Changes in secondary structure follow the dissociation of human insulin hexamers: a circular dichroism study

Vacuum UV circular dichroism spectra measured down to 178 nm for hexameric 2-zinc human insulin, zinc-free human insulin, and the two engineered and biologically active monomeric mutants, [B/S9D] and [B/S9D,T27E] human insulin, show significant differences. The secondary structure analysis of the 2-zinc human insulin (T6) in neutral solution was determined: 57% helix, 1% beta-strand, 18% turn, and 24% random coil. This is very close to the corresponding crystal structure showing that the solution and solid structures are similar. The secondary structure of the monomer shows a 10-15% increase in antiparallel beta-structure and a corresponding reduction in random coil structure. These structural changes are consistent with an independent analysis of the corresponding difference spectra. The advantage of secondary structure analyses of difference spectra is that the contribution of odd spectral features stemming mainly from side chain chromophores is minimized and the sensitivity of the analyses improved. Analysis of the CD spectra of T6 2-zinc, zinc-free human insulin and monomeric mutant insulin by singular value decomposition indicates that the secondary structure changes following the dissociation of hexamers into dimers and monomers are two-state processes.     

Investigation of the cAMP receptor protein secondary structure by Raman spectroscopy

Raman spectroscopy was employed to examine the secondary structure of the cAMP receptor protein (CRP). Spectra were obtained over the range 400-1900 cm-1 from solutions of CRP and from CRP-cAMP cocrystals. The spectra of CRP dissolved in 30 mM sodium phosphate and 0.15 M NaCl buffered at either pH 6 or pH 8 or dissolved in 0.15-0.2 M NaCl at protein concentrations of 5, 15, and 30 mg/mL were examined. Estimates of the secondary structure distribution were made by analyzing the amide I region of the spectra (1630-1700 cm-1). CRP secondary structure distributions were essentially the same in either pH and at all protein concentrations examined. The amide I analyses indicated a structural distribution of 44% alpha-helix, 28% beta-strand, 18% turn, and 10% undefined for CRP in solution. Raman spectra of CRP-cAMP cocrystals differed from the spectra of CRP in solution. Some differences were assigned to interfering background bands, whereas other spectral differences were attributed to changes in CRP structure. Differences in the amide III region and in the intensity at 935 cm-1 were consistent with alterations in secondary structure. Analysis of the amide I region of the CRP-cAMP cocrystal spectrum indicated a secondary structure distribution of 37% alpha-helix, 33% beta-strand, 17% turn, and 12% undefined. This result is in agreement with a published secondary structure distribution derived from X-ray analysis of CRP-cAMP cocrystals (37% alpha-helix and 36% beta-strand).(ABSTRACT TRUNCATED AT 250 WORDS)     

Neuro-fuzzy structural classification of proteins for improved protein secondary structure prediction

Fourier transform infrared (FTIR) spectroscopy is a very flexible technique for characterization of protein secondary structure. Measurements can be carried out rapidly in a number of different environments based on only small quantities of proteins. For this technique to become more widely used for protein secondary structure characterization, however, further developments in methods to accurately quantify protein secondary structure are necessary. Here we propose a structural classification of proteins (SCOP) class specialized neural networks architecture combining an adaptive neuro-fuzzy inference system (ANFIS) with SCOP class specialized backpropagation neural networks for improved protein secondary structure prediction. Our study shows that proteins can be accurately classified into two main classes "all alpha proteins" and "all beta proteins" merely based on the amide I band maximum position of their FTIR spectra. ANFIS is employed to perform the classification task to demonstrate the potential of this architecture with moderately complex problems. Based on studies using a reference set of 17 proteins and an evaluation set of 4 proteins, improved predictions were achieved compared to a conventional neural network approach, where structure specialized neural networks are trained based on protein spectra of both "all alpha" and "all beta" proteins. The standard errors of prediction (SEPs) in % structure were improved by 4.05% for helix structure, by 5.91% for sheet structure, by 2.68% for turn structure, and by 2.15% for bend structure. For other structure, an increase of SEP by 2.43% was observed. Those results were confirmed by a "leave-one-out" run with the combined set of 21 FTIR spectra of proteins.     

Protein secondary structure from circular dichroism spectra

Circular dichroism spectra of proteins are extremely sensitive to secondary structure. Nevertheless, circular dichroism spectra should not be analyzed for protein secondary structure unless they are measured to at least 184 nm. Even if all the various types ofβ-turns are lumped together, there are at least 5 different types of secondary structure in a protein (α-helix, antiparallelβ-sheet, parallelβ-sheet,β-turn, and other structures not included in the first 4 categories). It is not possible to solve for these 5 parameters unless there are 5 equations. Singular value decomposition can be used to show that circular dichroism spectra of proteins measured to 200 nm contain only 2 pieces of information, while spectra measured to 190 nm contain about 4. Adding the constraint that the sum of secondary structures must equal 1 provides another piece of information, but even with this constraint, spectra measured to 190 nm simply do not analyze well for the 5 unknowns in secondary structure. Spectra measured to 184 nm do contain 5 pieces of information and we have used such spectra successfully to analyze a variety of proteins for their component secondary structures.     

Secondary structure of the mammalian 70-kilodalton heat shock cognate protein analyzed by circular dichroism spectroscopy and secondary structure prediction

Heat shock proteins are rapidly synthesized when cells are exposed to stressful agents that cause protein damage. The 70-kDa heat shock induced proteins and their closely related constitutively expressed cognate proteins bind to unfolded and aberrant polypeptides and to hydrophilic peptides. The structural features of the 70-kDa heat shock proteins that confer the ability to associate with diverse polypeptides are unknown. In this study, we have used circular dichroism (CD) spectroscopy and secondary structure prediction to analyze the secondary structure of the mammalian 70-kDa heat shock cognate protein (hsc 70). The far-ultraviolet CD spectrum of hsc 70 indicates a large fraction of alpha-helix in the protein and resembles the spectra one obtains from proteins of the alpha/beta structural class. Analysis of the CD spectra with deconvolution methods yielded estimates of secondary structure content. The results indicate about 40% alpha-helix and 20% aperiodic structure within hsc 70 and between 16-41% beta-sheet and 21-0% beta-turn. The Garnier-Osguthorpe-Robson method of secondary structure prediction was applied to the rat hsc 70 amino acid sequence. The predicted estimates of alpha-helix and aperiodic structure closely matched the values derived from the CD analysis, whereas the predicted estimates of beta-sheet and beta-turn were midway between the CD-derived values. Present evidence suggests that the polypeptide ligand binding domain of the 70-kDa heat shock protein resides within the C-terminal 160 amino acids [Milarski, K. L., & Morimoto, R. I. (1989) J. Cell Biol. 109, 1947-1962].(ABSTRACT TRUNCATED AT 250 WORDS)     

Accuracy of protein secondary structure determination from circular dichroism spectra based on immunoglobulin examples

Strong contribution of the aromatic amino acid side chain chromophores to the far-UV circular dichroism (CD) spectra substantially distorts a relatively weak CD signal originating from beta sheet, the main type of immunoglobulin secondary structure. In this study we compared the secondary structure calculated from the far-UV CD spectra with the X-ray data for three antibody Fab fragments. Calculations were performed with three different algorithms, using two sets of reference proteins. Low standard deviations between all six estimates indicate stable mathematical solutions. Despite pronounced differences in the shape and amplitude of the CD spectra, we found a strong correlation between CD and X-ray data in the secondary structure for every protein studied. The number and average length of the secondary structure elements estimated from the CD spectra closely resemble those of the X-ray data. Agreement between spectroscopic and crystallographic results demonstrates that modern methods of secondary structure calculation are resilient to distortions of the far-UV CD spectra of immunoglobulins caused by aromatic side chain chromophores.     

Native-like secondary structure of molten globules

The most common evidence for the existence of secondary structure in a globular protein is the presence of a strongly pronounced far-UV circular dichroism (CD) spectrum. Although CD spectra of native proteins are well described and their quantitative analysis is widely used, similar studies for denatured proteins have still to be done. Far-UV CD spectra of nine proteins in the native and the pH-induced molten globule states were acquired and analyzed. Singular value decomposition showed that the spectra of molten globules could be described as a superposition of at least three independent components (most likely alpha-, beta- and irregular structure). A self-consistent procedure of CD spectra analysis revealed the existence of a clear correlation between the shape of the molten globule spectra and the content of secondary structure elements in the corresponding native proteins, as determined from X-ray data. A mathematical expression of this correlation in terms of the Pierson coefficient amounts to the value of 0.9 for both the alpha-helix and the beta-structure. Thus, the secondary structure of proteins in the molten globule state is close to that in the native state.     

Determination of the secondary structure of proteins from the amide I band of the laser Raman spectrum

The amide I band in the laser Raman spectrum of proteins has been resolved into six components, each representing residues in a different type of secondary structure. These structure types are ordered or bihydrogen-bonded helix (believed to be located in the center of helical segments), disordered or monohydrogen-bonded helix (believed to be located at the ends of helical segments), antiparallel beta sheet, parallel beta sheet, reverse turn, and undefined. The Raman spectrum representing 100% of each type of residue conformation has been computed from the solvent-subtracted Raman spectra of ten proteins with known secondary structure, plus poly-l-lysine using a least-squares solution of the overdetermined system of equations. Linear combinations of these reference spectra were then fitted to the experimental amide I spectra of these and other proteins to estimate the fractions of residues in these conformations. Statistical tests suggest that the discrimination between bihydrogen-bonded helix and monohydrogen-bonded helix is significant as is the discrimination between parallel and antiparallel β-sheet. However, the discrimination between random structure and turns has not yet been accomplished by these studies. The absolute difference between X-ray and Raman estimates of structure for 17 protein samples is generally less than 6%. We conclude that detailed and reasonably accurate estimates of secondary structure can be derived from the amide I spectra of proteins.     

Analysis of protein circular dichroism spectra for secondary structure using a simple matrix multiplication

Inverse circular dichroism (CD) spectra are presented for each of the five major secondary structures of proteins: alpha-helix, antiparallel and parallel beta-sheet, beta-turn, and other (random) structures. The fraction of the each secondary structure in a protein is predicted by forming the dot product of the corresponding inverse CD spectrum, expressed as a vector, with the CD spectrum of the protein digitized in the same way. We show how this method is based on the construction of the generalized inverse from the singular value decomposition of a set of CD spectra corresponding to proteins whose secondary structures are known from X-ray crystallography. These inverse spectra compute secondary structure directly from protein CD spectra without resorting to least-squares fitting and standard matrix inversion techniques. In addition, spectra corresponding to the individual secondary structures, analogous to the CD spectra of synthetic polypeptides, are generated from the five most significant CD eigenvectors.     

Determination of the secondary structure content of proteins in aqueous solutions from their amide I and amide II infrared bands. Comparison between classical and partial least-squares methods

A method for estimating protein secondary structure from infrared spectra has been developed. The infrared spectra of H2O solutions of 13 proteins of known crystal structure have been recorded and corrected for the spectral contribution of water in the amide I and II region by using the algorithm of Dousseau et al. [Dousseau, F., Therrien, M., & Pézolet, M. (1989) Appl. Spectrosc. 43, 538-542]. This calibration set of proteins has been analyzed by using either a classical least-squares (CLS) method or the partial least-squares (PLS) method. The pure-structure spectra calculated by the classical least-squares method are in good agreement with spectra of poly(L-lysine) in the alpha-helix, beta-sheet, and undefined conformations. The results show that the best agreement between the secondary structure determined by X-ray crystallography and that predicted by infrared spectroscopy is obtained when both the amide I and II bands are used to generate the calibration set, when the PLS method is used, and when it is assumed that the secondary structure of proteins is composed of only four types of structure: ordered and disordered alpha-helices, beta-sheet, and undefined conformation. Attempts to include turns in the secondary structure estimation have led to a loss of accuracy. The standard deviation of the difference between X-ray and infrared secondary structure estimates with this method is 4.8% for the alpha-helix, 3.7% for the beta-sheet, and 5.1% for the undefined structure, whereas the regression coefficients are 0.95, 0.96, and 0.56, respectively. The spectra of the calibration proteins were also recorded in 2H2O solution.(ABSTRACT TRUNCATED AT 250 WORDS)     

SOMCD: method for evaluating protein secondary structure from UV circular dichroism spectra

This article presents SOMCD, an improved method for the evaluation of protein secondary structure from circular dichroism spectra, based on Kohonen's self-organizing maps (SOM). Protein circular dichroism (CD) spectra are used to train a SOM, which arranges the spectra on a two-dimensional map. Location in the map reflects the secondary structure composition of a protein. With SOMCD, the prediction of beta-turn has been included. The number of spectra in the training set has been increased, and it now includes 39 protein spectra and 6 reference spectra. Finally, SOM parameters have been chosen to minimize distortion and make the network produce clusters with known properties. Estimation results show improvements compared with the previous version, K2D, which, in addition, estimated only three secondary structure components; the accuracy of the method is more uniform over the different secondary structures.     

The secondary structure of calcium pump protein in light sarcoplasmic reticulum and reconstituted in a single lipid component as determined by Raman spectroscopy

Raman spectra have been measured of the following samples: active calcium pump protein in light sarcoplasmic reticulum (SR) membranes, lipids extracted from light SR membranes, active calcium pump protein reconstituted in dielaidoylphosphatidylcholine (DEPC), and pure DEPC. The spectra of native SR lipids and of pure DEPC are different, and yet when these spectra are subtracted from the spectra of the respective protein-lipid complexes, the resulting amide I spectra of the calcium pump protein are the same, indicating that appropriate criteria have been chosen for subtraction of the spectrum of a lipid. This spectrum has been analyzed for secondary structure with the following results. The SR calcium pump protein contains 51 +/- 5% helix, in agreement with a prediction of secondary structure obtained from an analysis of the sequence, and 21 +/- 4% beta-strand. In addition, the presence of protein broadens and lowers the main melting transition of DEPC.     

Purification of homogeneous gamma-cystathionase and study of its structure by circular dichroism

Rat liver gamma-cystathionase has been purified to homogeneity (verified by SDS electrophoresis and ultracentrifugation). The secondary and tertiary structures of the enzyme were studied by circular dichroism spectra. Our studies revealed that the holoenzyme molecule comprises approximately 22% of alpha-helices, 14% of beta-structure, 14% of beta-bends, and 50% of unordered structure. Conformational alterations of the enzyme molecule resulting from enzyme PLP elimination, reduction with sodium borohydride and irreversible inhibition by propargylglycine were examined. The enzyme's secondary structure was shown to be stable whereas the tertiary structure is labile. Saturation with PLP maintains the enzyme's optimal (catalytically active) tridimensional structure. Sodium dodecylsulfate alters its secondary (the amount of alpha-helix being raised to 34%) and tertiary structures.     

Analysis of the secondary structure of urokinase by the circular dichroism method

The secondary structure of urokinase with molecular weight 33 000 dalton was studied by the circular dichroism method. The secondary structure parameters were calculated based on the protein reference CD spectra resulted in the following secondary structure parameters: approximately 30% aminoacid residues constitute the alpha-helical regions, the same amount forms the beta-structure and an essential fractions contributes the beta-turns. Conformational stability of urokinase to alkaline pH (up to 11.6) and high temperature (up to 80 degrees) in 0.1 M phosphate buffer pH 6.6 was found.     

Evaluation of the information content in infrared spectra for protein secondary structure determination

Fourier-transform infrared spectroscopy is a method of choice for the experimental determination of protein secondary structure. Numerous approaches have been developed during the past 15 years. A critical parameter that has not been taken into account systematically is the selection of the wavenumbers used for building the mathematical models used for structure prediction. The high quality of the current Fourier-transform infrared spectrometers makes the absorbance at every single wavenumber a valid and almost noiseless type of information. We address here the question of the amount of independent information present in the infrared spectra of proteins for the prediction of the different secondary structure contents. It appears that, at most, the absorbance at three distinct frequencies of the spectra contain all the nonredundant information that can be related to one secondary structure content. The ascending stepwise method proposed here identifies the relevance of each wavenumber of the infrared spectrum for the prediction of a given secondary structure and yields a particularly simple method for computing the secondary structure content. Using the 50-protein database built beforehand to contain as little fold redundancy as possible, the standard error of prediction in cross-validation is 5.5% for the alpha-helix, 6.6% for the beta-sheet, and 3.4% for the beta-turn.     

An infrared and circular dichroism combined approach to the analysis of protein secondary structure.

Selected regions of infarred (ir) and circular dichroism (CD) spectral data from 10 proteins were combined and analyzed by a factor analysis method. The regions consisted of the area normalized amide I region from 1700 to 1600 cm-1 for the ir spectra and from 178 to 240 nm for the CD spectra. Each CD spectrum was scaled by a factor of 0.5 before appending the data to the ir spectral data. The scaling factor was deemed necessary to account for relative intensity differences between the ir and CD data and provided nearly optimum agreement between secondary structure estimated by the combined approach to secondary structure determined by X-ray crystallography. The ir/CD combined approach to estimation of helix, beta-sheet, beta-turn, and other or undefined secondary structure agreed with X-ray crystallographic determined structure better than estimation using data from either method alone. Correlation coefficients between X-ray and ir/CD combined secondary structure determinations were 0.99 for helix, 0.90 for beta-sheet, 0.70 for beta-turn, and 0.78 for other structure. The four most significant eigenvectors or basis spectra from eigenanalysis of the ir/CD data are presented as well as generalized inverse spectra for four secondary structures.     

Effect of lysine modification on the secondary structure of ovalbumin

In order to determine the effect of chemical modification of the -amino groups on the secondary structure of ovalbumin, we prepared six acetylated (17, 36, 54, 70, 82, and 98%) and four succinylated derivatives (25, 50, 72, and 97%) of the protein. Native ovalbumin and the acylated derivatives were homogeneous as revealed by the electrophoretic pattern. The UV-absorption and fluorescence spectra changed progressively with the extent of modification. However, circular dichroic (CD) studies indicated that acylation of 15 of the 20 lysine residues had little effect on the secondary structure of ovalbumin. Acylation of the remaining five lysine residues resulted in a fairly severe change in the secondary structure. The -helical content decreased from about 31% in the native state to 16.5% in the 97% succinylated ovalbumin and to 21.5% in the 98% acetylated derivative. A comparison of these data with the spectral and hydrodynamic data of Qasim and Salahuddin (1978) suggested that the secondary structure of ovalbumin is more resistant to acylation than is the tertiary structure and, thus, the tertiary and the secondary structures are, to some extent, mutually independent. Raising thepH to 11.2 did not alter the secondary structure of ovalbumin and increasing the ionic strength by more than 20-fold did not reverse the loss of helical structure in 97% succinylated protein. These two observations suggest that the change in secondary structure upon maximal acylation may not only involve electrostatic effects, but also certain other factors, such as steric hindrance due to the entering bulky groups.     

Secondary structure of substance P bound to liposomes in organic solvents and in solution from Raman and CD spectroscopy.

The membrane lipid phase may be an important mediator of the peptide-receptor interaction. In order to understand the mechanism of this interaction, it is important to know the peptide structure, not only in the hydrophobic lipid bilayer environment, but also at the bilayer surface and in solution. To investigate this problem we have measured the secondary structure of the 11-residue neuropeptide substance P (SP) and its fragments in aqueous solutions, in membrane mimetic solvents, and associated with lipid bilayers using Raman and CD spectroscopy. Raman and CD spectra of SP bound to liposomes indicate a less than 20% helix content. We interpret these results to indicate that SP contains virtually no helix when bound to negatively charged liposomes. These spectra are similar to spectra of peptides in type I and III beta-turns. SP forms between 10 and 30% (1-3 residues) helical structure in sodium dodecyl sulfate micelles and less than 10% helix in methanol and trifluoroethanol. The binding of SP to negatively charged liposomes significantly changes the structure of the lipid acyl chains, decreasing order in some cases and increasing it in others. Raman spectra of SP in water indicates that SP near 30 mM forms an ensemble of structures in water that is distinct from completely unfolded peptide and from the aggregated beta-sheet form observed in saline solutions. We conclude from our CD results that methods used to quantitate secondary structure from CD spectra of short peptides cannot be used to distinguish between very short helical segments and beta-turns.     

Sequence-specific assignment of 1H-NMR resonance and determination of the secondary structure of Jingzhaotoxin-I

Jingzhaotoxin-I （JZTX-I） purified from the venom of the spider Chilobrachys jingzhao is a novel neurotoxin preferentially inhibiting cardiac sodium channel inactivation by binding to receptor site 3.The structure of this toxin in aqueous solution was investigated using 2-D ^1H-NMR techniques. The complete sequence-specific assignments of proton resonance in the ^1H-NMR spectra of JZTX-I were obtained by analyzing a series of 2-D spectra, including DQF-COSY, TOCSY and NOESY spectra, in n20 and D20. All the backbone protons except for Gin4 and more than 95% of the side-chain protons were identified by dαN,dαδ, dβN and dNN connectivities in the NOESY spectrum. These studies provide a basis for the furtherdeter mination of the solution conformation of JZTX-I. Furthermore, the secondary structure of JZTX-I was identified from NMR data. It consists mainly of a short triple-stranded antiparallel β-sheet with Trp7-Cys9, Phe20-Lys23 and Leu28-Trp31. The characteristics of the secondary structure of JZTX-I are similar to those of huwentoxin-I （HWTX-I） and hainantoxin-IV （HNTX-IV）, whose structures in solution havepre viously been reported.     

Nucleolin promotes secondary structure in ribosomal RNA

The effect of nucleolin on the secondary structure of RNA was studied using circular dichroism (CD). Nucleolin caused decreases in the main positive bands and shifts to higher wavelengths in the CD spectra of synthetic polynucleotides such as poly(G) and poly(A) indicating helix destabilizing activity. In contrast, nucleolin effected increases in signal and shifts to lower wavelengths of the peaks of CD spectra of ribosomal RNA, suggesting enhancement of secondary structure. Another major nucleolar RNA binding protein, B23, had helix destabilizing activity but did not enhance RNA secondary structure. It is proposed that nucleolin promotes formation of secondary structure in preribosomal RNA during the early stages of ribosome biogenesis.