Three-dimensional solution structure of apo-neocarzinostatin from Streptomyces carzinostaticus determined by NMR spectroscopy

Protein-protein interactions and selection: generation of molecule-binding proteins on the basis of tertiary structural information

Antibodies and their fragments are attractive binding proteins because their high binding strength is generated by several hypervariable loop regions, and because high-quality libraries can be prepared from the vast gene clusters expressed by mammalian lymphocytes. Recent explorations of new genome sequences and protein structures have revealed various small, nonantibody scaffold proteins. Accurate structural descriptions of protein-protein interactions based on X-ray and NMR analyses allow us to generate binding proteins by using grafting and library techniques. Here, we review approaches for generating binding proteins from small scaffold proteins on the basis of tertiary structural information. Identification of binding sites from visualized tertiary structures supports the transfer of function by peptide grafting. The local library approach is advantageous as a go-between technique for grafted foreign peptide sequences and small scaffold proteins. The identification of binding sites also supports the construction of efficient libraries with a low probability of denatured variants, and, in combination with the design for library diversity, opens the way to increasing library density and randomized sequence lengths without decreasing density. Detailed tertiary structural analyses of protein-protein complexes allow accurate description of epitope locations to enable the design of and screening for multispecific, high-affinity proteins recognizing multiple epitopes in target molecules.

Cold instability of aponeocarzinostatin and its stabilization by labile chromophore

The conformational stability of aponeocarzinostatin, an all-beta-sheet protein with 113 amino-acid residues, is investigated by thermal-induced equilibrium unfolding between pH 2.0 and 10.0 with and without urea. At room temperature, the protein is stable in a pH range of 4.0-10.0, whereas the stability of the protein drastically decreases below pH 4.0. The thermal unfolding of aponeocarzinostatin is reversible and follows a two-state mechanism. By two-dimensional unfolding studies, the enthalpy change, heat capacity change, and free energy change for unfolding of the protein are estimated. Circular dichroism profiles suggest that this protein undergoes both heat- and cold-induced unfolding. The ellipticity changes at far- and near-UV circular dichroism suggest that the tertiary structure is disrupted but the secondary structure remains folded at low temperatures. Interestingly, the labile enediyne chromophore, which is highly stabilized by the protein, is able to protect the protein against cold-induced unfolding, but not the heat-induced unfolding.

Solution NMR Structure Investigation for Releasing Mechanism of Neocarzinostatin Chromophore from the Holoprotein

Holo-neocarzinostatin (holo-NCS) is a complex protein carrying the anti-tumor active enediyne ring chromophore by a scaffold consisting of an immunoglobulin-like seven-stranded anti-parallel beta-barrel. Because of the labile chromophore reflecting its extremely strong DNA cleavage activity and complete stabilization in the complex, holo-NCS has attracted much attention in clinical use as well as for drug delivery systems. Despite many structural analyses for holo-NCS, the chromophore-releasing mechanism to trigger prompt attacks on the target DNA is still unclear. We determined the three-dimensional structure of the protein and the internal motion by multinuclear NMR to investigate the releasing mechanism. The internal motion studied by 13C NMR methine relaxation experiments showed that the complex has a rigid structure for its loops as well as the beta-barrel in aqueous solution. This agrees with the refined NMR solution structure, which has good convergence in the loop regions. We also showed that the chromophore displayed a similar internal motion as the protein moiety. The structural comparison between the refined solution structure and x-ray crystal structure indicated characteristic differences. Based on the findings, we proposed the chromophore-releasing mechanism by a three-state equilibrium, which sufficiently describes both the strong binding and the prompt releasing of the chromophore. We demonstrated that we could bridge the dynamic properties and the static structure features with simple kinetic assumptions to solve the biochemical function.

Affinity transfer by CDR grafting on a nonimmunoglobulin scaffold

Neocarzinostatin (NCS) is a small "all beta" protein displaying the same overall fold as immunoglobulins. This protein possesses a well-defined hydrophobic core and two loops structurally equivalent to the CDR1 and CDR3 of immunoglobulins. NCS is the most studied member of the enediynechromoprotein family, and is clinically used as an antitumoral agent. NCS has promise as a drug delivery vehicle if new binding specificities could be conferred on its protein scaffold. Previous studies have shown that the binding specificity of the crevasse can be extended to compounds completely unrelated to the natural enediyne chromophore family. We show here that it is possible to introduce new interaction capacities to obtain a protein useful for drug targeting by modifying the immunoglobulin CDR-like loops. We transferred the CDR3 of the VHH chain of camel antilysozyme immunoglobulin to the equivalent site in the corresponding loop of neocarzinostatin. We then evaluated the stability of the resulting structure and its affinity for lysozyme. The engineered NCS-CDR3 presents a structure similar to that of the wild-type NCS, and is stable and efficiently produced. ELISA, ITC, and SPR measurements demonstrated that the new NCS-CDR3 specifically bound lysozyme.

In vitro evolution of the binding specificity of neocarzinostatin, an enediyne-binding chromoprotein

Neocarzinostatin is the most studied member of the enediyne-chromoprotein family, and is clinically used as an antitumoral agent. Neocarzinostatin could be a promising drug delivery vehicle if new binding specificities could be conferred to its protein scaffold. We used in vitro evolution methods to demonstrate that this approach is feasible. We created large libraries containing between 1.7 x 10(8) and 1.4 x 10(9) independent clones, where up to 13 side chains pointing toward the binding crevice were randomly substituted. We then used phage display to select variants that bind to a model ligand (testosterone) which is unrelated to the natural ligand of neocarzinostatin. Several different binders were selected from each library. The corresponding proteins were expressed in Escherichia coli and their affinities and specificities were characterized in detail. K(D) values of about 20 nM were obtained for streptavidin-bound testosterone. The K(D) of selected proteins for free soluble testosterone are between 7 and 55 microM and therefore higher than the K(D) for streptavidin-bound testosterone. The spacer and streptavidin used during selection contributed to the high affinity of the selected binders for the target. Binding studies of 15 different steroids related to testosterone allowed us to determine that C3, 4, 5, 6, and 7 on cycles A and B and the conjugated 3 oxo group of the steroid molecule were essential for molecular recognition. Other testosterone analogues substituted on C1, 2, 9, 11, 15, and 17 were not discriminated from testosterone. These results demonstrate that the binding specificity of this protein family can be extended to compounds that are completely unrelated to the natural enediyne chromophore family. This type of highly expressed, stable proteins with tailored binding properties have a wide potential range of applications.

Key interactions in neocarzinostatin, a protein of the immunoglobulin fold family

Neocarzinostatin (NCS) is a seven-stranded beta-sandwich protein, the folding of which is similar to that of the variable domains of immunoglobulins (Ig). The investigation of the backbone dynamics of apo-NCS [Izadi-Pruneyre et al. (2001) Protein Sci., 10, 2228-2240] enabled us to identify the involvement of long side-chain residues in maintaining the rigidity of this beta-protein. In the perspective of using this protein for drug targeting, this raises the following question: do these residues also play a key role in the stabilization of the beta-sheet? To investigate this problem, various genetically engineered variants were constructed by mutating these residues to amino acids with shorter aliphatic side chains. These substitutions have no effects on the global fold. However, an important destabilization of the protein, higher than that expected for a simple 'large-to-small' substitution of buried hydrophobic residues, is observed for three mutants, V34A, V21A and V95A. Interestingly, the nature of the residues in these positions is highly conserved in the other Ig-like proteins. The absence of an evolutionary relationship between NCS and the other Ig-like proteins strongly suggests that this hydrophobic core is characteristic of the Ig-fold itself.

Dynamic transition associated with the thermal denaturation of a small Beta protein

We studied the temperature dependence of the picosecond internal dynamics of an all-beta protein, neocarzinostatin, by incoherent quasielastic neutron scattering. Measurements were made between 20 degrees C and 71 degrees C in heavy water solution. At 20 degrees C, only 33% of the nonexchanged hydrogen atoms show detectable dynamics, a number very close to the fraction of protons involved in the side chains of random coil structures, therefore suggesting a rigid structure in which the only detectable diffusive movements are those involving the side chains of random coil structures. At 61.8 degrees C, although the protein structure is still native, slight dynamic changes are detected that could reflect enhanced backbone and beta-sheet side-chain motions at this higher temperature. Conversely, all internal dynamics parameters (amplitude of diffusive motions, fraction of immobile scatterers, mean-squared vibration amplitude) rapidly change during heat-induced unfolding, indicating a major loss of rigidity of the beta-sandwich structure. The number of protons with diffusive motion increases markedly, whereas the volume occupied by the diffusive motion of protons is reduced. At the half-transition temperature (T = 71 degrees C) most of backbone and beta-sheet side-chain hydrogen atoms are involved in picosecond dynamics.

Solution Structure of a Novel Chromoprotein Derived from Apo-Neocarzinostatin and a Synthetic Chromophore

The natural complex Neocarzinostatin comprises a labile chromophore noncovalently bound to an 11.2 kDa protein. We present the first high-resolution structure of a novel complex derived from the recombinant apoprotein bound to a non-natural synthetic chromophore. Fluorescence and nuclear magnetic resonance spectroscopy were used to probe the strength and location of binding. Binding occurred in a location similar to that observed for the chromophore in the natural Neocarzinostatin complex, but with a distinct orientation. These results provide structural evidence that the apoprotein can readily accommodate small druglike entities, other than the natural chromophore within its binding cleft. The clinical use of the natural complex described by others, together with the results reported here, suggests potential applications for small molecule binding by apo-Neocarzinostatin.

Key interactions in the immunoglobulin-like structure of apo-neocarzinostatin: evidence from nuclear magnetic resonance relaxation data and molecular dynamics simulations

The three-dimensional structure of apo-neocarzinostatin (apo-NCS, MW: ca.11000, antitumoral chromophore carrier protein) is based on a seven-stranded antiparallel beta-sandwich, very similar to the immunoglobulin folding domain. We investigated the backbone dynamics of apo-NCS by (13)C-NMR relaxation measurements and molecular dynamics simulation. Model-free parameters determined from the experimental data are compared with a 1.5-nsec molecular simulation of apo-NCS in aqueous solution. This comparison provides an accurate description of both local and collective movements within the protein. This analysis enabled us to correlate dynamic processes with key interactions of this beta-protein. Local motions that could be relevant for the intermolecular association with the ligand are also described.

Solution structures of C-1027 apoprotein and its complex with the aromatized chromophore

C-1027 is one of the most potent antitumor antibiotic chromoproteins, and is a 1:1 complex of an enediyne chromophore having DNA-cleaving ability and a carrier apoprotein. The three-dimensional solution structures of the 110 residue (10.5 kDa) C-1027 apoprotein and its complex with the aromatized chromophore have been determined separately by homonuclear two-dimensional nuclear magnetic resonance methods. The apoprotein is mainly composed of three antiparallel beta-sheets: four-stranded beta-sheet (43-45, 52-54; 30-38; 92-94; 104-106), three-stranded beta-sheet (4-6; 17-22; 61-66), and two-stranded beta-sheet (70-72; 83-85). The overall structure of the apoprotein is very similar to those of other chromoprotein apoproteins, such as neocarzinostatin and kedarcidin. A hydrophobic pocket with approximate dimensions of 14 A x 12 A x 8 A is formed by the four-stranded beta-sheet and the three loops (39-42; 75-79; 97-100). The holoprotein (complex form with the aromatized chromophore) structure reveals that the aromatized chromophore is bound to the hydrophobic pocket found in the apoprotein. The benzodihydropentalene core of the chromophore is located in the center of the pocket and other substituents (beta-tyrosine, benzoxazine, and aminosugar moieties) are arranged around the core. Major binding interactions between the apoprotein and the chromophore are likely the hydrophobic contacts between the core of the chromophore and the hydrophobic side-chains of the pocket-forming residues, which is supplemented by salt bridges and/or hydrogen bonds. Based on the holoprotein structure, we propose possible mechanisms for the stabilization and the release of chromophore by the apoprotein.

Heat-induced unfolding of neocarzinostatin, a small all-β protein investigated by small-angle X-ray scattering 1 1Edited by M. F. Moody

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.

Characterization of the denatured states distribution of neocarzinostatin by small-angle neutron scattering and differential scanning calorimetry

The denatured states of a small globular protein, apo-neocarzinostatin (NCS), have been characterized using several techniques. Structural properties were investigated by optical spectroscopy techniques and small-angle neutron scattering (SANS), as a function of guanidinium chloride (GdmCl) concentration. SANS experiments show that in heavy water, the protein keeps its native size at GdmCl concentrations below 2.5 M. A sharp transition occurs at about 3.6 M GdmCl, and NCS behaves like an excluded volume chain above 5 M. The same behavior is observed in deuterated buffer by fluorescence and circular dichroism measurements. For the H(2)O buffer, the transition occurs with lower concentration of denaturant, the shift being about 0.6 M. 8-Anilino-1-naphthalenesulfonate (ANS) was used as a hydrophobic fluorescent probe for studying the early stages of protein unfolding. Protein denaturation modifies the fluorescence intensity of ANS, a maximum of intensity being detected close to 2 M GdmCl in hydrogenated buffer, which shows the existence of at least one intermediate state populated at the beginning of the unfolding pathway. Differential scanning calorimetry (DSC) was used to obtain thermodynamic values for NCS denaturation. The melting curves recorded between 20 and 90 degrees C in the presence of various GdmCl concentrations (0-3 M) cannot be explained by a simple two-state model. Altogether, the data presented in this paper suggest that before unfolding the protein explores a distribution of states which is centered around compact states at denaturant concentrations below 2 M in H(2)O, and then shifts to less structured states by increasing denaturant concentrations.

Release of the neocarzinostatin chromophore from the holoprotein does not require major conformational change of the tertiary and secondary structures induced by trifluoroethanol

Neocarzinostatin is a potent enediyne antitumor antibiotic complex in which a chromophore is noncovalently bound to a carrier protein. The protein regulates availability of the drug by proper release of the biologically active chromophore. To understand the physiological mechanism of the drug delivery system, we have examined the trifluoroethanol (TFE)-induced conformational changes of the protein with special emphasis on their relation to the release of the chromophore from holoneocarzinostatin. The effect of the alpha helix-inducing agent, TFE, on all the beta-sheet neocarzinostatin proteins was studied by circular dichroism, fluorescence, and (1)H NMR studies. By using binding of anilinonaphthalene sulfonic acid as a probe, we observed that the protein exists in a stable, partially structured intermediate state around 45-50% TFE, which is consistent with the results from tryptophan fluorescence and circular dichroism studies. The native state is stable until 20% TFE and is half-converted into the intermediate state at 30% TFE, which starts to collapse beyond 50%. High pressure liquid chromatographic analysis of the release of the chromophore caused by TFE treatment at 0 degrees C suggests that the release process, which occurs below 20% TFE, does not result from an observable conformational change in the protein. Kinetic measurements of the release of chromophore at 25 degrees C reveal that TFE does stimulate the rate of release, which increases sharply at 15% and reaches a maximum at 20% TFE, although no major secondary or tertiary structural change of the carrier protein is observed under these same conditions. Our data suggest that chromophore release results from a fluctuation of the protein structure that is stimulated by TFE. Complete release of the chromophore occurs at TFE concentrations where no overall observable unfolding of the apoprotein is seen. Thus, the results suggest that denaturation of the protein by TFE is not a necessary step for release of the tightly bound chromophore.

Reinvestigation of the proteolytic activity of neocarzinostatin

Neocarzinostatin (NCS) is the most studied member of a family of chromoproteins secreted by a range of actinomycetes species. It has been proposed that in addition to their antitumoral activity related to the bound chromophores, this group of related proteins could be a secreted proteases superfamily. With the aim of dissecting the molecular basis of the proteolytic activity of NCS, an expression system allowing efficient expression of apo-NCS in Escherichia coli was constructed. The recombinant protein was properly folded and functional. Its histone-specific proteolytic activity was similar to the activity described for the natural protein. Further analyses unambiguously demonstrated that the proteolytic activity could be physically separated from NCS. This activity is therefore due not to NCS itself but to minor contaminating proteases, the nature of which differed in the recombinant and natural NCS preparations. The histone degradation test commonly used to monitor proteolytic activity is extremely sensitive and may easily generate false-positive results. These results strongly suggest that the possible proteolytic activity of the proteins of this family should be critically reconsidered.

Simple and accurate determination of global tau(R) in proteins using (13)C or (15)N relaxation data

In the study of protein dynamics by (13)C or (15)N relaxation measurements different models from the Lipari-Szabo formalism are used in order to determine the motion parameters. The global rotational correlation time tau(R) of the molecule must be estimated prior to the analysis. In this Communication, the authors propose a new approach in determining an accurate value for tau(R) in order to realize the best fit of R(2) for the whole sequence of the protein, regardless of the different type of motions atoms may experience. The method first determines the highly structured regions of the sequence. For each corresponding site, the Lipari-Szabo parameters are calculated for R(1) and NOE, using an arbitrary value for tau(R). The chi(2) for R(2), summed over the selected sites, shows a clear minimum, as a function of tau(R). This minimum is used to better estimate a proper value for tau(R).

Assignment of the protonated 13C resonances of apo-neocarzinostatin by 2D heteronuclear NMR spectroscopy at natural abundance

Nearly complete assignment of the protonated carbon resonances of apo-neocarzinostatin, a 113-amino acid antitumor antibiotic carrier protein, has been achieved at natural 13C abundance using heteronuclear 2D experiments. Most of the cross peaks in the proton-carbon correlation map were identified by the combined use of HMQC, HMQC-RELAY and HMQC-NOESY spectra, using already published proton chemical shifts. However, double-DEPT and triple-quantum experiments had to be performed for the edition of CH and CH2 side-chain groups, respectively, which were hardly visible on HMQC-type maps. The triple-quantum pulse sequence was adapted from its original scheme to be applicable to a natural abundance sample. The correlation between carbon chemical shifts and the apo-neocarzinostatin structure is discussed. In particular, 13C alpha secondary shifts correlate well with the backbone conformation. These shifts also yield information about the main-chain flexibility of the protein. Assignments reported herein will be used further for interpretation of carbon relaxation times in a study of the internal dynamics of apo-neocarzinostatin.

Crystal structure of neocarzinostatin, an antitumor protein-chromophore complex

Structures of the protein-chromophore complex and the apoprotein form of neocarzinostatin were determined at 1.8 angstrom resolution. Neocarzinostatin is composed of a labile chromophore with DNA-cleaving activity and a stabilizing protein. The chromophore displays marked nonlinearity of the triple bonds and is bound noncovalently in a pocket formed by the two protein domains. The chromophore pi-face interacts with the phenyl ring edges of Phe52 and Phe78. The amino sugar and carbonate groups of the chromophore are solvent exposed, whereas the epoxide, acetylene groups, and carbon C-12, the site of nucleophilic thiol addition during chromophore activation, are unexposed. The position of the amino group of the chromophore carbohydrate relative to C-12 supports the idea that the amino group plays a role in thiol activation.

Crystal structure of apo-neocarzinostatin at 0.15-nm resolution

The three-dimensional structure of apo-neocarzinostatin, an antitumour antibiotic protein isolated from Streptomyces carzinostaticus, has been determined by X-ray diffraction at 0.15-nm resolution and refined to R = 17.2%. The crystal structure of neocarzinostatin is similar to that of the related proteins actinoxanthin and macromomycin. It is also in good agreement with the solution structure determined by NMR spectroscopy. The protein molecule consists of a seven-stranded antiparallel beta-sandwich and a smaller lobe formed by two beta-ribbons. A deep cleft between the two lobes is a putative chromophore binding site. Side chains of Trp39, Leu45, Phe52, Phe78 and the disulphide Cys37-Cys47 aligning the binding cleft in neocarzinostatin suggest the importance of hydrophobic interactions in stabilizing the chromophore molecule. Comparison of the atomic models of neocarzinostatin, actinoxanthin and macromomycin reveals functional residues which might determine specificity towards different chromophores.

The seven-stranded beta-barrel structure of apo-neocarzinostatin as compared to the immunoglobulin domain

The three-dimensional structure of apo-NCS, as revealed by proton NMR, is based on an antiparallel seven-stranded beta-barrel. This fold is frequently encountered in protein structures, especially for immunoglobulin domains. The strands forming the barrel are joined by flexible loops of which three are implicated in the ligand binding site of these proteins. In this paper a preliminary comparison is given with respect to the static and dynamic properties of both the constant beta-barrel and the active loops for apo-NCS and the variable VH domain of an immunoglobulin Fab' fragment.