Structural and immunological characterization of recombinant ovomucoid expressed in Escherichia coli

The expression of recombinant allergens is becoming new insights of an important diagnosis and the therapy of allergies as well as molecular approaches to immunological and structural studies of allergens. Ovomucoid is a major food allergens in the hen's egg white which causes immediate food-hypersensitivity reactions mainly in children. A gene coding for the cDNA representing an entire ovomucoid molecule has been cloned in Escherichia coli under the control of T5 promoter fused with six-Histidine tag at the amino terminal end. Upon induction, the E. coli cells, harbouring this construct, expressed the recombinant protein as a soluble fraction and the recombinant ovomucoid protein was purified to electrophoeretic homogeneity using Ni²⁺ nitrilotriacetic acid agarose affinity chromatography. Immunoblot analysis showed that human IgE and IgG binding activities of the recombinant ovomucoid was identical to that of native analogue. The antigenicity and allergenicity of recombinant ovomucoid were almost same as that of native form when tested with an ELISA using six individual patient's serum. CD spectra indicated that that the recombinant ovomucoid has more -helix and less -structure than native form. These results show that the recombinant ovomucoid constructed in this study could be used for further studies on the immunological and structural studies of ovomucoid.     

Infrared spectra of outer and cytoplasmic membranes of Escherichia coli

Outer and cytoplasmic membranes of Escherichia coli were prepared by a method based on isopyenic centrifugation on a sucrose gradient. The infrared spectra of solid films of these membranes were studied. The cytoplasmic membrane had an amide I band at 1657 cm^?1 and an amide II band at 1548 cm^?1. The outer membrane had a broad amide I band at 1631–1657 cm^?1 and an amid II band at 1548 cm^?1 with a shoulder at 1520–1530 cm^?1. Upon deuteration, the amide I band of the cytoplasmic membrane shifted to 1648 cm^?1, whereas the band at 1631 cm^?1 of the outer membrane remained unchanged. After extraction of lipids with chloroform and methanol, the infrared spectra in the amide I and amide II regions of both membranes remained unchanged. Although the outer membrane specifically contained lipopolysaccharide, this could not account for the difference in the infrared spectra of outer and cytoplasmic membranes. It is concluded that a large portion of proteins in the outer membrane is a β-structured polypeptide, while this conformation is found less, if at all in the cytoplasmic membrane.     

Raman spectroscopic study of tropomyosin denaturation

Raman spectra of the pH denaturation of tropomyosin are presented. In the native state tropomyosin has an alpha-helical content of nearly 90%, but this value drops rapidly as the pH is raised above 9.5. The Raman spectrum of the native state is characterized by a strong amide I line appearing at 1655 cm^?1, very weak scattering in the amide III region around 1250 cm^?1, and a medium-intensity line at 940 cm^?1. When the protein is pH-denatured, a strong amide III line appears at 1254 cm^?1 and the 940 cm^?1 line becomes weak. The intensities of the latter two lines are a sensitive measure of the alpha-helical and disordered chain content. These results are consistent with the helix-to-coil studies of the polypeptides. The Raman spectra of α-casein and prothrombin, proteins thought to have little or no ordered secondary structure, are investigated. The amide III regions of both spectra display strong lines at 1254 cm^?1 and only weak scattering is observed at 940 cm^?1, features characteristic of the denatured tropomyosin spectrum. The amide I mode of α-casein appears at 1668 cm^?1, in agreement with the previously reported spectra of disordered polypeptides, poly-L -glutamic acid and poly-L -lysine at pH 7.0 and mechanically deformed poly-L -alanine.     

Raman scattering of collagen, gelatin, and elastin.

The Raman spectra of collagen, gelatin, and elastin are presented. The Raman lines in the latter two spectra are assigned by deuterating the amide N-H groups in gelatin and by studying the superposition spectra of the constituent amino acids. Two lines appear at 1271 and 1248 cm^?1 in the spectra of collagen and gelatin that can be assigned to the amide III mode. Possibly, the appearance of two amide III lines is related to the biphasic nature of the tropocollagen molecule, i.e., proline-rich (nonpolar) and proline-poor (polar) regions distributed along the chain. The melting, or collagen-to-gelatin transition, in water-soluble calf skin collagen is studied and the 1248-cm^?1 amide III line is assigned to the 3₁ helical regions of the tropocollagen molecule. Elastin is thought to be mostly random and the Raman spectrum confirms this assertion. Strong amide I and III lines appear at 1668 and 1254 cm^?1, respectively, and only weak scattering is observed at 938 cm^?1. These features have been shown to be characteristic of the disordered conformation in proteins.     

Fourier transform IR spectroscopy of collagen and gelatin solutions: deconvolution of the amide I band for conformational studies

The ir spectra of lathyritic rat skin collagen and calf skin gelatin solutions at a variety of temperatures were obtained using Fourier transform ir spectroscopy and a 9-reflection, 2-pass ZnSe prism sample cell. The spectra were then deconvolved (based on Kauppinnen's method) and the behavior of the amide I band at ～ 1650 cm^?1 observed in detail. Throughout the temperature range studied (4–50°C), three component absorption peaks within the amide I band (at 1633, 1643, and 1660 cm^?1) are common to the spectra irrespective of the degree of triple helix content of the sample. Changes in the relative intensities of these component peaks are, however, conformationally dependent. During denaturation of the triple helix, the dominant 1660-cm^?1 component in the native collagen spectrum diminishes and the 1633-cm^?1 peak becomes relatively intensified. The inherently strong basicity of the carbonyl group of the proline residues together with the frequent occurrence of this imino acid in the X position of the Gly-X-Y triplet of collagen largely accounts for the ?30-cm^?1 shift of the amide I band during denaturation. Temperature and conformationally dependent changes in the fine structure of the amide I band from dilute solutions of collagen can be monitored in a reproducible and quantitative fashion.     

Raman spectroscopic study of mechanically deformed poly-L-alanine

Raman spectroscopy has been used in investigating the conformational transitions of poly-L -alanine (PLA) induced by mechanical deformation. We see evidence of the alpha-helical, antiparallel beta-sheet, and a disordered conformation in PLA. The disordered conformation has not been discussed in previous infrared and X-ray diffraction investigations and may have local order similar to the left-handed 3₁ poly glycine helix. The amide III mode in the Raman spectrum of PLA is more sensitive than the amide I and II modes to changes in secondary structure of the polypeptide chain. Several lines below 1200 cm^?1 are conformationally sensitive and may generally be useful in the analysis of Raman spectra of proteins. A line at 909 cm^?1 decreases in intensity after deformation of PLA. In general only weak scattering is observed around 900 cm^?1 in the Raman spectra of antiparallel beta-sheet polypeptides. The Raman spectra of the amide N–H deuterated PLA and poly-L -leucine (PLL) in the alpha-helical conformation and poly-L -valine (PLV) in the beta-sheet conformation are presented. Splitting is observed in the amide III mode of PLV and the components of this mode are assigned. The Raman spectrum of an alpha-helical random copolymer of L -leucine and L -glutamic acid is shown to be consistent with the spectra of other alphahelical polypeptides.     

Structural analysis of some soluble elastins by means of FT‐IR and 2D IR correlation spectroscopy

Fourier transform infrared (FT‐IR) spectroscopy combined with 2D correlation spectroscopy has been used to offer some information about stability and structure of some soluble elastins. Temperature has been chosen as the perturbation to monitor the infrared behavior of various soluble elastins, namely, α‐elastin p, α‐elastin, and k‐elastin. In the 3800–2700 cm^?1 region, the H‐containing groups were analyzed. The bonded hydroxyls are found to decrease prior to the NH‐related hydrogen bonds and also to the conformational reorganization of hydrocarbon chains. The transition temperatures were evaluated and they were found to agree with those obtained from DSC data. The FTIR spectra and their 2nd derivatives denote that α‐ elastins exhibited amide‐I, ‐II and ‐III bands at 1656, 1539 and 1236 cm^?1, respectively, while in k‐elastin these bands were found at 1652 cm^?1 for amide I, 1540 cm^?1 for amide II and 1248 cm^?1 for amide III. The macroscopic IR finger‐print method, which combines: general IR spectra, secondary derivative spectra, and 2D‐IR correlation spectra, is useful to discriminate different elastins. Thus using the differences of the position and intensity of the bands from “fingerprint region” of studied elastins, which include the peaks assigned to C?O, C? C groups from α‐helix, β‐turn, and the peaks assigned to the amide groups, it is possible to identify and discriminate elastins from each others. Furthermore, the pattern of 2D‐IR correlation spectra under thermal perturbation, allow their direct identification and discrimination. © 2010 Wiley Periodicals, Inc. Biopolymers 93: 1072–1084, 2010. This article was originally published online as an accepted preprint. The “Published Online” date corresponds to the preprint version. You can request a copy of the preprint by emailing the Biopolymers editorial office at biopolymers@wiley.com     

Fourier transform infrared studies of ribonuclease in H2O and 2H2O solutions

Fourier transform infrared transmission spectra have been obtained of the enzyme ribonuclease in both H₂O and ²H₂O. The resolution of the spectra have been enhanced by Fourier self-deconvolution procedures. The infrared spectrum of ribonuclease changes during exchange of the enzyme's amide hydrogens for deuterium and the exchange has been followed in the amide I and amide II spectral regions. The amide I band shifts towards lower wavenumbers during both the fast and slow phases of hydrogen exchange and the interpretation of these shifts has aided the band assignments. In particular these studies have allowed an assignment to be made for the high frequency component of the β-strand absorption that differs from that proposed previously. This paper represents the first example of the use of deconvoluted Fourier transform infrared spectra in conjunction with hydrogen-deuterium exchange in order to aid in the assignment of a proteins's infrared bands.     

Occurrence and characterization of stable intermediate state(s) in the unfolding of ovomucoid by guanidine hydrochloride

Reversible unfolding of ovomucoid by guanidine hydrochloride, as followed by viscosity and difference-spectral measurements at 25°C, pH6, occurred in two distinct steps involving at least three major conformational states, namely the native, intermediate and completely denatured states, occurring respectively in 60mm-sodium phosphate buffer, 3.5m-guanidine hydrochloride and 6m-guanidine hydrochloride. The overall native conformation of ovomucoid, as indicated by its intrinsic viscosity (5.24ml/g) and gel-filtration behaviour, differs significantly from that of a typical globular protein. Exposures of tyrosine residues in native ovomucoid measured by difference spectroscopy following perturbation with glycerol, ethylene glycol and dimethyl sulphoxide were, respectively, 0.42, 0.56 and 0.57. Of the exposed phenolic groups only one titrated normally (pK_int., 9.91, electrostatic-interaction factor, w, 0.04). Results on difference spectra, solvent perturbation, phenolic titration and intrinsic viscosity (7.4ml/g) taken together showed that, although ovomucoid in 3.5m-guanidine hydrochloride was significantly unfolded, it retained a degree of native structure, removable with 6m-guanidine hydrochloride. In the latter, all the six tyrosine residues were available for titration, and the intrinsic viscosity of ovomucoid increased to 9.4ml/g. Furthermore, the characteristic fine structures in circular-dichrosim spectra of ovomucoid, associated with the elements of native structure, were abolished in 6m-guanidine hydrochloride, suggesting that the completely denatured state is structureless and presumably behaves as a cross-linked random coil. The latter state has been shown by analysis of the results on guanidine hydrochloride-dependence of the transition, intermediatedenatured, to be less stable than the intermediate state under native conditions by about 46kJ/mol at 25°C. Attempts have been made to interpret the above results in the light of available information on the amino acid sequence of ovomucoid.     

Raman scattering of chymotrypsinogen A, ribonuclease, and ovalbumin in the aqueous solution and solid state

The Raman spectra of three globular proteins, beef pancreas chymotrypsinogen A, beef pancreas ribonuclease, and hen egg white ovalbumin have been obtained in the solid state and aqueous solution. X-ray diffraction and circular dichroism evidence have indicated that these proteins have a low α-helical content and a large fraction of the residues in the unordered and β-sheet conformation. The frequencies and intensities of the amide I and amide III lines are consistent with assignments based on the Raman spectra of polypeptides. The intense amide III lines observed in all the spectra would be expected for proteins with a low fraction of the residues in the α-helical conformation. Several spectra changes occur upon dissolution of the proteins in water and may be associated with further hydration of the proteins. The spectrum of thermally denatured chymotrypsinogen is presented. A 3 cm^–1 decrease in the frequency of the amide I line of the protein dissolved in D₂O upon heating was observed. This observation is consistent with a denaturation mechanism allowing only slight changes in the secondary structure but an increase in solvent penetration upon going from the native to the reversibly denatured state.     

Vibrational circular dichroism in amino acids and peptides. 7. Amide stretching vibrations in polypeptides

Vibrational circular dichroism (VCD) spectra for the principal amide stretching vibrations, amide A (N? H stretch) and amide I (predominantly C?O stretch), are presented and analyzed for a variety of polypeptides dissolved in chloroform, as well as for two examples in D₂O. Our results for poly(γ-benzyl-L -glutamate) confirm the first and only previous report of VCD in polypeptides carried out by Singh and Keiderling [(1981) Biopolymers 20 , 237–240]. Collectively, our spectra show that the sense of the bisignate VCD in these two regions depends on the sense of α-helicity and not on the absolute configuration of the constituent amino acids. This conclusion is established by obtaining VCD for the two polypeptides, poly(β-benzyl-L -asparate) and poly(im-benzyl-L -histidine), that form left-handed as opposed to right-handed α-helices. A new amide band having significant VCD intensity owing to its Fermi resonance interaction with the N? H stretching mode has been identified as a weak shoulder on the low-frequency side of the amide A band near 3200 cm^?1 and is assigned as a combination band of the amide I and amide II vibrations. VCD spectra of polypeptides in D₂O solution, although weak, have been successfully measured in the amide I region, where spectra appear to be more complicated due to the presence of solvated and internally hydrogen-bonded amide groups. Strong monosignate contributions to the VCD in the amide A and amide I regions for some of the polypeptides indicate coupling of an electronic nature between these two regions and is deduced by an application of the concept of local sum rules of rotational strength. It appears that a detailed understanding of the VCD obtained for polypeptides will not only be diagnostic of secondary structure, but also of more subtle structural and vibrational effects that give rise to local, intrinsic chirality in the amide vibrations.     

Laser Raman scattering of cobramine B, a basic protein from cobra venom

Cobramine B, a small basic protein from cobra venom, is selected as a model for studying the scattering intensity of tyrosyl ring vibrations in the Raman spectra of proteins. All three tyrosines in this protein appear to be “buried” in the interior of the molecule and probably involved in interactions which are similar to those of the three “buried” tyrosines in RNase A when it is dissolved in water. Spectral evidence is presented and discussed. The Raman spectra in the 300–1800 cm^?1 region of cobramine B in the solid and solution are compared quantitatively. Several differences exist between the two spectra and may be interpreted in terms of difference in conformation. In the amide I region, a strong single line was observed at 1672 cm^?1 both in the solid and solution spectra, suggesting that this protein may contain a large fraction of antiparallel-β structure. This is supported by the presence of a line at 1235 cm^?1 in the amide III region, which is also characteristic of β-structure. The resolved peaks at 1254 and 1270 cm^?1 indicate the coexistence of some hydrogen-bonded random-coil and some α-helix with the β-structure.     

Fourier transform-infrared spectroscopic methods for microbial ecology: analysis of bacteria,bacteri-polymer mixtures and biofilms

Fourier transform-infrared (FT-IR) spectroscopy has been used to rapidly and nondestructively analyze bacteria, bacteria-polymer mixtures, digester samples and microbial biofilms. Diffuse reflectance FT-IR (DRIFT) analysis for freeze-dried, powdered samples offered a means of obtaining structural information. The bacteria examined were divided into two groups. The first group was characterized by a dominant amide I band and the second group of organisms displayed an additional strong carbonyl stretch at ～ 1740 cm^?1. The differences illustrated by the subtraction spectra obtained for microbes of the two groups suggests that FT-IR spectroscopy can be utilized to recognize differences in microbial community structure. Calculation of specific band ratios has enabled to composition of bacteria and extracellular or intracellular storage product polymer mixtures to be determined for bacteria-gum (amide I/carbohydrate C-O-～ 1150 cm^?1) and bacteria-poly-β-hydroxybutyrate (amide I/carbonyl ～ 1740 cm^?1). The key band ratios correlate with the compositions of the material and provide useful information for the application of FT-IR sepectroscopy to environmental biofilm samples and for distinguishing bacteria grown under differing nutrient conditions. DRIFT spectra have been obtained for biofilms produced by Vibrio natriegens on stainless steel disks. Between 48 and 144 h, an increase in bands at ～ 1740 cm^?1 was seen in FT-IR spectra of V. natriegens biofilm. DRIFT spectra of mixed culture effluents of anaerobic digesters show differences induced by shifts in input feedstocks. The use of flow-through attenuated total reflectance has permitted in situ real-time changes in biofilm formation to be monitored and provides a powerful tool for understanding the interactioni within adherent microbial consortia.     

Low-frequency infrared bands and chain conformations of polypeptides

Infrared spectra of polypeptides were measured in the region of 1800–400 cm^?1. For the α-helical form, disordered form, and antiparallel-chain β-form, amide V band- arising from N-H out-of-plane bending models were observed at 610–620, around 650, and 700–705 cm^?1, respectively, and amide V′ bands arising from N-D out-of-plane bending modes were observed at 455–465, around 510, and a 515–530 cm^?1, respectively. These correlations are useful for conformation diagnoses, particularly for copolyamino-acids or proteins which are not oriented. The nature of low-frequency amide bands are discussed with reference to potential energy distributions calculated for the α-helical form and β form.     

Vibrational Circular Dichroism Spectra of Proteins in the Amide III Region: Measurement and Correlation of Bandshape to Secondary Structure

Vibrational circular dichroism (VCD) spectra have been measured for 23 globular proteins dissolved in H₂O/phosphate buffer over the 1400 to 1100 cm⁻¹region which encompasses the amide III mode. Spectral responses characteristic of the dominant secondary structure type were found as broad features at ∼1300 cm⁻¹, with the extreme forms having positive VCD for highly helical proteins and negative VCD for highly sheet-containing proteins. Quantitative correlation with secondary structure was carried out using previously developed factor analysis and restricted multiple regression (FA/RMR) techniques. Since the absorbance intensity of the amide III mode is difficult to determine due to overlap with other transitions, an alternative, absolute intensity-independent, simple structural analysis method was used. A linear regression was developed between the fractional components of secondary structure for the protein set and the overlap integrals of the normalized spectra from the set with that of a selected protein. The results of this simple method are quite comparable to those of the FA/RMR approach for analysis with amide III VCD. On the other hand, test calculations with the new method when used with electronic CD spectra are not as good as FA/RMR due to its more intensity-dependent relationship with secondary structure.     

Does Solid-state <Superscript>15</Superscript>N NMR Spectroscopy Detect all Soil Organic Nitrogen?

Virtually all of the N detected by ¹⁵N cross polarization (CP) NMR spectra of four HF-treated soil clay fractions is amide N. However, the intensity of this ¹⁵N CP NMR signal (per unit N) is 27–57% lower than detected for a wheat protein, gliadin. There are two possible explanations – either the amide N in the soil clay fractions produces proportionately less NMR signal than does the amide N in gliadin, or part of the N in the soil clay fractions produces little or no NMR signal. The cross polarization dynamics of the gliadin amide resonance and amide resonances detected for the soil clay fractions are very similar and thus should produce similar amounts of signal, ruling out the first possibility. Therefore up to half or even more of the organic N in these soil clay fractions must be in a form that is insensitive to NMR detection. For a model compound (caffeine), non-protonated heterocyclic N produced less than 20% of the signal of an equivalent amount of amide N in gliadin. Results from several ¹³C NMR techniques provide further evidence that much of the undetected N in the soil clay fractions may be heterocyclic.     

Solid-state 15N NMR analysis of highly 15N-enriched plant materials

Solid-state ¹⁵N NMR spectroscopy was used to determine the chemical nature of nitrogen in ¹⁵N-enriched material from the roots and stems of wheat (Triticum aesitivum), field pea (Pisum sativum) and kikuyu grass (Pennisetum clandestinum) and from the roots, stems and leaves of a eucalyptus species (Eucalyptus globulus). Nitrogen-15 cross polarization (CP) spectra of the materials were all very similar, with 64–75% of total signal assigned to amide N. Spin counting analysis indicated that 37–80% of potential signal was accounted for in the CP spectra, and that NMR observability using the CP technique (N _obs -CP) was higher for stems and leaves than for roots, and higher for wheat and eucalyptus than for peas and kikuyu. The ¹⁵N direct polarization (DP) spectra contained higher proportions of signal assigned to amine (up to 22%) and nitrate (up to 17%), and less assigned to amide N (50–72%) than the corresponding CP spectra. Spin counting analysis indicated that 68–93% of potential signal was accounted for in the DP spectra, confirming the DP technique to be more quantitatively reliable than CP.     

Characterization of β-bend ribbon spiral forming peptides using electronic and vibrational CD

Terminally blocked (L-Pro-Aib)_n and Aib-(L-Pro-Aib)_n sequential oligopeptides are known to form right-handed β-bend ribbon spirals under a variety of experimental conditions. Here we describe the results of a complete CD and ir characterization of this subtype of 3₁₀-helical structure. The electronic CD spectra were obtained in solvents of different polarity in the 260-180 nm region. The vibrational CD and Fourier transform ir (FTIR) spectra were measured in deuterochloroform solution in the amide I and amide II (1750-1500 cm^?1) regions. The critical chain length for full development of the β-bend ribbon spiral structure is found to be five to six residues. Spectral effects related to concentration-induced stabilization of the structures of the longer peptides were seen in the resolution-enhanced FTIR spectra. Comparison to previous studies of (Aib)_n and (Pro)_n oligomers indicate that the low frequency of the amide I mode is due to the interaction of secondary and tertiary amide bonds and not to a strong difference in conformation from a regular 3₁₀-helix. © 1995 John Wiley & Sons, Inc.     

Identification of a protein-binding surface by differential amide hydrogen-exchange measurements. Application to Bowman-Birk serine-protease inhibitor.

The binding surface of soybean trypsin/chymotrypsin Bowman-Birk inhibitor in contact with alpha-chymotrypsin has been identified by measurement of the change in amide hydrogen-exchange rates between free and chymotrypsin-bound inhibitor. Exchange measurements were made for the enzyme-bound form of the inhibitor at pH 7.3, 25 degrees C using fast-flow affinity chromatography and direct measurement of exchange rates in the protein complex from one-dimensional and two-dimensional nuclear magnetic resonance spectra. The interface is characterized by a broad surface of contact involving residues 39 through 48 of the anti-chymotryptic domain beta-hairpin as well as residues 32, 33 and 37 in the anti-chymotryptic domain loop of the inhibitor. A number of residues in the anti-tryptic domain of the protein also have an altered exchange rate, suggesting that there are changes in the protein conformation upon binding to chymotrypsin. These changes in amide exchange behavior are discussed in light of a model of the complex based on the X-ray crystallographic structure of turkey ovomucoid inhibitor third domain bound to a alpha-chymotrypsin, and the structure of free Bowman-Birk inhibitor determined in solution by two-dimensional nuclear magnetic resonance spectroscopy. The chymotrypsin-binding loop of Bowman-Birk inhibitor in the model is remarkably similar to the binding loop conformation in crystal structures of enzyme-bound polypeptide chymotrypsin inhibitor-I from potatoes, turkey ovomucoid inhibitor third domain, and chymotrypsin inhibitor-II from barley seeds.     

Raman spectra of chemically modified lysozyme. Oxindole derivatives.

The Raman spectra of oxidation products of lysozyme have been investigated. The protein was oxidized by N-bromosuccinimide and dimethyl sulfoxide/HCl. Depending on the experimental conditions one to six tryptophan residues are oxidized to oxindole. The most prominent difference between the spectra of lysozyme and its oxindole derivatives is the strong band at 1017 cm^?1 which displaces the tryptophan peak at 1010 cm^?1. Other tryptophan bands are also weakened corresponding to the number of the tryptophan side chains destroyed. Shifts are observed in the amide I and in the amide III regions sensitive to conformational changes. These shifts indicate conformational differences in the higher oxidized species and in the native enzyme, although the amide III maxima overlap with a strong oxindole band. Similar effects are observed in the range of the C-C stretching vibrations of the peptide backbone. If more than one tryptophan side chain is oxidized changes have also been found in the S-S stretching range. The evaluation of this effect is difficult because of the strong oxindole vibration appearing in this region. In species oxidized by great excess of N-bromosuccinimide the tyrosine vibrations can no longer be detected, indicating the modification of this amino acid too.