Secreted production of collagen-inspired gel-forming polymers with high thermal stability in Pichia pastoris

Previously, we have shown that gel-forming triblock proteins, consisting of random coil middle blocks and trimer-forming (Pro-Gly-Pro)(9) end blocks, are efficiently produced and secreted by the yeast Pichia pastoris. These end blocks had a melting temperature (T(m)) of ～41°C (at 1.1 mM of protein). The present work reveals that an increase of T(m) to ～74°C, obtained by extension of the end blocks to (Pro-Gly-Pro)(16), resulted in a five times lower yield and partial endoproteolytic degradation of the protein. A possible cause could be that the higher thermostability of the longer (Pro-Gly-Pro)(16) trimers leads to a higher incidence of trimers in the cell, and that this disturbs secretion of the protein. Alternatively, the increased length of the proline-rich (Pro-Gly-Pro)(n) domain may negatively influence ribosomal translation, or may result in, for example, hydrophobic aggregation or membrane-active behavior owing to the greater number of closely placed proline residues. To discriminate between these possibilities, we studied the production of molecules with randomized end blocks that are unable to form triple helices. The codon- and amino acid composition of the genes and proteins, respectively, remained unchanged. As these nontrimerizing molecules were secreted intact and at high yield, we conclude that the impaired secretion and partial degradation of the triblock with (Pro-Gly-Pro)(16) end blocks was triggered by the occurrence of intracellular triple helices. This degradation was overcome by using a yapsin 1 protease disruptant, and the intact secreted polymer was capable of forming self-supporting gels of high thermal stability.     

Energetic basis of molecular recognition in a DNA aptamer

The thermal stability and ligand binding properties of the L-argininamide-binding DNA aptamer (5'-GATCGAAACGTAGCGCCTTCGATC-3') were studied by spectroscopic and calorimetric methods. Differential calorimetric studies showed that the uncomplexed aptamer melted in a two-state reaction with a melting temperature T(m)=50.2+/-0.2 degrees C and a folding enthalpy DeltaH(0)(fold)=-49.0+/-2.1 kcal mol(-1). These values agree with values of T(m)=49.6 degrees C and DeltaH(0)(fold)=-51.2 kcal mol(-1) predicted for a simple hairpin structure. Melting of the uncomplexed aptamer was dependent upon salt concentration, but independent of strand concentration. The T(m) of aptamer melting was found to increase as L-argininamide concentrations increased. Analysis of circular dichroism titration data using a single-site binding model resulted in the determination of a binding free energy DeltaG(0)(bind)=-5.1 kcal mol(-1). Isothermal titration calorimetry studies revealed an exothermic binding reaction with DeltaH(0)(bind)=-8.7 kcal mol(-1). Combination of enthalpy and free energy produce an unfavorable entropy of -TDeltaS(0)=+3.6 kcal mol(-1). A molar heat capacity change of -116 cal mol(-1) K(-1) was determined from calorimetric measurements at four temperatures over the range of 15-40 degrees C. Molecular dynamics simulations were used to explore the structures of the unligated and ligated aptamer structures. From the calculated changes in solvent accessible surface areas of these structures a molar heat capacity change of -125 cal mol(-1) K(-1) was calculated, a value in excellent agreement with the experimental value. The thermodynamic signature, along with the coupled CD spectral changes, suggest that the binding of L-argininamide to its DNA aptamer is an induced-fit process in which the binding of the ligand is thermodynamically coupled to a conformational ordering of the nucleic acid.     

Trends in the 5' vs. 3' flanks of oligonucleotides in eukaryotic and prokaryotic genomes: the asymmetric roles played by cytosine and guanine.

Studies of sequence context preferences of oligonucleotides composed of (G/C)n and (A/T)m blocks (n + m = 3,4,5) unravel strong patterns. Comparisons of the 5' and 3' nearest neighbor doublets flanking these oligomers reveal the preference of (G/C)2 to be positioned immediately next to the (A/T)m block, enclosing it by (G/C) nucleotides rather than extending the (G/C)n block. That is, for a (G/C)n(A/T)m oligomer and a (G/C)2 doublet, (G/C)n(A/T)m(G/C)2 greater than (G/C)n + 2 (A/T)m. Similarly for an (A/T)m(G/C)n oligomer, (G/C)2(A/T)m(G/C)n greater than (A/T)m(G/C)n + 2. In an analogous manner, (A/T)2 flanking doublets prefer enclosing the (G/C)n blocks, although these patterns are weaker. Here we show a strong, direct relationship between the magnitude of the trends and the presence of Cs in the (G/C)n block in the (G/C)n(A/T)m oligomer, and the presence of Gs in the complementary (A/T)m(G/C)n oligomers. The trends are stronger in eukaryotic than in prokaryotic sequences. They are stronger for longer (G/C)n and shorter (A/T)m blocks. We suggest that the preference for (A/T)m to be enclosed by (G/C) rather than be flanked by them on only one side is related to DNA structure and DNA-protein interaction. Sequences of the (G/C)(A/T)(G/C) type may have more homogeneous minor groove geometry. In particular, the strong G vs. C asymmetry in the trends may be related to pyrimidine-purine junctions, possibly to CG sequences.     

In vitro hydrolysis of poly(l-lactide) crystalline residues as extended-chain crystallites: II. Effects of hydrolysis temperature

The effects of hydrolysis temperature on the hydrolysis behavior and mechanism of poly(l-lactide) crystalline residues or extended-chain crystallites were investigated in phosphate-buffered solution (50-97 degrees C), using gel permeation chromatography and differential scanning calorimetry (DSC). The hydrolysis of the crystalline residues proceeded from their surface composed of very short chains with a free end along the chain direction, irrespective of hydrolysis temperature, but the hydrolysis from their lateral surface could not be traced. The activation energy of hydrolysis for the crystalline residues (extended-chain crystallites) was evaluated to be 18.0 kcal mol(-1) (75.2 kJ mol(-1)). The monotonic melting temperature (T(m)) and crystallinity decreases occurred after their initial very small increases, excluding the monotonic crystallinity decrease at 97 degrees C with no initial increase. The T(m) decrease reflects the decreased thickness of the crystalline residues. The equilibrium T(m) of the crystalline residues (extended-chain crystallites) was estimated to be 464.5-464.9 K. The free energy values for the surface composed of very short chains with a free end, which are neighboring the air (or nitrogen during DSC scanning), were calculated to be 55.6-56.4 erg cm(-2) for heat of fusion per unit mass = 135 J g(-1). The obtained surface free energy values are significantly higher than that for the surface composed of folding chains, tie chains, and the chains with a free end, which are neighboring the same kind of amorphous chains (39.9 erg cm(-2)).     

Thermodynamic, spectroscopic, and equilibrium binding studies of DNA sequence context effects in four 40 base pair deoxyoligonucleotides

Effects of different end sequences on melting, circular dichroism spectra (CD), and enzyme binding properties were investigated for four 40 base pair, non-self-complementary duplex DNA oligomers. The center sequences of these oligoduplexes have either of two 22 base pair modules flanked on both sides by sequences differing in AT content. Temperature-induced melting transitions monitored by differential scanning calorimetry (DSC) and ultraviolet absorbance were measured for the six duplexes in buffered 115 mM Na(+) solutions. Values of the melting transition enthalpy, DeltaH(cal), and entropy, DeltaS(cal), were obtained directly from DSC experiments. Melting transition parameters, DeltaH(vH) and DeltaS(vH), were also estimated from a van't Hoff analysis of optical melting curves collected as a function of DNA concentration, assuming that the melting transition is two-state. Melting free energies (20 degrees C) evaluated from DSC melting experiments on the four duplex DNAs ranged from -52.2 to -77.5 kcal/mol. Free energies based on the van't Hoff analysis were -37.9 to -58.8 kcal/mol. Although the values are different, trends in the melting free energies of the four duplex DNAs as a function of sequence were identical in both DSC and optical analyses. Subject to several assumptions, values for the initiation free energy were estimated for each duplex, defined as DeltaG(int) = DeltaG(cal) - DeltaG(pred), where DeltaG(cal) is the experimental free energy at 20 degrees C determined from the experimentially measured values of the transition enthalpy, DeltaH(cal), and entropy, DeltaS(cal). The predicted free energy of the sequence, DeltaG(pred)(20 degrees C), is obtained using published nearest-neighbor sequence stability values. For three of the four duplexes, values of DeltaG(int) are essentially nil. In contrast, the duplex with 81.8% GC has a considerably higher estimate of DeltaG(int) = 7.1 kcal/mol. The CD spectra for the six duplexes collected over the wavelength range from 200 to 320 nm are also sequence-dependent. Factor analysis of the CD spectra by singular value decomposition revealed that the experimental CD spectra could be reconstructed from linear combinations of two minor and one major subspectra. Changes in the coefficients of the major subspectrum for different sequences reflect incremental sequence-dependent variations of the CD spectra. Equilibrium binding by BamHI restriction endonuclease to the 40 base pair DNAs whose central eight base pairs contain the recognition sequence for BamHI restriction enzyme bounded by A.T base pairs, 5'-A-GGATCC-A-3' was investigated. Binding assays were performed by titering BamHI against a constant concentration of each of the duplex DNA substrates, in the absence of Mg(2+), followed by analysis by gel retardation. Under the conditions employed, the enzyme binds but does not cleave the DNAs. Results of the assays revealed two binding modes with retarded gel mobilities. Binding isotherms for the fraction of bound DNA species versus enzyme concentration for each binding mode were constructed and analyzed with a simple two-step equilibrium binding model. This analysis provided semiquantitative estimates on the equilibrium binding constants for BamHI to the four DNAs. Values obtained for the binding constants varied only 7-fold and ranged from 6 x 10(-)(8) to 42 x 10(-)(8) M, with binding free energies from -8.6 to -9.7 (+/- 0.2) kcal/mol depending on the sequence that flanks the enzyme binding site. Unlike what was found earlier in binding studies of the 22 base pair duplexes that constitute the core modules of the present 40-mers [Riccelli, P. V., Vallone, P. M., Kashin, I., Faldasz, B. D., Lane, M. J., and Benight, A. S. (1999) Biochemistry 38, 11197-11208], no obvious relationship between binding and stability was found for these longer DNAs. Apparently, effects of flanking sequence stability on restriction enzyme binding may only be measurable in very short duplex deoxyoligonucl     

Thermal transitions of DMPG bilayers in aqueous solution: SAXS structural studies

Dimyristoylphosphatidylglycerol (DMPG) has been extensively studied as a model for biological membranes, since phosphatidylglycerol is the most abundant anionic phospholipid in prokaryotic cells. At low ionic strengths, this lipid presents a peculiar thermal behavior, with two sharp changes in the light scattering profile, at temperatures named here T(on)(m) and T(off)(m). Structural changes involved in the DMPG thermal transitions are here investigated by small angle X-ray scattering (SAXS), and compared to the results yielded by differential scanning calorimetry (DSC) and electron spin resonance (ESR). The SAXS results show a broad peak, indicating that DMPG is organized in single bilayers, for the range of temperature studied (10-45 degrees C). SAXS intensity shows an unusual effect, starting to decrease at T(on)(m), and presenting a sharp increase at T(off)(m). The bilayer electron density profiles, obtained from modeling the SAXS curves, show a gradual decrease in electron density contrast (attributed to separation between charged head groups) and in bilayer thickness between T(on)(m) and T(off)(m). Results yielded by SAXS, DSC and ESR indicate that a chain melting process starts at T(on)(m), but a complete fluid phase exists only for temperatures above T(off)(m), with structural changes occurring at the bilayer level in the intermediate region.     

Chitin oligosaccharide binding to a family GH19 chitinase from the moss Bryum coronatum

Substrate binding of a family GH19 chitinase from a moss species, Bryum coronatum (BcChi-A, 22 kDa), which is smaller than the 26 kDa family GH19 barley chitinase due to the lack of several loop regions ('loopless'), was investigated by oligosaccharide digestion, thermal unfolding experiments and isothermal titration calorimetry (ITC). Chitin oligosaccharides [β-1,4-linked oligosaccharides of N-acetylglucosamine with a polymerization degree of n, (GlcNAc)(n), n = 3-6] were hydrolyzed by BcChi-A at rates in the order (GlcNAc)(6) > (GlcNAc)(5) > (GlcNAc)(4) > (GlcNAc)(3). From thermal unfolding experiments using the inactive BcChi-A mutant (BcChi-A-E61A), in which the catalytic residue Glu61 is mutated to Ala, we found that the transition temperature (T(m) ) was elevated upon addition of (GlcNAc)(n) (n = 2-6) and that the elevation (ΔT(m)) was almost proportional to the degree of polymerization of (GlcNAc)(n). ITC experiments provided the thermodynamic parameters for binding of (GlcNAc)(n) (n = 3-6) to BcChi-A-E61A, and revealed that the binding was driven by favorable enthalpy changes with unfavorable entropy changes. The change in heat capacity (ΔC(p)°) for (GlcNAc)(6) binding was found to be relatively small (-105 ± 8 cal·K(-1) ·mol(-1)). The binding free energy changes for (GlcNAc)(6), (GlcNAc)(5), (GlcNAc)(4) and (GlcNAc)(3) were determined to be -8.5, -7.9, -6.6 and -5.0 kcal·mol(-1), respectively. Taken together, the substrate binding cleft of BcChi-A consists of at least six subsites, in contrast to the four-subsites binding cleft of the 'loopless' family 19 chitinase from Streptomyces coelicolor. DATABASE: Chitinase, EC 3.2.1.14.     

Correcting for heat capacity and 5'-TA type terminal nearest neighbors improves prediction of DNA melting temperatures using nearest-neighbor thermodynamic models

Nearest-neighbor thermodynamic (NNT) models currently provide some of the most accurate predictions of melting thermodynamics, including melting temperature (T(m)) values, for short DNA duplexes. Inherent to all existing NNT models is the assumption that ΔH° and ΔS° for the helix-to-coil transition are temperature invariant. Here we investigate the impact that this zero-ΔC(p) assumption has on the accuracy of T(m) predictions for 128 DNA duplexes. Previous and new melting thermodynamic data are analyzed to establish an estimate of ΔC(p)(bp), the heat capacity change per base pair, of 42 ± 16 cal mol(-1) K(-1) bp(-1), as well as an optimal thermodynamic reference temperature (T(ref)) of 53 ± 5 °C. These results were used to modify the unified NNT model to properly account for the temperature dependence of ΔH° and ΔS° and thereby extend the range over which T(m) is accurately predicted. This new approach is shown to be especially useful for duplexes that melt at a T(m) greater than 70 °C. Thermodynamic data collected by differential scanning calorimetry (DSC) for 16 duplexes designed to melt over a broad temperature range were used to verify the values of ΔC(p)(bp) and T(ref) and to show that ΔC(p)(bp) is essentially constant above 37 °C. Additional DSC analysis of 12 duplex sequences containing all 10 nearest neighbors allowed for errors associated with different terminal nearest neighbors to be examined and showed that duplexes containing one or more terminal 5'-TA groups are significantly more stable than predicted by the unified NNT model. A correction to improve prediction of the hybridization thermodynamics of duplexes with terminal 5'-TA groups is provided.     

Thermodynamic stability of DNA tandem mismatches

The thermodynamics of nine hairpin DNAs were evaluated using UV-monitored melting curves and differential scanning calorimetry (DSC). Each DNA has the same five-base loop and a stem with 8-10 base pairs. Five of the DNAs have a tandem mismatch in the stem, while four have all base pairs. The tandem mismatches examined (ga/ga, aa/gc, ca/gc, ta/ac, and tc/tc) spanned the range of stability observed for this motif in a previous study of 28 tandem mismatches. UV-monitored melting curves were obtained in 1.0 M Na(+), 0.1 M Na(+), and 0.1 M Na(+) with 5 mM Mg(2+). DSC studies were conducted in 0.1 M Na(+). Transition T(m) values were unchanged over a 50-fold range of strand concentration. Model-independent enthalpy changes (DeltaH degrees ) evaluated by DSC were in good agreement (+/-8%) with enthalpy values determined by van't Hoff analyses of the melting curves in 0.1 M Na(+). The average heat capacity change (DeltaC(p)) associated with the hairpin to single strands transitions was estimated from plots of DeltaH degrees and DeltaS degrees with T(m) and ln T(m), respectively, and from profiles of DSC curves. The average DeltaC(p) values (113 +/- 9 and 42 +/- 27 cal x K(-1) x mol(-1) of bp), were in the range of values reported in previous studies. Consideration of DeltaC(p) produced large changes in DeltaH degrees and DeltaS degrees extrapolated from the transition region to 37 degrees C and smaller but significant changes to free energies. The loop free energy of the five tandem mismatches at 37 degrees C varied over a range of approximately 4 kcal x mol(-1) for each solvent.     

Thermodynamic, spectroscopic, and equilibrium binding studies of DNA sequence context effects in six 22-base pair deoxyoligonucleotides.

Effects of different end sequences on stability, circular dichroism spectra (CD), and enzyme binding properties were investigated for six 22-base pair, non-self-complementary duplex DNA oligomers. The center sequences of these deoxyoligonucleotides have 8-14 base pairs in common and are flanked on both sides by sequences differing in context and A-T content. Temperature-induced melting transitions monitored by differential scanning calorimetry (DSC) and ultraviolet absorbance were measured for the six duplexes in buffered 115 mM Na(+) solutions. Values of the melting transition enthalpy, DeltaH(cal), and entropy, DeltaS(cal), were obtained directly from DSC experiments. Melting transition parameters, DeltaH(vH) and DeltaS(vH), were also estimated from van't Hoff analysis of optical melting curves collected as a function of DNA concentration, assuming a two-state melting transition. Melting free energies (20 degrees C) of the six DNAs evaluated from DSC experiments ranged from -18.7 to -32.7 kcal/mol. van't Hoff estimates of the free energies ranged from -18.5 to -48.0 kcal/mol. With either method, the trends in free energy as a function of sequence were identical. Equilibrium binding by BamHI restriction endonuclease to the 22-base pair DNAs was also investigated. The central eight base pairs of all six molecules, 5'-A-GGATCC-A-3', contained a BamHI recognition sequence bounded by A-T base pairs. Magnesium free binding assays were performed by titering BamHI against a constant concentration of each of the deoxyoligonucleotide substrates and analyzing reaction products by gel retardation. Binding isotherms of the total amount of bound DNA versus protein concentration were constructed which provided semiquantitative estimates of the equilibrium dissociation constants for dissociation of BamHI from the six DNA oligomers. Dissociation constants ranged from 0.5 x 10(-)(9) to 12.0 x 10(-)(9) M with corresponding binding free energies of -12.5 to -10.6 (+/-0. 1) kcal/mol. An inverse relationship is found when binding and stability are compared.     

Artificial mixed-linked β-glucans produced by glycosynthase-catalyzed polymerization: tuning morphology and degree of polymerization

The glycosynthase derived from Bacillus licheniformis 1,3-1,4-β-glucanase was able to polymerize glycosyl fluoride donors (G4)(m)G3GαF (m = 0-2, G = Glcβ) leading to artificial mixed-linked β-glucans with regular sequences and variable β1,3 to β1,4 linkage ratios. With the E134A glycosynthase mutant, polymers had average molecular masses (M(w)) of 10-15 kDa. Whereas polymer 2 ([4G4G3G](n)) was an amorphous precipitate, the water-insoluble polymers 1 ([4G3G](n)) and 3 ([4G4G4G3G](n)) formed spherulites of 10-20 μm diameter. With the more active E134S glycosynthase mutant, polymerization led to high molecular mass polysaccharides, where M(w) was linearly dependent on enzyme concentration. Remarkably, a homo-polysaccharide [4G4G4G3G](n) with M(w) as high as 30.5 kDa (n ≈ 47) was obtained, which contained a small fraction of products up to 70 kDa, a value that is in the range of the molecular masses of low viscosity cereal 1,3-1,4-β-glucans, and among the largest products produced by a glycosynthase. Access to a range of novel tailor-made β-glucans through the glycosynthase technology will allow to evaluate the implications of polysaccharide fine structures in their physicochemical properties and their applications as biomaterials, as well as to provide valuable tools for biochemical characterization of β-glucan degrading enzymes and binding modules.     

Studies of DNA dumbbells. III. Theoretical analysis of optical melting curves of dumbbells with a 16 base-pair duplex stem and Tn end loops (n = 2, 3, 4, 6, 8, 10, 14).

Optical melting curves of seven DNA dumbbells with the 16 base-pair duplex sequence 5'G-C-A-T-A-G-A-T-G-A-G-A-A-T-G-C3' linked on both ends by Tn (n = 2, 3, 4, 6, 8, 10, and 14) loops measured in 30, 70, and 120 mM Na+ are analyzed in terms of the numerically exact statistical thermodynamic model of DNA melting. The construction and characterization of these molecules were described in the previous paper (Amaratunga et al., 1992). As was recently reported for hairpins (T. M. Paner, M. Amaratunga, M. J. Doktycz, and A. S. Benight, 1990, Biopolymers, Vol. 29, pp. 1715-1734) theoretically calculated melting curves were fitted to experimental curves by simultaneously adjusting the parameters representing loop and circle formation to optimize the fits. The systematically determined empirical parameters provide evaluations of the free energies of hairpin loop formation delta Gloop (n) and single-strand circles delta Gcircle (N), as a function of end loop size, n = 2-14, and circle size, N = 32 + 2n. The dependence of these quantities on solvent ionic strength over the range from 30 to 120 mM Na+ was evaluated. An approximately analytical expression for the partition function Q(T) of the dumbbells was formulated that allowed a means for determining the transition enthalpy delta H degrees and entropy delta S degrees for every dumbbell, revealing the dependence of these quantities on loop size. In this multistate approach a manifold of partially melted intermediate microstates are considered and therefore no assumptions regarding the nature of the melting transitions (that they are two-state) are required. The transition thermodynamic parameters were also determined from a van't Hoff analysis of the melting curves. Comparisons between the results of the multistate analysis and the two-state van't Hoff analysis revealed significant differences for the dumbbells with larger end loops, indicating that the melting transitions of the larger looped dumbbells deviate considerably from two-state behavior. Results are then compared with published melting studies of much larger DNA dumbbells (D. B. Naritsin and Y. L. Lyubchenko, 1990, Journal of Biomolecular Structure and Dynamics, Vol. 8, pp. 1-13), of small hairpins (Paner et al., 1990; M. J. Doktycz, T. M. Paner, M. Amaratunga and A. S. Benight, 1990, Biopolymers, Vol. 30, pp. 829-845) and another dumbbell (A. S. Benight, J. M. Schurr, P. F. Flynn, B. R. Reid, and D. E. Wemmer, 1988) Journal of Molecular Biology, Vol. 200, pp. 377-399).(ABSTRACT TRUNCATED AT 400 WORDS)     

Stabilization of nucleic acid triplexes by high concentrations of sodium and ammonium salts follows the Hofmeister series

The thermal stability of the triplexes d(C(+)-T)(6):d(A-G)(6);d(C-T)(6) and d(T)(21):d(A)(21);d(T)(21) was studied in the presence of high concentrations of the anions Cl(-), HPO(4)(2-), CH(3)COO(-), SO(4)(2-) and ClO(4)(-). Thermally-induced triplex and duplex transitions were identified by UV- and CD-spectroscopy and T(m) values were determined from melting profiles. A thermodynamic analysis of triplex transitions shows the limitations of commonly used treatments for determining the associated release or uptake of salt, solute or water. Enhancement of the stability of these triplexes follows the rank order of the Hofmeister series for anions of sodium and ammonium salts, whereas water structure-breaking solutes have the opposite effect. The rank order for the Hofmeister series ClO(4)(-)相似文献   

Polymers from functional macrolactones as potential biomaterials: enzymatic ring opening polymerization, biodegradation, and biocompatibility

We systematically investigated a series of polymers derived from macrolactones, namely, pentadecalactone, hexadecalactone, and their unsaturated analogues ambrettolide and globalide as potential biomaterials. By enzymatic ring-opening polymerization these monomers can conveniently be polymerized to high molecular weight. The polymers are highly crystalline with melting points around 95 degrees C for the saturated polymers and lower melting points for the unsaturated polymers (46-55 degrees C). All polymers are nontoxic as measured by an MTT assay for metabolic cell activity of a 3T3 mouse fibroblast cell line. Degradation studies showed no hydrolytic or enzymatic degradability of the polymers, which was ascribed to the high crystallinity and hydrophobicity of the materials. The unsaturated polymers were cross-linked in the melt, yielding fully amorphous transparent materials with a gel content of 97%.     

Melting temperatures of nucleic acids: discrepancies in analysis

Melting temperature, T(m), is an important property of nucleic acid duplexes. It is typically determined from spectroscopic or calorimetric melting experiments. More than one analytical method has been used to extract T(m) values from experimental melting data. Unfortunately, different methods do not give the same results; the same melting data can be assigned different T(m) values depending upon which method is used to process that data. Inconsistencies or systematic errors between T(m)s reported in published data sets can be significant and add confusion to the field. Errors introduced from analysis can be greater than experimental errors, ranging from a fraction of degree to several degrees. Of the various methods, the most consistent and meaningful approach defines melting temperature as the temperature at the transition midpoint where half of the base pairs are melted and standard free energy is zero. Assuming a two-state melting behavior, we present here a set of general equations that can be used to reconcile these analytical T(m) differences and convert results to the correct melting temperatures at the transition midpoint. Melting temperatures collected from published sources, which were analyzed using different methods, can now be corrected for these discrepancies and compared on equal footing. The similar corrections apply to T(m) differences between calorimetric and spectroscopic melting curves. New algorithm for selection of linear sloping baselines, 2nd derivative method, is suggested, which can be used to automate melting curve analysis.     

Biosynthesis of polyesters and polyamide building blocks using microbial fermentation and biotransformation

Biopolymers can be a green alternative to fossil-based polymers and can contribute to environmental protection because they are produced using renewable raw materials. Biopolymers are composed of various small subunits (building blocks) that are the intermediates or end products of major metabolic pathways. Most building blocks are secreted directly outside of cells, making downstream processes easier and more economic. These molecules can be extracted from fermentation broth and polymerized to produce a variety of biopolymers, e.g., polybutylene terephthalate, polyethylene terephthalate, polytrimethylene terephthalate, nylon-5,4 and nylon-4,6, with applications in medicine, pharmaceuticals, and textiles. Microbes are unable to naturally produce these types of polymers; thus, the production of building blocks and their polymerization is a fascinating approach for the production of these polymers. In comparison to naturally occurring biopolymers, synthesized polymers have improved and controlled structures and higher purity. The production of monomer units provides a new direction for polymer science because new classes of polymers with unique properties that were not previously possible can be prepared. Furthermore, the engineering of microbes for building-block production is an easy process compared to engineering an entire biopolymer synthesis pathway in a single microbe. Polyesters and polyamide polymers have become an important part of human life, and their demand is increasing daily. In this review, recent approaches and technology are discussed for the production of polyester/polyamide building blocks, i.e., 2-hydroxyisobutyric acid, 3-hydroxypropionic acid, mandelic acid, itaconic acid, adipic acid, terephthalic acid, succinic acid, 1,3-propanediol, 2,3-butanediol, 1,4-butanediol, 1,3-butanediol, cadaverine, and putrescine.     

Melting of crosslinked DNA: VI. Comparison of influence of interstrand crosslinks and other chemical modifications formed by antitumor compounds on DNA stability

A computer modeling of thermodynamic properties of a long DNA of N base pairs that includes omega interstrand crosslinks (ICLs), or omega chemical modifications involving one strand (monofunctional adducts, intrastrand crosslinks) has been carried out. It is supposed in our calculation that both types of chemical modifications change the free energy of the helix-coil transition at sites of their location by deltaF. The value deltaF>0 corresponds to stabilization, i.e., to the increase in melting temperature. It is also taken into account that ICLs form additional loops in melted regions and prohibit strand dissociation after full DNA melting. It is shown that the main effect of interstrand crosslinks on the stability of long DNA's is caused by the formation of additional loops in melted regions. This formation increases DNA melting temperature (T(m)) much stronger than replacing omega base pairs of AT type with GC. A prohibition of strand dissociation after crosslinking, which strongly elevates the melting temperature of oligonucleotide duplexes, does not influence melting behavior of long DNA's (N>/=1000 bp). As was demonstrated earlier for the modifications involving one or the other strand, the dependence of the shift of melting temperature deltaT(m) on the relative number of modifications r = omega/(2N) is a linear function for any deltaF, and deltaT(m)(r) identical with 0 for the ideal modifications (deltaF=0). We have shown that deltaT(m)(r) is the same for periodical and random distribution if the absolute value of deltaF is less 2 kcal. The absolute value of deltaT(m)(r) at deltaF>2 kcal and deltaF<-2 kcal is higher for periodical distribution. For interstrand crosslinks, the character of the dependence deltaT(m)(r) is quite different. It is nonlinear, and the shape of the corresponding curve is strongly dependent on deltaF. For "ideal" interstrand crosslinks (deltaF=0), the function deltaT(m)(r) is not zero. It is monotone positive nonlinear, and its slope decreases with r. If r<0.004, then the entropy stabilizing effect of interstrand crosslinking itself exceeds the influence of a distortion of the double helix at sites of their location. The resulting deltaT(m)(r) is positive even in the case of the infinite destabilization at sites of the ICLs (deltaF--> -infinity). In general, stabilizing influence of interstrand crosslinks is almost fully compensated for by local structural distortions caused by them if 0相似文献   

Mechanical stability of single DNA molecules

Using a modified atomic force microscope (AFM), individual double-stranded (ds) DNA molecules attached to an AFM tip and a gold surface were overstretched, and the mechanical stability of the DNA double helix was investigated. In lambda-phage DNA the previously reported B-S transition at 65 piconewtons (pN) is followed by a second conformational transition, during which the DNA double helix melts into two single strands. Unlike the B-S transition, the melting transition exhibits a pronounced force-loading-rate dependence and a marked hysteresis, characteristic of a nonequilibrium conformational transition. The kinetics of force-induced melting of the double helix, its reannealing kinetics, as well as the influence of ionic strength, temperature, and DNA sequence on the mechanical stability of the double helix were investigated. As expected, the DNA double helix is considerably destabilized under low salt buffer conditions (相似文献   

Kinetic studies of DNA cleavage reactions catalyzed by an ATP-dependent deoxyribonuclease on a 27-MHz quartz-crystal microbalance

Catalytic DNA cleavage reactions by an ATP-dependent deoxyribonuclease (DNase) from Micrococcus luteus were monitored directly with a DNA-immobilized 27-MHz quartz-crystal microbalance (QCM). The 27-MHz QCM is a very sensitive mass-measuring device in aqueous solution, as the frequency decreases linearly with increasing mass on the electrode at a nanogram level. Three steps in ATP-dependent DNA hydrolysis reactions, including (1) binding of DNase to the end of double-stranded DNA (dsDNA) on the QCM electrode (mass increase), (2) degradation of one strand of dsDNA in the 3' --> 5' direction depending on ATP (mass decrease), and (3) release of the enzyme from the nonhydrolyzed 5'-free-ssDNA (mass decrease), could be monitored stepwise from the time dependencies of QCM frequency changes. Kinetic parameters for each step were obtained as follows. The binding constant (K(a)) of DNase to the dsDNA was determined as (28 +/- 2) x 10(6) M(-)(1) (k(on) = (8.0 +/- 0.3) x 10(3) M (-)(1) s(-)(1) and k(off) = (0.29 +/-0.01) x 10(-)(3) s(-)(1)), and it decreased to (0.79 +/- 0.16) x 10(6) M(-)(1) (k'(on) = (2.3 +/- 0.2) x 10(3) M (-)(1) s(-)(1) and k'(off) = (2.9 +/- 0.1) x 10(-)(3) s(-)(1)) for the completely nonhydrolyzed 5'-free ssDNA. This is the reason the DNase bound to the dsDNA substrate can easily release from the nonhydrolyzed 5'-free-ssDNA after the complete hydrolysis of the 3' --> 5' direction of the complementary ssDNA. K(a) values depended on the DNA structures on the QCM, and the order of these values was as follows: the dsDNA having a 4-base-mismatched base-pair end (3) > the dsDNA having a 5' 15-base overhanging end (2) > the dsDNA having a blunt end (1) > the ssDNA having a 3'-free end (4) > the ssDNA having a 5'-free end (5). Thus, DNase hardly recognized the free 5' end of ssDNA. Michaelis-Menten parameters (K(m) for ATP and k(cat)) of the hydrolysis process also could be obtained, and the order of k(cat)/K(m) was as follows: the dsDNA having a blunt end (1) approximately the dsDNA having a 4-base-mismatched base-pair end (3) > the ssDNA having a free 3' end (4) > the ssDNA having a free 5' end (5). Thus, DNase could not recognize and not hydrolyze the free 5' end of ssDNA. The DNA hydrolysis reaction could be driven by dATP and GTP (purine base) as well as ATP, whereas the cleavage efficiency was very low driven with UTP, CTP (pyrimidine base), ADP, and AMP.     

Applicability of urea in the thermodynamic analysis of secondary and tertiary RNA folding

The equilibrium folding of a series of self-complementary RNA duplexes and the unmodified yeast tRNA(Phe) is studied as a function of urea and Mg(2+) concentration with optical spectroscopies and chemical modification under isothermal conditions. Via application of standard methodologies from protein folding, the folding free energy and its dependence on urea concentration, the m value, are determined. The free energies of the RNA duplexes obtained from the urea titrations are in good agreement with those calculated from thermal melting studies [Freier, S. I., et al. (1986) Proc. Natl. Acad. Sci. U.S.A. 83, 9373]. The m value correlates with the length of the RNA duplex and is not sensitive to ionic conditions and temperature. The folding of the unmodified yeast tRNA(Phe) can be described by two Mg(2+)-dependent transitions, the second of which corresponds to the formation of the native tertiary structure as confirmed by hydroxyl radical protection and partial nuclease digestion. Both transitions are sensitive to urea and have m values of 0.94 and 1.70 kcal mol(-)(1) M(-)(1), respectively. Although the precise chemical basis of urea denaturation of RNA is uncertain, the m values for the duplexes and tRNA(Phe) are proportional to the amount of the surface area buried in the folding transition. This proportionality, 0.099 cal mol(-)(1) M(-)(1) A(-)(2), is very similar to that observed for proteins, 0.11 cal mol(-)(1) M(-)(1) A(-)(2) [Myers, J., Pace, N., and Scholtz, M. (1995) Protein Sci. 4, 2138]. These results indicate that urea titration can be used to measure both the free energy and the magnitude of an RNA folding transition.