Studies of DNA dumbbells. IV. Preparation and melting of a DNA dumbbell with the 16 base-pair sequence 5'G-T-A-T-C-C-C-T-C-T-G-G-A-T-A-C3' linked on the ends by dodecyl chains

High definition polyphosphoesters: between nucleic acids and plastics

Nucleic acids and synthetic polyphosphoester materials have been distinct fields – this review shows how these areas now comprise a continuum.

Stabilization of RNA hairpins using non-nucleotide linkers and circularization

An RNA hairpin is an essential structural element of RNA. Hairpins play crucial roles in gene expression and intermolecular recognition but are also involved in the pathogenesis of some congenital diseases. Structural studies of the hairpin motifs are impeded by their thermodynamic instability, as they tend to unfold to form duplexes, especially at high concentrations required for crystallography or nuclear magnetic resonance spectroscopy. We have elaborated techniques to stabilize the RNA hairpins by linking the free ends of the RNA strand at the base of the hairpin stem. One method involves stilbene diether or hexaethylene glycol linkers and circularization by T4 RNA ligase. Another method uses click chemistry to stitch the RNA ends with a triazole linker. Both techniques are efficient and easy to perform. They should be useful in making stable, biologically relevant RNA constructs for structural studies.

Synthesis and evaluation of new spacers for use as dsDNA end-caps

A series of aliphatic and aromatic spacer molecules designed to cap the ends of DNA duplexes have been synthesized. The spacers were converted into dimethoxytrityl-protected phosphoramidites as synthons for oligonucleotides synthesis. The effect of the spacers on the stability of short DNA duplexes was assessed by melting temperature studies. End-caps containing amide groups were found to be less stabilizing than the hexaethylene glycol spacer. End-caps containing either a terthiophene or a naphthalene tetracarboxylic acid diimide were found to be significantly more stabilizing. The former showed a preference for stacking above an A*T base pair. Spacers containing only methylene (-CH(2)-) and amide (-CONH-) groups interact weakly with DNA and consequently may be optimal for applications that require minimal influence on DNA structure but require a way to hold the ends of double-stranded DNA together.

Studies of DNA dumbbells VIII. Melting analysis of DNA dumbbells with dinucleotide repeat stem sequences

Melting curves and circular dichroism spectra were measured for a number of DNA dumbbell and linear molecules containing dinucleotide repeat sequences of different lengths. To study effects of different sequences on the melting and spectroscopic properties, six DNA dumbbells whose stems contain the central sequences (AA)(10), (AC)(10), (AG)(10), (AT)(10), (GC)(10), and (GG)(10) were prepared. These represent the minimal set of 10 possible dinucleotide repeats. To study effects of dinucleotide repeat length, dumbbells with the central sequences (AG)(n), n = 5 and 20, were prepared. Control molecules, dumbbells with a random central sequence, (RN)(n), n = 5, 10, and 20, were also prepared. The central sequence of each dumbbell was flanked on both sides by the same 12 base pairs and T(4) end-loops. Melting curves were measured by optical absorbance and differential scanning calorimetry in solvents containing 25, 55, 85, and 115 mM Na(+). CD spectra were collected from 20 to 45 degrees C and [Na(+)] from 25 to 115 mM. The spectral database did not reveal any apparent temperature dependence in the pretransition region. Analysis of the melting thermodynamics evaluated as a function of Na(+) provided a means for quantitatively estimating the counterion release with melting for the different sequences. Results show a very definite sequence dependence, indicating the salt-dependent properties of duplex DNA are also sequence dependent. Linear DNA molecules containing the (AG)(n) and (RN)(n), sequences, n = 5, 10, 20, and 30, were also prepared and studied. The linear DNA molecules had the exact sequences of the dumbbell stems. That is, the central repeat sequence in each linear duplex was flanked on both sides by the same 12-bp sequence. Melting and CD studies were also performed on the linear DNA molecules. Comparison of results obtained for the same sequences in dumbbell and linear molecular environments reveals several interesting features of the interplay between sequence-dependent structural variability, sequence length, and the unconstrained (linear) or constrained (dumbbell) molecular environments.

Structures and stabilities of small DNA dumbbells with Watson-Crick and Hoogsteen base pairs

The structures and stabilities of cyclic DNA octamers of different sequences have been studied by NMR and CD spectroscopy and by restrained molecular dynamics. At low oligonucleotide concentrations, some of these molecules form stable monomeric structures consisting of a short stem of two base pairs connected by two mini-loops of two residues. To our knowledge, these dumbbell-like structures are the smallest observed to date. The relative stabilities of these cyclic dumbbells have been established by studying their melting transitions. Dumbbells made up purely of GC stems are more stable than those consisting purely of AT base pairs. The order of the base pairs closing the loops also has an important effect on the stabilities of these structures. The NMR data indicate that there are significant differences between the solution structures of dumbbells with G-C base pairs in the stem compared to those with A-T base pairs. In the case of dumbbells with G-C base pairs, the residues in the stem form a short segment of a BDNA helix stabilized by two Watson-Crick base pairs. In contrast, in the case of d<pCATTCATT>, the stem is formed by two A-T base pairs with the glycosidic angles of the adenine bases in a syn conformation, most probably forming Hoogsteen base pairs. Although the conformations of the loop residues are not very well defined, the thymine residues at the first position of the loop are observed to fold back into the minor groove of the stem.

Studies of DNA dumbbells VII: evaluation of the next-nearest-neighbor sequence-dependent interactions in duplex DNA

Melting experiments were conducted on 22 DNA dumbbells as a function of solvent ionic strength from 25-115 mM Na(+). The dumbbell molecules have short duplex regions comprised of 16-20 base pairs linked on both ends by T(4) single-strand loops. Only the 4-8 central base pairs of the dumbbell stems differ for different molecules, and the six base pairs on both sides of the central sequence and adjoining loops on both ends are the same in every molecule. Results of melting analysis on the 22 new DNA dumbbells are combined with our previous results on 17 other DNA dumbbells, with stem lengths containing from 14-18 base pairs, reported in the first article of this series (Doktycz, Goldstein, Paner, Gallo, and Benight, Biopoly 32, 1992, 849-864). The combination of results comprises a database of optical melting parameters for 39 DNA dumbbells in ionic strengths from 25-115 mM Na(+). This database is employed to evaluate the thermodynamics of singlet, doublet, and triplet sequence-dependent interactions in duplex DNA. Analysis of the 25 mM Na(+) data reveals the existence of significant sequence-dependent triplet or next-nearest-neighbor interactions. The enthalpy of these interactions is evaluated for all possible triplets. Some of the triplet enthalpy values are less than the uncertainty in their evaluation, indicating no measurable interaction for that particular sequence. This finding suggests that the thermodynamic stability of duplex DNA depends on solvent ionic strength in a sequence-dependent manner. As a part of the analysis, the nearest-neighbor (base pair doublet) interactions in 55, 85, and 115 mM Na(+) are also reevaluated from the larger database.

Efficient synthesis of DNA dumbbells using template-induced chemical ligation in double-stranded polynucleotides closed by minihairpin fragments

The chemical ligation of 17 50-54-membered nicked DNA dumbbells with different closing fragments, nick positions, and nucleotides facing the nick were investigated. T4, T5, GTA4C, GCGA2GC, and GCGA3GC sequences were chosen as the closing fragments. The nicks were placed in the center of the duplex stem or were adjacent to the closing fragments. N-(3-dimethylaminopropyl)-N'-ethylcarbodiimide and cyanogen bromide were used as the condensing agents. We showed that the ligation efficiency is 10%-90% depending on the sequence of the closing fragments, nick position, and nucleotides facing the nick. Coupling yields of 80%-90% were observed when the nick was situated in the middle of the molecule between two T residues or was adjacent to GCGA2GC or GCGA3GC minihairpins. In the last case, the reacting 3'-phosphate and 5'-hydroxy groups were brought close together by only two base pair minihairpins. The coupling yields did not depend on the nature of the condensing agent. On the basis of the results obtained, we believe a rational design of nicked DNA dumbbells has been developed for efficient chemical synthesis of closed dumbbells.

Melting of cross-linked DNA. III. Calculation of differential melting curves

In our previous papers I and II (D. Y. Lando et al, J. Biomol. Struct. Dynam. (1997) v. 15, N1, p. 129-140, p. 141-150), two methods were developed for calculation of melting curves of cross-linked DNA. One of them is based on Poland's and another on the Fixman-Freire approach. In the present communication, III, a new theoretical method is developed for computation of differential melting curves of DNAs cross-linked by anticancer drugs and their inactive analogs. As Poland's approach, the method allows study of the influence of the loop entropy factor, delta(n), on melting behavior (n is the length of a loop in base pairs). However the method is much faster and requires computer time that inherent for the most rapid Fixman-Freire calculation approach. In contrast to the computation procedures described before in communications I and II, the method is suitable for computation of differential melting curves in the case of long DNA chains, arbitrary loop entropy factors of melted regions and arbitrary degree of cross-linking including very low values that occur in vivo after administration of antitumor drugs. The method is also appropriate for DNAs without cross-links. The results of calculation demonstrate that even very low degree of cross-linking alters the DNA differential melting curve. Cross-linking also markedly strengthens the influence of particular function delta(n) upon melting behavior.

Melting of cross-linked DNA: II. Influence of interstrand linking on DNA stability

In the previous paper (D.Y. Lando, J. Biomol. Struct. Dynam, 15, 129-140 (1997)) the melting of cross-linked DNA with N base pairs and omega interstrand cross-links has been considered theoretically. In the present study on the basis of these results, two simple schemes are developed for the computation of melting curves of cross-linked DNA. The investigation of influence of interstrand linking on DNA stability has been carried out by computer simulation. It is shown that the relative concentration of cross-links, CCT = omega/N, their distribution along a DNA molecule, and particular values of the entropy factors of small loops formed by cross-links in melted regions strongly affect the DNA melting temperature, Tm. On the contrary, for DNA without cross-links, a ten-fold increase or decrease in the entropy factors of small loops does not cause the Tm variation. The comparison of the results of calculation with experimental data suggests that the majority of types of cross-link neither maintain ordered parallel orientation of bases in melted regions nor increase considerably the thermostability of cross-linked base pairs. Four different ways of influence of interstrand cross-linking on the DNA double helix stability are considered. It is shown that cross-linking significantly enhances the influence of single strand stiffness in melted regions on DNA melting behavior.

Melting of cross-linked DNA: I. Model and theoretical methods

Covalent and strong coordination binding to DNA of a large number of antitumour drugs and other compounds leads to interstrand cross-link formation. To investigate cross-link influence on double helix stability, two methods are developed for the calculation of melting curves. The first method is based on Poland's approach. It requires computer time proportional to u.N, where u is the average distance (in base pairs) between neighboring cross-links and N is the number of base pairs in the DNA chain. The method is more suitable when u is not large, and small loops formed by interstrand cross-links in melted regions strongly affect DNA melting. The computer time for the second method, based on the Fixman-Freire approach, does not depend on the number of cross-links and is proportional to I.N (I is the number of exponential functions used for a decomposition of the loop entropy factor). It is more appropriate when N and u are large, and therefore particular values of the entropy factors of small loops do not influence DNA melting behavior.

Studies of DNA dumbbells. VI. Analysis of optical melting curves of dumbbells with a sixteen-base pair duplex stem and end-loops of variable size and sequence

Optical melting curves of 22 DNA dumbbells with the 16-base pair duplex sequence 5'-G-C-A-T-C-A-T-C-G-A-T-G-A-T-G-C-3' linked on both ends by single-strand loops of A, or C, sequences (iota = 2, 3, 4, 6, 8, 10, 14). T sequences (iota = 2, 3, 4, 6, 8, 10), and G iota sequences (iota = 2, 4) were measured in phosphate buffered solvents containing 30, 70, and 120 mM Na+. For dumbbells with loops comprised of at least three nucleotides, stability is inversely proportional to end-loop size. Dumbbells with loops comprised of only two nucleotide bases generally have lower stabilities than dumbbells with three base nucleotide loops. Experimental melting curves were analyzed in terms of the numerically exact (multistate) statistical thermodynamic model of DNA dumbbell melting previously described (T. M. paner, M. Amaratunga & A. S. Benight (1992), Biopolymers 32, 881). Theoretically calculated melting curves were fitted to experimental curves by simultaneously adjusting model parameters representing statistical weights of intramolecular hairpin loop and single-strand circle states. The systematically determined empirical parameters provided evaluations of the energetics of hairpin loop formation as a function of loop size, sequence, and salt environment. Values of the free energies of hairpin loop formation delta Gloop(n > iota) and single-strand circles, delta Gcir(N) as a function of end-loop size, tau = 2-14, circle size, N = 32 + 2 iota, and loop sequence were obtained. These quantities were found to depend on end-loop size but not loop sequence. Their empirically determined values also varied with solvent ionic strength. Analytical expressions for the partition function Q(T) of the dumbbells were evaluated using the empirically evaluated best-fit loop parameters. From Q(T), the melting transition enthalpy delta H, entropy delta S, and free energy delta G, were evaluated for the dumbbells as a function of end-loop size, sequence, and [Na+]. Since the multistate analysis is based on the numerically exact model, and considers a statistically significant number of theoretically possible partially melted states, it does not require prior assumptions regarding the nature of the melting transition, i.e., whether or not it occurs in a two-state manner. For comparison with the multistate analysis, thermodynamic transition parameters were also evaluated directly from experimental melting curves assuming a two-state transition and using the graphical van't Hoff analysis. Comparisons between results of the multistate and two-state analyses suggested dumbbells with loops comprised of six or fewer residues melted in a two-state manner, while the melting processes for dumbbells with larger end-loops deviate from two-state behavior. Dependence of thermodynamic transition parameters on [Na+] as a function of loop size suggests single-strand end-loops have different counterion binding properties than the melted circle. Results are compared with those obtained in an earlier study of dumbbells with the slightly different stem sequence 5'-G-C-A-T-A-G-A-T-G-A-G-A-A-T-G-C-3' linked on the ends by T iota loops (iota = 2, 3, 4, 6, 8, 10, 14).

NMR studies of DNA duplexes singly cross-linked by different synthetic linkers

Molecular modelling studies resulted in the design of a variety of non-nucleotidic covalent linkers to bridge the 3'-end of the (+)-strand and the 5'-end of the (-)-strand in DNA duplexes. Three of these linkers were synthesized and used to prepare singly cross-linked duplexes d(GTGGAATTC)-linker-d(GAATTCCAC). Linker I is an assembly of a propylene-, a phosphate- and a second propylene-group and is thought to mimic the backbone of two nucleotides. Linkers II and III consist of five and six ethyleneglycol units, respectively. The melting temperatures of the cross-linked duplexes are 65 degrees C for I and 73 degrees C for II and III, as compared with 36 degrees C for the corresponding non-linked nonadeoxynucleotide duplex. The three cross-linked duplexes were structurally characterized by nuclear magnetic resonance spectroscopy. The 1H and 31P resonance assignments in the DNA stem were obtained using standard methods. For the resonance assignment of the linker protons, two-dimensional 1H-31P heteronuclear COSY and two-quantum-experiments were used. Distance geometry calculations with NOE-derived distance constraints were performed and the resulting structures were energy-minimized. In duplex I, the nucleotides flanking the propylene-phosphate-propylene-linker do not form a Watson-Crick base pair, whereas in duplexes II and III the entire DNA stem is in a B-type double helix conformation.

Structural Optimization of Non-Nucleotide Loop Replacements for Duplex and Triplex DNAs

Described are studies systematically exploring structural effects in he use of ethylene glycol (EG) oligomers as non-nucleotide replacements for nucleotide loops in duplex and triplex DNAs. The new structurally optimized loop replacements are more stabilizing in duplexes and triplexes than previously described EG-based linkers. A series of compounds ranging in length from tris(ethylene glycol) to octakis(ethylene glycol) are derivatized as monodimethoxytrityl ethers on one end and phosphoramidites on the other, to enable their incorporation into DNA strands by automated methods. These linker molecules span lengths ranging from 13 to 31 Å in extended conformation. They are incorporated into a series of duplex-forming and triplex-forming sequences, and the stabilities of the corresponding helixes are measured by thermal denaturation. In the duplex series, results show that the optimum linker is the one derived from heptakis(ethylene glycol), which is longer than most previous loop replacements studied. This affords a helix with greater thermal stability than one with a natural T(4) loop. In the triplex series, the loop replacements were examined in four separate situations, in which the loop lies in the 5' or 3' orientation and the central purine target strand is short or extends beyond the loop. Results show that in all cases the loop derived from octakis(ethylene glycol) (EG(8)) gives the greatest stability. In the cases where the target strand is short, the EG(8)-linked probe strands bind with affinities in some cases greater than those with a natural pentanucleotide (T(5)) loop. For the cases where the target strand extends beyond the linker, the EG(8)-linked strands are much lower in the 5' loop orientation than in the 3' loop orientation. It is found that extension by one additional nucleotide in one of the bonding domains in the EG-linked series can result in considerably greater stabilities with long target strands. Overall, the data show that optimum loop replacements are longer than would be expected from simple distance analysis. The results are discussed in relation to expected lengths and geometries for double and triple helixes. The findings will be usefull in the design of synthetically modified nucleic acids for use as diagnostic probes, as biochemical tools, and as potential therapeutic agents.