates from the Protein Data Bank and 13C NMR chemical shift data in aqueous solution reported for 40 proteins. The 13C CP/MAS NMR chemical shifts of Ala, Ser and Gly residues of Bombyx mori silk fibroin in silk I and silk II forms were used along with 13C CP/MAS NMR chemical shifts of Ala residues of Samia cynthia ricini silk fibroin in beta-sheet and alpha-helix forms for the structure analyses of silk fibroins. The allowed regions in the 13C chemical shift contour plots for C alpha and C beta carbons of Ala and Ser residues for the structures in silk fibroins, i.e. Silk II, Silk I and alpha-helix, were determined using their 13C isotropic NMR chemical shifts in the solid state. There are two area of the phi,psi map which satisfy the observed Silk I chemical shift data for both the C alpha and C beta carbons of Ala and Ser residues in the 13C chemical shift contour plots.