Structure and stability of gamma-crystallins. Denaturation and proteolysis behavior

The denaturation behavior of bovine lens gamma-crystallin fractions II, III, and IV and their susceptibility to proteolysis in vitro was compared to determine whether differences in their stability could play a role in cataract formation. Tertiary and secondary structure changes induced by increasing concentrations of urea, guanidine hydrochloride, and sodium dodecyl sulfate and by increasingly alkaline pH were followed by near-UV and far-UV circular dichroism, Trp fluorescence emission, and exposure of sulfhydryl groups. Major differences were found in the denaturation and proteolysis behavior of the three gamma-crystallin fractions. In general, the unfolding of gamma-II and gamma-III crystallins is rather gradual, suggesting the presence of intermediate unfolding states; in contrast, the order-disorder transition of gamma-IV crystallin is abrupt. The gamma-IV crystallin fraction is the most stable in urea and guanidine hydrochloride, but is most susceptible to nonspecific proteolysis and alkaline pH denaturation. Differences in denaturation and proteolysis behavior are attributed to the inherent differences in the tertiary structures of these crystallins.     

Predicted secondary and tertiary structures of carp gamma-crystallins with high methionine content: role of methionine residues in the protein stability.

A systematic structural comparison of several carp gamma-crystallins with high methionine contents was made by the secondary-structure prediction together with computer model-building based on the established X-ray structure of calf gamma-II crystallin. The overall surface hydrophilicity profile and the distribution of helices, beta-sheets, and beta-turns along the polypeptide chains are very similar among these carp gamma-crystallins. In addition, their general polypeptide packing is close to the characteristic 2 domain/4 motif Greek key three-dimensional conformation depicted for the calf gamma-II crystallin. Interestingly, most hydrophobic methionine residues are located on the protein surface with only a few buried inside the protein surface or in the interface between two motifs of each domain. The exposed hydrophobic and polarizable methionine cluster on the protein surface may have a bearing on the crystallin stability and dense packing in the piscine species, and probably also provides a malleable nonpolar surface for the interaction with other crystallin components for the maintenance of a clear and transparent lens.     

Comparison of the gamma-crystallins isolated from eye lenses of shark and carp. Unique secondary and tertiary structure of shark gamma-crystallin

gamma-Crystallin isolated from the shark of cartilaginous fishes was compared with the cognate gamma-crystallin from the carp of bony fishes. Distinct differences in amino acid compositions, primary, secondary and tertiary structures were found. The most salient features of shark gamma-crystallin lie in the fact that this crystallin possessed a significant alpha-helical structure in the peptide backbone as revealed by circular dichroism study, in contrast to those orthologous gamma-crystallins from other vertebrate species including bony fishes which all show a predominant beta-sheet secondary structure. The tertiary structure as reflected in the intrinsic microenvironments of various aromatic amino acids in the native crystallins also shows unambiguous differences between these two classes of gamma-crystallins. N-Terminal sequence analysis corroborates the structural differences between shark and carp gamma-crystallins. gamma-Crystallin from the more primitive shark seems to be more in line with the main evolutionary phylogeny leading to the modern mammalian gamma-crystallin.     

Prediction of the secondary and tertiary structure of plastocyanin.

The amino acid sequences of nine plastocyanins were examined using four published methods for the prediction of secondary structure in proteins. The results of the four methods were combined in such a way as to maximize agreement, and the position of alpha helices, beta sheets, and beta turns in plastocyanin was predicted. From this result and other information, such as the position of conserved residues and the requirements for coordination of copper, a preliminary model for the mainchain folding of the molecule was presented.     

Structure and stability of gamma-crystallins: tryptophan, tyrosine, and cysteine accessibility

The solute perturbation techniques of fluorescence of tryptophan (Trp) and dye-labeled thiol groups of cysteine as well as phosphorescence of tyrosine (Tyr) were utilized to obtain information on the relative solvent exposure and accessibility of these residues in gamma-crystallins. Both acrylamide and iodide quenchers were used to evaluate the quenching parameters in terms of accessibility and charge characteristics of the proteins. Stern-Volmer plots reveal the presence of more than one class of Trp residues in gamma-III and gamma-IV, and these residues in gamma-II are least accessible compared to the other two. Both steady-state and lifetime quenching studies of the dye-labeled fluorescence indicate that distinct differences also exist among these crystallins in cysteine (Cys) accessibilities. All three proteins, gamma-II, gamma-III, and gamma-IV, show two distinct lifetime components of the dye-labeled Cys residues. Both components of gamma-II undergo dynamic quenching, whereas only the major component of the other two crystallins is affected by the quenchers. Addition of acrylamide causes a decrease in Tyr phosphorescence of gamma-III and gamma-IV, but no change in the emission of gamma-II. The decrease is attributed to the formation of a nonemittive ground-state complex between the acrylamide and Tyr of the proteins; the association constant, Ka, calculated from the emission data, has been considered as a measure of Tyr accessibility. Ka values indicate that Tyr residues in gamma-III are most exposed and accessible compared to those in the other two proteins. Results of quenching by iodide ion reveal significant differences in the surface charge of the proteins.(ABSTRACT TRUNCATED AT 250 WORDS)     

The effects of deoxyribonucleic acid secondary structure on tertiary structure.

The secondary structure of supercoiled DNA was varied by changes in ionic strength. For I = 0.075-0.4 the structure remained in the previously established branched form with only minor alterations in molecular dimensions. In 4M-NaCl, which induces linear DNA to change its secondary structure to the C structure and brings about an increase in the superhelix density of the molecule, no extra branches were observed on the molecules. The limiting factors that dictate supercoil structure seem to be the number and position of potential branch points and the proximity with which the two intertwining DNA strands can approach each other on the arms of the branches. This value is close to 10nm under the conditions described, and is 14-15nm at I = 0.2. It is suggested that such values should be borne in mind when models of chromosome structure are being constructed.     

An NMR approach to tRNA tertiary structure in solution.

Atomic coordinates of E. Coli tRNA1Val have been generated from the X-ray crystal structure of Yeast tRNAPhe by base substitution followed by idealization...     

An insight into domain structures and thermal stability of gamma-crystallins.

The thermal behavior of gamma II, gamma IIIA, gamma IIIB, and gamma IVA crystallin, from calorimetric and spectral studies, has been analyzed in terms of selective unfolding of domains, interdomain interactions, conformational stability, and the existence of intermediates in the order-disorder transition equilibrium. The major endothermic transition (Tm) observed calorimetrically for all four fractions occurs between 67 and 78 degrees C, with enthalpy change (delta H) from 80 to 150 kcal/mol, values that agree reasonably well with those from spectroscopic measurements. gamma II and gamma IIIB show a second thermal event at T less than Tm whereas gamma IIIA and gamma IVA showed no additional transition. Urea-induced equilibrium unfolding of gamma II at acidic pH, unlike gamma IVA, is biphasic as monitored by CD and fluorescence, indicating the existence of an intermediate. The absence of a cooperative transition in gamma IVA in acidic urea and the appearance of a single endotherm in differential scanning calorimetry at low pH have been attributed to a structured intermediate that melts at low temperature. The difference in the folding/unfolding of gamma II and gamma IVA has been explained by subtle differences in the packing arrangement of their two domains and interactions between them. Thermal aggregation of gamma-crystallins could be prevented either by preincubation with ionic detergents or at low pH or in the presence of chemical denaturant, indicating that the protein surface charge and solvent polarity influence their stability. An increase in the 8-anilino-1-naphthalenesulfonate-bound fluorescence during heat denaturation also suggests that the thermal aggregation is governed by hydrophobic interactions.     

Nuclear magnetic resonance study of the solution structure of alpha 1-purothionin. Sequential resonance assignment, secondary structure and low resolution tertiary structure

The solution structure of the 45-residue plant protein, alpha 1-purothionin, is investigated by nuclear magnetic resonance (n.m.r.) spectroscopy. Using a combination of two-dimensional n.m.r. techniques to demonstrate through-bond and through-space (less than 5 A) connectivities, the 1H n.m.r. spectrum of alpha 1-purothionin is assigned in a sequential manner. The secondary structure elements are then delineated on the basis of a qualitative interpretation of short-range nuclear Overhauser effects (NOE) involving the NH, C alpha H and C beta H protons. There are two helices extending from residues 10 to 19 and 23 to 28, two short beta-strands from residues 3 to 5 and 31 to 34 which form a mini anti-parallel beta-sheet, and five turns. In addition, a number of long-range NOE connectivities are assigned and a low resolution tertiary structure is proposed.     

Eukaryotic DNAs in solution contain characteristic components of tertiary structure.

For natural eukaryotic DNA in solution, we suggest the existence of secondary-helix components superponed to parts of the DNA double helices. In a previous report we found, for calf thymus DNA in solution and of different mean molar mass Mr, an electrostatically driven rise of the hydrodynamically operative contour length of the double helix. This result was derived from Mr-dependent systematic deviations from the almost but not exactly linear plots of intrinsic viscosity [eta] as a function of 1/cs1/2 (cs = Na+ concentration) accurately determined by a titration technique [K.G. and K.E.R., Nucl. Acids Res. 8, 2807 (1980)]. In order to discriminate between DNA elongation contributions caused by secondary or by tertiary structure effects, respective measurements have now been extended to different temperatures for two eukaryotic and two prokaryotic DNA species. The slope of the curves obtained for the (apparent) gradual elongation effect as a function of temperature is negative for the eukaryotic DNAs investigated and is smaller and positive for the prokaryotic species, thus revealing different underlying main elongation mechanisms. We propose that, for the eukaryotic DNA samples, an electrostatically driven partial abolition of tertiary structure components is responsible for the prevailing part of the DNA elongation effect measured. (A helix elongation of this type may be the result of an abolition of an apparent helix shortening as realized in a very high degree on formation of nucleosome chains or in a less degree by DNA molecules with a respective evolutionarily fitted tertiary structure). For the smaller effects of prokaryotic DNA species something like a base breathing seems to dominate. Recent literature results support such an interpretation.     

Spectroscopic methods for analysis of protein secondary structure

Several methods for determination of the secondary structure of proteins by spectroscopic measurements are reviewed. Circular dichroism (CD) spectroscopy provides rapid determinations of protein secondary structure with dilute solutions and a way to rapidly assess conformational changes resulting from addition of ligands. Both CD and Raman spectroscopies are particularly useful for measurements over a range of temperatures. Infrared (IR) and Raman spectroscopy require only small volumes of protein solution. The frequencies of amide bands are analyzed to determine the distribution of secondary structures in proteins. NMR chemical shifts may also be used to determine the positions of secondary structure within the primary sequence of a protein. However, the chemical shifts must first be assigned to particular residues, making the technique considerably slower than the optical methods. These data, together with sophisticated molecular modeling techniques, allow for refinement of protein structural models as well as rapid assessment of conformational changes resulting from ligand binding or macromolecular interactions. A selected number of examples are given to illustrate the power of the techniques in applications of biological interest.     

Evidence for tertiary structure in natural single stranded RNAs in solution.

Binding isotherms (20 degrees C) of ethidium bromide to a number of tRNA species at various ionic strengths indicate that i) the number ni of intercalation sites is high 7 to 11 per molecule, in the low salt form III, but small, 2 to 1, at high Mg2+ or Na+ when form I predominates. ii) modification of tRNA at strategic positions for 3D folding prevents full expression of intercalation restriction iii) maximal restriction is obtained at salt concentrations higher than needed for full conversion to form I. It is inferred that restriction, which is not observed with bihelical RNA (or DNA), requires the native tRNA 3D structure but also some physical coupling between the region of 3D folding and bihelical arms. Ribosomal RNAs, some viral RNAs, mRNA from sheep mammary gland as well as the random copolymers Poly UG, Poly AUG, Poly AUCG all exhibit intercalation restriction. Hence 3D folding of the polyribonucleotide chains appears to be a feature common to single-stranded RNAs when free in solution under physiological conditions.     

A nuclear magnetic resonance study of secondary and tertiary structure in yeast tRNAPhe.

We present experimental evidence which confirms recently proposed ring current prediction methods for assigning hydrogen-bond proton nuclear magnetic resonance (NMR) spectra from tRNA (Robillard, G. T., Tarr, C. E., Vosman, F., & Berendsen, H. J. C. (1976) Nature (London) 262, 363-369; Robillard, G. T., Tarr, C. E., Vosman, F., & Sussman, J. L. (1977) Biophys. Chem. 6, 291-298). The evidence is a series of temperature-dependent studies on yeast tRNAPhe monitoring both the high- and low-field NMR spectral regions, which are correlated with independent optical and temperature-jump (temp-jump) studies performed under identical ionic strength conditions. Using assignments derived from the new prediction methods, the melting patterns of the hydrogen-bonded resonances agree with those expected on the basis of optical, temp-jump, and NMR studies on the high-field spectral region. The implication of these results is that previous assignment procedures are at least partially incorrect and, therefore, studies based on those procedures must be reexamined.     

A secondary and tertiary structure editor for nucleic acids

A major difficulty in the evaluation of secondary and tertiarystructures of nucleic acids is the lack of convenient methodsfor their construction and representation. As a first step ina study of the symbolic representation of biopolymers, we reportthe development of a structure editor written in Pascal, permittingmodel construction on the screen of a personal computer. Theprogram calculates energies for helical regions, allows user-definedhelices and displays the secondary structure of a nucleic acidbased on a user-selected set of helices. Screen and printeroutputs can be in the form of a backbone or the letters of theprimary sequence. The molecule can then be displayed in a formatwhich simulates its three-dimensional structure. Using appropriateglasses, the molecule can be viewed on the screen in three dimensions.Other options include the manipulation of helices and single-strandedregions which results in changes in the spatial relationshipbetween different regions of the molecule. The editor requiresan IBM or compatible PC, 640 kbyte memory and a medium or highresolution graphics card. Received on September 19, 1987; accepted on November 15, 1987     

The secondary structure of histone IV and its stability.

The secondary structure within histone IV and its fragments obtained by cyanogen bromide (CNBr) and cleavage at Met 84 has been examined by circular dichroism and spectophotometric pH titration measurements. These studies have confirmed the existence of stable secondary structure within the C-terminal fragment of histone IV (C-peptide which can be perturbed only by 6M urea at pH greater than 8 or 8 M guanidine-HCL. In contrast, the N-terminal fragment (N-peptide) appears to lack significant secondary structure at low ionic strengths but acquires approximately 15% betasheet conformation and 5% alpha-helix upon aggregation at ionic strengths larger than or equal to 0.4. The rates of nitration of the N- and C-peptides by tetranitromethane (TNM) have also been measured as a function of ionic strengths. Under comparable conditions, the rate constant for nitration of the N-peptide was found to be about six times greater than that for the C-peptide, further evidence in support of the presence of stable secondary structure within the C-terminal region of histone IV. After binding these histone IV fragments to DNA, however, the nitration reaction rate constants for the N- and C-peptide in the bound form are found to be 2% and 27% of the corresponding free peptides. Reconstituted nucleohistone IV is about 10% as reactive to TNM as histone IV at comparable ionic strength.     

Methanol-induced tertiary and secondary structure changes of granulocyte-colony stimulating factor

We have studied methanol-induced conformational changes in rmethuG-CSF at pH 2.5 by means of circular dichroism (CD), fluorescence and infrared (IR) spectroscopy, and 8-anilino-1-naphthalene sulfonic acid (ANS) binding. Methanol has little effect on the secondary and tertiary structures of rmethuG-CSF when its concentration is in the range of 0 to 20% (v/v). At 30% (v/v) methanol, rmethuG-CSF has ANS binding ability. In the methanol concentration range of 30 to 70% (v/v) the amount of alpha-helix decreases a little, and the tertiary structure decreases significantly. At methanol concentrations above 70% (v/v), a transition to a more helical state occurs, while there is little change in the tertiary structure, and no ANS binding ability. Thermal denaturation studies involving CD have demonstrated that as the methanol concentration increases the melting temperature and the cooperativity of transition decrease, and the transition covers a much wider range of temperature. It seems that the decreased cooperativity means an increase in the concentration of partially folded intermediate states during the unfolding of rmethuG-CSF.     

An extension of secondary structure prediction towards the prediction of tertiary structure

Secondary structure prediction parameters and optimised decision constants for use with the method of Garnier et al. [(1978) J. Mol. Biol. 120, 97-120] have been derived for two new and distinct substates of beta-structure. These we term internal and external on the basis of their hydrogen bonding patterns. The profiles of the amino acids for several of the parameters are considerably different in the two substates. Predictions using the new parameters attempt to distinguish the strands at the core of the beta-sheet from those at its edges and so restrict the possible topologies in tertiary structure prediction. The potential application of these parameters is illustrated for the class of beta/alpha proteins.