The thermal stability of DNA fragments with tandem mismatches at a d(CXYG).d(CY'X'G) site.

Temperature-Gradient Gel Electrophoresis (TGGE) was employed to determine the thermal stabilities of 28 DNA fragments, 373 bp long, with two adjacent mismatched base pairs, and eight DNAs with Watson-Crick base pairs at the same positions. Heteroduplex DNAs containing two adjacent mismatches were formed by melting and reannealing pairs of homologous 373 bp DNA fragments differing by two adjacent base pairs. Product DNAs were separated based on their thermal stability by parallel and perpendicular TGGE. The polyacrylamide gel contained 3.36 M urea and 19.2 % formamide to lower the DNA melting temperatures. The order of stability was determined in the sequence context d(CXYG).d(CY'X'G) where X.X' and Y.Y" represent the mismatched or Watson-Crick base pairs. The identity of the mismatched bases and their stacking interactions influence DNA stability. Mobility transition melting temperatures (T u) of the DNAs with adjacent mismatches were 1.0-3.6 degrees C (+/-0.2 degree C) lower than the homoduplex DNA with the d(CCAG).d(CTGG) sequence. Two adjacent G.A pairs, d(CGAG).d(CGAG), created a more stable DNA than DNAs with Watson-Crick A.T pairs at the same sites. The d(GA).d(GA) sequence is estimated to be 0.4 (+/-30%) kcal/mol more stable in free energy than d(AA).d(TT) base pairs. This result confirms the unusual stability of the d(GA).d(GA) sequence previously observed in DNA oligomers. All other DNAs with adjacent mismatched base pairs were less stable than Watson-Crick homoduplex DNAs. Their relative stabilities followed an order expected from previous results on single mismatches. Two homoduplex DNAs with identical nearest neighbor sequences but different next-nearest neighbor sequences had a small but reproducible difference in T u value. This result indicates that sequence dependent next neighbor stacking interactions influence DNA stability.     

Structural studies of DNA fragments: the G.T wobble base pair in A, B and Z DNA; the G.A base pair in B-DNA

The crystal structures of five double helical DNA fragments containing non-Watson-Crick complementary base pairs are reviewed. They comprise four fragments containing G.T base pairs: two deoxyoctamers d(GGGGCTCC) and d(GGGGTCCC) which crystallise as A type helices; a deoxydodecamer d(CGCGAATTTGCG) which crystallises in the B-DNA conformation; and the deoxyhexamer d(TGCGCG), which crystallises as a Z-DNA helix. In all four duplexes the G and T bases form wobble base pairs, with bases in the major tautomer forms and hydrogen bonds linking N1 of G with O2 of T and O6 of G with N3 of T. The X-ray analyses establish that the G.T wobble base pair can be accommodated in the A, B or Z double helix with minimal distortion of the global conformation. There are, however, changes in base stacking in the neighbourhood of the mismatched bases. The fifth structure, d(CGCGAATTAGCG), contains the purine purine mismatch G.A where G is in the anti and A in the syn conformation. The results represent the first direct structure determinations of base pair mismatches in DNA fragments and are discussed in relation to the fidelity of replication and mismatch recognition.     

Single base mismatches in DNA. Long- and short-range structure probed by analysis of axis trajectory and local chemical reactivity

We have devised a procedure to generate any single base mismatch in a constant sequence context, and have studied these from two points of view. (1) We have examined electrophoretic mobility of 458 base-pair fragments containing approximately centrally located single mismatches, in polyacrylamide gels, compared to fully matched DNA fragments. We found that no single mismatch caused a significant perturbation of gel mobility, and we conclude that all the mismatches may be accommodated within a helical geometry such that there is no alteration of the path of the helix axis in a straight DNA molecule. (2) We have studied all the single mismatches with respect to reactivity to a number of chemical probes. We found that: (a) No mispaired adenine bases are reactive to diethyl pyrocarbonate and are therefore not simply unpaired such that N-7 is exposed. (b) A number of mispaired thymine bases are reactive to osmium tetroxide, and cytosine bases to hydroxylamine. (c) Where crystal or nuclear magnetic resonance structures are available, the reactivity correlates with exposure of the pyrimidine 5,6 double bonds to attack in the major groove as a result of wobble base-pair formation. This is particularly clear for G.T and I.T base-pairs. (d) Reactivity of bases in mismatched pairs can be dependent on sequence context. (e) Reactivity of the C.C mismatch to hydroxylamine is suppressed at low pH, suggesting that a rearrangement of base-pairing occurs on protonation. The results overall are consistent with the formation of stacked intrahelical base-pairs wherever possible, resulting in no global distortion of the DNA structure, but specific enhancement of chemical reactivity in some cases.     

Structural Studies of DNA Fragments: The G·T Wobble Base Pair in A,B and Z DNA; The G·A Base Pair in B-DNA

Abstract

The crystal structures of five double helical DNA fragments containing non-Watson-Crick complementary base pairs are reviewed. They comprise four fragments containing G·T base pairs: two deoxyoctamers d(GGGGCTCC) and d(GGGGTCCC) which crystallise as A type helices; a deoxydodecamer d(CGCGAATTTGCG) which crystallises in the B-DNA conformation; and the deoxyhexamer d(TGCGCG), which crystallises as a Z-DNA helix. In all four duplexes the G and T bases form wobble base pairs, with bases in the major tautomer forms and hydrogen bonds linking N1 of G with 02 of T and 06 of G with N3 of T. The X-ray analyses establish that the G·T wobble base pair can be accommodated in the A, B or Z double helix with minimal distortion of the global conformation. There are, however, changes in base stacking in the neighbourhood of the mismatched bases. The fifth structure, d(CGCGAATTAGCG), contains the purine purine mismatch G·A where G is in the anti and A in the syn conformation. The results represent the first direct structure determinations of base pair mismatches in DNA fragments and are discussed in relation to the fidelity of replication and mismatch recognition.     

Relative specificities in binding of Watson-Crick base pairs by third strand residues in a DNA pyrimidine triplex motif.

The specificity of binding of Watson-Crick base pairs by third strand nucleic acid residues via triple helix formation was investigated in a DNA pyrimidine triplex motif by thermal melting experiments. The host duplex was of the type A10-X-A10: T10-Y-T10, and the third strand T10-Z-T10, giving rise to 16 possible triplexes with Z:XY inserts, 4 duplexes with the Watson-Crick base pairs (XY) and 12 duplexes with mismatch pairs (XZ), all of whose stabilities were compared. Two Z:XY combinations confirm the primary binding of AT and GC target pairs in homopurine.homopyrimidine sequences by T and C residues, respectively. All other Z:XY combinations in the T:AT environment result in triplex destabilization. While some related observations have been reported, the present experiments differ importantly in that they were performed in a T:AT nearest neighbor environment and at physiological ionic strength and pH, all of which were previously untested. The conclusions now drawn also differ substantially from those in previous studies. Thus, by evaluating the depression in Tm due to base triplet mismatches strictly in terms of third strand residue affinity and specificity for the target base pair, it is shown that none of the triplet combinations that destabilize qualify for inclusion in the third strand binding code for the pyrimidine triplex motif. Hence, none of the mismatch triplets afford a general way of circumventing the requirement for homopurine.homopyrimidine targets when third strands are predominated by pyrimidines, as others have suggested. At the same time, the applicability of third strand binding is emphasized by the finding that triplexes are equally or much more sensitive to base triplet mismatches than are Watson-Crick duplexes to base pair mismatches.     

The effect of base sequence on the stability of RNA and DNA single base bulges

Forty-eight RNA duplexes were constructed that contained all common single base bulges at six different locations. The stabilities of the RNAs were determined by temperature gradient gel electrophoresis (TGGE). The relative stability of a single base bulge was dependent on both base identity and the nearest neighbor context. The single base bulges were placed into two categories. A bulged base with no identical neighboring base was defined as a Group I base bulge. Group II-bulged bases had at least one neighboring base identical to it. Group II bulges were generally more stable than Group I bulges in the same nearest neighbor environments. This indicates that position degeneracy of an unpaired base enhances stability. Differences in the mobility transition temperatures between the RNA fragments with bulges and the completely base-paired reference RNAs were related to free energy differences. Simple models for estimating the free energy contribution of single base bulges were evaluated from the free energy difference data. The contribution of a Group I bulge 5'-(XNZ)-3'.5'-(Z'-X')-3' where N is the unpaired base and X.X' and Z.Z' the neighboring base pairs, could be well-represented (+/-0.34 kcal/mol) by the equation, DeltaG((X)(N)()(Z))(.)((Z)(')(-)(X)(')()) = 3.11 + 0. 40DeltaG(s)()((XZ))(.)((Z)(')(X)(')()). DeltaG(s)()((XZ))(. )((Z)(')(X)(')()) is the stacking energy of the closing base pair doublet. By adding a constant term, delta = -0.3 kcal/mol, to the right side of the above equation, free energies of Group II bulges could also be predicted with the same accuracy. The term delta represents the stabilizing effect due to position degeneracy. A similar equation/model was applied to previous data from 32 DNA fragments with single base bulges. It predicted the free energy differences with a similar standard deviation.     

Processing of mispaired and unpaired bases in heteroduplex DNA in E. coli

Bacteriophage lambda and phi X 174 DNAs, carrying sequenced mutations, have been used to construct in vitro defined species of heteroduplex DNA. Such heteroduplex DNAs were introduced by transfection, as single copies, into E. coli host cells. The progeny of individual heteroduplex molecules from each infective center was analyzed. The effect of the presence of GATC sequences (phi X 174 system) and of their methylation (lambda system) was tested. The following conclusions can be drawn: some mismatched base pairs trigger the process of mismatch repair, causing a localized strand-to-strand information transfer in heteroduplex DNA: transition mismatches G:T and A:C are efficiently repaired, whereas the six transversion mismatches are not always readily recognized and/or repaired. The recognition of transversion mismatches appears to depend on the neighbouring nucleotide sequence; single unpaired bases (frameshift mutation "mismatches") are recognized and repaired, some equally efficiently on both strands (longer and shorter), some more efficiently on the shorter (-1) strand; large non-homologies (about 800 bases) are not repaired by the Mut H, L, S, U system, but some other process repairs the non-homology with a relatively low efficiency; full methylation of GATC sequences inhibits mismatch repair on the methylated strand: this is the chemical basis of strand discrimination (old/new) in mismatch correction; unmethylated GATC sequences appear to improve mismatch repair of a G:T mismatch in phi X 174 DNA, but there may be some residual mismatch repair in GATC-free phi X 174, at least for some mismatches.(ABSTRACT TRUNCATED AT 250 WORDS)     

Thermodynamic characterization of single mismatches found in naturally occurring RNA

Many naturally occurring RNA structures contain single mismatches. However, the algorithms currently used to predict RNA structure from sequence rely on a minimal set of data for single mismatches, most of which occur rather infrequently in nature. As a result, several approximations and assumptions are used to predict the stability of RNA duplexes containing the most common single mismatches. Therefore, the relative frequency of single mismatches was determined by compiling and searching a database of 955 RNA secondary structures. Thermodynamic parameters for duplex formation, derived from optical melting experiments, are reported for 28 oligoribonucleotides containing frequently occurring single mismatches. These data were then combined with previous data to construct a dataset of 64 single mismatches, including the 30 most common in the database. Because of this increase in experimental thermodynamic parameters for single mismatches that occur frequently in nature, more accurate free energy calculations have resulted. To improve the prediction of the thermodynamic parameters for duplexes containing single mismatches that have not been experimentally measured, single mismatch-specific nearest neighbor parameters were derived. The free energy of an RNA duplex containing a single mismatch that has not been thermodynamically characterized can be calculated by: DeltaG degrees 37,single mismatch = DeltaG degrees 37,mismatch nt + DeltaG degrees 37,mismatch-NN interaction + DeltaG degrees 37,AU/GU. Here, DeltaG degrees 37,mismatch is -0.4, -2.1, and -0.3 kcal/mol for A.G, G.G, and U.U mismatches, respectively; DeltaG degrees 37,mismatch-NN interaction is 0.7, -0.5, 0.4, -0.4, and -1.0 kcal/mol for 5'YRR3'/3'RRY5', 5'RYY3'/3'YYR5', 5'YYR3'/3'RYY5', 5'YRY3'/3'RYR5', and 5'RRY3'/3'YYR5' mismatch-nearest neighbor combinations, respectively, when A and G are categorized as purines (R) and C and U are categorized as pyrimidines (Y); and DeltaG degrees 37,AU/GU is a penalty of 1.2 kcal/mol for replacing a G-C base pair with either an A-U or G-U base pair. Similar predictive models were also derived for DeltaH degrees single mismatch and DeltaS degrees single mismatch. These new predictive models, in conjunction with the reported thermodynamics for frequently occurring single mismatches, should allow for more accurate calculations of the free energy of RNA duplexes containing single mismatches and, furthermore, allow for improved prediction of secondary structure from sequence.     

Detecting base pair substitutions in DNA fragments by temperature-gradient gel electrophoresis.

A vertical gel electrophoresis apparatus is described which can distinguish DNA fragments differing by single base pair substitutions. The system employs a homogenous polyacrylamide gel containing urea-formamide and a temperature gradient which runs either perpendicular or parallel to the direction of electrophoresis. The temperature-gradient system simplifies several features of the denaturant-gradient system (1) and is relatively inexpensive to construct. Eight homologous 373 bp DNAs differing by one, two, or nine base pair substitutions were examined. DNA electrophoretic mobility changed abruptly with the temperature induced unwinding of DNA domains. GC to AT substitutions at different locations within the first melting domain, as well as an AT to TA transversion were separated with temperature gradients parallel to the electrophoretic direction. The relative stabilities of the DNAs observed in the gels were compared to predictions of DNA melting theory. General agreement was observed however complete correspondence was not obtained.     

Thermodynamic characterization of naturally occurring RNA single mismatches with G-U nearest neighbors

Due to their prevalence and roles in biological systems, single mismatches adjacent to G-U pairs are important RNA structural elements. Since there are only limited experimental values for the stability of single mismatches adjacent to G-U pairs, current algorithms using free energy minimization to predict RNA secondary structure from sequence assign predicted thermodynamic values to these types of single mismatches. Here, thermodynamic data are reported for frequently occurring single mismatches adjacent to at least one G-U pair. This experimental data can be used in place of predicted thermodynamic values in algorithms that predict secondary structure from sequence using free energy minimization. When predicting the thermodynamic contributions of previously unmeasured single mismatches, most algorithms apply the same thermodynamic penalty for an A-U pair adjacent to a single mismatch and a G-U pair adjacent to a single mismatch. A recent study, however, suggests that the penalty for a G-U pair adjacent to a tandem mismatch should be 1.2 +/- 0.1 kcal/mol, and the penalty for an A-U pair adjacent to a tandem mismatch should be 0.5 +/- 0.2 kcal/mol [Christiansen, M. E. and Znosko, B. M. (2008) Biochemistry 47, 4329-4336]. Therefore, the data reported here are combined with the existing thermodynamic dataset of single mismatches, and nearest neighbor parameters are derived for an A-U pair adjacent to a single mismatch (1.1 +/- 0.1 kcal/mol) and a G-U pair adjacent to a single mismatch (1.4 +/- 0.1 kcal/mol).     

Dimer of 2,7-diamino-1,8-naphthyridine for the detection of mismatches formed by pyrimidine nucleotide bases

Discrimination of base mismatches from normal Watson-Crick base pairs in duplex DNA constitutes a key approach to the detection of single nucleotide polymorphisms (SNPs). We have developed a sensor for a surface plasmon resonance (SPR) assay system to detect G-G, A-A, and C-C mismatch duplexes by employing a surface upon which mismatch-binding ligands (MBLs) are immobilized. We synthesized a new MBL consisting of 2,7-diamino-1,8-naphthyridine (damND) and immobilized it onto a CM5 sensor chip to carry out the SPR assay of DNA duplexes containing a single-base mismatch. The SPR sensor with damND revealed strong responses to all C-C mismatches, and sequence-dependent C-T and T-T mismatches. Compared to ND- and naphthyridine-azaquinolone hybrid (NA)-immobilized sensor surfaces, with affinity to mismatches composed of purine nucleotide bases, the damND-immobilized surface was useful for the detection of the mismatches composed of pyrimidine nucleotide bases.     

Mismatches and bubbles in DNA

Single mismatches in the DNA double helix form nucleation sites for bubbles. Although the overall melting temperature of the duplex is affected to different degrees depending on the probe length, the statistical weights of the bubble states around the defect are always strongly affected. Here we show experimentally that a single mismatch has indeed a dramatic effect on the distribution of intermediate (bubble) states in the melting transition of DNA oligomers. For probe lengths in the range 20-40 bases, the mismatch transforms a transition with many intermediates into a nearly two-state transition. One surprising consequence is the existence of a regime where the sensitivity of a mismatch detection assay based on monitoring intermediate states would increase with probe length. Our results provide experimental constraints on how mismatches should be implemented in models of DNA melting, such as the widely used thermodynamic nearest neighbor model, to which we compare our data.     

Unusual duplex formation in purine rich oligodeoxyribonucleotides

The purine rich oligodeoxyribonucleotides 1C, d(ATGACGGAATA) and 2C, d(ATGAGCGAATA) alone exhibit highly cooperative melting transitions. Analysis of the concentration dependence of melting, and electrophoretic studies indicate that these oligomers can form an unusual purine rich offset double helix. The unusual duplex is predicted to contain four A.T, two G.C, and four G.A mismatch base pairs as well as a single A base stacked on the 3' end of each chain of the helix. Other possible models for the duplex are unlikely because they are predicted to contain many base pairs of low stability. Changing the central sequence to CGG or GGG should destabilize the duplex and this is observed. The unusual duplex of 2C is more stable than the duplex of 1C indicating that the stability of G.A base pairs is quite sensitive to the surrounding sequence. Addition of 1C and 2C to their complementary pyrimidine strands results in normal duplexes of similar stability. We feel that the unusual duplexes are significantly stabilized by the intrinsic stacking tendency of purine bases.     

Effects of metal binding to mismatched base pairs on DNA-mediated charge transfer

Photoinduced hole transfer reaction in DNA duplex bearing cytosine-cytosine (CC) or thymine-thymine (TT) mismatched base pairs as metal-ion binding sites was studied using polyacrylamide gel electrophoresis. Site-specific binding of silver (I) ion to a CC mismatched base pair as well as non-specific binding to multiple sites of nucleobases in the DNA suppressed hole migration through the sequence. In the case of mercury (II) binding to duplex DNA containing single TT mismatch at N3 of the pyrimidine rings, little effect on the efficiency of hole transfer was observed, which is in accordance with a recent theoretical prediction. On the other hand, addition of Hg(II) to duplex containing tandem TT base pairs remarkably reduced hole transfer efficiency, although the calculation has suggested such binding could form high degree of electronic coupling between the hole carrier bases.     

Structures of mismatched base pairs in DNA and their recognition by the Escherichia coli mismatch repair system.

The Escherichia coli mismatch repair system does not recognize and/or repair all mismatched base pairs with equal efficiency: whereas transition mismatches (G X T and A X C) are well repaired, the repair of some transversion mismatches (e.g. A X G or C X T) appears to depend on their position in heteroduplex DNA of phage lambda. Undecamers were synthesized and annealed to form heteroduplexes with a single base-pair mismatch in the centre and with the five base pairs flanking each side corresponding to either repaired or unrepaired heteroduplexes of lambda DNA. Nuclear magnetic resonance (n.m.r.) studies show that a G X A mismatch gives rise to an equilibrium between fully helical and a looped-out structure. In the unrepaired G X A mismatch duplex the latter predominates, while the helical structure is predominant in the case of repaired G X A and G X T mismatches. It appears that the E. coli mismatch repair enzymes recognize and repair intrahelical mismatched bases, but not the extrahelical bases in the looped-out structures.     

Thermodynamics-structure relationship of single mismatches in RNA/DNA duplexes

Thermodynamics of 66 RNA/DNA duplexes containing single mismatches were measured by UV melting methods. Stability enhancements for rG. dT mismatches were the largest of all mismatches examined here, while rU.dG mismatches were not as stable. The methyl group on C5 of thymine enhanced the stability by 0.12 approximately 0.53 kcal mol(-)(1) depending on the identity of adjacent Watson-Crick base pairs, whereas the 2'-hydroxyl group in ribouridine stabilized the duplex by approximately 0.6 kcal mol(-)(1) regardless of the adjacent base pairs. Stabilities induced by the methyl group in thymine, the 2'-hydroxyl group of ribouridine, and an nucleotide exchange at rG.dT and rU.dG mismatches were found to be independent of each other. The order for the mismatch stabilities is rG.dT > rU. dG approximately rG.dG > rA.dG approximately rG.dA approximately rA. dC > rA.dA approximately rU.dT approximately rU.dC > rC.dA approximately rC.dT, although the identity of the adjacent base pairs slightly altered the order. The pH dependence stability and structural changes were suggested for the rA.dG but not for rG.dA mismatches. Comparisons of trinucleotide stabilities for G.T and G.U pairs in RNA, DNA, and RNA/DNA duplexes indicate that stable RNA/DNA mismatches exhibit a stability similar to RNA mismatches while unstable RNA/DNA mismatches show a stability similar to that of DNA mismatches. These results would be useful for the design of antisense oligonucleotides.     

Effects of bulge composition and flanking sequence on the kinking of DNA by bulged bases

We recently showed that bulged bases kink duplex DNA, with the degree of kinking increasing in roughly equal increments as the number of bases in the bulge increases from one to four [Hsieh, C.-H., & Griffith, J.D. (1989) Proc. Natl. Acad. Sci. U.S.A. 86, 4833-4837]. Here we have examined the kinking of DNA by single A, C, G, or T bulges with different neighboring base pairs. Synthetic 30 base pair (bp) duplex DNAs containing 2 single-base bulges spaced by 10 bp were ligated head to tail, and their electrophoretic behavior in highly cross-linked gels was examined. All bulge-containing DNAs showed marked electrophoretic retardations as compared to non-bulge-containing DNA. Regardless of the sequence of the flanking base pairs, purine bulges produced greater retardations than pyrimidine bulges. Furthermore, C and T bulges produced the same retardations as did G and A bulges. Bulged DNA containing different flanking base pairs showed marked differences in electrophoretic mobility. For C-bulged DNA, the greatest retardations were observed with G.C neighbors, the least with T.A neighbors, and an intermediate amount with a mixture of neighboring base pairs. For A-bulged DNA, the retardations were greatest with G.C neighbors, less with T.A neighbors, even less with a mixture of neighboring base pairs, and finally least with C.G neighbors. Thus flanking base pairs affect C-bulged DNA and A-bulged DNA differently, and G.C and C.G flanking base pairs were seen to have very different effects. These results imply an important role of base stacking in determining how neighboring base pairs influence the kinking of DNA by a single-base bulge.     

DNA triple-helix formation at target sites containing duplex mismatches

We have studied the formation of DNA triple helices at target sites that contain mismatches in the duplex target. Fluorescence melting studies were used to examine a series of parallel triple helices that contain all 64 N.XZ triplet combinations at the centre (where N, X and Z are each of the four natural DNA bases in turn). Similar experiments were also performed with N=bis-amino-U (BAU) (for stable recognition of AT base pairs) and N=S (for recognition of TA inversions). We find that the introduction of a duplex mismatch destabilises the C+.GZ, T.AZ and G.TZ triplets. A similar effect is seen with BAU.AZ triplets. In contrast, other base combinations, based on non-standard triplets such as C.AZ, T.TZ, G.CZ and A.CZ are stabilised by the presence of a duplex mismatch. In each case S binds to sites containing duplex mismatches better than the corresponding Watson-Crick base pairs.     

Structures of Escherichia coli DNA mismatch repair enzyme MutS in complex with different mismatches: a common recognition mode for diverse substrates

We have refined a series of isomorphous crystal structures of the Escherichia coli DNA mismatch repair enzyme MutS in complex with G:T, A:A, C:A and G:G mismatches and also with a single unpaired thymidine. In all these structures, the DNA is kinked by ~60° upon protein binding. Two residues widely conserved in the MutS family are involved in mismatch recognition. The phenylalanine, Phe 36, is seen stacking on one of the mismatched bases. The same base is also seen forming a hydrogen bond to the glutamate Glu 38. This hydrogen bond involves the N7 if the base stacking on Phe 36 is a purine and the N3 if it is a pyrimidine (thymine). Thus, MutS uses a common binding mode to recognize a wide range of mismatches.     

Mismatches in DNA double strands: thermodynamic parameters and their correlation to repair efficiencies.

The helix-coil transitions of the 16 octadecameric DNA duplexes dCGTCGTTTXACAACGTCG X dCGACGTTGTX1AAACGACG with A, T, G, and C for X and X1 were measured by UV-absorption. This sequence was taken from former studies of in vivo determination of efficiencies of mismatch repair (Kramer, Kramer, and Fritz (1984) Cell 38, 879-887). The thermodynamic parameters for double strand and mismatch formation have been obtained by evaluating the partition function of a stack model which allowed for loop formation. As a result the mismatches could be classified into wobble base pairs (T/G, G/G, C/A, A/A, A/G), open base pairs, i.e. permanent loops (T/T, C/T, T/C, C/C), and intermediate or weak base pairs (G/T, A/C, G/A). There is no correlation between Tm and the biological repair efficiency of X/X1. The structure classes, however, as described above show a close correlation: Open base pairs show the lowest repair efficiencies, whereas mismatches with high repair efficiency always belong to the structural class of wobble base pairs. Because of the palindromic nearest neighbors of the variation site X/X1, the influence of next-nearest neighbor interactions could be detected and be estimated to about 1 kJ/mol for one stack.