Different effects of 4-hydroxyproline and 4-fluoroproline on the stability of collagen triple helix

Differential scanning calorimetry (DSC) analyses of a series of collagen model peptides suggest that 4-hydroxyproline (Hyp) and 4-fluoroproline (fPro) have different effects on the stability of the collagen triple helices according to the sequence of amino acids and stereochemistry at the 4 positions of these imino acids. The thermodynamic parameters indicate that the enhanced stabilities are classified into two different types: the enthalpy term is primarily responsible for the enhanced stability of the triple helix of (Pro-Hyp(R)-Gly)(10), whereas the entropy term dominates the enhanced stability of (Pro-fPro(R)-Gly)(10). The difference between the molecular volumes observed in solution and intrinsic molecular volumes calculated from the crystal structure indicates the different hydration states of these peptides. (Pro-Hyp(R)-Gly)(10) is highly hydrated compared to (Pro-Pro-Gly)(10), which contributes to the larger enthalpy. In contrast, the volume of (Pro-fPro(R)-Gly)(10) shows a smaller degree of hydration than that of (Pro-Pro-Gly)(10). The entropic cost of forming the triple helix of the fPro-containing peptides is compensated by a decrease in an ordered structure of water molecules surrounding the peptide molecule, although the contribution of enthalpy originating from the hydration is reduced. These arguments about the different contribution of entropic and enthalpic terms were successfully applied to interpret the stability of the triple helix of (fPro(S)-Pro-Gly)(10) as well.     

Collagen-like triple helix formation of synthetic (Pro-Pro-Gly)10 analogues: (4(S)-hydroxyprolyl-4(R)-hydroxyprolyl-Gly)10, (4(R)-hydroxyprolyl-4(R)-hydroxyprolyl-Gly)10 and (4(S)-fluoroprolyl-4(R)-fluoroprolyl-Gly)10.

For the rational design of a stable collagen triple helix according to the conventional rule that the pyrrolidine puckerings of Pro, 4-hydroxyproline (Hyp) and 4-fluoroproline (fPro) should be down at the X-position and up at the Y-position in the X-Y-Gly repeated sequence for enhancing the triple helix propensities of collagen model peptides, a series of peptides were prepared in which X- and Y-positions were altogether occupied by Hyp(R), Hyp(S), fPro(R) or fPro(S). Contrary to our presumption that inducing the X-Y residues to adopt a down-up conformation would result in an increase in the thermal stability of peptides, the triple helices of (Hyp(S)-Hyp(R)-Gly)(10) and (fPro(S)-fPro(R)-Gly)(10) were less stable than those of (Pro-Hyp(R)-Gly)(10) and (Pro-fPro(R)-Gly)(10), respectively. As reported by B?chinger's and Zagari's groups, (Hyp(R)-Hyp(R)-Gly)(10) which could have an up-up conformation unfavorable for the triple helix, formed a triple helix that has a high thermal stability close to that of (Pro-Hyp(R)-Gly)(10). These results clearly show that the empirical rule based on the conformational preference of pyrrolidine ring at each of X and Y residues should not be regarded as still valid, at least for predicting the stability of collagen models in which both X and Y residues have electronegative groups at the 4-position.     

The crystal structure of the collagen-like polypeptide (glycyl-4(R)-hydroxyprolyl-4(R)-hydroxyprolyl)9 at 1.55 A resolution shows up-puckering of the proline ring in the Xaa position

The collagen triple helix is characterized by the repeating sequence motif Gly-Xaa-Yaa, where Xaa and Yaa are typically proline and (2S,4R)-4-hydroxyproline (4(R)Hyp), respectively. Previous analyses have revealed that H-(Pro-4(R)Hyp-Gly)(10)-OH forms a stable triple helix, whereas H-(4(R)Hyp-Pro-Gly)(10)-OH does not. Several theories have been put forth to explain the importance of proline puckering and conformation in triple helix formation; however, the details of how they affect triple helix stability are unknown. Underscoring this, we recently demonstrated that the polypeptide Ac-(Gly-4(R)Hyp-4(R)Hyp)(10)-NH(2) forms a triple helix that is more stable than Ac-(Gly-Pro-4(R)Hyp)(10)-NH(2). Here we report crystal the structure of the H-(Gly-4(R)Hyp-4(R)Hyp)(9)-OH peptide at 1.55 A resolution. The puckering of the Yaa position 4(R)Hyp in this structure is up (Cgamma exo), as has been found in other collagen peptide structures. Notably, however, the 4(R)Hyp in the Xaa position also takes the up pucker, which is distinct from all other collagen structures. Regardless of the notable difference in the Xaa proline puckering, our structure still adopts a 7/2 superhelical symmetry similar to that observed in other collagen structures. Thus, the basis for the observed differences in the thermodynamic data of the triple helix<--> coil transition between our peptide and other triple helical peptides likely results from contributions from the unfolded state. Indeed, the unfolded state of the H-(Gly-4(R)Hyp-4(R)Hyp)(9)-OH peptide seems to be stabilized by a preformed polyproline II helix in each strand, which could be explained by the presence of a unique repeating intra-strand water-mediated bridge observed in the H-(Gly-4(R)Hyp-4(R)Hyp)(9)-OH structure, as well as a higher amount of trans peptide bonds.     

Computed free energy differences between point mutations in a collagen-like peptide

We studied the results of mutating alanine --> glycine at three positions of a collagen-like peptide in an effort to develop a computational method for predicting the energetic and structural effects of a single point genetic mutation in collagen, which is associated with the clinical diagnosis of Osteogenesis Imperfecta (OI). The differences in free energy of denaturation were calculated between the collagen-like peptides [(POG)(4)(POA)(POG)(4)](3) and [(POG)(10)](3) (POG: proline-hydroxyproline-glycine).* Our computational results, which suggest significant destabilization of the collagen-like triple-helix upon the glycine --> alanine mutations, correlate very well with the experimental free energies of denaturation. The robustness of our collagen-like peptide model is shown by its reproduction of experimental results with both different simulation paths and different lengths of the model peptide. The individual free energy for each alanine --> glycine mutation (and the reverse free energy, glycine --> alanine mutation) in the collagen-like peptide has been calculated. We find that the first alanine introduced into the triple helix causes a very large destabilization of the helix, but the last alanine introduced into the same position of an adjacent chain causes a very small change in the peptide stability. Thus, our results demonstrate that each mutation does not contribute equally to the free energy. We find that the sum of the calculated individual residues' free energy can accurately model the experimental free energy for the whole peptide.     

Hydroxylation-induced stabilization of the collagen triple helix. Acetyl-(glycyl-4(R)-hydroxyprolyl-4(R)-hydroxyprolyl)(10)-NH(2) forms a highly stable triple helix

The collagen triple helix is one of the most abundant protein motifs in animals. The structural motif of collagen is the triple helix formed by the repeated sequence of -Gly-Xaa-Yaa-. Previous reports showed that H-(Pro-4(R)Hyp-Gly)(10)-OH (where '4(R)Hyp' is (2S,4R)-4-hydroxyproline) forms a trimeric structure, whereas H-(4(R)Hyp-Pro-Gly)(10)-OH does not form a triple helix. Compared with H-(Pro-Pro-Gly)(10)-OH, the melting temperature of H-(Pro-4(R)Hyp-Gly)(10)-OH is higher, suggesting that 4(R)Hyp in the Yaa position has a stabilizing effect. The inability of triple helix formation of H-(4(R)Hyp-Pro-Gly)(10)-OH has been explained by a stereoelectronic effect, but the details are unknown. In this study, we synthesized a peptide that contains 4(R)Hyp in both the Xaa and the Yaa positions, that is, Ac-(Gly-4(R)Hyp-4(R)Hyp)(10)-NH(2) and compared it to Ac-(Gly-Pro-4(R)Hyp)(10)-NH(2), and Ac-(Gly-4(R)Hyp-Pro)(10)-NH(2). Ac-(Gly-4(R)Hyp-4(R)Hyp)(10)-NH(2) showed a polyproline II-like circular dichroic spectrum in water. The thermal transition temperatures measured by circular dichroism and differential scanning calorimetry were slightly higher than the values measured for Ac-(Gly-Pro-4(R)Hyp)(10)-NH(2) under the same conditions. For Ac-(Gly-4(R)Hyp-4(R)Hyp)(10)-NH(2), the calorimetric and the van't Hoff transition enthalpy DeltaH were significantly smaller than that of Ac-(Gly-Pro-4(R)Hyp)(10)-NH(2). We postulate that the denatured states of the two peptides are significantly different, with Ac-(Gly-4(R)Hyp-4(R)Hyp)(10)-NH(2) forming a more polyproline II-like structure instead of a random coil. Two-dimensional nuclear Overhauser effect spectroscopy suggests that the triple helical structure of Ac-(Gly-4(R)Hyp-4(R)Hyp)(10)-NH(2) is more flexible than that of Ac-(Gly-Pro-4(R)Hyp)(10)-NH(2). This is confirmed by the kinetics of amide (1)H exchange with solvent deuterium of Ac-(Gly-4(R)Hyp-4(R)Hyp)(10)-NH(2), which is faster than that of Ac-(Gly-Pro-4(R)Hyp)(10)-NH(2). The higher transition temperature of Ac-(Gly-4(R)Hyp-4(R)Hyp)(10)-NH(2), can be explained by the higher trans/cis ratio of the Gly-4(R)Hyp peptide bonds than that of the Gly-Pro bonds, and this ratio compensates for the weaker interchain hydrogen bonds.     

Synthesis, structure and biomimetic properties of Cu(II)-Cu(II) and Cu(II)-Zn(II) binuclear complexes: possible models for the chemistry of Cu-Zn superoxide dismutase

Four imidazolate-bridged binuclear copper(II)-copper(II) and copper(II)-zinc(II) complexes viz., [(Bipy)(2)Cu-Im-Cu(Bipy)(2)](ClO(4))(3).CH(3)OH, [(Phen)(2)Cu-Im-Cu(Phen)(2)](BF(4))(3).2CH(3)OH, [(Bipy)(2)Cu-Im-Zn(Bipy)(2)](BF(4))(3), and [(Phen)(2)Cu-Im-Zn(Phen)(2)](BF(4))(3), (Bipy=2,2'-Bipyridyl, Phen=1-10-Phenanthroline and Im=imidazolate ion) were synthesized as a possible models for superoxide dismutase (SOD). Complex [(Bipy)(2)Cu-Im-Cu(Bipy)(2)](ClO(4))(3).CH(3)OH has been structurally characterized. This complex crystallizes in the triclinic space group P1, with the unit parameters a=8.88(5) A, b=13.79(17) A, c=20.18(18) A, alpha=76.424(8)(o), beta=85.888(6)(o), gamma=82.213(7). The metal-nitrogen bond length from 1.972-2.273 A and the distance Cu-Cu is 5.92 A. The five-coordinate geometry about the copper(II) ion is square pyramidal. Magnetic moment and electron paramagnetic resonance (e.p.r.) spectral measurements of the homobinuclear complexes have shown an antiferromagnetic exchange interaction. From the e.p.r. and UV-Vis spectral measurement studies, these complexes have been found to be stable (pH 8.5-10.5 for 1, 10.5 for 2,3 and 8.5 for 4). These complexes catalyse the dismutation of superoxide radical (O(2)(-)) at biological pH. All the observations indicate that these complexes act as good possible models for superoxide dismutase.     

Single diastereomers of unsymmetrical tris-spirocyclic cyclotriphosphazenes based on 1,1'-bi-2-naphthol--synthesis and structures

Diastereoselective synthesis and characterization of chiral unsymmetrical tris-spirocyclic cyclotriphosphazenes based on chiral 1,1'-bi-2-naphthol (BINOL) are reported. Specifically, the chiral compounds (-)N(3)P(3)[1,1'-O(2)(C(10)H(6))(2)](O-2,2'C(6)H(4)-C(6)H(4)O)Cl(2) [(-)-4] and (-)N(3)P(3)[1,1'-O(2)(C(10)H(6))(2)](OCH(2)CH(2)NMe)(2) [(-)-5] are prepared by starting with the chiral mono-spiro compound (-)N(3)P(3)[1,1'-O(2)(C(10)H(6))(2)]Cl(4) [(-)-3]. Synthesis of four other chiral spirocyclics, N(3)P(3)[1,1'-O(2)(C(10)H(6))(2)](OCH(2)CH(2) NMe)(O-2,2'C(6)H(4)-C(6)H(4)O)[(-)-6 and (+)-6], N(3)P(3)[1,1'-O(2)(C(10)H(6))(2)](NMe(2))(4) [(-)-7], N(3)P(3)[1,1'-O(2)(C(10)H(6))(2)](O-2,2'C(6)H(4)-C(6)H(4)O)(NMeCH(2)CH(2)OH)(2) [(-)-8 and (+)-8], and N(3)P(3)[1,1'-O(2)(C(10)H(6))(2)](O-2,2'C(6)H(4)-C(6)H(4)O)[NHCH(2)CH(2)CH(2)Si(OEt)(3)](2) (9) is also reported herein. Compounds 4-6 are obtained in the solid state diastereoselectively and their X-ray structures have been determined and discussed. The diastereoselectivity is also shown by structural characterization of two distinct isomers in the case of 6 [(-)-6 and (+)-6, respectively] by starting with precursor of 3 having (R) or (S)-BINOL residue. The (1)H NMR spectra of 7 and 8 exhibit doublets with virtual coupling for the methyl protons, consistent with the chiral nature of the binaphthoxy residue. The potential of 9, which hydrolyzes readily in CDCl(3) solution, as a useful precursor for chiral polymer applications is highlighted.     

Hydroxylation-induced stabilization of the collagen triple helix. Further characterization of peptides with 4(R)-hydroxyproline in the Xaa position

4(R)-Hydroxyproline in the Yaa position of the -Gly-Xaa-Yaa-repeated sequence of collagen plays a crucial role in the stability of the triple helix. Since the peptide (4(R)-Hyp-Pro-Gly)10 does not form a triple helix, it was generally believed that polypeptides with a -Gly-4(R)-Hyp-Yaa-repeated sequence do not form a triple helix. Recently, we found that acetyl-(Gly-4(R)-Hyp-Thr)10-NH2 forms a triple helix in aqueous solutions. To further study the role of 4(R)-hydroxyproline in the Xaa position, we made a series of acetyl-(Gly-4(R)-Hyp-Yaa)10-NH2 peptides where Yaa was alanine, serine, valine, and allo-threonine. We previously hypothesized that the hydroxyl group of threonine might form a hydrogen bond to the hydroxyl group of 4(R)hydroxyproline. In water, only the threonine- and the valine-containing peptides were triple helical. The remaining peptides did not form a triple helix in water. In 1,2- and in 1,3-propanediol at 4 degrees C, all the soluble peptides were triple helical. From the transition temperature of the triple helices, it was found that among the examined residues, threonine was the most stable residue in the acetyl-(Gly-4(R)-Hyp-Yaa)10-NH2 peptide. The transition temperatures of the valine- and allo-threonine-containing peptides were 10 degrees lower than those of the threonine peptide. Surprisingly, the serine-containing peptide was the least stable. These results indicate that the stability of these peptides depends on the presence of a methyl group as well as the hydroxyl group and that the stereo configuration of the two groups is essential for the stability. In the threonine peptide, we hypothesize that the methyl group shields the interchain hydrogen bond between the glycine and the Xaa residue from water and that the hydroxyl groups of threonine and 4(R)hydroxyproline can form direct or water-mediated hydrogen bonds.     

The triple helical structure and stability of collagen model peptide with 4(S)-hydroxyprolyl-Pro-Gly units

Extensive studies on the structure of collagen have revealed that the hydroxylation of Pro residues in a variety of model peptides with the typical (X-Y-Gly)(n) repeats (X and Y: Pro and its analogues) represents one of the major factors influencing the stability of triple helices. While(2S,4R)-hydroxyproline (Hyp) at the position Y stabilizes the triple helix, (2S,4S)-hydroxyproline (hyp) at the X-position destabilizes the helix as demonstrated that the triple helix of (hyp-Pro-Gly)(15) is less stable than that of (Pro-Pro-Gly)(15) and that a shorter peptide (hyp-Pro-Gly)(10) does not form the helix. To clarify the role of the hydroxyl group of Pro residues to play in the stabilization mechanism of the collagen triple helix, we synthesized and crystallized a model peptide (Pro-Hyp-Gly)(4) -(hyp-Pro-Gly)(2) -(Pro-Hyp-Gly)(4) and analyzed its structure by X-ray crystallography and CD spectroscopy. In the crystal, the main-chain of this peptide forms a typical collagen like triple helix. The majority of hyp residues take down pucker with exceptionally shallow angles probably to relieve steric hindrance, but the remainders protrude the hydroxyl group toward solvent with the less favorable up pucker to fit in a triple helix. There is no indication of the existence of an intra-molecular hydrogen bond between the hydroxyl moiety and the carbonyl oxygen of hyp supposed to destabilize the triple helix. We also compared the conformational energies of up and down packers of the pyrrolidine ring in Ac-hyp-NMe(2) by quantum mechanical calculations.     

Synthesis, structure and luminescence studies of heterometallic gold(I)-copper(I) and -silver(I) alkynyl clusters/aggregates.

A series of pentanuclear gold(I)-copper(I) and -silver(I) mixed-metal alkynyl complexes, [(n)Bu(4)N][Au(3)M(2)(C triple bond CC(6)H(4)R-p)(6)] [M = Cu, R = OMe, O(n)Bu, O(n)Hex, Me, Et; M = Ag, R = Et, O(n)Hex] have been synthesized. The complexes were found to be emissive both in the solid state and in fluid solutions. DFT calculations at the B3LYP level of theory were performed on [Au(3)M(2)(C triple bond CC(6)H(4)Me-p)(6)](-) (M = Cu, Ag) to provide an understanding on the electronic structure of the complexes.     

The peptides acetyl-(Gly-3(S)Hyp-4(R)Hyp)10-NH2 and acetyl-(Gly-Pro-3(S)Hyp)10-NH2 do not form a collagen triple helix

Hydroxylation of proline residues in the Yaa position of the Gly-Xaa-Yaa repeated sequence to 4(R)-hydroxyproline is essential for the formation of the collagen triple helix. A small number of 3(S)-hydroxyproline residues are present in most collagens in the Xaa position. Neither the structural nor a biological role is known for 3(S)-hydroxyproline. To characterize the structural role of 3(S)-hydroxyproline, the peptide Ac-(Gly-3(S)Hyp-4(R)Hyp)10-NH2 was synthesized and analyzed by circular dichroism spectroscopy, analytical ultracentrifugation, and 1H nuclear magnetic resonance spectroscopy. At 4 degrees C in water the circular dichroism spectrum indicates that this peptide was in a polyproline-II-like secondary structure with a positive peak at 225 nm similar to Ac-(Gly-Pro-4(R)Hyp)10-NH2. The positive peak at 225 nm almost linearly decreases with increasing temperature to 95 degrees C without an obvious transition. Although the peptide Ac-(Gly-Pro-4(R)Hyp)10-NH2 forms a trimer at 10 degrees C, sedimentation equilibrium experiments indicate that Ac-(Gly-3(S)Hyp-4(R)Hyp)10-NH2 is a monomer in water at 7 degrees C. To study the role of 3(S)-hydroxyproline in the Yaa position, we synthesized Ac-(Gly-Pro-3(S)Hyp)10-NH2. This peptide also does not form a triple helix in water. 1H Nuclear magnetic resonance spectroscopy data (including line widths and nuclear Overhauser effects) are entirely consistent, with neither Ac-(Gly-3(S)Hyp-4(R)Hyp)10-NH2 nor Ac-(Gly-Pro-3(S)Hyp)10-NH2 forming a triple helix in water. Therefore 3(S)-hydroxyproline destabilizes the collagen triple helix in either position. In contrast, when 3(S)-hydroxyproline is inserted as a guest in the highly stable -Gly-Pro-4(R)Hyperepeated host sequence, Ac-(Gly-Pro-4(R)Hyp)3-Gly-3(S)Hyp-4(R)Hyp-(Gly-Pro-4(R)Hyp)4-Gly-Gly-NH2 forms as stable a trimer (Tm=49.6 degrees C) as Ac-(Gly-Pro-4(R)Hyp)8-Gly-Gly-NH2 (Tm=48.9 degrees C). Given that Ac-(Gly-Pro-4(R)Hyp)3-Gly-4(R)Hyp-Pro-(Gly-Pro-4(R)Hyp)4-Gly-Gly-NH2 forms a triple helix nearly as stable as the above two peptides (Tm=45.0 degrees C) and the knowledge that Ac-(Gly-4(R)Hyp-Pro)10-NH2 does not form a triple helix, we conclude that the host environment dominates the structure of host-guest peptides and that these peptides are not necessarily accurate predictors of triple helical stability.     

Folding and misfolding of the collagen triple helix: Markov analysis of molecular dynamics simulations

Folding and misfolding of the collagen triple helix are studied through molecular dynamics simulations of two collagenlike peptides, [(POG)₁₀]₃ and [(POG)₄POA(POG)₅]₃, which are models for wild-type and mutant collagen, respectively. To extract long time dynamics from short trajectories, we employ Markov state models. By analyzing thermodynamic and kinetic quantities calculated from the Markov state models, we examine folding mechanisms of the collagen triple helix and consequences of glycine mutations. We find that the C-to-N zipping of the collagen triple helix must be initiated by a nucleation event consisting of formation of three stable hydrogen bonds, and that zipping through a glycine mutation site requires a renucleation event which also consists of formation of three stable hydrogen bonds. Our results also suggest that slow kinetics, rather than free energy differences, is mainly responsible for the stability of the collagen triple helix.     

The crystal structure of a collagen-like polypeptide with 3(S)-hydroxyproline residues in the Xaa position forms a standard 7/2 collagen triple helix

Collagen has a triple helical structure comprising strands with a repeating Xaa-Yaa-Gly sequence. L-Proline (Pro) and 4(R)-hydroxyl-L-proline (4(R)Hyp) residues are found most frequently in the Xaa and Yaa positions. However, in natural collagen, 3(S)-hydroxyl-L-proline (3(S)Hyp) occurs in the Xaa positions to varying extents and is most common in collagen types IV and V. Although 4(R)Hyp residues in the Yaa positions have been shown to be critical for the formation of a stable triple helix, the role of 3(S)Hyp residues in the Xaa position is not well understood. Indeed, recent studies have demonstrated that the presence of 3(S)Hyp in the Xaa positions of collagen-like peptides actually has a destabilizing effect relative to peptides with Pro in these locations. Whether this destabilization is reflected in a local unfolding or in other structural alterations of the collagen triple helix is unknown. Thus, to determine what effect the presence of 3(S)Hyp residues in the Xaa positions has on the overall conformation of the collagen triple helix, we determined the crystal structure of the polypeptide H-(Gly-Pro-4(R)Hyp)3-(Gly-3(S)Hyp-4(R)Hyp)2-(Gly-Pro-4(R)Hyp)4-OH to 1.80 A resolution. The structure shows that, despite the presence of the 3(S)Hyp residues, the peptide still adopts a typical 7/2 superhelical symmetry similar to that observed in other collagen structures. The puckering of the Xaa position 3(S)Hyp residues, which are all down (Cgamma-endo), and the varphi/psi dihedral angles of the Xaa 3(S)Hyp residues are also similar to those of typical collagen Pro Xaa residues. Thus, the presence of 3(S)Hyp in the Xaa positions does not lead to large structural alterations in the collagen triple helix.     

4-chloroprolines: synthesis, conformational analysis, and effect on the collagen triple helix

Collagen is an abundant, triple-helical protein comprising three strands of the repeating sequence: Xaa-Yaa-Gly. (2S)-Proline and (2S,4R)-4-hydroxyproline (Hyp) are common in the primary structure of collagen. Here, we use nonnatural proline derivatives to reveal determinants of collagen stability. Specifically, we report high-yielding syntheses of (2S,4S)-4-chloroproline (clp) and (2S,4R)-4-chloroproline (Clp). We find that the molecular structure of Ac-Clp-OMe in the solid state is virtually identical to that of Ac-Hyp-OMe. In contrast, the conformational properties of Ac-clp-OMe are similar to those of Ac-Pro-OMe. Ac-Clp-OMe has a stronger preference for a trans amide bond than does Ac-Pro-OMe, whereas Ac-clp-OMe has a weaker preference. (Pro-Clp-Gly)(10) forms triple helices that are significantly more stable than those of (Pro-Pro-Gly)(10). Triple helices of (clp-Pro-Gly)(10) have stability similar to those of (Pro-Pro-Gly)(10). Unlike (Pro-Clp-Gly)(10) and (clp-Pro-Gly)(10), (clp-Clp-Gly)(10) does not form a stable triple helix, presumably due to a deleterious steric interaction between proximal chlorines on different strands. These data, which are consistent with previous work on 4-fluoroprolines and 4-methylprolines, support the importance of stereoelectronic and steric effects in the stability of the collagen triple helix and provide another means to modulate that stability. (     

Delivery of floxuridine derivatives to cancer cells by water-soluble organometallic cages

The self-assembly of 2,4,6-tris(pyridin-4-yl)-1,3,5-triazine (tpt) triangular panels with p-cymene (pPr(i)C(6)H(4)Me) ruthenium building blocks and 2,5-dioxydo-1,4-benzoquinonato (dobq) or 5,8-dioxydo-1,4-naphthoquinonato (donq) bridges, in the presence of a pyrenyl-nucleoside derivatives (pyreneR), affords the triangular prismatic host-guest compounds [(pyrene-R)?Ru(6)(pPr(i)C(6)H(4)Me)(6)(tpt)(2)(dobq)(3)](6+) ([(pyrene-R)?1](6+)) and [(pyrene-R)?Ru(6)(pPr(i)C(6)H(4)Me)(6)(tpt)(2)(donq)(3)](6+) ([(pyrene-R)?2](6+)), respectively. The inclusion of six monosubstitutedpyrenyl-nucleosides (pyrene-R1 = 5'-(1-pyrenyl butanoate)-2'-deoxyuridine, pyrene-R2 = 5-fluoro-5'-(1-pyrenyl butanoate)-2'-deoxyuridine, pyrene-R3 = 5'-{N-[1-oxo-4-(1-pyrenyl)butyl]-glycyl}-2'-deoxyuridine, pyrene-R4 = 5-fluoro-5'-{N-[1-oxo-4-(1-pyrenyl)butyl]-glycyl}-2'-deoxyuridine, pyrene-R5 = 5-fluoro-5'-{N-[1-oxo-4-(1-pyrenyl)butyl]-phenylalanyl}-2'-deoxyvuridine, pyrene-R6 = 5-fluoro-5'-{N-[1-oxo-4-(1-pyrenyl)butyl]-phenylalanyl}-2'-deoxyuridine) has been accomplished. The carceplex nature of [(pyrene-R)?1](6+) with the pyrenyl moiety firmly encapsulated in the hydrophobic cavity of the cage with the nucleoside groups pointing outward was confirmed by NMR spectroscopy and electrospray ionization mass spectrometry (ESI-MS), while the host-guest nature of [(pyrene-R)?2](6+) was studied in solution by NMR techniques. In contrast to the floxuridine compounds used in the clinic, the host-guest complexes are highly water-soluble. Consequently, the cytotoxicities of these water-soluble compounds have been established using human ovarian A2780 and A2780cisR cancer cells. All the host-guest systems are more cytotoxic than the empty cages alone [1][CF(3)SO(3)](6) (IC(50) = 23 μM) and [2][CF(3)SO(3)](6) (IC(50) = 10 μM), the most active compound [pyrene-R4?1][CF(3)SO(3)](6)being 2 orders of magnitude more cytotoxic (IC(50) = 0.3 μM) on these human ovarian cancer cell lines (A2780 and A2780cisR).     

Peptide helices based on alpha-amino acids

Relevant parameters and stereochemical consequences of helices [alpha-helix, 3(10)-helix, beta-bend ribbon spiral, gamma-helix, 2.0(5)-helix, poly(Pro)(n) type-I and -II helices, and collagen triple helix] of peptides based on alpha-amino acids for use as templates in various branches of chemistry are briefly discussed.     

Computational investigations of structural changes resulting from point mutations in a collagen-like peptide

The results of 0.5-1.0 ns molecular dynamics simulations of the collagen-like peptides [(POG)4(POA)(POG)4]3 and [(POG)9]3 (POG: proline-hydroxyproline-glycine) are presented. All simulations were performed using the AMBER-94 molecular mechanical force field with a shell of TIP3P waters surrounding the peptides. The initial geometries for the collagen-like peptides included an x-ray crystallographic structure, a computer-generated structure, a [(POG)9]3 structure modeled from the x-ray structure, and the x-ray structure with crystallographic waters replaced with a shell of modeled TIP3P waters. We examined the molecular dynamics peptide residue rms deviation fluctuations, dihedral angles, molecular and chain end-to-end distances, helical parameters, and peptide-peptide and peptide-solvent hydrogen-bonding patterns. Our molecular dynamics simulations of [(POG)4(POA)(POG)4]3 show average structures and internal coordinates similar to the x-ray crystallographic structure. Our results demonstrate that molecular dynamics can be used to reproduce the experimental structures of collagen-like peptides. We have demonstrated the feasibility of using the AMBER-94 molecular mechanical force field, which was parameterized to model nucleic acids and globular proteins, for fibril proteins. We provide a new interpretation of peptide-solvent hydrogen bonding and a peptide-peptide hydrogen bonding pattern not previously reported in x-ray studies. Last, we report on the differences; in particular with respect to main-chain dihedral angles and hydrogen bonding, between the native and mutant collagen-like peptides.     

Recognition of base mismatches in DNA by 5,6-chrysenequinone diimine complexes of rhodium(III): a proposed mechanism for preferential binding in destabilized regions of the double helix

5,6-chrysenequinone diimine (chrysi) complexes of rhodium(III) have been shown to be versatile and specific recognition agents for mismatched base pairs in DNA. The design of these compounds was based on the hypothesis that the sterically expansive chrysi ligand, which should be too wide to readily intercalate into B-DNA, would bind preferentially in the destabilized regions of the DNA helix near base mismatches. In this work, this recognition hypothesis is comprehensively explored. Comparison of the recognition patterns of the complex [Rh(bpy)(2)(chrysi)](3+) with a nonsterically demanding analogue, [Rh(bpy)(2)(phi)](3+) (phi = 9,10-phenanthrenequinone diimine), demonstrates that the chrysi ligand does indeed disfavor binding to B-DNA and generate mismatch selectivity. Examination of mismatch recognition by [Rh(bpy)(2)(chrysi)](3+) in both constant and variable sequence contexts using photocleavage assays indicates that the recognition of base mismatches is influenced by the amount that a mismatch thermodynamically destabilizes the DNA helix. Thermodynamic binding constants for the rhodium complex at a range of mismatch sites have been determined by quantitative photocleavage titration and yield values which vary from 1 x 10(6) to 20 x 10(6) M(-)(1). These mismatch-specific binding affinities correlate with independent measurements of thermodynamic destabilization, supporting the hypothesis that helix destabilization is a factor determining the binding affinity of the metal complex for the mismatched site. Although not the only factor involved in the binding of [Rh(bpy)(2)(chrysi)](3+) to mismatch sites, a model is proposed where helix destabilization acts as the "door" which permits access of the sterically demanding intercalator to the base stack.     

Repetitive interactions observed in the crystal structure of a collagen-model peptide, [(Pro-Pro-Gly)9]3

The crystal structure of a collagen-model peptide [(Pro-Pro-Gly)(9)](3) has been determined at 1.33 A resolution. Diffraction data were collected at 100 K using synchrotron radiation, which led to the first structural study of [(Pro-Pro-Gly)(n)](3) under cryogenic conditions. The crystals belong to the P2(1) space group with cell parameters of a = 25.95, b = 26.56, c = 80.14 Angstroms and beta = 90.0 degrees. The overall molecular conformation was consistent with the left-handed 7/2-helical model with an axial repeat of 20 A for native collagen. A total of 332 water molecules were found in an asymmetric unit. Proline residues in adjacent triple-helices exhibited three types of hydrophobic interactions. Furthermore, three types of hydrogen-bonding networks mediated by water molecules were observed between adjacent triple-helices. These hydrophobic interactions and hydrogen-bonding networks occurred at intervals of 20 Angstroms along the c-axis based on the previous sub-cell structures [(Pro-Pro-Gly)(n)](3) (n = 9, 10), which were also seen in the full-cell structure of [(Pro-Pro-Gly)(10)](3). Five proline residues at the Y position in the X-Y-Gly triplet were found in a down-puckering conformation, this being inconsistent with the recently proposed propensity-based hypothesis. These proline residues were forced to adopt opposing puckering because of the prevailing hydrophobic interaction between triple-helices compared with the Pro:Pro stacking interaction within a triple-helix.