Three-State Diagram for DNA

Abstract

Experimental phase diagrams (A form, B form, Coil) were built in the coordinates (a, alcohol fraction: T, temperature) for the natural DNAs and poly d(A-T). The main parameter of the B-A transition,—cooperativity length, v _o, was estimated by the slopes of the branches A-B, A-Coil, B-Coil in the vicinity of the triple point: v _o +AD0- 10-20 base pairs, which corresponds to the energy for the B/A junction of 1.2–1.8 kcal/mol.

We discovered two new effects which are due to the coexistence of the three different conformations in one polymeric molecule: an increase in the melting temperature above that for the ‘ideal’ triple point (i.e. for the case of the ideal phase transitions); a widening of the melting curve within the B-A transition range.

The physics of these phenomena is discussed.     

A 31P NMR analysis of the helix to coil transition of natural DNA samples: evidence for the existence of different conformational states.

The helix to coil transitions of calf thymus and salmon sperm DNA were probed by ³¹P nuclear magnetic resonance spectroscopy. Both the helical and coil forms were observed in the melting region indicating slow exchange between the two forms with an estimated rate of interconversion ? 36 sec^?1 at 70°C. At least three different signals were also observed at temperatures significantly above the Tm, suggesting three classes of conformational states. One of these classes has a significantly lower T₁ than the other two indicating considerable residual structure in this form. The four only partially resolved signals indicate that the phosphate residues have very similar chemical shift environments. From the experimentally observed small chemical shift differences between the helical and coil forms, it is concluded that the gauche, gauche, conformation predominates in the coil form as has been found for the helix.     

Heat denaturation of alpha-tropomyosin and its fragments

The reasons for three heterogeneity of tropomyosin melting curves are considered. It is shown that this phenomenon is due to the molecular heterogeneity of the preparation. Different states of the SH-groups as well as the different stability of molecule regions. The melting curves of alpha-tropomyosin and two of its fragments are obtained. The thermodynamic parameters stabilizing their helical structure are determined. The existence of a thermodynamical transition at 31 degrees C is shown for alpha-tropomyosin leading to the loss of the ability of the molecule to form supra-molecular structures.     

The Kinetics of DNA Helix-Coil Subtransitions

Abstract

The kinetic analysis of individual helix-coil subtransitions was performed by comparing melting and renaturation profiles obtained at different temperature change rates. The duration of the three transition stages and its dependence on temperature and ionic strength were determined for a T7 phage DNA fragment. The obtained temperature dependence of the melting time for a stretch flanked by melted regions is in quantitative agreement with that predicted by the theory of slow processes (V.V. Anshelevich, A.V. Vologodskii, A.V. Lukashin, M.D. Frank-Kamenetskii, Biopolymers 23, 39 (1984)). The reasons are discussed for the increasing relaxation time of this stretch in the middle of its transition with decreasing ionic strength.

The zipping kinetics of a melted region under essentially nonequilibrium conditions was examined for T7 fragment and pAO3 DNAs. The obtained temperature dependence of the zipping time is in quantitative agreement with calculations based on the theory of slow processes.

The renaturation times of stretches flanked by helical regions proved fairly small even at a low ionic strength. These times are several orders of magnitude smaller than the renaturation times of the same stretches with one helical boundary. A formal application of the theory of slow processes failed to account for the small renaturation times of stretches that are zipped from both ends. This is probably due to the non-allowance for the changing entropy of the loop linking two helix-coil boundaries migrating towards each other.

Slow processes have been revealed in the intramolecular melting of Col E1 DNA at a high ionic strength. The reason for the long relaxation time of one subtransition is the large size of the loop that separates the melting stretch from the helical part of the molecule. This result can be accounted for by the theory of slow processes.     

Melting of Cross-Linked DNA IV. Methods for Computer Modeling of Total Influence on DNA Melting of Monofunctional Adducts,Intrastrand and Interstrand Cross-Links Formed by Molecules of an Antitumor Drug

Abstract

A theoretical method is developed for calculation of melting curves of covalent complexes of DNA with antitumor drugs. The method takes into account all the types of chemical modifications of the double helix caused by platinum compounds and DNA alkylating agents: 1) monofunctional adducts bound to one nucleotide; 2) intrastrand cross-links which appear due to bidentate binding of a drug molecule to two nucleotides that are included into the same DNA strand; 3) interstrand cross-links caused by bidentate binding of a molecule to two nucleotides of different strands. The developed calculation method takes into account the following double helix alterations at sites of chemical modifications: 1) a change in stability of chemically modified base pairs and neighboring ones, that is caused by all the types of chemical modifications; 2) a change in the energy of boundaries between helical and melted regions at sites of chemical modification (local alteration of the factor of cooperativity of DNA melting), that is caused by all the types of chemical modifications, too; 3) a change in the loop entropy factor of melted regions that include interstrand cross-links; 4) the prohibition of divergence of DNA strands in completely melted DNA molecules, which is caused by interstrand cross-links only. General equations are derived, and three calculation methods are proposed to calculate DNA melting curves and the parameters that characterize the helix-coil transition.     

Left handed DNA in synthetic and topologically constrained form V DNA and its implications in protein recognition

We have investigated structural transitions in Poly(dG-dC) and Poly(dG-Me⁵dC) in order to understand the exact role of cations in stabilizing left-handed helical structures in specific sequences andthe biological role, if any, of these structures. From a novel temperature dependent Z ⇌ B transition it has been shown that a minor fluctuation in Na⁺ concentration at ambient temperature can bring about B to Z transition. Forthe first time, wehave observed a novel Z⇌B⇌Zuble transition in poly(dG-Me⁵dC) as the Na⁺ concentration is gradually increased. This suggests that a minor fluctuation in Na⁺ concentration in conjunction with methylation may transform small stretches of CG sequences from one conformational state to another. These stretches could probably serve as sites for regulation. Supercoiled formV DNA reconstituted from pBR322 and pβG plasmids have been studied as model systems, in order to understand the nature and role of left-handed helical conformation in natural sequences. A large portion of DNA in form V, obtained by reannealing the two complementary singlestranded circles is forced to adopt left-handed double helical structure due to topological constraints (L _k = 0). Binding studies with Z-DNA specific antibody and spectroscopic studies confirm the presence of left-handed Z-structure in the pβG and pβR322 form V DNA. Cobalt hexamine chloride, which induces Z-form in Poly(dG-dC) stabilizes the Z-conformation in form V DNA even in the non-alternating purine-pyrimidine sequences. A reverse effect is observed with ethidium bromide. Interestingly, both topoisomerase I and II (from wheat germ) act effectively on form V DNA to give rise to a species having an electrophoretic mobility on agarose gel similar to that of open circular (form II) DNA. Whether this molecule is formed as a result of the left-handed helical segments of form V DNA undergoing a transition to the right-handed B-form during the topoisomerase action remains to be solved.     

Modeling the bacterial flagellum by an elastic network of rigid bodies

Bacteria such as Escherichia coli propel themselves by rotating a bundle of helical filaments, each driven by a rotary motor embedded in the cell membrane. Each filament is an assembly of thousands of copies of the protein flagellin which assumes two different states. We model the filament by an elastic network of rigid bodies that form bonds with one another according to a scheme suggested by Namba and Vondervistz (1997 Q. Rev. Biophys. 30 1-65) and add additional binding sites at the inner part of the rigid body. Our model reproduces the helical parameters of the 12 possible polymorphic configurations very well. We demonstrate that its energetical ground state corresponds to the normal helical form, usually observed in nature, only when inner and outer binding sites of the rigid body have a large axial displacement. This finding correlates directly to the elongated shape of the flagellin molecule. An Ising Hamiltonian in our model directly addresses the two states of the flagellin protein. It contains an external field that represents external parameters which allow us to alter the ground state of the filament.     

Calorimetry of rat tail tendon collagen before and after denaturation: the heat of fusion of its absorbed water

The specific heat, of rat tail tendon at various water contents was measured as a function of temperature. The resulting graphs showed peaks arising from the melting, near 50°C, of helical material in the collagen, and from the melting of absorbed water in the range -40°C to 0°C. The heat of melting of helical material was 11.7 cal per gram of dry tendon. Determination of the heat and temperature of fusion of the absorbed water allowed resolution of the water into four states in the case of tendon before denaturation, and three states after denaturation. The four states are (1) water not freezable on cooling to - 70°C, (2) freezable water with-both heat and temperature of fusion different from the values for ordinary water, (3) freezable water with the heat of fusion of ordinary water, but a different temperature of fusion, and (4) water not distinguished from ordinary water. The fourth state was absent in denatured tendon. The results are discussed in terms of increasing size of clusters of absorbed water molecules.     

Differential self assembly of amphiphilic helical peptides

Summary A series of amphiphilic, helical peptides was designed and synthesized to investigate the components necessary for formation of helical bundles with differing aggregation states. Minimalistic sequences were employed for the peptides which contained either four (Leu4), six (Leu6) or eight (Leu8) leucine residues within a sixteen amino acid sequence. All peptides were highly helical as evaluated by circular dichroism, and the helical content of each peptide exhibited a concentration dependence. Size exclusion chromatography confirmed aggregation states of dimer/trimer forLeu4, tetramer forLeu6, and hexamer octamer forLeu8. Disulfide crosslinking studies also confirmed that the dimer ofLeu4 favored a parallel orientation with respect to the helical dipole. This systematic study clearly defines the role of hydrophobicity in the self assembly of helical peptides; peptides with a small hydrophobic face favor small bundle sizes, whereas peptides containing larger hydrophobic faces form correspondingly larger helical bundles.     

Conformational Variability of Poly(dA-dT)·Poly(dA-dT) and Some Other Deoxyribonucleic Acids Includes a Novel Type of Double Helix

Abstract

The article reviews data indicating that poly(dA-dT)?poly (dA-dT) is able of adopting three distinct double helical structures in solution, of which only the A form conforms to classical notions. The other two structures have dinucleotides as double helical repeats. At low salt concentrations poly(dA-dT)?poly(dA-dT) adopts a B-type alternating conformation which is exceptionally variable. Its architecture can gradually move in the limits demarcated by the CD spectra with inverted long wavelength CD bands and the ³¹P NMR spectra with a very low and a 0.6 ppm separation of two resonances. Contrary to Z-DNA, the ³¹P NMR spectrum of the limiting alternating B conformation of poly(dA-dT)?poly(dA-dT) is characterized by an upfield shift of one resonance. We attribute the exceptional conformational flexibility of the alternating B conformation to the unequal tendency of bases in the dA-dT and dT-dA steps to stack.

However, by assuming the limiting alternating B conformation, the variability of the synthetic DNA is not exhausted. Specific agents make it isomerize into another conformation by a fast, two-state mechanism, which is reflected by a further deepening of the negative long wavelength CD band and a downfield shift of the ³¹P NMR resonance of poly (dA-dT)?poly(dA-dT) that was constant in the course of the gradual alterations of the alternating B conformation. These changes are, however, qualitatively different from the way poly(dG-dC)?poly(dG-dC) behaves in the course of the B-Z isomerization. Poly(dG-dC) ?poly(dG-dC) displays purine-pyrimidine (dGpdC) resonance in the characteristic downfield position, while the downfield resonance of poly(dA-dT)?poly(dA-dT) belongs to the pyrimidine-purine (dTpdA) phosphodiester linkages. Consequently, phosphodiester linkages in the purine-pyrimidine steps play a similar role in the appearance of the Z form to the pyrimidine-purine phosphodiesters in the course of the isomerization of poly(dA-dT)?poly(dA-dT). This excludes that the high-salt structures of poly(dA-dT)?poly(dA-dT) and poly(dG-dC)?poly(dG-dC) are members of the same conformational family. We call the high-salt conformation of poly(dA-dT)?poly(dA-dT) X-DNA.

It furthermore follows from the review that synthetic molecules of DNA with alternating purine-pyrimidine sequences of bases can adopt either the Z form or the X form, or even both, depending on the environmental conditions. This introduces a new dimension into the DNA double helix conformational variability. The possible biological relevance of the X form is suggested by experiments with linear molecules of natural DNA. These indicate that Arich regions in natural DNAs can isomerize into the X form while the bulk of the molecule remains in the B form. The coexistence of both structures in a single DNA molecule may be understood in view of the favourable kinetic and thermodynamic properties with which the X form appears.     

Sequential folding of transfer RNA: A nuclear magnetic resonance study of successively longer tRNA fragments with a common 5′ end

Most folding studies on proteins and nucleic acids have been addressed to the transition between the folded and unfolded states of an intact molecule, where an entire residue sequence is present during the folding event. However, since these polymers are synthesized sequentially from one terminus to the other in vivo, their folding pathways may be influenced greatly by the sequential appearance of the residues as a function of time.The three-dimensional structure of yeast tRNA^Phe in the crystalline state is correlated with 360 MHz proton nuclear magnetic resonances from three fragments plus an intact molecule of the tRNA that share a common 5′ end and are in a solution condition similar to that of the crystal structure. This has allowed identification of folded structures present in the fragments and presumably present in the growing tRNA molecule as it is being synthesized from the 5′ end. The experiments show that only the correct stems are formed in the fragments; no additional or competing helical region is produced. This suggests that in the biosynthesis of this tRNA, correct folding of helical stems occurs before the entire molecule is formed. Further, some of the tertiary interactions (hydrogen bonds) found in the crystal structure are also probably present before the synthesis is completed. These findings are generalized to consider the precursor of the tRNA as well as other tRNAs.     

Essential dynamics of reversible peptide folding: memory-free conformational dynamics governed by internal hydrogen bonds

A principal component analysis has been applied on equilibrium simulations of a beta-heptapeptide that shows reversible folding in a methanol solution. The analysis shows that the configurational space contains only three dense sub-states. These states of relatively low free energy correspond to the "native" left-handed helix, a partly helical intermediate, and a hairpin-like structure. The collection of unfolded conformations form a relatively diffuse cloud with little substructure. Internal hydrogen-bonding energies were found to correlate well with the degree of folding. The native helical structure folds from the N terminus; the transition from the major folding intermediate to the native helical structure involves the formation of the two most C-terminal backbone hydrogen bonds. A four-state Markov model was found to describe transition frequencies between the conformational states within error limits, indicating that memory-effects are negligible beyond the nanosecond time-scale. The dominant native state fluctuations were found to be very similar to unfolding motions, suggesting that unfolding pathways can be inferred from fluctuations in the native state. The low-dimensional essential subspace, describing 69% of the collective atomic fluctuations, was found to converge at time-scales of the order of one nanosecond at all temperatures investigated, whereas folding/unfolding takes place at significantly longer time-scales, even above the melting temperature.     

The Impact of Dyskeratosis Congenita Mutations on the Structure and Dynamics of the Human Telomerase RNA Pseudoknot Domain

Abstract

The pseudoknot domain is a functionally crucial part of telomerase RNA and influences the activity and stability of the ribonucleoprotein complex. Autosomal dominant dyskeratosis congenita (DKC) is an inherited disease that is linked to mutations in telomerase RNA and impairs telomerase function. In this paper, we present a computational prediction of the influence of two base DKC mutations on the structure, dynamics, and stability of the pseudoknot domain. We use molecular dynamics simulations, MM-GBSA free energy calculations, static analysis, and melting simulations analysis. Our results show that the DKC mutations stabilize the hairpin form and destabilize the pseudoknot form of telomerase RNA. Moreover, the P3 region of the predicted DKC-mutated pseudoknot structure is unstable and fails to form as a defined helical stem. We directly compare our predictions with experimental observations by calculating the enthalpy of folding and melting profiles for each structure. The enthalpy values are in very good agreement with values determined by thermal denaturation experiments. The melting simulations and simulations at elevated temperatures show the existence of an intermediate structure, which involves the formation of two UU base pairs observed in the hairpin form of the pseudoknot domain.     

Molecular dipole effects on tuning electron transfer in a porphine–quinone complex: a DFT and TDDFT study

The effect of a strong electric field generated by molecular dipoles on the ground state electronic structure and the Q and B states as well as the lowest charge transfer (CT) excited state of porphine–2,5-dimethyl-1,4-benzoquinone (PQ) complex has been investigated theoretically. Density functional theory DFT and time-dependent DFT (TDDFT) with the BH&HLYP hybrid functional have been applied in these calculations. The molecular dipole effect was generated by imposing one or two helical homopeptides consisting of eight α-aminoisobutyric acid residues (Aib₈) close to the PQ complex. The molecular dipoles in a close proximity to the PQ complex expose it to an electric field of the order of magnitude of 10⁹ V/m. The presence of the ambient molecular dipoles affects mainly the energy of the lowest CT state and barely the energies of the Q and B states. The molecular dipoles affect the energies of the excited states in a similar way as an external electrostatic field. Hence, the electric field induced by the molecular dipoles of the helical peptides could be used analogously to the external electrostatic field to control electron transfer (ET) in the PQ complex.     

Thermodynamics of Forming a Parallel DNA Crossover

The process of genetic recombination involves the formation of branched four-stranded DNA structures known as Holliday junctions. The Holliday junction is known to have an antiparallel orientation of its helices, i.e., the crossover occurs between strands of opposite polarity. Some intermediates in this process are known to involve two crossover sites, and these may involve crossovers between strands of identical polarity. Surprisingly, if a crossover occurs at every possible juxtaposition of backbones between parallel DNA double helices, the molecules form a paranemic structure with two helical domains, known as PX-DNA. Model PX-DNA molecules can be constructed from a variety of DNA molecules with five nucleotide pairs in the minor groove and six, seven or eight nucleotide pairs in the major groove. A topoisomer of the PX motif is the juxtaposed JX₁ molecule, wherein one crossover is missing between the two helical domains. The JX₁ molecule offers an outstanding baseline molecule with which to compare the PX molecule, so as to measure the thermodynamic cost of forming a crossover in a parallel molecule. We have made these measurements using calorimetric and ultraviolet hypochromicity methods, as well as denaturing gradient gel electrophoretic methods. The results suggest that in relaxed conditions, a system that meets the pairing requirements for PX-DNA would prefer to form the PX motif relative to juxtaposed molecules, particularly for the 6:5 structure.     

Conformational Characteristics of Mixed Sugar Puckered Deoxytetranucleoside Triphosphate d-GpCpGpC from Energy Minimization Studies

Abstract

As a continuation of our theoretical studies on nucleic acid subunit systems, in this article we consider the case of the tetranucleoside d-GpCpGpC, the minimally ideal representative unit for analyzing the relative stabilities of different forms of homo- and mixed helical conformation of polynucleotides. The four sugar rings are kept so as to generate B-genus, B+A genus and Z-genus conformations. Twenty five helical conformational states which resulted from judicious mixing of A-, B-, C-, W-, and Z-, states locally are subjected to energy minimization permitting the 19 dihedral angles to vary simultaneously. Conformational states corresponding to regular helical forms and mixed helical forms, when analyzed provide valuable information as to the local conformational flexibility and transitions available to polynucleotides.     

How does the mood stabilizer lithium bind ATP,the energy currency of the cell: Insights from solid-state NMR

BackgroundLithium, in the form of a salt, is a mood stabilizer and a leading drug for the treatment of bipolar disorder. It has a very narrow therapeutic range and a variety of side effects. Lithium can replace magnesium and other cations in enzymes and small molecules, among them ATP, thereby affecting and inhibiting many biochemical pathways. The form of binding of lithium ions to ATP is not known.MethodsHere we extract the binding environment of lithium in solid ATP using a multi-nuclear multi-dimensional solid-state NMR approach.ResultsWe determine that the coordination sphere of lithium includes, at a distance of 3.0(±0.4) Å, three phosphates; the two phosphates closest to the ribose ring from one ATP molecule, and the middle phosphate from another ATP molecule. A water molecule most probably completes the fourth coordination. Despite the use of excess lithium in the preparations, sodium ions still remain bound to the sample, at distances of 4.3–5.5 Å from Li, and coordinate the first phosphate and two terminal phosphates.ConclusionsSolid-state NMR enables to unravel the exact coordination of lithium in ATP showing binding to three phosphates from two molecules, none of which are the terminal gamma phosphate.General significanceThe methods we use are applicable to study lithium bound to a variety of ATP-bound enzymes, or to other cellular targets of lithium, consequently suggesting a molecular basis for its mode of action.     

Molecular structure for microbial polysaccharides: conformation of the Klebsiella serotype K9 capsular polysaccharide

Fibre type X-ray diffraction patterns have been obtained from oriented, semicrystalline films prepared from the sodium salt form of the bacterial capsular polysaccharide of Klebsiella serotype K9. The molecule has a pentasaccharide repeating sequence, with four neutral residues in the backbone and a glucoronic acid side chain. A novel feature of the molecule is the incorporation of α-l-rhamnose residues, one 1,2 linked and two 1,3 linked in the backbone. Analysis of the X-ray diffraction results indicate an extended three-fold helical conformation with an axially projected chemical repeat of 1.377 nm. Both left and right handed helices have been examined using linked atom least squares techniques to optimize the stereochemistry while simultaneously meeting the observed helical parameters.     

NMR evidence for forming highly populated helical conformations in the partially folded hNck2 SH3 domain

Recent studies of several proteins implied that the folding of β-proteins may follow a nonhierarchical mechanism in which two major transitions are essential, i.e., the collapse of a random coil to form a nonnative helical intermediate, followed by a transformation into the native β-structure. We report that the first hNck2 SH3 domain, assuming an all-β barrel in the native form, can be reversibly transformed into a stable and nonnative helical state by acid-unfolding. We also conducted extensive NMR and mutagenesis studies that led to two striking findings: 1), NMR analysis reveals that in the helical state formed at pH 2.0, the first and last β-strands in the native form become unstructured, whereas the rest is surprisingly converted into two highly populated helices with a significantly limited backbone motion; and 2), a conserved four-residue sequence is identified on the second β-strand, a mutation of which suddenly renders the SH3 domain into a helical state even at pH 6.5, with NMR conformational and dynamic properties highly similar to those of the wild-type at pH 2.0. This observation implies that the region might contribute key interactions to disrupt the helical state, and to facilitate a further transformation into the native SH3 fold in the second transition.