Morphology and primary crystal structure of a silk-like protein polymer synthesized by genetically engineered Escherichia coli bacteria

The morphology and primary crystal structure of SLPF, a protein polymer produced by genetically engineered Escherichia coli bacteria, were characterized. SLPF is a segmented copolymer consisting of amino acid sequence blocks modeled on the crystalline segments of silk fibroin and the cell attachment domain of human fibronectin. Wide angle x-ray scattering (WAXS), transmission electron microscopy (TEM), selected area electron diffraction (SAED), and molecular simulations were used to analyze the primary crystal structure of SLPF. TEM experiments conducted on SLPF droplets cast from formic acid on amorphous carbon film demonstrated that these protein films have a microstructure formed of woven sheaves. The sheaves are composed of well-defined whisker crystallites. The width of the whiskers, 11.8 ± 2.2 nm, may be correlated to the length of the silk-like segment in SLPF as predicted by molecular simulations. WAXS data, TEM images, SAED, patterns, molecular simulations, and theoretical diffraction patterns all were consistent with the crankshaft model proposed for Silk I by Lotz and Keith. © 1994 John Wiley & Sons, Inc.     

The crystal structure of Bombyx mori silk fibroin at the air–water interface

A new crystalline polymorph of Bombyx mori silk, which forms at the air–water interface, has been characterized. A previous study found this structure to be trigonal, and to be distinctly different than the two previously observed silk crystal structures, silk I and silk II. This new structure was named silk III. Identification of this new silk polymorph was based on evidence from transmission electron microscopy and electron diffraction, coupled with molecular modeling. In the current paper, additional data enables us to refine our model of the silk III structure. Some single crystal electron diffraction patterns indicate a deviation in symmetry away from a perfect trigonal unit cell to monoclinic unit cell. The detailed shape of the powder diffraction peaks also supports a monoclinic cell. The monoclinic crystal structure has an nonprimitive unit cell incorporating a slightly distorted hexagonal packing of silk molecular helices. The chains each assume a threefold helical conformation, resulting in a crystal structure similar to that observed for polyglycine II, but with some additional sheet-like packing features common to the threefold helical crystalline forms of many glycine-rich polypeptides. © 1997 John Wiley & Sons, Inc. Biopoly 42: 705–717, 1997     

Conformational energy studies of beta-sheets of model silk fibroin peptides. I. Sheets of poly(Ala-Gly) chains

A new model structure is proposed for the silk I form of the crystalline domains of Bombyx mori silk fibroin and the corresponding crystal form of poly(L-Ala-Gly). It was deduced from conformational energy computations on stacked sheet structures of poly(L-Ala-Gly). The novel sheet structure contains interstrand hydrogen bonds but is composed of anti-parallel polypeptide chains whose conformation differs from that of the antiparallel beta-sheets that constitute the silk II structure. The strands of the new sheet have a two-residue repeat, in which the Ala residues adopt a right-handed and the Gly residues a left-handed sheet-like conformation. The computed unit cell is orthorhombic, with cell dimensions a = 8.94 A, b = 6.46 A, and c = 11.26 A. The model accounts for most spacings in the observed fiber x-ray diffraction patterns of silk I and of the silk-I-like form of poly(L-Ala-Gly), and it is consistent with nmr and ir spectroscopic data. As a test of the computations, the well-established beta-sheet structure of silk II and the corresponding form of poly(L-Ala-Gly) have been reproduced. The computed energies for the two forms of poly(L-Ala-Gly) indicate that the silk-II-like form is more stable, by about 1.0 kcal/mol per residue. The main difference between the two structures is the orientation of the Ala side chains of neighboring strands in each sheet. In the Pauling-Corey beta-sheet and in the silk II form, referred to as an "in-register" structure, the Ala side chains of every strand point to the same side of a sheet. In the silk I structure, referred to as "out-of-register," the side chains of Ala residues in adjacent strands point to opposite sides of the sheet.     

Orientation of silk III at the air-water interface.

A threefold helical crystal structure of Bombyx mori silk fibroin has been observed in films prepared from aqueous silk fibroin solutions using the Langmuir Blodgett (LB) technique. The films were studied using a combination of transmission electron microscopy and electron diffraction techniques. Films prepared at a surface pressure of 16.7 mN/m have a uniaxially oriented crystalline texture, with the helical axis oriented perpendicular to the plane of the LB film. Films obtained from the air-water interface without compression have a different orientation, with the helical axes lying roughly in the plane of the film. In both cases the d-spacings observed in electron diffraction are the same and match a threefold helical model crystal structure, silk III, described in previous publications. Differences in the relative intensities of the observed reflections in both types of oriented samples, as compared to unoriented samples, allows estimations of orientation distributions and the calculations of orientation parameters. The orientation of the fibroin chain axis in the plane of the interfacial film for uncompressed samples is consistent with the amphiphilic behavior previously postulated to drive the formation of the threefold helical silk III conformation.     

Silk I structure in Bombyx mori silk foams.

Single crystals of Bombyx mori silk fibroin in the metastable silk I polymorph have been produced using a new foaming technique. Foams of silk protein are generated by bubbling pure nitrogen gas through an aqueous solution of regenerated silk fibroin. The foamed material is collected, dried, and then sonicated to yield individual crystals which were examined using transmission electron microscopy and electron diffraction. It is found that slightly acidic conditions in the solution from which the foam was generated favor the formation of silk II while neutral to slightly basic solutions favor silk I formation. More dilute solutions favor the formation of silk II while more concentrated solutions (about 7 wt.% or greater) favor the formation of silk I. X-ray powder diffraction patterns from the dried silk I foams displayed features highly indicative of silk I. We also report the first single crystal electron diffraction patterns of silk I. These patterns indicate a large unit cell, possibly 22.66 x 5.70 x 20.82 A. with six chains of six residues, Gly-Ala-Gly-Ala-Gly-Ser. Although we have not fully characterized this complex structure it appears that the chain is nearly fully extended and thus our data is consistent with models possessing general features similar to those proposed by Fossey SA, Nemethy G, Gibson KD, Scheraga HA. (Biopolymers 1991;31:1529-1541).     

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.     

X-ray structural study of noncrystalline regenerated Bombyx mori silk fibroin

X-ray diffraction measurements of regenerated Bombyx mori silk fibroin were carried out to determine its structural characteristic from an analysis of differential radial distribution functions (DRDFs). The temperature dependence of X-ray diffraction patterns from noncrystalline and crystal structures of regenerated silk fibroin was investigated using a high temperature furnace. Time resolved X-ray diffraction profiles were also obtained to construct kinematical models of structural changes caused by the addition of water. DRDFs, calculated from the experimental data, were compared with the DRDFs simulated on the basis of the Monte Carlo method. In order to model the noncrystalline structures, structural units were assumed to be parts of the crystalline structure of silk and those with appropriate structural defects reported previously. From the comparison of experimental and simulated DRDFs, it was determined that noncrystalline regenerated silk consisted of locally ordered atomic sheets similar to the atomic arrangement in the silk I crystal (Type-I sheets), and the final state of the structural change was noncrystalline, consisting of small crystallites, the structure of which is similar to that of silk II (Type-II crystallites). Time resolved DRDFs were also qualitatively interpreted by both the ordering of Type-I sheets and structural changes from Type-I to Type-II. The formation of the small Type-II crystallites obtained in this study was consistent with the nucleation of silk II by birefringence measurements of silk glands and the spinneret of Bombyx mori silkworm reported previously. X-ray diffraction should be a useful technique to understand the structural characteristics of noncrystalline organic materials.     

X-ray structural study of noncrystalline regenerated Bombyx mori silk fibroin

X-ray diffraction measurements of regenerated Bombyx mori silk fibroin were carried out to determine its structural characteristic from an analysis of differential radial distribution functions (DRDFs). The temperature dependence of X-ray diffraction patterns from noncrystalline and crystal structures of regenerated silk fibroin was investigated using a high temperature furnace. Time resolved X-ray diffraction profiles were also obtained to construct kinematical models of structural changes caused by the addition of water. DRDFs, calculated from the experimental data, were compared with the DRDFs simulated on the basis of the Monte Carlo method. In order to model the noncrystalline structures, structural units were assumed to be parts of the crystalline structure of silk and those with appropriate structural defects reported previously. From the comparison of experimental and simulated DRDFs, it was determined that noncrystalline regenerated silk consisted of locally ordered atomic sheets similar to the atomic arrangement in the silk I crystal (Type-I sheets), and the final state of the structural change was noncrystalline, consisting of small crystallites, the structure of which is similar to that of silk II (Type-II crystallites). Time resolved DRDFs were also qualitatively interpreted by both the ordering of Type-I sheets and structural changes from Type-I to Type-II. The formation of the small Type-II crystallites obtained in this study was consistent with the nucleation of silk II by birefringence measurements of silk glands and the spinneret of Bombyx mori silkworm reported previously. X-ray diffraction should be a useful technique to understand the structural characteristics of noncrystalline organic materials.     

Conformational transitions in model silk peptides

Protein structural transitions and beta-sheet formation are a common problem both in vivo and in vitro and are of critical relevance in disparate areas such as protein processing and beta-amyloid and prion behavior. Silks provide a "databank" of well-characterized polymorphic sequences, acting as a window onto structural transitions. Peptides with conformationally polymorphic silk-like sequences, expected to exhibit an intractable beta-sheet form, were characterized using Fourier transform infrared spectroscopy, circular dichroism, and electron diffraction. Polymorphs resembling the silk I, silk II (beta-sheet), and silk III (threefold polyglycine II-like helix) crystal structures were identified for the peptide fibroin C (GAGAGS repetitive sequence). Two peptides based on silk amorphous sequences, fibroin A (GAGAGY) and fibroin V (GDVGGAGATGGS), crystallized as silk I under most conditions. Methanol treatment of fibroin A resulted in a gradual transition from silk I to silk II, with an intermediate state involving a high proportion of beta-turns. Attenuated total reflectance Fourier transform infrared spectroscopy has been used to observe conformational changes as the peptides adsorb from solution onto a hydrophobic surface. Fibroin C has a beta-strand structure in solution but adopts a silk I-like structure upon adsorption, which when dried on the ZnSe crystal contains silk III crystallites.     

Spider silk fibre extrusion: combined wide- and small-angle X-ray microdiffraction experiments

The major and minor ampullate silks from live Nephila senegalensis (Tetragnathidae) and the major ampullate silk from Euprostenops spp. (Pisauridae) spiders were investigated in situ by X-ray diffraction during forced silking. Wide- (WAXS) and small-angle (SAXS) scattering patterns were obtained at the same time. WAXS data show that the thread at the exit of the spigots already contains beta-sheet poly(alanine) crystallites. SAXS data suggest the presence of microfibrils with an axial repeating period of approximately 8 nm for both Nephila and Euprostenops. Minor ampullate (MI) Nephila silk, however, does not show this axial repeat which is probably due to a higher amount of crystal forming poly(alanine). A microfibrillar morphology, connected by a network of random polymer chains, can explain the presence of highly oriented crystallites, an oriented halo and a diffuse background in the WAXS patterns. At high reeling speeds, bound water is co-extruded with the fibre. It can be squeezed out of the fibre by friction at a needle. Under natural conditions it is the spider's tarsal claws which might serve to squeeze out the water to improve the mechanical properties of the thread during dragline production.     

Equivalence of the projected structure of thin catalase crystals preserved for electron microscopy by negative stain,glucose or embedding in the presence of tannic acid

Thin crystals of beef liver catalase have been examined by electron microscopy following various preservation procedures. In the first part of this investigation, micrographs of three principal projections were obtained from thin sections of micro-crystals embedded in the presence of tannic acid. Computer reconstructions confirmed the space group assignment of P2₁2₁2₁ and permitted the packing arrangement of the catalase tetramers to be deduced to a resolution of about 20 Å. These results corroborate the packing model for this crystal form proposed by Unwin (1975) on the basis of molecular modeling of one projection. In the second part of this investigation, the projected structures of the thin crystals in various preserving media were compared. The negative contrasting of crystals embedded in the presence of tannic acid was confirmed by direct comparison with nonembedded, negatively stained thin platelet crystals. In addition, good agreement at 20 Å resolution was observed between the structure of negatively stained crystals and the structure of crystal platelets preserved in glucose and examined by lowdose methods, while moderate agreement was established with the published data of Taylor (1978) for crystals embedded in thin ice films. Tannic acid alone was also found to serve as a suitable medium for preserving catalase crystals to a resolution of 3.7 Å as judged by electron diffraction. Overall, we demonstrate that projections obtained from thin sections of catalase crystals embedded in the presence of tannic acid can provide a reliable, negatively contrasted representation of the protein structure to 20 Å resolution. Examination of sectioned crystals could thus provide a useful adjunct to X-ray crystallographic studies of protein crystals and three-dimensional reconstruction of crystal thin sections should ultimately be possible.     

Thermally induced alpha-helix to beta-sheet transition in regenerated silk fibers and films

The structure of thin films cast from regenerated solutions of Bombyx mori cocoon silk in hexafluoroisopropyl alcohol (HFIP) was studied by synchrotron X-ray diffraction during heating. A solid-state conformational transition from an alpha-helical structure to the well-known beta-sheet silk II structure occurred at a temperature of approximately 140 degrees C. The transition appeared to be homogeneous, as both phases do not coexist within the resolution of the current study. Modulated differential scanning calorimetry (DSC) of the films showed an endothermic melting peak followed by an exothermic crystallization peak, both occurring near 140 degrees C. Oriented fibers were also produced that displayed this helical molecular conformation. Subsequent heating above the structural transition temperature produced oriented beta-sheet fibers very similar in structure to B. mori cocoon fibers. Heat treatment of silk films at temperatures well below their degradation temperature offers a controllable route to materials with well-defined structures and mechanical behavior.     

The chemical structure and the crystalline structures of Bombyx mori silk fibroin.

Some recent data (i.e. published in the last ten years) on the chemical and crystalline structures of B. mori silk are reviewed. The main emphasis is put on the crystallizable portion of silk fibroin, including its chemical constitution and its molecular conformation (at the crystallographic unit-cell level) in the two crystalline modifications : the beta pleated sheet and the silk I structures. The structural aspects are based on a discussion of X-ray and electron diffraction data, and on conformational energy analyses of a model (Ala-Gly)n polypeptide of silk fibroin.     

Flexibility regeneration of silk fibroin in vitro

Although natural silk fibers have excellent strength and flexibility, the regenerated silk materials generally become brittle in the dry state. How to reconstruct the flexibility for silk fibroin has bewildered scientists for many years. In the present study, the flexible regenerated silk fibroin films were achieved by simulating the natural forming and spinning process. Silk fibroin films composed of silk I structure were first prepared by slow drying process. Then, the silk fibroin films were stretched in the wet state, following the structural transition from silk I to silk II. The difference between the flexible film and different brittle regenerated films was investigated to reveal the critical factors in regulating the flexibility of regenerated silk materials. Compared with the methanol-treated silk films, although having similar silk II structure and water content, the flexible silk films contained more bound water rather than free water, implying the great influence of bound water on the flexibility. Then, further studies revealed that the distribution of bound water was also a critical factor in improving silk flexibility in the dry state, which could be regulated by the nanoassembly of silk fibroin. Importantly, the results further elucidate the relation between mechanical properties and silk fibroin structures, pointing to a new mode of generating new types of silk materials with enhanced mechanical properties in the dry state, which would facilitate the fabrication and application of regenerated silk fibroin materials in different fields.     

Using focus ion beam to prepare crystal lamella for electron diffraction

Electron diffraction provides a powerful tool to solve the structures of small protein crystals. However, strong interactions between the electrons and the materials limit the application of the electron crystallographic method on large protein crystals with micrometer or larger sizes. Here, we used the focused ion beam (FIB) equipped on the scanning electron microscope (SEM) to mill a large crystal to thin lamella. The influences of the milling on the crystal lamella were observed and investigated, including radiation damage on the crystal surface during the FIB imaging, deformation of the thin crystal lamella, and variation in the diffraction intensities under electron radiation. These observations provide important information to optimize the FIB milling, and hence is important to obtain high-quality crystal samples for routine structure determination of protein crystals using the electron cryo-microscope.     

Bombyx mori silk fibroin liquid crystallinity and crystallization at aqueous fibroin-organic solvent interfaces.

A banded morphology has been observed for Bombyx mori silk fibroin films obtained from an aqueous hexane interface; the period of the banding is approximately 1 microm. Morphology and diffraction from different regions of the banded structure suggest that it is a free surface formed by a cholesteric liquid crystal. Truncated hexagonal lamellar crystallites of B. mori silk fibroin have been observed in films formed in the surface excess layer of fibroin at the interface between aqueous fibroin and hexane or chloroform. Based on initial crystallographic evidence, a three-fold helical conformation has been ascribed to the fibroin chains within the crystals. The chain conformation and crystalline habit appear to be similar to the silk III structure previously observed at the air-water interface (Valluzzi R, Gido SP. Biopolymers 1997;42:705-717; Valluzzi R, Gido S, Zhang W, Muller W, Kaplan D. Macromolecules 1996;29:8606-8614) but the crystalline packing is different. Diffraction data obtained for the crystallites are similar to diffraction behavior for a collagen-like model peptide. Diffraction patterns obtained from crystallized regions of the banded morphology can be indexed using the same unit cell as the hexagonal lamellar crystallites. Surfactancy of fibroin and subsequent aggregation and mesophase formation may help to explain the liquid crystallinity reported for silk, which is long suspected to play a role in the biological silk spinning process (Valluzzi R, Gido SP. Biopolymers 1997;42:705-717; Willcox, P. J.; Gido, SP, Muller W, Kaplan DL. Macromolecules 1996:29:5106-5110; Magoshi J, Magoshi Y, Nakamura S. In: Kaplan D, Adams W, Farmer B, Viney C, editors, Mechanism of Fiber Formation of Silkworm. Washington, DC: American Chemical Society 1994:292-310; Magoshi J, Magoshi Y, Nakamura S. J Appl Polym Sci Appl Polym Symp 1985;41:187-204; Magoshi J, Magoshi Y, Nakamura S. Polym Commun 1985;26:309.).     

Polymorphic forms of 1,2-dipalmitoyl-sn-glycerol: a combined X-ray and electron diffraction study

Quantitative crystallographic structure analyses are carried out for two polymorphic forms of 1,2-dipalmitoyl-sn-glycerol. A single crystal X-ray determination on the higher melting beta'L-form reveals that the hairpin conformer structure is essentially identical to that of the dilauroyl homolog reported earlier (I. Pascher, S. Sundell and H. Hauser (1981) J. Mol. Biol. 153, 791-806) with inclined acyl chain packing in the O perpendicular methylene subcell. Lamellar electron diffraction intensity data from epitaxially crystallized samples were used to determine the structure of the lower melting alpha L-form. The chains pack in the hexagonal subcell and are perpendicular to the lamellar surface. An appropriately oriented molecular model based on the beta'L-polymorph does not lead to a satisfactory structure solution but models based on the conformationally different 1,2-diglyceride moiety of several phospholipid structures does lead to a closer match to the observed diffraction data. In this proposed packing model for the alpha L-form, the hydroxyl oxygens are somewhat farther away from the unit cell origin than in the beta'L-form crystal structure, and, in combination with the different molecular conformation, this might explain the observed stability of this crystal polymorph against acyl shifts.     

The microstructure of isotropic vapor-deposited carbon films

The structure of thin, vapor-deposited carbon films was characterized by transmission electron microscopy and electron diffraction. Selected area electron diffraction showed very weak and broad peaks, indicating that these carbons contain extremely small crystallites whose dimension in the crystallographic c-direction is about 8 to 10 a. The observed diffraction bands are (h, k, 1 = 0) type reflections, which suggests that individual crystallites consist of graphitic layer planes stacked in parallel groups but with no order between atoms in adjacent planes (turbostratic). The carbon films exhibit no preferred orientation, indicating that the small crystallites are randomly oriented in the film and that the films are therefore isotropic. The measured density (1.8 g/cm3) and the structure of the vapor-deposited carbons are accordingly similar to those of low-temperature isotropic (LTI) pyrolytic carbons.     

Cross-beta order and diversity in nanocrystals of an amyloid-forming peptide

The seven-residue peptide GNNQQNY from the N-terminal region of the yeast prion protein Sup35, which forms amyloid fibers, colloidal aggregates and highly ordered nanocrystals, provides a model system for characterizing the elusively protean cross-beta conformation. Depending on preparative conditions, orthorhombic and monoclinic crystals with similar lath-shaped morphology have been obtained. Ultra high-resolution (<0.5A spacing) electron diffraction patterns from single nanocrystals show that the peptide chains pack in parallel cross-beta columns with approximately 4.86A axial spacing. Mosaic striations 20-50 nm wide observed by electron microscopy indicate lateral size-limiting crystal growth related to amyloid fiber formation. Frequently obtained orthorhombic forms, with apparent space group symmetry P2(1)2(1)2(1), have cell dimensions ranging from /a/=22.7-21.2A, /b/=39.9-39.3A, /c/=4.89-4.86A for wet to dried states. Electron diffraction data from single nanocrystals, recorded in tilt series of still frames, have been mapped in reciprocal space. However, reliable integrated intensities cannot be obtained from these series, and dynamical electron diffraction effects present problems in data analysis. The diversity of ordered structures formed under similar conditions has made it difficult to obtain reproducible X-ray diffraction data from powder specimens; and overlapping Bragg reflections in the powder patterns preclude separated structure factor measurements for these data. Model protofilaments, consisting of tightly paired, half-staggered beta strands related by a screw axis, can be fit in the crystal lattices, but model refinement will require accurate structure factor measurements. Nearly anhydrous packing of this hydrophilic peptide can account for the insolubility of the crystals, since the activation energy for rehydration may be extremely high. Water-excluding packing of paired cross-beta peptide segments in thin protofilaments may be characteristic of the wide variety of anomalously stable amyloid aggregates.     

Structural analysis of T4 DNA helix destabilizing protein (gp32 I) crystal by electron microscopy

Low dose electron diffraction and imaging techniques have been applied to the study of the crystalline structure of gp32*I, a DNA helix destabilizing protein derived from bacteriophage T4 gene 32 protein. A quantitative analysis of intensities from electron diffraction patterns from tilted, multilayered gp32*I crystal has provided the unit cell thickness of the crystal. The three-dimensional phases indicate that the space group P2(1)2(1)2. By taking into account the unit cell volume and the solvent content in the crystal, it was deduced that there is one gp32*I molecule in each asymmetric unit. A projected density map of unstained, glucose-embedded gp32*I crystal was synthesized with amplitudes from electron diffraction intensities and phases from electron images with reflections out to 7.6 A. Because of the similarity in the scattering density between glucose and protein, this projected map cannot be interpreted with certainty. A low resolution three-dimensional reconstruction shows that the protein molecule is about 90 A long and about 20 A in diameter. Because the dimer is formed around a dyad axis, the protein molecules comprising it must be arranged head-to-head. This dimeric arrangement of the proteins in the unit cell may be implicated as one of the conformational states of this protein in solution.