Heat-induced unfolding of neocarzinostatin, a small all-beta protein investigated by small-angle X-ray scattering.

Neocarzinostatin is an all-beta protein, 113 amino acid residues long, with an immunoglobulin-like fold. Its thermal unfolding has been studied by small-angle X-ray scattering. Preliminary differential scanning calorimetry and fluorescence measurements suggest that the transition is not a simple, two-state transition. The apparent radius of gyration is determined using three different approaches, the validity of which is critically assessed using our experimental data as well as a simple, two-state model. Similarly, each step of data analysis is evaluated and the underlying assumptions plainly stated. The existence of at least one intermediate state is formally demonstrated by a singular value decomposition of the set of scattering patterns. We assume that the pattern of the solution before the onset of the transition is that of the native protein, and that of the solution at the highest temperature is that of the completely unfolded protein. Given these, actually not very restrictive, boundary constraints, a least-squares procedure yields a scattering pattern of the intermediate state. However, this solution is not unique: a whole class of possible solutions is derived by adding to the previous linear combination of the native and completely unfolded states. Varying the initial conditions of the least-squares calculation leads to very similar solutions. Whatever member of the class is considered, the conformation of this intermediate state appears to be weakly structured, probably less than the transition state should be according to some proposals. Finally, we tried and used the classical model of three thermodynamically well-defined states to account for our data. The failure of the simple thermodynamic model suggests that there is more than the single intermediate structure required by singular value decomposition analysis. Formally, there could be several discrete intermediate species at equilibrium, or an ensemble of conformations differently populated according to the temperature. In the latter case, a third state would be a weighted average of all non native and not completely unfolded states of the protein but, since the weights change with temperature, no meaningful curve is likely to be derived by a global analysis using the simple model of three thermodynamically well-defined states.

[1]  P. Vachette,et al.  Improved Signal-to-Background Ratio in Small-Angle X-ray Scattering Experiments with Synchrotron Radiation using an Evacuated Cell for Solutions , 1997 .

[2]  S Doniach,et al.  Characterization of transient intermediates in lysozyme folding with time-resolved small-angle X-ray scattering. , 1999, Journal of molecular biology.

[3]  D Baker,et al.  Long-range order in the src SH3 folding transition state. , 2000, Proceedings of the National Academy of Sciences of the United States of America.

[4]  K. Hodgson,et al.  The Radius of Gyration of an Apomyoglobin Folding Intermediate , 1995, Science.

[5]  M. Kataoka,et al.  Trifluoroethanol‐induced conformational transition of hen egg‐white lysozyme studied by small‐angle X‐ray scattering , 1997, FEBS letters.

[6]  D I Svergun,et al.  Protein hydration in solution: experimental observation by x-ray and neutron scattering. , 1998, Proceedings of the National Academy of Sciences of the United States of America.

[7]  Peter Schurtenberger,et al.  Scattering Functions of Semiflexible Polymers with and without Excluded Volume Effects , 1996 .

[8]  M. Desmadril,et al.  Characterization of the denatured states distribution of neocarzinostatin by small-angle neutron scattering and differential scanning calorimetry. , 2001, Biochemistry.

[9]  S Doniach,et al.  A lysozyme folding intermediate revealed by solution X-ray scattering. , 1996, Journal of molecular biology.

[10]  J. Lee,et al.  Apparent radii of the native, stable intermediates and unfolded conformers of the alpha-subunit of tryptophan synthase from E. coli, a TIM barrel protein. , 1999, Biochemistry.

[11]  W. G. Miller,et al.  Dimensions of protein random coils. , 1968, Biochemistry.

[12]  P. Debye,et al.  Molecular-weight determination by light scattering. , 1947, The Journal of physical and colloid chemistry.

[13]  P. Privalov,et al.  Energetics of the alpha-lactalbumin states: a calorimetric and statistical thermodynamic study. , 1994, Biochemistry.

[14]  M. Gruebele,et al.  Mapping the transition state of the WW domain β-sheet , 2000 .

[15]  R. Duplessix,et al.  Scattering function of polystyrene , 1987 .

[16]  P. Wolynes,et al.  The Energy Landscape Theory of Protein Folding , 1998 .

[17]  D. Baker,et al.  Chain collapse can occur concomitantly with the rate-limiting step in protein folding , 1999, Nature Structural Biology.

[18]  K. Freed,et al.  Penetration function and second virial coefficient for linear and regular star polymers , 1984 .

[19]  V. Favaudon,et al.  The seven-stranded beta-barrel structure of apo-neocarzinostatin as compared to the immunoglobulin domain. , 1992, Biochimie.

[20]  K. Kuwajima,et al.  Structural characterization of the molten globule of α‐lactalbumin by solution X‐ray scattering , 1997, Protein science : a publication of the Protein Society.

[21]  D P Kharakoz,et al.  Partial volumes and compressibilities of extended polypeptide chains in aqueous solution: additivity scheme and implication of protein unfolding at normal and high pressure. , 1997, Biochemistry.

[22]  K. Soda,et al.  The compact and expanded denatured conformations of apomyoglobin in the methanol‐water solvent , 2008, Protein science : a publication of the Protein Society.

[23]  L. Fetler,et al.  X-ray scattering titration of the quaternary structure transition of aspartate transcarbamylase with a bisubstrate analogue: influence of nucleotide effectors. , 1995, Journal of molecular biology.

[24]  V. Uversky,et al.  Anion-induced folding of Staphylococcal nuclease: characterization of multiple equilibrium partially folded intermediates. , 1998, Journal of molecular biology.

[25]  D. J. Strydom,et al.  Neocarzinostatin: spectral characterization and separation of a non-protein chromophore. , 1979, Biochemical and biophysical research communications.

[26]  S. Radford,et al.  Kinetic studies of β-sheet protein folding , 1998 .

[27]  P. Vachette,et al.  Role of hydrophobic interactions in yeast phosphoglycerate kinase stability , 2000, Proteins.

[28]  Y. Amemiya,et al.  Kinetic refolding of beta-lactoglobulin. Studies by synchrotron X-ray scattering, and circular dichroism, absorption and fluorescence spectroscopy. , 1998, Journal of molecular biology.

[29]  M. Desmadril,et al.  Reinvestigation of the Proteolytic Activity of Neocarzinostatin , 2000, Journal of bacteriology.

[30]  J. Clarke,et al.  The folding of an immunoglobulin-like Greek key protein is defined by a common-core nucleus and regions constrained by topology. , 2000, Journal of molecular biology.

[31]  G. Rowe,et al.  Influence of the solvent on the conformational-dependent properties of random-coil polypeptides. I. The mean-square of the end-to-end distance and of the dipole moment. , 1990, Biophysical chemistry.

[32]  V. Favaudon,et al.  Poly(deoxyadenylic-deoxythymidylic acid) damage by radiolytically activated neocarzinostatin. , 1985, Biochemistry.

[33]  M. Bycroft,et al.  Folding of a dimeric β‐barrel: Residual structure in the urea denatured state of the human papillomavirus E2 DNA binding domain , 2008, Protein science : a publication of the Protein Society.

[34]  Luis Serrano,et al.  The folding transition state between SH3 domains is conformationally restricted and evolutionarily conserved , 1999, Nature Structural Biology.

[35]  M. Kataoka,et al.  Chain-like conformation of heat-denatured ribonuclease A and cytochrome c as evidenced by solution X-ray scattering. , 1998, Folding & design.

[36]  F. Boué,et al.  Lysozyme-lysozyme interactions in under- and super-saturated solutions: a simple relation between the second virial coefficients in H2O and D2O , 1997 .

[37]  A. V. Semenyuk,et al.  Small-angle-scattering-data treatment by the regularization method , 1988 .

[38]  Structure and dynamics of an acid-denatured protein G mutant. , 2000, Biochemistry.

[39]  E. Cota,et al.  Folding of beta‐sandwich proteins: Three‐state transition of a fibronectin type III module , 2008, Protein science : a publication of the Protein Society.

[40]  C. Royer,et al.  Exploring the temperature-pressure phase diagram of staphylococcal nuclease. , 1999, Biochemistry.

[41]  C. Cantor,et al.  Biophysical chemistry. Part III, The behavior of biologicalmacromolecules , 1980 .

[42]  T. Vorherr,et al.  Small-angle X-ray scattering study of calmodulin bound to two peptides corresponding to parts of the calmodulin-binding domain of the plasma membrane Ca2+ pump. , 1991, Biochemistry.

[43]  S. Finet,et al.  Second virial coefficient: variations with lysozyme crystallization conditions , 1999 .

[44]  E. Cota,et al.  Folding studies of immunoglobulin-like beta-sandwich proteins suggest that they share a common folding pathway. , 1999, Structure.

[45]  Robert B. Russell,et al.  New roles for structure in biology and drug discovery , 2000, Nature Structural Biology.

[46]  K. Hodgson,et al.  Transient dimer in the refolding kinetics of cytochrome c characterized by small-angle X-ray scattering. , 1999, Biochemistry.

[47]  J. Smith,et al.  How random is a highly denatured protein? , 1994, Biophysical chemistry.

[48]  L. Povirk,et al.  Binding of the nonprotein chromophore of neocarzinostatin to deoxyribonucleic acid. , 1980, Biochemistry.

[49]  D. Engelman,et al.  Mutations can cause large changes in the conformation of a denatured protein. , 1993, Biochemistry.

[50]  Y. Amemiya,et al.  pH-dependent unfolding of aspergillopepsin II studied by small-angle X-ray scattering. , 2000, Biochemistry.

[51]  O. Kratky,et al.  Röntgenuntersuchung gelöster Fadenmoleküle , 1949 .

[52]  D. Baker,et al.  NMR characterization of residual structure in the denatured state of protein L. , 2000, Journal of molecular biology.

[53]  V. Bloomfield,et al.  Light scattering from wormlike chains with excluded volume effects , 1968, Biopolymers.

[54]  S M Gruner,et al.  Compactness of the denatured state of a fast-folding protein measured by submillisecond small-angle x-ray scattering. , 1999, Proceedings of the National Academy of Sciences of the United States of America.

[55]  D. Leeson,et al.  Protein folding and unfolding on a complex energy landscape. , 2000, Proceedings of the National Academy of Sciences of the United States of America.

[56]  D. Madern,et al.  Stability against denaturation mechanisms in halophilic malate dehydrogenase "adapt" to solvent conditions. , 1994, Journal of molecular biology.

[57]  J. D. Cloizeaux Form Factor of an Infinite Kratky-Porod Chain , 1973 .

[58]  C. Dobson,et al.  A partially unfolded structure of the alkaline-denatured state of pepsin and its implication for stability of the zymogen-derived protein. , 2000, Biochemistry.

[59]  V. Favaudon,et al.  Three-dimensional solution structure of apo-neocarzinostatin from Streptomyces carzinostaticus determined by NMR spectroscopy. , 1992, European journal of biochemistry.

[60]  D. Herschlag,et al.  Small angle X-ray scattering reveals a compact intermediate in RNA folding , 2000, Nature Structural Biology.

[61]  G. Fournet,et al.  Small‐Angle Scattering of X‐Rays , 1956 .

[62]  R. Filfil,et al.  Volumetric and spectroscopic characterizations of the native and acid-induced denatured states of staphylococcal nuclease. , 2000, Journal of molecular biology.

[63]  T. Chalikian,et al.  On volume changes accompanying conformational transitions of biopolymers. , 1998, Biopolymers.

[64]  C Chothia,et al.  Conservation of folding and stability within a protein family: the tyrosine corner as an evolutionary cul-de-sac. , 2000, Journal of molecular biology.

[65]  L Serrano,et al.  Similarities between the spectrin SH3 domain denatured state and its folding transition state. , 2000, Journal of molecular biology.

[66]  J. Clarke,et al.  Two proteins with the same structure respond very differently to mutation: the role of plasticity in protein stability. , 2000, Journal of molecular biology.

[67]  D. Svergun,et al.  CRYSOL : a program to evaluate X-ray solution scattering of biological macromolecules from atomic coordinates , 1995 .

[68]  Y. Griko Denaturation Versus Unfolding: Energetic Aspects of Residual Structure in Denatured α-Lactalbumin , 1999, Journal of protein chemistry.

[69]  D I Svergun,et al.  Solution structure of the ternary complex between aminoacyl-tRNA, elongation factor Tu, and guanosine triphosphate. , 1998, Biochemistry.

[70]  C. J. Bond,et al.  Towards a complete description of the structural and dynamic properties of the denatured state of barnase and the role of residual structure in folding. , 2000, Journal of molecular biology.

[71]  J. Clarke,et al.  Folding and stability of a fibronectin type III domain of human tenascin. , 1997, Journal of molecular biology.

[72]  K. Hodgson,et al.  Protein denaturation: a small-angle X-ray scattering study of the ensemble of unfolded states of cytochrome c. , 1998, Biochemistry.

[73]  Analysis of the components present in kinetics (or titration) curves. , 1983, Journal of biochemical and biophysical methods.

[74]  P. Flory Principles of polymer chemistry , 1953 .

[75]  K. Hodgson,et al.  Kinetics of lysozyme refolding: structural characterization of a non-specifically collapsed state using time-resolved X-ray scattering. , 1998, Journal of molecular biology.

[76]  J. Onuchic,et al.  The energy landscape theory of protein folding: insights into folding mechanisms and scenarios. , 2000, Advances in protein chemistry.

[77]  C. Saudan,et al.  Denaturant-induced movement of the transition state of protein folding revealed by high-pressure stopped-flow measurements. , 2000, Proceedings of the National Academy of Sciences of the United States of America.

[78]  M. Desmadril,et al.  Study of thermally and chemically unfolded conformations of a small β-protein by means of small-angle neutron scattering , 2000 .

[79]  Jean Zinn-Justin,et al.  Critical Exponents for the N Vector Model in Three-Dimensions from Field Theory , 1977 .

[80]  S. Jackson,et al.  How do small single-domain proteins fold? , 1998, Folding & design.

[81]  David Baker,et al.  Experiment and theory highlight role of native state topology in SH3 folding , 1999, Nature Structural Biology.

[82]  Multistep denaturation of Borrelia burgdorferi OspA, a protein containing a single-layer beta-sheet. , 1999, Biochemistry.

[83]  P. Vachette,et al.  Stopped-flow solution scattering using synchrotron radiation: apparatus, data collection and data analysis. , 1983, Journal of biochemical and biophysical methods.

[84]  O. Glatter,et al.  19 – Small-Angle X-ray Scattering , 1973 .

[85]  T. Pan,et al.  Mg2+-dependent compaction and folding of yeast tRNAPhe and the catalytic domain of the B. subtilis RNase P RNA determined by small-angle X-ray scattering. , 2000, Biochemistry.