Forces maintaining the DNA double helix.

Despite the common acceptance that the enthalpy of DNA duplex unfolding does not depend on temperature and is greater for the CG base pair held by three hydrogen bonds than for the AT base pair held by only two, direct calorimetric measurements have shown that the enthalpic and entropic contributions of both base pairs are temperature dependent and at all temperatures are greater for the AT than the CG pair. The temperature dependence results from hydration of the apolar surfaces of bases that become exposed upon duplex dissociation. The larger enthalpic and entropic contributions of the AT pair are caused by water fixed by this pair in the minor groove of DNA and released on duplex dissociation. Analysis of the experimental thermodynamic characteristics of unfolding/refolding DNA duplexes of various compositions shows that the enthalpy of base pairing is negligibly small, while the entropic contribution is considerable. Thus, DNA base pairing is entropy driven and is coupled to the enthalpy driven van der Waals base pair stacking. Each of these two processes is responsible for about half the Gibbs energy of duplex stabilization, but all the enthalpy, i.e., the total heat of melting, results from dissociation of the stacked base pairs. Both these processes tightly cooperate: while the pairing of conjugate bases is critical for recognition of complementary strands, stacking of the flat apolar surfaces of the base pairs reinforces the DNA duplex formed.

Forces maintaining the DNA double helix and its complexes with transcription factors.

Precise calorimetric studies of DNA duplexes of various length and composition have revised several long-held beliefs about the forces holding together the double helix and its complexes with the DNA binding domains (DBDs) of transcription factors. Heating DNA results in an initial non-cooperative increase of torsional oscillations in the duplex, leading to cooperative dissociation of its strands accompanied by extensive heat absorption and a significant heat capacity increment. The enthalpy and entropy of duplex dissociation are therefore temperature dependent quantities. When compared at the same temperature the enthalpic and entropic contributions the CG base pair are less than that of the AT pair - not more as previously assumed from the extra hydrogen bond. Thus the stabilizing effect of the CG base pair comes from its smaller entropic contribution. The greater enthalpic and entropic contributions of the AT pair result from water fixed by its polar groups in the minor groove of DNA. This water is also responsible for the so-called "nearest-neighbour effects" used to explain the sequence-dependent stabilities of DNA duplexes. Removal of this water by binding DBDs to the minor groove makes this an entropy driven process, in contrast to major groove binding which is enthalpy driven. Analysis of the forces involved in maintaining DNA-DBD complexes shows that specificity of DBD binding is provided by enthalpic interactions, while the electrostatic component that results from counter-ion dispersal is entirely entropic and not sequence-specific. Although the DNA double helix is a rather rigid construction, binding of DBDs to its minor groove often results in considerable DNA bending without the expenditure of significant free energy. This suggests that the rigidity of the DNA duplex comes largely from the water fixed to AT pairs in the minor groove, the loss of which then enables sharp bending.

Translational Entropy and DNA Duplex Stability.

Investigation of folding/unfolding DNA duplexes of various size and composition by superprecise calorimetry has revised several long-held beliefs concerning the forces responsible for the formation of the double helix. It was established that: 1) the enthalpy and the entropy of duplex unfolding are temperature dependent, increasing with temperature rise and having the same heat capacity increment for CG and AT pairs; 2) the enthalpy of AT melting is greater than that of the CG pair, so the stabilizing effect of the CG pair in comparison with AT results not from its larger enthalpic contribution (as expected from its extra hydrogen bond), but from the larger entropic contribution of the AT pair that results from its ability to fix ordered water in the minor groove and release it upon duplex unfolding; 3) the translation entropy, resulting from the appearance of a new kinetic unit on duplex dissociation, determines the dependence of duplex stability on its length and its concentration (it is an order-of-magnitude smaller than predicted from the statistical mechanics of gases and is fully expressed by the stoichiometric correction term); 4) changes in duplex stability on reshuffling the sequence (the "nearest-neighbor effect") result from the immobilized water molecules fixed by AT pairs in the minor groove; and 5) the evaluated thermodynamic components permit a quantitative expression of DNA duplex stability.

Role of water in the formation of macromolecular structures.

This review shows that water in biological systems is not just a passive liquid solvent but also a partner in the formation of the structure of proteins, nucleic acids and their complexes, thereby contributing to the stability and flexibility required for their proper function. Reciprocally, biological macromolecules affect the state of the water contacting them, so that it is only partly in the normal liquid state, being somewhat ordered when bound to macromolecules. While the compaction of globular proteins results from the reluctance of their hydrophobic groups to interact with water, the collagen superhelix is maintained by water forming a hydroxyproline-controlled frame around this coiled-coil macromolecule. As for DNA, its stability and rigidity are linked to water fixed by AT pairs in the minor groove: this leads to the enthalpic contribution of AT pairs exceeding that of GC pairs, but this is overbalanced by their greater entropy contribution, with the result that AT pairs melt at lower temperatures than GCs. Loss of this water drives transcription factor binding to the minor groove.

The energetic basis of the DNA double helix: a combined microcalorimetric approach.

Microcalorimetric studies of DNA duplexes and their component single strands showed that association enthalpies of unfolded complementary strands into completely folded duplexes increase linearly with temperature and do not depend on salt concentration, i.e. duplex formation results in a constant heat capacity decrement, identical for CG and AT pairs. Although duplex thermostability increases with CG content, the enthalpic and entropic contributions of an AT pair to duplex formation exceed that of a CG pair when compared at the same temperature. The reduced contribution of AT pairs to duplex stabilization comes not from their lower enthalpy, as previously supposed, but from their larger entropy contribution. This larger enthalpy and particularly the greater entropy results from water fixed by the AT pair in the minor groove. As the increased entropy of an AT pair exceeds that of melting ice, the water molecule fixed by this pair must affect those of its neighbors. Water in the minor groove is, thus, orchestrated by the arrangement of AT groups, i.e. is context dependent. In contrast, water hydrating exposed nonpolar surfaces of bases is responsible for the heat capacity increment on dissociation and, therefore, for the temperature dependence of all thermodynamic characteristics of the double helix.

The linker of the interferon response factor 3 transcription factor is not unfolded.

Interferon response factor 3 (IRF-3) is a transcription factor that plays an essential role in controlling the synthesis of interferon-ß (IFN-ß) and is a protein consisting of two well-defined domains, the N-terminal DNA-binding and the C-terminal dimerization domains, connected by a 75-residue linker, supposedly unfolded. However, it was not clear whether in intact IRF-3 this linker segment of the chain, which carries the nuclear export signal and includes a region of high helical propensity, remains unfolded. This has been investigated using nuclear magnetic resonance by ligating the (15)N-labeled linker to the unlabeled N-terminal and C-terminal domains. It was found that, while the linker alone is indeed in a completely unfolded state, when ligated to the C-terminal domain it shows some ordering, and this ordering becomes much more pronounced when the linker is also ligated to the N-terminal domain. Thus, in intact IRF-3, the linker represents a folded structural domain; i.e., IRF-3 is a three-domain globular protein. Light scattering studies of wild-type IRF-3 showed that these three domains are tightly packed, and therefore, the dimer of IRF-3, which is formed upon phosphorylation of its C-terminal domains following virus invasion, must be a rather rigid and compact construction. One would then expect that binding of such a dimer to its tandem recognition sites PRDIII and PRDI, which are located on opposing faces of the IFN-ß enhancer DNA, should result in deformation of the DNA. Analysis of the characteristics of binding of the monomeric and dimeric IRF-3 to the enhancer DNA indeed showed that formation of this complex requires considerable work for deformation of its components, most likely bending of the DNA. Such bending was confirmed by atomic force microscopy of dimeric IRF-3 bound to the PRDII-PRDI tandem recognition sites placed at the middle of a 300 bp DNA probe. Bending of DNA by IRF-3 must be significant in the assembly and function of the IFN-ß enhancer.

Interpreting protein/DNA interactions: distinguishing specific from non-specific and electrostatic from non-electrostatic components.

We discuss the effectiveness of existing methods for understanding the forces driving the formation of specific protein-DNA complexes. Theoretical approaches using the Poisson-Boltzmann (PB) equation to analyse interactions between these highly charged macromolecules to form known structures are contrasted with an empirical approach that analyses the effects of salt on the stability of these complexes and assumes that release of counter-ions associated with the free DNA plays the dominant role in their formation. According to this counter-ion condensation (CC) concept, the salt-dependent part of the Gibbs energy of binding, which is defined as the electrostatic component, is fully entropic and its dependence on the salt concentration represents the number of ionic contacts present in the complex. It is shown that although this electrostatic component provides the majority of the Gibbs energy of complex formation and does not depend on the DNA sequence, the salt-independent part of the Gibbs energy--usually regarded as non-electrostatic--is sequence specific. The CC approach thus has considerable practical value for studying protein/DNA complexes, while practical applications of PB analysis have yet to demonstrate their merit.

The cost of DNA bending.

Experimental data on protein-DNA interactions highlight a surprising peculiarity of protein binding to the minor groove: in contrast to major groove binding, which proceeds with heat release and does not induce substantial deformation of DNA, minor groove binding takes place at AT-rich sites, proceeds with heat absorption and results in significant DNA bending. By forming a highly ordered and dense spine in the minor groove of AT-rich DNA, water plays an essential role in defining the energetic signature of protein-minor groove binding. Removal of this water requires minimal work and results in significant loss of rigidity in the DNA, which can then easily acquire the conformation imposed by the bound protein. Therefore the introduction of substantial bends into the DNA is not energetically expensive.

Microcalorimetry of proteins and their complexes.

Ultrasensitive microcalorimetric techniques for measuring the heat capacities of proteins in dilute solutions over a broad temperature range (DSC) and the heats of protein reactions at fixed temperatures (ITC) are described and the methods of working with these instruments are considered. Particular attention is paid to analyzing the thermal properties of individual proteins, their stability, the energetics of their folding, and their association with specific macromolecular partners. Use of these calorimetric methods is illustrated with examples of small compact globular proteins, small proteins having loose noncompact structure, multidomain proteins, and protein complexes, particularly with DNA.

Use of fluorescence resonance energy transfer (FRET) in studying protein-induced DNA bending.

The specific association of many DNA-binding proteins with DNA frequently results in significant deformation of the DNA. Protein-induced DNA bends depend on the protein, the DNA sequence, the environmental conditions, and in some cases are very substantial, implying that DNA bending has important functional significance. The precise determination of the DNA deformation caused by proteins under various conditions is therefore of importance for understanding the biological role of the association. This review considers methods for the investigation of protein-induced DNA bending by measuring the change in fluorescence resonance energy transfer (FRET) between fluorophores placed at the ends of the target DNA duplex. This FRET technique is particularly efficient when the protein-induced bend in the DNA is considerable and results in a significant decrease in the distance between the DNA ends bearing the fluorophores. However, in the case of small bends the change of distance between the ends of short DNA duplexes, as typically used in protein binding experiments (about 16-20 bp), is too small to be detected accurately by FRET. In such cases the change of the distance between the fluorophores can be increased by using levers attached to the binding site, that is, using two bulges to construct a U-shaped DNA in which the central part contains the protein-binding site and the fluorophores are attached to the ends of the perpendicularly directed arms.

Mechanisms of activation of interferon regulator factor 3: the role of C-terminal domain phosphorylation in IRF-3 dimerization and DNA binding.

The interferon regulatory transcription factor (IRF-3) is activated by phosphorylation of Ser/Thr residues clustered in its C-terminal domain. Phosphorylation of these residues, which increases the negative charge of IRF-3, results in its dimerization and association with DNA, despite the increase in repulsive electrostatic interactions. To investigate this surprising effect, the dimerization of IRF-3 and two phosphomimetic mutants, 2D (S396D, S398D) and 5D (S396D, S398D, S402D, T404D and S405D), and their binding to single-site PRDI and double-site PRDIII-PRDI DNA sequences from the IFN-beta enhancer have been studied. It was found that: (a) the mutations in the C-terminal domain do not affect the state of the DNA-binding N-terminal domain or its ability to bind target DNA; (b) in the 5D-mutant, the local increase of negative charge in the C-terminal domain induces restructuring, resulting in the formation of a stable dimer; (c) dimerization of IRF-3 is the basis of its strong binding to PRDIII-PRDI sites since binding of 5D to the single PRDI site is similar to that of inactivated IRF-3. Analysis of the binding characteristics leads to the conclusion that binding of dimeric IRF-3 to the DNA with two tandem-binding sites, which are twisted by approximately 100 degrees relative to each other, requires considerable work to untwist and/or bend the DNA.

DNA bending by charged peptides: electrophoretic and spectroscopic analyses.

We are testing the idea that placement of fixed charges near one face of the DNA double helix can induce DNA bending by a purely electrostatic mechanism. If stretching forces between DNA phosphates are significant, fixed charges should induce DNA bending by asymmetrically modulating these forces. We have previously tested this hypothesis by adding charged residues to small bZIP DNA binding peptides and monitoring DNA bending using electrophoretic phasing assays. Our results were consistent with an electrostatic model of DNA bending in predicted directions. We now confirm these observations with fluorescence resonance energy transfer (FRET). Using a "U"-shaped DNA probe, we report that DNA bending by charged bZIP peptides is readily detected by FRET. We further show that charged bZIP peptides cause DNA bending rather than DNA twisting.

Microcalorimetry of biological macromolecules.

The capabilities of contemporary differential scanning and isothermal titration microcalorimetry for studying the thermodynamics of protein unfolding/refolding and their association with partners, particularly target DNA duplexes, are considered. It is shown that the predenaturational changes of proteins must not be ignored in studying the thermodynamics of formation of their native structure and their complexes with partners, particularly their cognate DNA duplexes.

What drives proteins into the major or minor grooves of DNA?

The energetic profiles of a significant number of protein-DNA systems at 20 degrees C reveal that, despite comparable Gibbs free energies, association with the major groove is primarily an enthalpy-driven process, whereas binding to the minor groove is characterized by an unfavorable enthalpy that is compensated by favorable entropic contributions. These distinct energetic signatures for major versus minor groove binding are irrespective of the magnitude of DNA bending and/or the extent of binding-induced protein refolding. The primary determinants of their different energetic profiles appear to be the distinct hydration properties of the major and minor grooves; namely, that the water in the A+T-rich minor groove is in a highly ordered state and its removal results in a substantial positive contribution to the binding entropy. Since the entropic forces driving protein binding into the minor groove are a consequence of displacing water ordered by the regular arrangement of polar contacts, they cannot be regarded as hydrophobic.

The extended arms of DNA-binding domains: a tale of tails.

DNA-binding domains (DBDs) frequently have N- or C-terminal tails, rich in lysine and/or arginine and disordered in free solution, that bind the DNA separately from and in the opposite groove to the folded domain. Is their role simply to increase affinity for DNA or do they have a role in specificity, that is, sequence recognition? One approach to answering this question is to analyze the contribution of such tails to the overall energetics of binding. It turns out that, despite similarities of amino acid sequence, three distinct categories of DBD extension exist: (i) those that are purely electrostatic and lack specificity, (ii) those that are largely non-electrostatic with a high contribution to specificity and (iii) those of mixed character that show sequence preference. Because in all cases the tails also increase the affinity for target DNA, they represent a crucial component of the machinery for selective gene activation or repression.

Forces driving the binding of homeodomains to DNA.

Homeodomains are helix-turn-helix type DNA-binding domains that exhibit sequence-specific DNA binding by insertion of their "recognition" alpha helices into the major groove and a short N-terminal arm into the adjacent minor groove without inducing substantial distortion of the DNA. The stability and DNA binding of four representatives of this family, MATalpha2, engrailed, Antennapedia, and NK-2, and truncated forms of the last two lacking their N-terminal arms have been studied by a combination of optical and microcalorimetric methods at different temperatures and salt concentrations. It was found that the stability of the free homeodomains in solution is rather low and, surprisingly, is reduced by the presence of the N-terminal arm for the Antennapedia and NK-2 domains. Their stabilities depend significantly upon the presence of salt: strongly for NaCl but less so for NaF, demonstrating specific interactions with chloride ions. The enthalpies of association of the homeodomains with their cognate DNAs are negative, at 20 degrees C varying only between -12 and -26 kJ/mol for the intact homeodomains, and the entropies of association are positive; i.e., DNA binding is both enthalpy- and entropy-driven. Analysis of the salt dependence of the association constants showed that the electrostatic component of the Gibbs energy of association resulting from the entropy of mixing of released ions dominates the binding, being about twice the magnitude of the nonelectrostatic component that results from dehydration of the protein/DNA interface, van der Waals interactions, and hydrogen bonding. A comparison of the effects of NaCl/KCl with NaF showed that homeodomain binding results in a release not only of cations from the DNA phosphates but also of chloride ions specifically associated with the proteins. The binding of the basic N-terminal arms in the minor groove is entirely enthalpic with a negative heat capacity effect, i.e., is due to sequence-specific formation of hydrogen bonds and hydrophobic interactions rather than electrostatic contacts with the DNA phosphates.

Stability and DNA binding ability of the DNA binding domains of interferon regulatory factors 1 and 3.

The thermodynamic properties and DNA binding ability of the N-terminal DNA binding domains of interferon regulatory factors IRF-1 (DBD1) and IRF-3 (DBD3) were studied using microcalorimetric and optical methods. DBD3 is significantly more stable than DBD1: at 20 degrees C the Gibbs energy of unfolding of DBD3 is -28.6 kJ/mol, which is 2 times larger than that of DBD1, -14.9 kJ/mol. Fluorescence anisotropy titration experiments showed that at this temperature the association constants with the PRDI binding site are 1.1 x 10(6) M(-)(1) for DBD1 and 3.6 x 10(6) M(-)(1) for DBD3, corresponding to Gibbs energies of association of -34 and -37 kJ/mol, respectively. However, the larger binding energy of DBD3 is due to its larger electrostatic component, while its nonelectrostatic component is smaller than that of DBD1. Therefore, DBD1 appears to have more sequence specificity than DBD3. Binding of DBD1 to target DNA is characterized by a substantially larger negative enthalpy than binding of DBD3, implying that the more flexible structure of DBD1 forms tighter contacts with DNA than the more rigid structure of DBD3. Thus, the strength of the DBDs' specific association with DNA is inversely related to the stability of the free DBDs.

Kinetics and thermodynamics of the unfolding and refolding of the three-stranded alpha-helical coiled coil, Lpp-56.

Temperature-induced reversible unfolding and refolding of the three-stranded alpha-helical coiled coil, Lpp-56, were studied by kinetic and thermodynamic methods, using CD spectroscopy, dynamic light scattering, and scanning calorimetry. It was found that both unfolding and refolding reactions of this protein in neutral solution in the presence of 100 mM NaCl are characterized by unusually slow kinetics, which permits detailed investigation of the mechanism of these reactions. Kinetic analyses show that the unfolding of this coiled coil represents a single-stage first-order reaction, while the refolding represents a single-stage third-order reaction. The activation enthalpy and entropy for unfolding do not depend noticeably on temperature and are both significantly greater than those for the folding reaction, which show a significant dependence on temperature. The activation heat capacity change for the unfolding reaction is close to zero, while it is quite significant for the folding reaction. The correlation between the activation and structural parameters obtained for the Lpp-56 coiled coil suggests that interhelical van der Waals interactions are disrupted in the transition state, which is nevertheless still compact, and water has not yet penetrated into the interface; the transition from the transient state to the unfolded state results in hydration of exposed apolar groups of the interface and the disruption of helices. The low propensity for the Lpp-56 strands to fold and associate is caused by the high number of charged groups at neutral pH. On one hand, these charges give rise to considerable repulsive forces destabilizing the helical conformation of the strands. On the other hand, they align the folded helices in parallel and in register so that the apolar sides face each other, and the oppositely charged groups may form salt links, which are important for the formation of the trimeric coiled coil. A decrease in pH, which eliminates the salt links, dramatically decreases the stability of Lpp-56; its structure becomes less rigid and unfolds much faster.

Thermodynamic signature of GCN4-bZIP binding to DNA indicates the role of water in discriminating between the AP-1 and ATF/CREB sites.

The energetic basis of GCN4-bZIP complexes with the AP-1 and ATF/CREB sites was investigated by optical methods and scanning and isothermal titration microcalorimetry. The dissociation constant of the bZIP dimer was found to be significantly higher than that of its isolated leucine zipper domain: at 20 degrees C it is 1.45microM and increases with temperature. To avoid complications from dissociation of this dimer, DNA binding experiments were carried out using an SS crosslinked version of the bZIP. The thermodynamic characteristics of the bZIP/DNA association measured at different temperatures and salt concentrations were corrected for the contribution of refolding the basic segment upon binding, determined from the scanning calorimetric experiments. Fluorescence anisotropy titration experiments showed that the association constants of the bZIP at 20 degrees C with the AP-1 and ATF/CREB binding sites do not differ much, being 1.5nM and 6.4nM, corresponding to Gibbs energies of -49kJmol(-1) and -46kJmol(-1), respectively. Almost half of the Gibbs energy is attributable to the electrostatic component, resulting from the entropic effect of counterion release upon DNA association with the bZIP and is identical for both sites. In contrast to the Gibbs energies, the enthalpies of association of the fully folded bZIP with the AP-1 and ATF/CREB sites, and correspondingly the entropies of association, are very different. bZIP binding to the AP-1 site is characterized by a substantially larger negative enthalpy and non-electrostatic entropy than to the ATF/CREB site, implying that the AP-1 complex incorporates significantly more water molecules than the ATF/CREB complex.