Melting temperature of surface-tethered DNA

A method for the accurate determination of the melting temperature (T_m) of surface-immobilized DNA duplexes that exploits the fluorescence-quenching properties of gold is reported. A thiolated single-stranded DNA probe is chemisorbed onto a gold surface and then hybridized to a fluorophore-labeled complementary sequence. On formation of the duplex, the fluorescence of the label is effectively quenched by the gold surface. As the temperature is increased and the duplex denatures, the fluorophore label moves away from the gold surface and the fluorescence signal is again observed. The increase in fluorescence is measured as the temperature is ramped, and using first-derivative plots, the T_m is determined. To demonstrate the approach, the T_m of the cystic fibrosis DF508 mutation was determined in three different phases: in solution, in suspension immobilized on gold nanoparticles, and immobilized on gold film-coated substrate. The technique was further applied to optimize conditions for differentiation between a surface-immobilized DF508 mutant probe and a mutant/wild-type target exploiting increasing stringency in varying salt and formamide concentrations. The approach has application in optimization of assay conditions for biosensors that use gold substrates as well as in melting curve analysis.     

Determination of melting temperature and temperature melting range for DNA with multi-peak differential melting curves

Many factors that change the temperature position and interval of the DNA helix–coil transition often also alter the shape of multi-peak differential melting curves (DMCs). For DNAs with a multi-peak DMC, there is no agreement on the most useful definition for the melting temperature, T_m, and temperature melting width, ΔT, of the entire DNA transition. Changes in T_m and ΔT can reflect unstable variation of the shape of the DMC as well as alterations in DNA thermal stability and heterogeneity. Here, experiments and computer modeling for DNA multi-peak DMCs varying under different factors allowed testing of several methods of defining T_m and ΔT. Indeed, some of the methods give unreasonable “jagged” T_m and ΔT dependences on varying relative concentration of DNA chemical modifications (r_b), [Na⁺], and GC content. At the same time, T_m determined as the helix–coil transition average temperature, and ΔT, which is proportional to the average absolute temperature deviation from this temperature, are suitable to characterize multi-peak DMCs. They give smoothly varying theoretical and experimental dependences of T_m and ΔT on r_b, [Na⁺], and GC content. For multi-peak DMCs, T_m value determined in this way is the closest to the thermodynamic melting temperature (the helix–coil transition enthalpy/entropy ratio).     

Effect of low-energy microwaves on DNA stability in solution

DNA isolated from liver of healthy and tumor-bearing (sarcoma 45) rats was irradiated in water-salt solution with weak microwaves (64.5 GHz, 50 μW/cm²). The heat stability of DNA increased with irradiation time (a raise of 1.5°C in T _m for “tumor” DNA after 90 min, without changes in ΔT), which may be associated with dehydration of the surrounding Na⁺ ions.     

Electrochemical measurement of DNA hybridization using nanosilver as label and horseradish peroxidase as enhancer

A simple and sensitive electrochemical DNA biosensor based on in situ DNA amplification with nanosilver as label and horseradish peroxide (HRP) as enhancer has been designed. The thiolated oligomer single-stranded DNA (ssDNA) was initially directly immobilized on a gold electrode, and quartz crystal microbalance (QCM) gave the specific amount of ssDNA adsorption of 6.3 ± 0.1 ng/cm². With a competitive format, hybridization reaction was carried out via immersing the DNA biosensor into a stirred hybridization solution containing different concentrations of the complementary ssDNA and constant concentration of nanosilver-labeled ssDNA, and then further binding with HRP. The adsorbed HRP amount on the probe surface decreased with the increment of the target ssDNA in the sample. The hybridization events were monitored by using differential pulse voltammetry (DPV) with the adsorbed HRP toward the reduction of H₂O₂. The reduction current from the enzyme-generated product was related to the number of target ssDNA molecules in the sample. A detection of 15 pmol/L for target ssDNA was obtained with the electrochemical DNA biosensor. Additionally, the developed approach can effectively discriminate complementary from non-complementary DNA sequence, suggesting that the similar enzyme-labeled DNA assay method hold great promises for sensitive electrochemical biosensor applications.     

Helix–coil transition and conformational studies of protamine–DNA complexes

Protamine–DNA complexes prepared by the method of direct and slow mixing in 2.5 × 10^?4M EDTA, pH 8.0, have been studied by thermal denaturation and circular dichroism. The complexes show biphasic melting with T_m at about 50 °C corresponding to the melting of free DNA regions and T_m′ at about 92 °C corresponding to the melting of protamine-bound regions. In protamine-bound regions there are 1.38 amino acid residues per nucleotide, indicating a nearly completely charge neutralization. T_m is increased but T_m′ is not when the ionic strength of the buffer is raised. This also supports a full charge neutralization in protamine-bound regions. The circular dichroism of the complexes can be decomposed into two components, Δ_ε0 of free DNA regions in B-form conformation and Δ_εb of protamine-bound regions in a characteristic conformation neither that of B- nor C-form but somewhere between them.     

Solution conformations of B. subtilis ribosomal 5S RNA: a calorimetric study

The unfolding of B. subtilis 5S RNA is examined by direct calorimetric measurement in the presence of various concentrations of Na⁺ and Mg²⁺. The composite differential scanning calorimetry (DSC) curve is analyzed into 3–5 individual two-state melting transitions. In the absence of added Na⁺ or Mg²⁺, the 5S RNA segments melt together at T_m = 40°C. Addition of Na⁺ stabilizes the molecular structure (T_m = 56°C) and widens the melting temperature range, so that up to five component transitions are observed. Addition of Mg²⁺ alone produces a very stable structure (T_m = 75°C) with highly cooperative melting. Finally, addition of both Na⁺ and Mg²⁺ produces the highest stability (T_m = 76°C). The results are interpreted according to hypothetical secondary and tertiary base-pairing schemes. The conformational changes demonstrated here may facilitate the movement of the protein synthesis machinery during RNA translation.     

Helix-coil transition in nucleoprotein. Effect of ionic strength on thermal denaturation of polylysine-DNA complexes

Thermal denaturation of direct-mixed and reconstituted polylysine–DNA complexes in 2.5 × 10^?4 M EDTA, pH 8.0 and various concentrations of NaCl has been studied. For both complexes, increasing ionic strength of the solution raises T_m, the melting temperature of free base pairs. The linear dependence of T_m on log Na⁺ indicates that the concept of electrostatic shielding on phosphate lattice of an infinitely long pure DNA by Na⁺ can be applied to short free DNA segments in a nucleoprotein. For a direct-mixed polylysine–DNA complex, the melting temperature of bound base pairs T_m′ remains constant at various ionic strengths. On the other hand, the T_m′ in a reconstituted polylysine–DNA complex is shifted to lower temperature at higher ionic strength. This phenomenon occurs for reconstituted complex with long polylysine of one thousand residues or short polylysine of one hundred residues. It is shown that such a decrease of T_m′ is not due to a reduction of coupling melting between free and bound regions in a complex when the ionic strength is raised. It is also not due to intermolecular or intramolecular change from a reconstituted to a direct-mixed complex. It is suggested that this phenomenon is due to structural change on polylysine-bound regions by ionic strength. It is suggested further that Na⁺ may replace water molecules and bind polylysine-bound regions in a reconstituted complex. Such a dehydration effect destabilizes these regions and lowers T_m′. This explanation is supported by circular dichroism (CD) results.     

Estimation of the diversity between DNA calorimetric profiles,differential melting curves and corresponding melting temperatures

The Poland–Fixman–Freire formalism was adapted for modeling of calorimetric DNA melting profiles, and applied to plasmid pBR 322 and long random sequences. We studied the influence of the difference (H_GC?H_AT) between the helix‐coil transition enthalpies of AT and GC base pairs on the calorimetric melting profile and on normalized calorimetric melting profile. A strong alteration of DNA calorimetrical profile with H_GC?H_AT was demonstrated. In contrast, there is a relatively slight change in the normalized profiles and in corresponding ordinary (optical) normalized differential melting curves (DMCs). For fixed H_GC?H_AT, the average relative deviation (S) between DMC and normalized calorimetric profile, and the difference between their melting temperatures (T_cal?T_m) are weakly dependent on peculiarities of the multipeak fine structure of DMCs. At the same time, both the deviation S and difference (T_cal?T_m) enlarge with the temperature melting range of the helix‐coil transition. It is shown that the local deviation between DMC and normalized calorimetric profile increases in regions of narrow peaks distant from the melting temperature.     

Studies on poly(L-lysine50, L-tyrosine50)-DNA interaction

Interaction between poly(Lys⁵⁰, Tyr⁵⁰) and DNA has been studied by absorption, circular dichroism (CD), and fluorescence spectroscopy and thermal denaturation in 0.001M Tris, pH 6.8. The binding of this copolypeptide to DNA results in an absorbance enhancement and fluorescence quenching on tyrosine. There is also an increase in the tyrosine CD at 230 nm. The CD of DNA above 250 nm is slightly shifted to the longer wavelength which is qualitatively similar to, but quantitatively much smaller than, that induced by polylysine binding. At physiological pH the poly(Lys⁵⁰, Tyr⁵⁰)–DNA complex is soluble until there is one lysine and one tyrosine per nucleotide in the complex. The same ratio of amino acid residues to nucleotide has also been observed in copolypeptide-bound regions of the complex. The addition of more poly(Lys⁵⁰, Tyr⁵⁰) to DNA yields a constant melting temperature, T_m′, for bound base pairs at 90°C which is close to that of polylysine-bound DNA under the same condition. The melting temperature, T_m, of free base pairs at about 60°C on the other hand, is increased by 10°C as more copolypeptide is bound to DNA. As the temperature is raised, both absorption and CD spectra of the complexes with high coverage are changed, suggesting structural alteration, perhaps deprotonation, on bound tyrosine. The results in this report also suggest that intercalation of tyrosine in DNA is unlikely to be the mode of binding.     

Microcalorimetric Investigation of DNA,poly(dA)poly(dT) and poly[d(A-C)]poly[d(G-T)] Melting in the Presence of Water Soluble (Meso tetra (4 N oxyethylpyridyl) Porphyrin) and its Zn Complex

Abstract

Thermodynamic parameters of melting process (δH_m, T_m, δT_m) of calf thymus DNA, poly(dA)poly(dT) and poly(d(A-C))·poly(d(G-T)) were determined in the presence of various concentrations of TOEPyP(4) and its Zn complex. The investigated porphyrins caused serious stabilization of calf thymus DNA and poly poly(dA)poly(dT), but not poly(d(A-C))poly(d(G-T)). It was shown that TOEpyp(4) revealed GC specificity, it increased T_m of satellite fraction by 24°C, but ZnTOEpyp(4), on the contrary, predominately bound with AT-rich sites and increased DNA main stage T_m by 18°C, and T_m of poly(dA)poly(dT) increased by 40 °C, in comparison with the same polymers without porphyrin. ZnTOEpyp(4) binds with DNA and poly(dA)poly(dT) in two modes—strong and weak ones. In the range of r from 0.005 to 0.08 both modes were fulfilled, and in the range of r from 0.165 to 0.25 only one mode—strong binding—took place. The weak binding is characterized with shifting of T_m by some grades, and for the strong binding T_m shifts by ～ 30–40°C. Invariability of ΔH_m of DNA and poly(dA)poly(dT), and sharp increase of T_m in the range of r from 0.08 to 0.25 for thymus DNA and 0.01–0.2 for poly(dA)poly(dT) we interpret as entropic character of these complexes melting. It was suggested that this entropic character of melting is connected with forcing out of H₂O molecules from AT sites by ZnTOEpyp(4) and with formation of outside stacking at the sites of binding. Four-fold decrease of calf thymus DNA melting range width ΔT_m caused by increase of added ZnTO- Epyp(4) concentration is explained by rapprochement of AT and GC pairs thermal stability, and it is in agreement with a well-known dependence, according to which ΔT～T_GC-T_AT for DNA obtained from higher organisms (L. V. Berestetskaya, M. D. Frank-Kamenetskii, and Yu. S. Lazurkin. Biopolymers 13, 193–205 (1974)). Poly (d(A-C))poly(d(G-T)) in the presence of ZnTOEpyp(4) gives only one mode of weak binding. The conclusion is that binding of ZnTOEpyp(4) with DNA depends on its nucleotide sequence.     

On the hydration of DNA. I. Preferential hydration and stability of DNA in concentrated trifluoroacetate solution

The hydration of DNA is an important factor in the stability of its secondary structure. Methods for measuring the hydration of DNA in solution and the results of various techniques are compared and discussed critically. The buoyant density of native and denatured T-7 bacteriophage DNA in potassium trifluoroacetate (KTFA) solution has been measured as a function of temperature between 5 and 50°C. The buoyant density of native DNA increased linearly with temperature, with a dependence of (2.3 ± 0.5) × 10^?4 g/cc-°C. DNA which has been heat denatured and quenched at 0°C in the salt solution shows a similar dependence of buoyant density on temperature at temperatures far below the T_m, and above the T_m. However, there is an inflection region in the buoyant density versus T curve over a wide range of temperatures below the T_m. Optical density versus temperature studies showed that this is due to the. inhibition by KTFA of recovery of secondary structure on quenching. If the partial specific volume is assumed to be the same for native and denatured DNA, the loss of water of hydration on denaturation is calculated to be about 20% in KTFA at a water activity of 0.7 at 25°C. By treating the denaturation of DNA as a phase transition, an equation has immmi derived relating the destabilizing effect of trifluoroacetate to the loss of hydration on denaturation. The hydration of native DNA is abnormally high in the presence of this anion, and the loss of hydration on denaturation is greater than in CsCl. In addition, trifluoroacetate appears to decrease the ΔHof denaturation.     

Synthesis of Polyoxamic Acid (2-Amino-2-deoxy-l-xylonic Acid

The rate of precipitation of the retrograded amylose product from a dil. amylose solution was determined by the centrifugal method. The results showed that the relation of the quantity of precipitate vs. time did not fit the typical second order reaction for the coalescence of colloidal particles but fitted the crystallization formula, in appearance.

The rate of precipitation was in proportion to (c-c_a)^1.5, where c is the amylose concentration and c_a the concentration of the dil. solution phase in the phase-separated solution. When the temperature dependence of the rate was treated according to the crystallization of polymers, it was found that the rate was in proportion to T_m²/T(ΔT)², where T_m is the melting point of the polymer in solution and ΔT is (T_m?T). The T_m thus obtained was 120°C for an amylose solution. These results suggested a certain correlation between the amylose retrogradation and the crystallization.     

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

The preparation and melting of a 16 base-pair duplex DNA linked on both ends by C¹²H²⁴ (dodecyl) chains is described. Absorbance vs temperature curves (optical melting curves) were measured for the dodecyl-linked molecule and the same duplex molecule linked on the ends instead by T₄ loops. Optical melting curves of both molecules were measured in 25, 55, and 85 mM Na⁺ and revealed, regardless of [Na ⁺], the duplex linked by dodecyl loops is more stable by at least 6°C than the same duplex linked by T₄ loops. Experimental curves in each salt environment were analyzed in terms of the two-state and multistate theoretical models. In the two-state, or van't Hoff analysis, the melting transition is assumed to occur in an all-or-none manner. Thus, the only possible states accessible to the molecule throughout the melting transition are the completely intact duplex and the completely melted duplex or minicircle. In the multistate analysis no assumptions regarding the melting transition are required and the statistical occurrence of every possible partially melted state of the duplex is explicitly considered. Results of the analysis revealed the melting transitions of both the dodecyl-linked molecule and the dumbbell with T₄ end loops are essentially two state in 25 and 55 mM Na⁺. In contrast, significant deviations from two-state behavior were observed in 85 m MNa⁺. From our previously published melting data of DNA dumbbells with T_n end loops where n = 2, 3, 4, 6, 8, 10, 14 [T. M. Paner, M. Amaratunga, and A. S. Benight, (1992) Biopolymers, Vol. 32, pp. 881–892] and the dumbbell with T₄ end loops of this study, a plot of d(T_m)/d ln [Na⁺] was constructed. Extrapolation of this data to n = 1 intersects with the value of d (T_m)/d ln [Na⁺] obtained for the alkyl-linked dumbbell, suggesting the salt-dependent stability of the alkyl-linked molecule behaves as though the duplex of this molecule were linked by end loops comprised of a single T residue. © 1993 John Wiley & Sons, Inc.     

The effect of deuterium oxide on the stability of the collagen model peptides H‐(Pro‐Pro‐Gly)10‐OH,H‐(Gly‐Pro‐4(R)Hyp)9‐OH,and Type I collagen

The collagen triple helix has a larger accessible surface area per molecular mass than globular proteins, and therefore potentially more water interaction sites. The effect of deuterium oxide on the stability of collagen model peptides and Type I collagen molecules was analyzed by circular dichroism and differential scanning calorimetry. The transition temperatures (T_m) of the protonated peptide (Pro‐Pro‐Gly)₁₀ were 25.4 and 28.7°C in H₂O and D₂O, respectively. The increase of the T_m of (Pro‐Pro‐Gly)₁₀ measured calorimetrically at 1.0°C min^?1 in a low pH solution from the protonated to the deuterated solvent was 5.1°C. The increases of the T_m for (Gly‐Pro‐4(R)Hyp)₉ and pepsin‐extracted Type I collagen were measured as 4.2 and 2.2°C, respectively. These results indicated that the increase in the T_m in the presence of D₂O is comparable to that of globular proteins, and much less than reported previously for collagen model peptides [Gough and Bhatnagar, J Biomol Struct Dyn 1999, 17, 481–491]. These experimental results suggest that the interaction of water molecules with collagen is similar to the interaction of water with globular proteins, when the ratio of collagen to water is very small and collagen is monomerically dispersed in the solvent. © 2009 Wiley Periodicals, Inc. Biopolymers 93: 93–101, 2010. This article was originally published online as an accepted preprint. The “Published Online” date corresponds to the preprint version. You can request a copy of the preprint by emailing the Biopolymers editorial office at biopolymers@wiley.com     

Equilibrium and kinetics of thermal unfolding of yeast 5.8S ribosomal RNA in aqueous salt solutions

Equilibrium and kinetics of thermal melting of yeast 5.8S ribosomal RNA in aqueous NaCl were investigated by differential thermal melting and temperature jump methods. Two peaks were observed in each of the melting curves at 1 mM-1 M Na⁺ and linearity between each melting temperature T_m and log[Na⁺] was found at [Na⁺> 10 mM. From the difference spectrum ratio, $\text{d}\text{A}{}_{280}\text{d}\text{A}{}_{260}$, the G-C content in the local structures was calculated to be 91 and 56%. The temperature jump to 70–85°C in aqueous 30 mM Na⁺ of the RNA solution induced first-order kinetics, from which the kinetically determined melting curve was calculated. The curve could be approximately described in a Gaussian form with a T_m which agrees well with the high T_m in the static melting curve at 30 mM Na⁺. The kinetic properties of the reaction indicated a double helix-coil transition. However, the temperature jump to 20–60°C did not induce monophasic kinetics. The kinetic amplitude of the slow component showed a T_m which corresponded to the low T_m in the static melting curve at 30 mM Na⁺. The slow relaxation had the characteristics of a double helix-to-coil transition. However, contributions from very fast processes including single strand unstacking, were most noticeable in the low temperature melting region of the static curve. The thermodynamic parameters of both transitions from double helix to coil were analysed in detail. Both activation energies for helix formation were negative, and the nucleation is thought to follow a process similar to that in oligonucleotides. Values of T_m and enthalpy change of both helix-coil transitions indicated the cloverleaf model as the most plausible one for some limited regions of yeast 5.8S RNA among the previously proposed models: burp gun, cloverleaf and Rubin's models.     

Interaction between tryptophan‐Sm(III) complex and DNA with the use of a acridine orange dye fluorophor probe

The interaction of the Trp–Sm(III) complex with herring sperm DNA (hs‐DNA) was investigated with the use of acridine orange (AO) dye as a spectral probe for UV‐vis spectrophotometry and fluorescence spectroscopy. The results showed that the both the Trp–Sm(III) complex and the AO molecule could intercalate into the double helix of the DNA. The Sm(III)–(Trp)₃ complex was stabilized by intercalation into the DNA with binding constants: K^?_25°C = 7.14 × 10⁵ L·mol^?1 and K^?_37°C = 5.28 × 10⁴ L·mol^?1, and it could displace the AO dye from the AO–DNA complex in a competitive reaction. Computation of the thermodynamic functions demonstrates that Δ_rH_m^? is the primary driving power of the interaction between the Sm(III)(Trp)₃ complex and the DNA. The results from Scatchard and viscometry methods suggested that the interaction mode between the Sm(III)(Trp)₃ complex and the hs‐DNA is groove binding and weak intercalation binding. Copyright © 2015 John Wiley & Sons, Ltd.     

Unique Properties of Nucleic Acid from <Emphasis Type="Italic">Bacillus subtilis</Emphasis> Phage SP-15

BACTERIOPHAGE SP-15 is a large, generalized transducing phage of Bacillus subtilis and B. licheniformis. The DNA extracted from the purified phage has unusual physical properties: its melting temperature (T_m) in 0.15 M NaCl, 0.015 M sodium citrate (SSC) is very low, 61.5° C and its buoyant density in neutral CsCl is very high, 1.761 g/ml.¹. We describe here additional unique features of SP-15 DNA: the presence of (1) a new modified pyrimidine which partially replaces the thymine; (2) a compound which reacts with orcinol as a pentose; (3) alkali-sensitive phosphodiester bonds; and (4) glucose.     

Nuclear DNA Ligase and Its Action on Chromatin DNA in Neuronal, Glial and Liver Nuclei Isolated from Adult Guinea Pigs

Abstract: DNA ligase activities were measured in neuron-rich and glial nuclear preparations and liver nuclei isolated from adult guinea pigs. The enzymatic properties of cerebral and liver nuclear DNA ligases were studied with isolated nuclei and nuclear extracts. ATP (K_m= 46–48 μM) and bivalent cation (Mg²⁺ or Mn²⁺) were required for the maximal activities in cerebral and liver nuclei. β-Mercaptoethanol did not affect the activities, but N-ethylmaleimide and p-chloromercuribenzoate completely inhibited the activities. Deoxyadenosine-5′-triphosphate partially inhibited the activities in both cerebral and liver nuclei. An interdependent effect of Na⁺ and Mg²⁺ on the enzyme activities was observed. A high concentration (200 mM) of Na⁺ activated both enzymes and shifted to the acid side the optimal pH for both enzymes. DNA ligase was more easily extracted with lower concentrations of NaCl from liver nuclei than from cerebral nuclei, but the extraction curves from both nuclear species reached a plateau level (92% of total activities of nuclear enzymes) at 200 mM-NaCl. Apparent K_m for the substrate [³²P]phosphoryl DNA was determined according to a modification of the Michaelis-Menten equation, which was applied for the case where an unknown amount of substrate nicks in chromatin DNA coexisted with the nicks in exogenous substrate DNA. Neuronal and glial nuclear enzymes had similar K_m values (about 20 μg of [³²P]phosphoryl DNA/ml), but the liver nuclear enzyme had a higher K_m value (54 μg of [³²P]phosphoryl DNA/ml). The modified Michaelis-Menten equation provided the amounts of nicks available as substrate in chromatin DNA of isolated nuclei. Neuronal and glial nuclei contained 1.5 and 0.29 pmol of nicks/μg of nuclear DNA, respectively, in contrast to an intermediate amount of nicks in liver nuclei (0.63 pmol/μg of nuclear DNA). DNA ligase activity in neuronal nuclei [312 units (fmol of 5′-phosphomonoester converted into a phosphatase-resistant form per min at 37°C) per μg of nuclear DNA] was 11-fold higher than that in glial nuclei [28.7 units/μg of nuclear DNA]. Liver nuclei contained an intermediate activity [54.7 units/μg of nuclear DNA].     

The Parallel and Antiparallel Triplex Formation and Stability of Self Complementary Oligonucleotides Containing 2′-Fluoro-arabinosyl Thymine and 5-Methyl-2′-Deoxycytidine

Abstract

We examined the effects of 1–(2-deoxy -2-fluoro-β-D-arabinofuranosyl)-thymine (or FMAU, a potent antiviral nucleoside) on the stability of duplex and triplexes. When compared the stability of the self-complementary 5′-A₅T₅ duplex with 5′-A₅X₅ (X = FMAU), duplex containing FMAU has much higher melting temperature (T_m). 5′-A₆T₅T₃X₃T₅F₃X₃ and T₃X₃T₅A₆T₅F₃X₃ form the parallel and antiparallel triplexes T₃X₃: A₆:X₃X₃, respectively. The former exhibited the typical T:A:T triplex behavior with only one melting temperature at 70 °C and 45 °c in 1.0 M and 0.2 M NaCl solution, respectively, whereas the latter has two T_m values at 56 °C and 28 °C in 1.0 M solution. FMAU clearly stabilize the triplex structure as A₆T₂₂ which forms the parallel triplex T₆:A₆:T₆ has also only one T_m at 54 °C and 37 °C in high and iow salt concentration solutions, respectively. A 31mer 5′-TCCTCCTTTTTTAGGAGGATTTTTTGGTGGT and 5′-TCCTCCTTTTTTAGGAGGATTTTTTX'X'TX'X'T (X' = 2′-deoxy-5-methylcytidine) were prepared to study their triplex forming potential. The former was found to have a week interaction of the Watson-Crick duplex with the mismatched third-strand at all pH. The latter formed a stable triplex at lower pH consistent with required protonation on the 5-methylcytosine base. For these studies we developed a simple PC desktop spreadsheet program to calculate the first derivative profile of the melting curve data.

This paper is dedicated to Prof. Jacques H. van Boom on the occasion of his 60th birthday.