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Schematic representation of the apparent disparate destabilization rankings for CNC and GNG bulged duplexes as a function of base identity and flanking residues. The eight heteroduplexes are arranged/ranked according to bulge base identity (A, T, C and G appear from top to bottom) and flanking residues (CC and GG positioned in the left and right columns, respectively). The bulge-induced destabilization energies (ΔΔG in kcal/mol) are expressed relative to the parent dodecamer with the respective heteroduplexes color-coded according to their corresponding category: Red Boxes represent highly destabilized bulges that exhibit non-two-state melting behavior, whereas Blue Boxes comprise moderately destabilizing bulges that undergo ideal two-state dissociation. The magnitude of energetic destabilization (ΔΔG) may be enhanced when a specific bulge base is positioned between Gs (A and C) or within Cs (T and G) as viewed in the horizontal comparisons. Moreover, the trends observed for CNC versus GNG bulges are quite distinct in terms of the overall ΔΔG magnitudes as noted in the vertical comparisons.

Schematic representation of the apparent disparate destabilization rankings for CNC and GNG bulged duplexes as a function of base identity and flanking residues. The eight heteroduplexes are arranged/ranked according to bulge base identity (A, T, C and G appear from top to bottom) and flanking residues (CC and GG positioned in the left and right columns, respectively). The bulge-induced destabilization energies (ΔΔG in kcal/mol) are expressed relative to the parent dodecamer with the respective heteroduplexes color-coded according to their corresponding category: Red Boxes represent highly destabilized bulges that exhibit non-two-state melting behavior, whereas Blue Boxes comprise moderately destabilizing bulges that undergo ideal two-state dissociation. The magnitude of energetic destabilization (ΔΔG) may be enhanced when a specific bulge base is positioned between Gs (A and C) or within Cs (T and G) as viewed in the horizontal comparisons. Moreover, the trends observed for CNC versus GNG bulges are quite distinct in terms of the overall ΔΔG magnitudes as noted in the vertical comparisons.

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DNA bulges are biologically consequential defects that can arise from template-primer misalignments during replication and pose challenges to the cellular DNA repair machinery. Calorimetric and spectroscopic characterizations of defect-containing duplexes reveal systematic patterns of sequence-context dependent bulge-induced destabilizations. These...

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... analysis of single base bulges embedded within a common host duplex reveals that it is difficult to define in general/ predictive terms the origins of bulge-induced thermo- dynamic and extrathermodynamic influences. This challenge is apparent when evaluating the impact of 'inserting' a base within either the sense or anti-sense strand of the parent GG/CC dodecamer, as illustrated in Figure 5. Inspection of the rows in Figure 5 reveals that the magnitude of destabilization observed for a particular bulge may be greater when the unpaired base is either positioned between Gs (i.e. ...
Context 2
... analysis of single base bulges embedded within a common host duplex reveals that it is difficult to define in general/ predictive terms the origins of bulge-induced thermo- dynamic and extrathermodynamic influences. This challenge is apparent when evaluating the impact of 'inserting' a base within either the sense or anti-sense strand of the parent GG/CC dodecamer, as illustrated in Figure 5. Inspection of the rows in Figure 5 reveals that the magnitude of destabilization observed for a particular bulge may be greater when the unpaired base is either positioned between Gs (i.e. A and C) or between Cs (i.e. ...
Context 3
... and G). Moreover, the ÁÁG ranking for a particular bulge base embedded within the CNC and GN 0 G contexts are quite distinct, as evidenced when comparing the respective columns in Figure 5. In the section that follows, we propose an alternative analysis to explore the potential origins of bulge-induced energetic perturbations that may be rationalized in terms of a 'con- certed/coupled' dependence on both base and flanking residue identity. ...

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... These efforts have complemented biophysical studies of canonical DNA with detailed thermodynamic analysis of lesion impacts on duplex energetics [31][32][33][34][35][36][37][38][39][40][41][42] as well as lesion recognition and repair by DNA glycosylases [23,29,43,44]. While establishing the foundation required for understanding the energetic basis of complex biological systems, the Breslauer research group has focused on gene transcription regulation, repair, and replication [29,30,39,45,46]. Professor Breslauer's impressive academic career spanning five decades is chronicled in a recent retrospective [23] as his research group continues to pursue effective therapeutic interventions for combating and treating infectious diseases such as the SAR-CoV-2 pandemic [47]. ...
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... These energy databases also characterize DNA structures that contain biologically consequential mismatches (37,38), modified bases/lesions (37,(39)(40)(41)(42)(43)(44)(45)(46)(47), as well as nonduplex secondary structures, including the energetics of triplexes (48)(49)(50)(51)(52), tetraplexes (53-56) (associated with modulating telomere stability and epigenetic modifications) (57,58), and higher order, functionally relevant DNA assemblies (59)(60)(61)(62)(63)(64). My laboratory's triplex DNA studies were performed in collaboration with Peter Dervan's group, whom I knew well from our time together as graduate students at Yale. ...
... These energy databases also characterize DNA structures that contain biologically consequential mismatches (37,38), modified bases/lesions (37,(39)(40)(41)(42)(43)(44)(45)(46)(47), as well as nonduplex secondary structures, including the energetics of triplexes (48)(49)(50)(51)(52), tetraplexes (53-56) (associated with modulating telomere stability and epigenetic modifications) (57,58), and higher order, functionally relevant DNA assemblies (59)(60)(61)(62)(63)(64). My laboratory's triplex DNA studies were performed in collaboration with Peter Dervan's group, whom I knew well from our time together as graduate students at Yale. ...
... The examples in Figure 1 underscore the need for comparative structural studies in parallel to the corresponding energy characterizations. Furthermore, the magnitudes of these structurally/conformationally "silent," lesion-induced energy perturbations were consistent with their destabilizing impact beyond the lesion site to create domains of genome instability (37,39,40,42,78). We proposed that such energetically perturbed domains may serve as initial DNA recognition elements for the machinery of repair, a phenomenon we referred to as energetic recognition (79). ...
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... Another peculiarity of mtDNA repeats is their quite short length, with majority of them shorter than 20 bases [1, 3, 5-7, 10, 20, 21]. Also, from the plethora of experimental DNAseq and/or RNAseq data as well as from the features of miRNA/mRNA interaction [69][70][71][72][73][74][75][76][77] it is known that there is a limit on the minimal length of DNA or RNA stretches that are useful for base-pairing (for example, perfect base pairing of 7-8 nucleotides of miRNA seed region is required for proper miRNA/mRNA interaction [69]). Thus, it is important to design an algorithm focused on short repeats -not all existed algorithms are able to work with imperfect repeats as short as 10 b.p. ...
... We allowed only non-tandem mismatches because of 1) the average length of previously known mitochondrial imperfect repeats is not more than 20 bases [1, 3, 5-7, 10, 20, 21]; 2) thermodynamics of duplex formation in the case of interspersed mismatches is additive, linear and wellestablished [74,75]; 3) the dependence of the duplex stability of tandem mismatch on the identity, length and context-specificity of the flanking base pairs [76]. Additionally, we keep off indels due to the same reasons (context-specific dependence of the bulges stability) [74,77]. These simplifications are biologically exceptionally meaningful due to short nature of mitochondrial imperfect repeats found in this study (on average 12 bases). ...
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... 27 This follows similar conclusions for DNA bulges. 20,28 Melting temperatures for single bulges in RNA hairpins [29][30][31] as well as for longer bulges 32 further highlight these shortcommings. Therefore, there is a motivation to go beyond the nearest- neighbor model but which are still computationally efficient to handle a large number of sequences. ...
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... Next, we investigated the influence of polyamine derivatives X0, X1 and X2 on duplex stability, inserted as bulges in the middle of the sequence (Table 1, entry ON7-ON9). The changes of duplex stability caused by single nucleotide bulges differ and depend on the type of flanking bases [46,47]. Incorporation of X0-X2 resulted in a lowering of melting temperature independently of polyamine residue. ...
... Yet, even three positive charges of a spermine residue do not neutralize the bulge effect as such. The observed changes of ΔG for the studied duplexes (ON7-ON9) are in the range observed for duplexes with a single bulge (ΔΔG, 2-6 kcal/mol) [46,47]. ...
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... Currently, only one study exists in which thermodynamic properties of 1-to 3-nt adenine or uracil bulge loop RNA were examined (Longfellow et al. 1990). Single-nucleotide bulge loops have been studied in both RNA and DNA constructs (Zhu and Wartell 1999;Tanaka et al. 2004;Blose et al. 2007;Minetti et al. 2010). A recent study examined the thermodynamic stability of the trinucleotide bulge loops in RNA (Murray et al. 2014). ...
... Single-base bulge loops have been extensively studied in DNA and RNA in 1 M NaCl (Tanaka et al. 2004;Blose et al. 2007;Minetti et al. 2010). Temperature-gradient gel electrophoresis has been performed on DNA and RNA single bulge loop constructs in one study where adenine and guanine 1-nt bulge loops had similar mobility for RNA and DNA constructs, implying similar structural conformations form in these constructs (Zhu and Wartell 1999). ...
... where N = number of nucleotides in the bulge, with N values measured between 1 and 5. Single-nucleotide bulge loops have been studied in DNA (LeBlanc and Morden 1991; Zhu and Wartell 1999;Minetti et al. 2010) but the data on larger bulge loops have not been systematically collected. In the LeBlanc and Morden study, the adenine and guanine single-nucleotide bulge loops DG W 37 loop parameters were 4.6 and 4.4 kcal/mol in the 5 ′ T-(Bulge)-T3 ′ helical context. ...
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Chapter
This chapter presents an overview of calorimetric methodology and its applications to study the thermodynamic properties of biological macromolecules. The narrative focuses primarily on experimental techniques that are utilized for the energetic characterization of association and dissociation processes, specifically isothermal titration calorimetry (ITC) and differential scanning calorimetry (DSC). The systems of interest are selected primarily on the basis of their relevance within the fields of biochemistry, bioengineering, and biotechnology. Special areas of emphasis include macromolecular association, folding, and recognition, encompassing protein—protein, protein—nucleic acid, and protein—ligand interactions.