 Research article
 Open Access
 Published:
Identification of DNAbinding protein target sequences by physical effective energy functions: free energy analysis of lambda repressorDNA complexes.
BMC Structural Biology volume 7, Article number: 61 (2007)
Abstract
Background
Specific binding of proteins to DNA is one of the most common ways gene expression is controlled. Although general rules for the DNAprotein recognition can be derived, the ambiguous and complex nature of this mechanism precludes a simple recognition code, therefore the prediction of DNA target sequences is not straightforward. DNAprotein interactions can be studied using computational methods which can complement the current experimental methods and offer some advantages. In the present work we use physical effective potentials to evaluate the DNAprotein binding affinities for the λ repressorDNA complex for which structural and thermodynamic experimental data are available.
Results
The binding free energy of two molecules can be expressed as the sum of an intermolecular energy (evaluated using a molecular mechanics forcefield), a solvation free energy term and an entropic term. Different solvation models are used including distance dependent dielectric constants, solvent accessible surface tension models and the Generalized Born model. The effect of conformational sampling by Molecular Dynamics simulations on the computed binding energy is assessed; results show that this effect is in general negative and the reproducibility of the experimental values decreases with the increase of simulation time considered. The free energy of binding for nonspecific complexes, estimated using the best energetic model, agrees with earlier theoretical suggestions. As a results of these analyses, we propose a protocol for the prediction of DNAbinding target sequences. The possibility of searching regulatory elements within the bacteriophage λ genome using this protocol is explored. Our analysis shows good prediction capabilities, even in absence of any thermodynamic data and information on the naturally recognized sequence.
Conclusion
This study supports the conclusion that physicsbased methods can offer a completely complementary methodology to sequencebased methods for the identification of DNAbinding protein target sequences.
Background
ProteinDNA recognition plays an essential role in the regulation of gene expression. Although a significant number of structures of DNA binding proteins have been solved in complex with their DNA binding sites increasing our understanding of recognition principles, most of the questions remain unanswered. Several studies showed that proteinDNA recognition could not be explained by a simple onetoone correspondence between amino acids and bases [1–3], even if hypothesized hydrogen bonding patterns and definite preferences have been actually found in experimentally solved structures [1]. Moreover regulatory proteins are known to recognize specific DNA sequences directly through atomic contacts between protein and DNA and/or indirectly through watermediated contacts and conformational changes [1, 4, 5]. The degree of redundancy and flexibility seems to suggest that the recognition mechanism is ambiguous, therefore the prediction of DNA target sequences is not straightforward [6].
DNA protein interactions can be studied using several different computational methods, which could offer several advantages compared to the current experimental methods, more laborious and slow. In the following we will indicate, for simplicity, DNAbinding protein target sequences with the more specific term "transcription factor binding sequences", although the first term is more general.
Computational tools for the identification of Transcription Factors (TF) binding sequences can be organized in two main approaches:

"sequence based methods" in which a central role is played by the statistical properties of the base distribution in the DNA regions which are expected to be involved in transcriptional regulation (see [7, 8] for a general review on the subject).

"structure based tools" which use the structural information on proteinDNA complexes derived from Xray crystallography and Nuclear Magnetic Resonance.
The main focus of this paper is on the second approach, although the best results will likely be obtained by tools able to combine in a clever way these two approaches.
Sequence based methods
This type of algorithms can in turn be divided into two broad groups:
ii) local search algorithms, including expectation maximization and various flavours of Gibbs sampling (see e.g. [17–20]).
It is important to stress that this type of studies cannot be based exclusively on the statistical features of the DNA regions presumably involved in transcriptional regulation, but must be complemented with independent information about gene regulation. In this respect three important sources of information may be used: the functional annotations collected in public databases, gene expression data on a global scale, and the so called 'phylogenetic footprinting'. In particular this last approach, thanks to the increasing number of sequenced genomes, has proved to be very effective in these last few years (see e.g. [21–30]). The major problem of all these tools is the large number of false positives, above all in the case of higher eukaryotes (for a thorough analysis of this problem see the interesting assessment of TF binding sites discovery tools reported in [31]). It is exactly to cope with this type of problem that it could be important to resort to structure based approaches.
Structure based methods
These methods can be broadly divided into two classes according to a nomenclature adopted in the context of protein structure prediction [32]:

i)
those based on knowledge based potentials (mostly statistical effective energy functions, SEEFs);
ii) those based on physical potentials (or physical effective energy functions, PEEFs).
SEEFs are energy functions derived from a dataset of known proteinDNA structures. A set of features is selected (e.g. nucleotideamino acid contacts, roll angles for DNA bases, interatomic distances, etc.); the process often involves parameter choices, like threshold on distances or interval binning. The statistical properties of these features are compared with apriori expectations and logodd scores are derived [6, 33–38]. At the most basic level, structures may be used to define contacts among DNA bases and protein amino acids and, for each pair of positions, the occurrences of nucleotides and amino acids contacts are used to derive effective potentials [36]. Moreover a statistical potential, taking into account contact geometry and spatial arrangement of contacting residues can be derived [6]. Recently interesting developments of this approach have been proposed ([38, 35, 5, 39]). The approach suffers from theoretical and practical problems. From the theoretical point of view potentials of mean force are not in general additive and the exact modelization of apriori expectations (or socalled reference state) may be difficult for complex systems (see e.g. [40]). The main practical problem is the requirement of a large number of sequences or binding experimental data since the available data may be biased towards specific classes of proteinDNA complexes. Moreover datasets generally do not contain unfavourable interactions between amino acids and bases since they entail proteinDNA complexes that occur naturally. Thus the statistical potential may predict correctly the wild type targets as opposed to incorrect ones, but it may not be as good at distinguishing among mutants.
Notwithstanding all caveats usage of SEEFs are widespread in the field of structural predictions. Provided that sufficient data are available these methods are reasonably fast and accurate, as demonstrated for instance in the field of protein structure prediction (see e.g [41]).
A more radical approach is to estimate the free energy of binding starting directly from the available (or homology built) proteinDNA complexes using physical effective energy functions (PEEFs). This approach has been successfully used in many contexts, ranging from estimation of DNA or proteinligand binding free energy to estimation of proteinDNA binding free energy (see e.g. [42, 43]). There are, however, many problems connected with the approach which are mainly due to:

i)
difficulties in estimating entropic effects;
ii) difficulties in properly estimating solvation effects;
No consensus has emerged on the choice of parameters (e.g. inner dielectric constant, surface tension coefficient, forcefield parameters) and on the protocols that should be applied;
iii) difficulties in estimating gasphase energy with available forcefields which are derived from the analysis of small compounds at equilibrium and do not take into account electrostatic polarization.
In order to get rid as far as possible of all these problems, binding free energies are expressed relative to a reference system and in most computational studies optimal parameters have been chosen for matching experimental data.
As far as proteinDNA complexes are concerned attempts to compute binding free energies using physics based approaches have started in the 1990s. The electrostatic component of the binding free energy has been studied according to continuum methods and its dependence on temperature and salt concentration has been computed [44–46]. Integration of electrostatics with other components including DNA conformational free energy has been extended from DNAligand complexes [47] and proteinpeptide complexes [48] to proteinDNA complexes [49]. Recently Wojciechowski et al. [50] studied the complex of telomerase end binding protein with single stranded DNA optimizing the weights of different contributions in order to reproduce binding data. The availability of the successful analytical generalized Born model treatment of electrostatics solvation effects enabled computation of binding energies with hybrid molecular mechanics/Generalized Born surface accessibility methods by Jayaram et al. [51]. The group of Kollman developed the molecular mechanics/Poisson Boltzmann surface accessibility (MM/PBSA) methodology and applied it extensively to biomolecular systems (see for a review of these applications [42, 43] and [42, 43, 43, 52] for important extensions of these ideas).
However, when MM/GBSA or MM/PBSA energy versus time plots are presented for explicit solvent molecular dynamics simulation snapshots, fluctuations in the range of tens to hundreds of kcal/mol are found, thus posing an issue on the reliability of averages. In this respect SEEFs appear much more robust energy estimation methods.
In a few very recent reports interesting results have been reported concerning the capability of hybrid methods to predict proteinDNA binding sites [53–57]. In this paper we focus on the application of PEEFs to a single DNA binding protein in complex with many different DNA sequences.
The availability of high resolution Xray crystal structure [58] and suitable experimental data makes the λ repressoroperator complex an interesting system for computational analysis of proteinDNA interaction. The bacteriophage λ repressor protein is a small, 92 amino acid, protein that binds the DNA as a dimer. Each monomer binds to an operator half site. The aminoterminal domain of λ repressor is responsible for DNA binding and the carboxyterminal domain is primarily responsible for dimerization [59]. Each monomer contains a typical helixturnhelix motif found in a variety of DNA binding proteins [4, 60]. The free energy of binding of λ repressor for wildtype O_{ R }1 operator DNA and of all possible single basepair substitutions within the operator have been experimentally measured using the filter binding assay technique and changes in the free energy of binding caused by the mutations have been determined [61]. Besides being a perfect playground to test our methods, the so called "λswitch" in which the λ repressor is involved is very interesting in itself (for a review see [62]). This "genetic" switch is tightly regulated by the λ repressor and the Cro proteins. In these last years this system, due to its relative simplicity and to the availability of rather precise experimental data attracted a lot of interest and various models (see for instance [63–65] and references therein) have been proposed to describe its behaviour. Despite these efforts in all these models there are still a few open problems which need to be understood. In particular it has been recently realized that in order to ensure the remarkable stability of the λ switch one should require a very high nonspecific affinity both for the λ repressor and for Cro [65, 66]. Such a prediction is very difficult to test experimentally but could rather directly be evaluated with the tools which we shall discuss in this paper. In fact one of the main goal of the test which we shall perform on the λ repressor will be the evaluation of its nonspecific binding energy and the comparison with the prediction of the model discussed in [66].
In the present work we apply different techniques to evaluate the binding affinities by means of computational methods. It is assumed that the relative free energy of binding of a protein to different DNA sequences may be expressed as the sum of a molecular mechanical term, that includes the nonbonded electrostatic and Van der Waals contributions, and a hydration term that can be further split in a polar and a hydrophobic contribution. Due to the peculiar nature of hydrogen bonds similar alternative models are tested where an energy term proportional to the number of hydrogen bonds is added.
The systems studied here differ only in one or two basepairs and therefore the inaccuracies implicit in the assumption of rigid docking, of the solvation model, of the treatment of entropy and in lack of a complete conformational search for side chains at proteinDNA interface should mostly cancel out in comparison. The aims of this paper are:

1)
to provide an assessment of the accuracy of different methods and protocols by comparison with experimental data;

2)
to provide a reliable estimate of nonspecific binding energies;

3)
to propose a protocol for the prediction of DNAbinding target sequences which makes no use of sequence information.
To pursue these objectives we make use of extensive computations and address several specific issues. In particular:

i)
we estimate optimal weights for different contributions to DNAprotein binding free energies using different solvation models;
ii) for 52 single basepair mutants we perform 1 ns molecular dynamics (MD) runs and we assess the effect of MD on the computed binding energies;
iii) we compute MM/GBSA binding energies for one thousand complexes where the bases of the double stranded DNA are substituted according to randomly generated DNA sequences in order to estimate nonspecific binding free energy;
iv) we scan the entire bacteriophage λ genome with the scoring profiles obtained from free energy computations. One of the profiles is obtained making use only of the structural data available for a single molecular complex, with no sequence information.
The statistical analysis of the results show that computational methods may offer a predictive tool truly complementary to sequencebased identification of DNAbinding protein target sequences. This is particularly important in view of the emergence of consensus protocols where the independence of the different methods is a prerequisite.
Results and discussion
Binding free energy changes between the λ repressor dimer and the DNA operator mutants have been calculated using different methodologies, as described in the Methods section.
MM/DDDCOONS
We calculated the binding free energy between the λ repressor dimer and the DNA operators, after having energyminimized every complex using a distance dependent dielectric constant (1r, 2r, 4r, 8r, respectively, in order to match subsequent energy evaluation). The interaction energy between the protein and the DNA, ΔU(${\overrightarrow{r}}_{1},\mathrm{...},{\overrightarrow{r}}_{n}$), has been evaluated using four values for ε (1r, 2r, 4r, 8r) then the solvation term ΔG_{ solv }has been determined according to the model of Oobatake et al. [54] using Eq. 2. The best scaling factors have been determined (together with the standard deviation computed according to Eq. 9) fitting the set of experimentally measured proteinDNA binding affinities and are reported in Table 1. The addition of a specific hydrogen bond term reduces the coefficients of the electrostatic term. The RMSD and the correlation coefficient r have been computed and a leaveoneout scheme has been adopted, in order to verify the performance of the model (Table 2). The same analysis has been performed for 5000 replicas of the dataset with one third of the set left out and used for crossvalidation. The average RMSD and correlation are essentially the same reported for the leaveoneout scheme reported in Table 2. From the same analysis variances of the coefficients have been estimated with essentially the same results as those reported in Table 1.
The best correlation coefficient (r = 0.703 for MM/DDDCOONS(+HB) model) has been obtained for ε = 4r, although values of ε = 2r and ε = 8r gave very similar results for both MM/DDDCOONS and MM/DDDCOONS(+HB) models. Except for the MM/DDDCOONS(+HB) model with ε = 1r, the Fstatistic shows that the model is significant (p < 0.001). The dielectric constant ε = 1r, which gives the worst results tends in many cases to overestimate binding free energy changes lower than 1.0 kcal/mol whereas binding free energy changes greater than 2 kcal/mol are underestimated. A similar behaviour has been observed for ε = 2r, 4r, 8r, even if these models are able to better reproduce binding free energy changes, in particular improvements have been obtained for values lower than 1.0 kcal/mol (Figure 1). The analysis of the best scaling coefficients is not straightforward because there is a strong correlation between the energy terms. For instance, for all ε models the electrostatic term is strongly anticorrelated with the OONS solvation term.
Moreover the estimated variance of coefficients is often very large. Notwithstanding these difficulties it is worth noting that some terms appear to be particularly important. For instance each proteinDNA hydrogen bond (when explicitly included in the model) appears to contribute 0.15 to 0.27 kcal/mol, depending on the electrostatic model assumed.
As expected the electrostatic term is reduced when hydrogen bonds are taken into account separately. For ε = 2r the best scaling coefficient x_{ DDDC }changes from 0.154 to 0.182 upon removal of the term proportional to the number of hydrogen bonds.
The correlation between the different contributions is reflected in the changes, with changing dielectric model, of the OONS term scaling factor, which is always strongly reduced by the scaling factor ranging from 0.075 to 0.066. Finally the constant term which takes into account common entropic terms (which can be estimated to be in the range 20 to 40 kcal/mol) and the free energy of binding of the reference complex (which implies the addition of 11.3 kcal/mol), expected to be in the range of 30 to 50 kcal/mol, is slightly larger than expected.
MM/DDDCHP
The OONS solvation term is accounting for both apolar and electrostatic solvation terms which should be already taken into account, at least partly, in the distance dependent dielectric constant. The same calculations described above have been performed using a similar approach in which the solvation term of the binding free energy is taken to be proportional to the polar/apolar accessible surface area of the molecule (see Eq. 6). The best scaling factors have been determined fitting the set of experimentally measured proteinDNA binding affinities (Table 1). The quality of the computed binding free energies ΔG_{ calc }has been assessed evaluating the linear correlation coefficient r and the root mean square deviation (RMSD) between calculated and experimental values. In order to verify the performance of the model, a leaveoneout scheme has been adopted (Table 2). The Fstatistic shows that the model is significant (p < 0.001).
All the values of the distance dependent dielectric constant which have been tested gave a quite high and similar linear correlation coefficient. The highest correlation value (r = 0.745) was obtained for ε = 2r for the MM/GBSA(+HB) model and the lowest ones for ε = 1r similar to the MM/DDDCOONS model. Generally, binding free energy changes lower than 1.0 kcal/mol are overestimated whereas binding free energy changes greater than 2 kcal/mol are underestimated in all the cases. More accurate predictions have been obtained for ε = 2r, in particular for values lower than 1.0 kcal/mol (Figure 2).
The optimal scaling coefficients are in the expected range (Table 1), in particular for ε = 2r, 4r, 8r the constant term x_{ const }is in the range 10–20 kcal/mol, moreover the coefficients x_{ H }and x_{ P }have the right order of magnitude of typically used surface tension coefficients for water biomolecular interface, even if the sign is incorrect. It should be noted however that there is a strong correlation (ranging in this case from 0.2 to 0.6) between the coefficients of most terms and the coefficient of the constant term.
Also for the present model the addition of an explicit hydrogen bond term reduces the coefficient of the electrostatic term as could be expected.
These results support the conclusion that, in general, there is no advantage in using the detailed solvation models compared to the simpler polar/apolar model, as far as the binding free energy is concerned. Based on the range of the scaling coefficients the two models appear of similar quality. Scaled free energy components for the MM/DDDCHP(+HB) model are reported in Table 3.
MM/GBSA
In this approach all structures have been energyminimized using the Generalized Born solvent model, then the binding free energy for every molecule has been calculated according to the MM/GBSA model using the Eq. 7. As in the previous cases, we determined the best scaling factors (and standard deviations according to Eq. 9) fitting the set of experimentally measured proteinDNA binding affinities (Table 4), then we assessed the quality of ΔG_{ calc }predictions evaluating the linear correlation coefficient r and the root mean square deviation (RMSD) between calculated and experimental values. Finally we verified the performance of the model, using the leaveoneout scheme (Table 2). The same analysis has been performed for 5000 replicas of the dataset with one third of the set left out and used for crossvalidation. The average RMSD and correlation are essentially the same reported for the leaveoneout scheme reported in Table 2. The standard deviations of the coefficients are essentially the same as reported in Table 4. Our calculation shows that the MM/GBSA(+HB) model gives the best performances (r = 0.746), although the linear correlation coefficient between calculated and experimental values differs slightly from the best values obtained from the other models. The Fstatistic shows that the model is significant (p < 0.001). Computed values versus experimental data are reported in Figure 3. As far as the scaling coefficients are concerned (see Table 4), it is worth noting that addition of an explicit hydrogen bond term has a dramatic effect on the coefficients of van der Waals and electrostatic terms, as could be expected, because the latter terms already take into account hydrogen bond energetics. For the MM/GBSA model (with no explicit term for hydrogen bonds) the coefficients of the electrostatic and GB solvation terms are 0.16 and 0.14 which correspond to a dielectric constant of ~6. Surface tension coefficients x_{ P }and x_{ H }(0.010 and 0.029 respectively) have the same order of magnitude of the commonly used surface tension coefficient (ca 0.02 kcal/mol Å^{2}), but opposite sign. However the terms proportional to the solvent accessible surface area are strongly correlated to each other and to the constant term.
The constant term is 11.7 kcal/mol, lower than what expected, probably as a consequence of the correlation of this term with the polar and hydrophobic surface area terms (the linear correlations of the coefficients are 0.51 and 0.75, respectively). The standard deviation of this term is however very large (28.0 kcal/mol).
Scaled free energy components for the MM/GBSA(+HB) model are reported in Table 5.
The analysis of Table 5 shows that the most important feature for computing the binding free energy is the number of intermolecular hydrogen bonds. The correlation of the associated energy term with the experimental free energy of binding is 0.58. Other terms are strongly correlated among each other and therefore it is difficult to single out specific contributions. The correlation between different energetic terms range from 0.99, for GB solvation energy and Coulombic energy, to 0.44, for GB solvation energy and polar area burial energy term.

18
single basepair mutants exhibit large (greater than 2.0 kcal/mol) unfavourable free energy of binding. Loss of hydrogen bonds contributes for 1 or 1.5 kcal/mol for mutants 14CG, 8AT, 8GC, 9AT, 18AT, 12TA, 12GC, while for other mutants the most important unfavourable contributions come mostly from Coulombic and van der Waals terms. It should be noted, however, that solvation terms are correlated with Coulombic and van der Waals terms.
This analysis is in general in line with the detailed analysis reported by Oobatake et al. [54], although the exact values of energy contributions differ.
Analysis of molecular dynamics trajectories
The procedure used for computing binding energies may suffer from incomplete relaxation and incomplete conformational sampling. An approach that has been used in the past for sampling more conformations and reduce the effect of fluctuations is to analyse snapshots from molecular dynamics runs. In many studies no scaling factor was applied at all, with good results.
We performed 1 ns of MD simulations for every structure in order to test the effectiveness of a first principles computation of binding free energies and to check the effect of molecular dynamics relaxation on the computed energies. We calculated the average value of every component of the binding free energy using snapshots taken every 50 ps, then we used the same set of fitting equations using average values to determine the best scaling factors. We chose to use the MM/GBSA(+HB) model for computing binding free energies because it gave good results on the starting structures and the coefficients can be used to monitor the quality of the fitting. Figure 3 The quality of the computed binding free energies ΔG_{ calc }has been assessed evaluating the linear correlation coefficient r and the root mean square deviation (RMSD) between calculated and experimental values (see Table 6). Results show that MD simulations do not improve the prediction capabilities of the model. Actually the linear correlation coefficient calculated averaging over 1.0 ns is 0.356, much lower than the correlation at t = 0.0 ns. Results obtained averaging over the time interval 0.0–0.5 ns, gave a linear correlation coefficient comparable to what obtained with other models on the starting structures (r = 0.534) but lower than the linear correlation coefficient obtained at t = 0.0 ns. The linear correlation coefficient between experimental values and the results obtained averaging over the time interval 0.5–1.0 ns, is r = 0.284, indicating that MD causes the loss of any correlation.
Moreover optimal scaling factors obtained averaging over the time interval 0.5–1.0 ns have the tendency to lose any physical meaning (Table 7). When optimal scaling factors obtained on the starting structure are used to compute binding free energies using average values, no correlation is detectable with experimental data. The value of the binding free energy change of every complex across 1 ns of simulation has been observed to strongly fluctuate, making it difficult to obtain an accurate estimate of it.
In order to verify whether this problem could have been circumvented using a larger conformational sampling, the simulations of 10 mutants have been extended to 4 ns, obtaining a total of 400 snapshots for every simulation. In particular we extended the simulations of the wild type complex and the best and the worst mutants (G17C25 and T14A28 respectively) with negative results. Although the system is most probably not fully equilibrated, it is reasonable to suspect that even longer (in the range of few tens ns) molecular dynamics simulations will not improve the results obtainable on the starting structures. The main reasons of failure of this approach are probably the large conformational fluctuations developing in MD simulations and the combination of relatively short molecular dynamics simulations with snapshots energy evaluation using the MM/GBSA(+HB) continuum model. Large conformational fluctuations observed in MD simulations are reflected in energetic fluctuations in the range of tens of kcal/mol, thus posing an issue on the reliability of the free energy average values. Moreover, since we observed that the results could not be improved extending the simulation time, it is reasonable to ascribe the failure of the method, at least partially, to inaccuracies in the force field parametrization. Actually, all force fields are based on numerous approximations, in particular nucleic acid force fields could suffer from two main problems which could give rise to inaccuracies. The first is that the target experimental data used in the optimization process are typically crystal structures of DNA and RNA. However, the presence of the lattice environment in crystals is known to influence the structure of DNA, limiting the transferability of crystal data to solution. The second is the treatment of electrostatics which is crucial in these simulations, given the polyanionic nature of DNA. In particular, the electrostatic polarization, which is an effect that can significantly reduce electrostatic interactions of partial atomic charges, is very important for accurate treatment of interactions in different environments, since significant structural changes of DNA may occur in response to environment.
Correct predictions
Table 8 shows the number of correct predictions, according to the criteria described in the Methods section. In the last column the number of cases in which the difference D = ΔG_{ exp } ΔG_{ calc } is lower than 0.3 kcal/mol, that is the number of the more accurate predictions, has been reported. It should be noted that the fitting of coefficients aims at minimizing the RMSD between calculated and experimental values and not at maximizing the number of "correct" predictions. When a simple simulated annealing procedure is applied to the coefficients the number of correct predictions can be increased by several units. It is instructive for instance to consider the MM/GBSA(+HB) model, where 41 "correct" predictions can be achieved with minor (mostly less than 10%) variations relative to the starting values of coefficients. From this qualitative point of view, the prediction capabilities of the different models can be compared. The best performing models appear to be the MM/DDDCHP model with ε = 2r. On average the DDDCHP model performs better than the similar DDDCOONS model. For ε = 1r results are worst than for higher ε values.
Molecular dynamics trajectories were analysed similarly, using average values for the different contributions to the free energy of binding. In particular the lowest number of correct predictions has been obtained averaging over the time interval 0.5–1.0 ns, actually there is no cases in which both ΔG_{ exp }and ΔG_{ calc }are <1.0 kcal/mol and the number of cases in which ΔG_{ exp }and ΔG_{ calc }are separated by less than 0.3 kcal/mol has been strongly reduced.
Generally, we observed that the number of cases in which ΔG_{ exp }and ΔG_{ calc }are both <1.0 kcal/mol decreases while the number of cases in which ΔG_{ exp }and ΔG_{ calc }are both > 1.0 kcal/mol remains nearly constant; however at the same time the number of cases in which ΔG_{ exp }and ΔG_{ calc }are separated by less than 0.3 kcal/mol strongly decreases, indicating that there is a reduction of the accuracy in reproducing experimental binding energies. Overall this analysis is consistent with the analyses reported in the previous sections.
Validation of the MM/GBSA model using the CroOR1 complex
The optimal scaling coefficients are likely to depend on the complex and mutants studied. In order to verify that such coefficients do not produce wild results when applied on different complexes with similar binding features we considered the Cro OR1 complexes which was obtained from crystallographic structure (PDB id. code: 6CRO) after mutation of 14 bases. The Cro protein belongs to the same family of λ repressor but to a different domain, according to SCOP classification [67] and it has very limited similarity with λ repressor although they bind DNA in a similar fashion. This system is therefore suited for testing the overall quality of the scaling procedure. Also for Cro a set of measurements for each mutant of the OR1 sequence is available [68]. When all contributions to the binding free energy, computed according to the MM/GBSA(+HB) model, are scaled by the coefficients determined on the λ repressor complexes the computed energies show a remarkable correlation coefficient of 0.62 with the experimental values, although the binding energies are overestimated by approximately 10 kcal/mol. This fact could reflect differences in the entropic contribution to binding (arising from restriction in side chain and backbone mobility) that are likely to be different for the two systems. Indeed, the crystallized Cro protein is roughly only two thirds of the repressor sequence. Notwithstanding the differences in overall binding energy, the binding differences for the mutants are on average reproduced by the energetic model.
As a further test, we performed the reverse analysis where the scaling coefficients are obtained on the CroOR1 complex and validated on the λ repressoroperator complex. Also in this case the computed energies show a remarkable correlation coefficient of 0.69 with the experimental values, although they are all underestimated by approximately 16 kcal/mol.
In order to verify how sensitive the scaling coefficients are to the experimental data used in the fit, we calculated the binding free energies of Cro and each mutant of the OR1 sequence according to the MM/GBSA model, using Eq. 7. Finally we combined the two experimental datasets of λ repressor and Cro and we refitted the model.
As in the previous cases, we calculated the best scaling factors fitting the set of experimentally measured proteinDNA binding affinities (Table 4), then we assessed the quality of ΔG_{ calc }predictions evaluating the linear correlation coefficient r and the root mean square deviation between calculated and experimental values. Finally we verified the performance of the model, using the leaveoneout scheme. The best performance has been obtained for the MM/GBSA(+HB) model, which gives a correlation coefficient r of 0.69 and a rmsd of 0.74 for Cro and a correlation coefficient r of 0.67 and a rmsd of 0.83 for the two combined systems. The same analysis has been performed for 5000 replicas of the dataset with one third of the set left out and used for crossvalidation. The average RMSD and correlation are essentially the same reported for the leaveoneout scheme. From the same analysis variances of the coefficients have been estimated with essentially the same results as those reported in Table 4. As far as the scaling coefficients are concerned (see Table 4), by comparing the results obtained for λ, Cro and the two combined systems, we can observe that the sets of values obtained for λ and λ + Cro are all in the same range except for the constant term, probably as a consequence of the fact that the entropic contribution to binding are likely different for the two systems. However it is worth noting that the standard deviation of this term is very large in both cases. As far as the scaling coefficients obtained for Cro, they are rather different from the others, except for x_{ vdw }and x_{ HB }, which scale the Van der Waals and Hbonds contributions respectively. However we observed that the electrostatic and GB solvation terms are strongly correlated to each other (the linear correlation coefficient is 0.998), as well as the constant term and the polar and hydrophobic surface area terms (the linear correlation of the coefficients is 0.645 and 0.784). The standard deviation of the constant term is also very large (see Table 4). Overall these results validate the approach for predicting binding free energies for similar proteinDNA complexes.
Analysis of nonspecific proteinDNA binding
In order to study nonspecific proteinDNA binding one thousand random DNA sequences have been generated and each sequence has been threaded onto the DNA phosphate backbone of the crystal structure in order to obtain a set of structural models with new DNA sequences. Minimization was performed according to the protocol described in the Methods section. We refer to to this set of complexes as to the "nonspecific" set.
Binding free energies for each member of the generated nonspecific set have been computed according to the MM/GBSA(+HB) model, using the optimal scaling factors determined by fitting the 52 experimental data (see Table 4).
We calculated the Zscores of both the random structures and the single basepair mutants, i.e. the distribution of the difference between the binding free energy of a complex and the average energy of the nonspecific set, normalized by the standard deviation of the computed energies. Zscores represent the specificity of a complex, with larger negative values corresponding to higher specificity. Figure 4 shows the distribution of computed energies. The distribution of the Zscores of the single basepair mutant complexes, is found at the negative tail of the nonspecific distribution, indicating that these complexes are more stable than the complexes formed with a DNA random sequence, as one expects. The computed energies have an average difference of 4.8 kcal/mol and a standard deviation of 2.2 kcal/mol, giving thus an average zscore for the single basepair mutants of 2.14 and 2.87 for the lowest computed energy in the set. The average nonspecific binding energy seems surprisingly low (meaning that it implies that a rather large fraction of λ repressors present in the cell is actually nonspecifically bound to DNA) but, remarkably enough, it agrees within the errors with the value proposed in [66] as a way to explain the impressive stability of the λswitch.
It is interesting to compare the computed free energies of binding for the nonspecific DNA complexes with those expected based on single mutants binding energies under the assumption of additivity. The expected free energies are higher than those computed by optimal scaling of contributions. The average difference, with respect to the specifically bound sequence, are 18.4 kcal/mol and 6.1 kcal/mol, respectively. This has been interpreted as a consequence of the fact that adjacent multiple substitutions may introduce additional energy minima compared to single mutations in a tight complex. This result is in line with the saturation effect in observed vs. predicted binding energy that has been described by Stormo and coworkers [69, 70] and recently experimentally demonstrated [71]. It is also interesting to note that the nonspecific binding energy is comparable to the energy computed by Northrup and coworkers for loosely docked complex of Cro to noncognate DNA [72], which implies that the mode of binding may substantially change for nonspecifically bound DNA sequences. This would be consistent with the capability of the protein of sliding along DNA, which would not be feasible for a tight complex.
Identification of putative transcription factor binding sites
The aim of this section is to understand whether the methods described here can be used for searching genomes for candidate transcription factor binding sites.
In particular we aim at verifying:

i)
whether the MM/GBSA(+HB) model is able to identify transcription factor binding sites in the absence of thermodynamic data about single basepair mutants, but just knowing the recognized sequence;
ii) whether some predictions can still be afforded in the absence of thermodynamic data and of any information on recognized sequences. The latter situation could be encountered when a model of the complex is built by homology and differences in protein DNAcontacting residues imply a different specificity.
Identification of putative transcription factor binding sites knowing the bound sequence
The analysis in the previous section used knowledge about single basepair mutants which is rarely available. Here we ask what predictions can be made when no thermodynamic data on mutants or wildtype sequence binding is available, but the cognate sequence is available. One thousand random DNA sequences were generated and the corresponding structural models were built by performing mutations on the double stranded DNA in the complex crystal structure using the program WHATIF [73]. Structures were energy minimized using the same protocol used for the MM/GBSA(+HB) methodology. Assuming that random sequences will have a larger free energy of binding compared to the bound sequence, optimal scaling parameters were sought in order to make the free energy difference in binding with respect to the naturally occurring complex equal to 10.0 kcal/mol. This value is arbitrary, albeit not unrealistic. Eq. 7 is solved (in a least square sense) subtracting the row corresponding to the wildtype complex from all other rows, and fixing all the energy differences equal 10.0. The differences in Coulombic, van der Waals, GB solvation energy, polar and apolar surface area and number of hydrogen bonds, with respect to wildtype complex, have been tabulated and the optimal scaling parameters have been determined.
The free energies computed on the random sequences have been used to compute single basepair mutant free energies as described in the Methods section. The single basepair mutant energies for the wild type sequence have been reset to 0.0 (this assumes that the specific bound sequence is known) and the lowest computed single basepair mutant binding energy has been subtracted from all other values.
The plot of computed single basepair mutant energies vs. experimental energies (computed under the hypothesis of additivity) shows a good correlation (0.58) but seems insufficient for predictive purposes. However, when the bacteriophage λ genome is scanned using the corresponding free energy matrix (see Methods), highaffinity binding sites are correctly recognized, and in general the energies computed using the matrix and those predicted based on addition of single basepair mutation effects are well correlated (corr. coeff. 0.74).
We asked what is the advantage of such computation compared to the simpler model that assigns a constant energy penalty to each mutation over the specific bound sequence. In such case the correlation between the computed and reference binding energies is slightly lower, but still significant (0.72). The advantage of using computational results over a much simpler single parameter approach seems therefore very limited, although the 1% best sites predicted by the MM/GBSA(+HB) energy and the simple mutation models display only 15% common sites, proving that the two methods are largely uncorrelated.
Identification of putative transcription factor binding sites without knowing the bound sequence
As a last test we simulate a realistic situation in which no thermodynamic data or information on the recognized sequences are available. We considered the set of one thousand random DNA sequences and the corresponding structural models built by performing mutations on the double stranded DNA in the complex crystal structure as the only information available. Obviously the crystallographic complex does contain information on the specific sequence because protein and DNA conformations are fitting each other in the complex. If nonspecific complexes were to be built by homology without knowing the exact DNA sequence bound, it is likely that side chains would be placed differently with different results. Finally, structures were energy minimized using the same protocol used for the MM/GBSA(+HB) methodology. As in the tests above we found optimal scaling factors in order to make all (nonspecific) binding free energies equal to 10.0 kcal/mol.
In order to avoid a trivial solution to the fitting problem with all coefficients equal 0.0 except the constant term equal 10.0, we follow a twostep procedure. In the first step we assume a reasonable value (30 kcal/mol) for the constant term which must be brought to the lefthand side of Eq. 7. Coulombic, van der Waals, GB solvation energy, polar and apolar surface area and number of hydrogen bonds have been evaluated, Eq. 7 is then solved (in a least square error sense) and the optimal scaling parameters have been determined. The lowest binding energy sequence according to the scaling parameters is determined. The row corresponding to this complex is subtracted from all other rows thus removing the constant term. In the second step the newly obtained matrix, which does not include the constant term anymore is used to find the best coefficients to make all the energy differences equal 10.0 kcal/mol. Therefore all energies are expressed relative to the lowest computed energy at the first step.
The free energies computed on the random sequences have been used to compute single basepair mutant free energies as described in the Methods section. At variance with the test performed above we do not set to 0.0 the energies of specific bound sequence (which is assumed here to be unknown). The correlation coefficient between computed and experimental energies (computed under the assumption of additivity) for the bacteriophage λ genome is 0.50 (Figure 5).
As a further test of the performance of the approach we generated the logo [74] of the 10 best binding sequences according to the thermodynamic data on single basepair mutants and those found with the present approach (Figure 6). An overall agreement between the two logos is apparent.
Conclusion
In the present work physical effective energy functions are used to estimate the free energy of binding of λ repressor to the DNA operator and single basepair mutants, for which thermodynamic data are available. Thermodynamic data allow one to study the best results achievable, with the modeling approach and energy functions presented here, with models that assume that the binding energy is a linear combination of different contributions.
Simple models that use a distance dependent dielectric constant and simple terms for surface area proportional energy contributions and for hydrogen bonding perform surprisingly well for values of ε ranging from 2r to 8r.
A twoparameter model for surface area proportional energy contributions performs better than the more complex model of Oobatake et al. [55], which was however not derived for usage in the more complex energy functions employed here.
The performance of MM/GBSA(+HB) and to a lesser extent MM/GBSA model is comparable to or superior to other models. A conclusion for the MM/GBSA model is that electrostatic energies should be reduced by a proper scaling factor corresponding to dielectric constants in the range of 6. This conclusion is reached also by a similar analysis of protein Crooperator mutants.
The effect of molecular dynamics on the computed binding free energies is in general negative and the reproducibility of the experimental values decreases with the increase of simulation time considered. This may be a consequence of the large fluctuations developing in MD simulations which probably would require a much longer simulation time. Moreover it is reasonable to take into account that the poor performance of the method can be partially caused by the errors in the force field used in MD simulations. Another plausible source of inaccuracy is the mismatch between the energy model and system representation used in MD simulation and those used for minimization and energy evaluation. It appears therefore that it is worth to invest more time in optimizing the starting structure, rather than for sampling the conformational space by molecular dynamics simulations, or, alternatively, to adopt different strategies for sampling protein and DNA flexibility [75].
The analysis of nonspecific complexes using the best performing energetic model with properly scaled coefficients allows to evaluate a nonspecific binding energy difference, with respect to the specific bound sequence, of 6.06 ± 2.17 kcal/mol, definitely lower than what expected based on an additive model (18.1 kcal/mol for the single basepair mutants computed energies). This result is in line with the saturation effect described by Stormo and coworkers [69, 70] and with the theoretical analysis of Bakk and Melzer [66].
Although the results presented on single basepair mutants are not exciting, using computational methods may be very useful for identifying transcription factor binding sites.
When no thermodynamic data are available but the specific bound sequence is known the computed MM/GBSA(+HB) free energies are slightly more predictive than a simple substitution profile which assigns a penalty for any point mutation.
The most interesting test performed here considers a realistic scenario where no information on the bound sequence is available. Even in this case MM/GBSA(+HB) energies are predictive.
This result has important consequences for the prediction of transcription factor binding sites which often use consensus methods. A prerequisite for the usefulness of consensus methods is that these are as independent of each other as possible. Since most methods use common prior knowledge and often related statistical methods, independence is not guaranteed. Methods which are based on completely independent principles, like those based on physical effective energy functions and free energy computations, offer a completely complementary methodology for deriving profile matrices for scanning entire genomes. The results reported here, with much caution because the structural model for the specific bound sequence is known and not modeled by homology or other methods, support usage of these methods for the identification of DNAbinding protein target sequences. In view of the very recent impressive results reported by the group of Baker [76] it is apparent that significant improvements to the approach described in this paper may be obtained by extensive refinement and screening of protein side chain conformation at proteinDNA interface.
Methods
Model building
Atomic coordinates of the λ repressor dimer bound to O_{ L }1 DNA operator were taken from the 1.8 Å resolution Xray crystal structure deposited in the Protein Data Bank [77] (PDB code 1LMB). The operator is 17 basepairs in length and is composed by two approximately symmetric parts, the "consensus half" (maintaining the notation of the PDB file, basepairs A19T23 to G11C31) and the "nonconsensus half" (basepairs T3A39 to G10C32) (see Figure 7). Since the coordinates of the NH_{2}terminal arm of the repressor bound to the nonconsensus half operator were not available, the lacking amminoacids were added using the protein bound to the consensus half operator. Using the program ProFit V2.2 [78], the C_{ α }carbons of the proteins have been superimposed and afterward the amino acids of the rotated structure have been added to the other one. Since the detailed Xray crystal structure is made up of λ repressor dimer and O_{ L }1 operator DNA while the experimental data concern the O_{ R }1 site, the WHATIF [73] program was used to substitute the basepair at position 5 to obtain the wildtype O_{ R }1 operator. All possible single basepair substitutions within the DNA sequence were generated using the program WHATIF [73].
Molecular Dynamics Simulations
Hydrogen atoms have been added using the program pdb2gmx of the GROMACS package [79, 80]. Every structure has been optimized performing 200 steps of energy minimization using the NAMD program, fixing all C_{ α }carbons and phosphate groups coordinates. A dielectric constant of 10 has been employed with a cutoff of 12 Å for nonbonded interactions.
The net charge of the system (36) has been neutralized placing a corresponding number of sodium counterions in energetically favourable positions. The electrostatic potential was calculated via numerical solutions of the PoissonBoltzmann equation using the University of Houston Brownian Dynamics (UHBD, version 6.x) program [81, 82]. A counterion was placed at the lowest potential position at 7.0 Å from any heavy atom of the solute. The cycle was repeated until the net charge of the system was 0.
The complex and counterions were solvated in a box of TIP3P [83] water molecules using the solvate module in the program VMD [84]. The resulting system contained about 4200 solute atoms and 50400 solvent atoms. The coordinates of the solute were fixed and the solvent was energy minimized using 100 steps of conjugate gradient. A solvent equilibration was carried out by performing molecular dynamics for 50 ps using a 1 fs time step to let the water molecules move to adjust to the conformation of the solute. The system was then energy minimized using 100 steps of conjugate gradient and, after 100 ps equilibration, 1ns MD simulations was performed using a 2fs timestep. A snapshot of the trajectory was stored every 10 ps for later analysis. The shakeH algorithm was used in order to fix bond length between each hydrogen and its mother atom to its nominal value and to extend the simulation timestep [85]. All molecular dynamics simulations of the complex were run under constant NPT conditions using the NAMD program [86]. The pressure of the system was coupled, through a Berendsenthermostat [87], to a pressure bath with target pressure 1.01325 bar and time constant 100 fs. The temperature has been kept to 300 K by simple velocity rescaling every picosecond. Longrange electrostatic interactions were treated by particle mesh Ewald (PME) method [88] employing a grid of 128 × 128 × 128 points. The cutoff was 12 Å and the tolerance was 10^{6} which resulted in an Ewald coefficient of 0.257952. The order for PME interpolation was 4.
The simulations were performed on a cluster composed by ten dualprocessor nodes based on Intel XeonTM 2.8 GHz, with hyperthreading technology.
Free energy calculations
The free energy of binding for each structure has been computed according to the framework reviewed by Gilson et al. [89] who derived the expression of the free energy of binding in terms of the microscopic properties of the two molecules involved, using standard statistical thermodynamics. Here, similar to other works employing continuum methods several simplifications are adopted. The free energy of binding for each complex minus the entropic contribution is expressed as the sum of the interaction energy between the protein and the DNA ΔU(${\overrightarrow{r}}_{1},\mathrm{...},{\overrightarrow{r}}_{n}$) and a solvation free energy term ΔG_{ solv }:
It has been assumed that the entropy restriction in internal degrees of freedom and overall rotation and translation degrees of freedom is the same for all complexes.
The effect that association has on intramolecular energy has been neglected. Moreover no extended conformational search has been performed for protein side chains and DNA, partly because this task is not easily accomplished and partly because large conformational changes often result in large molecular mechanics energy changes, so we aimed at keeping the systems to be compared as close as possible. The free energy of binding has been calculated using different methodologies detailed below. For all models alternative versions in which an energy term proportional to the number of hydrogen bonds has been added have been considered.
Except where noted, all contributions to the free energy of binding have been optimally scaled in order to best reproduce available experimental data (see later).
MM/DDDCOONS
In this method [54] electrostatic interactions have been estimated using a distance dependent dielectric constant (DDDC) while the solvation energy is proportional to the solvent accessible surface area through the atomic solvation parameters of Oobatake, Ooi, Nemethy and Scheraga (OONS) [55].
All structures have been energy minimized with 200 conjugate gradient steps, using a distancedependent dielectric constant (four values have been tested: 1r, 2r, 4r, 8r, with the distance r expressed in Å) and a cutoff of 12 Å. The molecular mechanics interaction energy U(${\overrightarrow{r}}_{1},\mathrm{...},{\overrightarrow{r}}_{n}$) was evaluated using CHARMM (version 27b2), a classic and welltested molecular mechanics forcefield [90, 91]. This term includes the nonbonded electrostatic and Van der Waals contributions. The solvation free energy term G_{ solv }has been calculated according to the model developed by Oobatake et al. [54]. This model consists in assigning every atom to one of 9 classes of chemical groups and assuming that the hydration free energy of every group i in a solute is proportional to its solvent accessible surface area (SASA) A_{ i }because the group can directly interact only with water molecules at the surface.
The proportionality constants ${g}_{i}^{hyd}$ have been determined from thermodynamic data on the transfer of small molecules from the gas phase into aqueous environment assuming the additivity of contributions from individual groups [55].
MM/DDDCHP
In a very similar approach the OONS 9parameter solvation model has been replaced by a simpler 2parameter hydrophobic, polar (HP) solvation model. Energy minimization protocol and tested values are the same as for the MM/DDDCOONS for proper comparison.
MM/GBSA
In this method the solvation free energy term is split in a polar (electrostatic) and a nonpolar (hydrophobic) term.
The polar term is computed using the Generalized Born approach [92]. All complexes have been energy minimized by 200 conjugate gradients minimization steps using the generalized Born model as implemented in the CHARMM program, then the solute and solvation energy terms have been computed for both the complex and the isolated molecules. The binding energy was then computed by subtraction. Doubling the number of minimization steps does not affect significantly the results.
The nonpolar term G^{nonpolar}, which takes into account the tendency of the nonpolar parts of the molecule to collapse, is taken to be proportional to the solventaccessible surface area A, i.e. G^{nonpolar}= γA, where the surface tension coefficient γ has been empirically determined to be equal to 20 cal Å ^{2} mol^{1} for this kind of applications [93].
A variant of this methodology including splitting the solvent accessible surface area into a polar and a hydrophobic contribution (i.e. using two different surface tension coefficients), and including a term proportional to the number of hydrogen bonds has been considered here.
Finding optimal scaling factors
The choice of methods and parameters in molecular mechanics/implicit solvent methods is subject to large uncertainties. In order to explore the best performance achievable with these methodologies, optimal scaling factors for the different contributions were searched that could best reproduce the experimental data. This approach is not new and it has been used successfully by other groups (see e. g. [57]). In practice it is expected that proper scaling is able to compensate for the many inaccuracies of the model. In general terms, the free energy of binding has been computed as a linear combination of contributions E_{ i }, with corresponding coefficients x_{ i }, i.e.:
where Δ represents the difference between the complex and the isolated protein and DNA molecules. Coefficients x_{1},...,x_{ n }have been found in order to best reproduce the 52 experimentally available free energies of binding. Contributions have been arranged in a 52 × n matrix A where each row corresponds to each structural model and each column corresponds to a different contribution to the free energy of binding. The experimental binding free energies have been arranged in a 52component vector ΔG_{ exptl }. The linear systemAx = ΔG_{ exptl }
where x is the ncomponent vector of coefficients, has been solved (in a least square sense) using singular value decomposition [94] and the best x_{ i }coefficients have been used to calculate binding energies ΔG_{ calc }. A constant term takes into account the entropy loss upon complexation and other possible contributions identical for all complexes.
A linear model, compared to more sophisticated methods, has the advantage that the number of adjustable parameters is limited and easily interpretable in physical terms.
In the following we detail the contributions considered for each energetic model.
The free energy of binding has been computed for the MM/DDDCOONS model according to the following equation:ΔG_{MM/DDDCOONS}= x_{ vdW }ΔE_{ vdW }+ x_{ DDDC }ΔE_{elec,DDDC}+ x_{ OONS }ΔG_{ OONS }+ x_{const.}(+x_{ HB }N_{ HB })
where ΔE_{ vdW }is the van der Waal contribution, ΔE_{elec,DDDC}is the Coulombic energy, computed with a distance dependent dielectric constant, ΔE_{ OONS }is the solvation energy according to the Oobatake et al. model [55] and N_{ HB }is the number of intermolecular hydrogen bonds.
As mentioned above, the coefficients bear physical meaning. For instance the term x_{ const }should account for rotational and translational entropy loss upon binding and it can be expected to be in the range 20–40 kcal/mol.
The term proportional to the number of hydrogen bonds was alternatively added in order to take into account possible inaccuracies in the treatment of these interactions by molecular mechanics and solvation terms. In practice every time this term is added the coefficients of molecular mechanics and solvation terms are greatly reduced thus avoiding double counting of hydrogen bond interactions.
A similar expression for the free energy of binding has been used for the MM/DDDCHP model:ΔG_{MM/DDDCHP}= x_{ vdW }ΔE_{ vdW }+ x_{ DDDC }ΔE_{elec,DDDC}+ x_{ H }ΔA_{ H }+ x_{ P }ΔA_{ P }+ x_{const.}(+x_{ HB }N_{ HB })
Here the coefficients x_{ H }and x_{ P }represent the surface tension coefficients multiplying hydrophobic and polar solvent accessible surface areas ΔA_{ H }and ΔA_{ P }, respectively. We expect these coefficients to be in the range of tens of cal Å^{2} mol^{1}.
The solvent accessible area has been also splitted in polar and hydrophobic area for finding optimal scaling parameters for the MM/GBSA methodology:ΔG_{MM/GBSA}= x_{ vdW }ΔE_{ vdW }+ x_{ Coul }ΔE_{ Coul }+ x_{ GB }ΔG_{ GB }+ x_{ H }ΔA_{ H }+ x_{ P }ΔA_{ P }+ x_{const.}(+x_{ HB }N_{ HB })
where ΔG_{ GB }is the generalized Born solvation energy. The coefficients x_{ Coul }and x_{ GB }are exactly and roughly, respectively, inversely proportional to the effective dielectric constant and are thus expected to be in the range 0.05 to 1.0.
Possible pitfalls of the method
Scaling energy terms for free energy evaluation of models which have been minimized without scaling such terms is clearly inconsistent. A correct procedure would be to iteratively find the optimal scaling factors, minimizing the energy using such scaling factors and repeating these two steps until convergence. This procedure faces some difficulties because an important term like the hydrogen bond term is discrete and does not have a counterpart in standard forcefields, where such interactions are described typically through electrostatic and van der Waals terms. Similarly the minimization of terms proportional to the solvent accessible surface area requires algorithms which are rarely available in molecular mechanics packages. A further difficulty is that any unbalance among forcefield terms might introduce distortions in molecular structure, notably of hydrogen bond lengths. Although the issue of iteratively fitting optimal scaling factors is worth being further investigated, here the approach of scaling factors has been applied in a more rough way. We have matched as far as possible the energetic model used for minimization with that used for fitting scaling factors, as mentioned above, but we have not minimized again the models using the scaling factors. A similar mismatch between conformational sampling and energy evaluation is implicit in the analysis of molecular dynamics snapshots. Other sources of error in this case are the large conformational (and energetic) fluctuations molecules undergo during simulation and in general the inaccuracy of implicit solvent methods (used in energy evaluation) where small energy differences arise from subtraction of rather large values. It should be noted that for molecular dynamics snapshots inaccuracies do not cancel out because there are no restrained parts in the molecules.
DNA sequence dependent deformability
An important aspect of proteinDNA interaction, addressed quantitatively by Olson and coworkers [39], is the capability of DNA sequences to adopt specific local conformations. The statistics of parameters and pairwise parameter correlations shows definite preferences. In the approach described above, changes in intramolecular energy terms are disregarded altogether by the assumption of rigid docking. The strains introduced in complex molecular structures, however, are typically relaxed over the structure and should have consequences on the intermolecular energy terms too. In order to assess the effect of DNA sequence dependent deformability we followed the approach of Olson and coworkers [39], who made available average parameters for the six parameters describing local geometry of a basepair step in BDNA, the force constant parameters for all pairwise deviation from equilibrium values and a program to analyse DNA structures [95].
The analysis was performed for the native structure parameters, simply replacing the identity of the basepair mutated, and on the mutated structures, minimized using the generalized Born model. For both cases poor correlation with experimental binding data was found. Remarkably, however, the native sequence was the third lowest energy sequence among all 52 sequences. Energy minimization in general increases the energy associated with the deformability of DNA. Computation of the fitness of a sequence to local geometry parameters gives important informations although it is likely that the computed energy is not accurate for conformations far from equilibrium. Inclusion of the DNA sequence dependent deformability energy in the analyses detailed below did not improve results significantly, notwithstanding the additional scaling parameter introduced for this purpose. For this reason this term was not considered further.
Performance analysis
After fitting scaling factors to experimental data, the root mean square difference between calculated and experimental data was computed. This quantity can provide however a poor evaluation of the predictive power of the calculations when the test systems are very similar. Therefore the correlation coefficient between calculated and experimental data was also computed. Optimal scaling factors were computed taking all the data available.
Fitting 52 experimental data with up to 7 parameters will always results in a positive correlation coefficient. In order to make sure that the results obtained are significant we performed different kind of analyses:

i)
a leaveoneout scheme has been adopted. All but one of the data were taken and the root mean square difference and correlation coefficient were computed using the set of data not used in the fitting procedure. The same scheme has been applied to 5000 replicates with one third of the data left out of the fitting procedure and used for RMSD and correlation coefficient computation.
ii) the variance of each linear coefficient has been estimated from the multiple regression analysis using the variance/covariance matrix and the square error of computed data, according to standard linear regression procedures [96]. In practice the standard deviation of experimental data has been estimated as
Then the variance of each coefficient has been estimated from the variance/covariance matrix of coefficients:
The different models considered employ a different number of fitting parameters and therefore different performances are expected. Although these parameters are often correlated, the analysis of the variance gives an immediate clue as to which variables are more important.
iii) analysis of variance (ANOVA) calculations have been performed and a significance test based on the Fstatistic and the corresponding confidence level has been computed [96].
iv) one thousand replicates of the original data has been generated with the column elements containing the experimental data randomly swapped. The average of the correlation coefficient between swapped experimental data and fitted data has been computed together with the standard deviation. The results of this computation (not reported) fully supports the results of the statistical analyses described above; Finally, a useful alternative to assess the quality of ΔG_{ calc }predictions and to compare the different models from a qualitative point of view, consists in determining the number of "correct predictions", defined as the number of cases in which both ΔG_{ exp }and ΔG_{ calc }are <1.0 kcal/mol, or >1.0 kcal/mol, or else separated by less than 0.3 kcal/mol. The threshold value of 1.0 kcal/mol requires some explanations. The experimental values of the free energy change relative to the wildtype operator O_{ R }1 have been calculated using the equation ΔG_{ exp }= 0.546 ln (K_{ d }of substituted sequence)/(K_{ d }of O_{ R }1) after having determined the dissociation constant of every mutant. It is simple to verify that the threshold value of 1.0 kcal/mol corresponds to a remarkable reduction in the dissociation constant of the mutant (ca. 5fold), with respect to the dissociation constant of the wildtype operator (K_{ d }of O_{ R }1 = 10^{9}), whereas values of ΔG higher than 1.0 kcal/mol correspond to a reduction in the dissociation constant from 5 (ΔG_{ exp }= 1.0 kcal/mol) to 25fold (ΔG_{ exp }= 3.4, which is the maximum value of ΔG_{ exp }). Therefore it is reasonable to define ΔG_{ calc }as correct, if both ΔG_{ exp }and ΔG_{ calc }are in one of the defined intervals or even if the difference D = ΔG_{ exp } ΔG_{ calc } is lower than 0.3 kcal/mol, which corresponds to a ratio between the dissociation constant of a mutant and the dissociation constant of the wildtype complex lower than 2.0.
Analysis of nonspecific proteinDNA binding
One thousand random DNA sequences were generated and the corresponding structural models were generated by performing mutations on the double stranded DNA in the complex crystal structure using the program WHATIF [73]. The resulting dataset of complexes was assumed to be representative of nonspecific proteinDNA complexes. We are interested in understanding how reliable is the method for predicting putative binding sites. The socalled Zscore of the specific bound sequence compared to random sequences has been considered. The Zscore is defined here as the distance of the free energy computed for the specific bound 17mer (ΔG) from the average nonspecific binding energy (< ΔG >), normalized by the standard deviation of the computed nonspecific binding energies (σ_{ G }).
Averages are performed over the one thousand random sequences. A large Zscore implies that the specific bound sequence can be distinguished from other nonspecific bound sequences. The structures were energy minimized using the same protocol used for MM/GBSA free energy estimation. For all minimized complexes the Coulombic energy, van der Waals energy, GB solvation energy, polar and apolar surface accessible area and intermolecular hydrogen bonds number were tabulated. For each model i of the 1000 random DNA sequence complexes the binding energy G(i) has been computed using different amounts of the experimental information available. Different analyses, detailed in the Results section, were performed. The possibility of using the data computed on the set of nonspecific complexes for defining a profile of the recognized DNA sequences has been explored as follows. The calculated binding energy values for the set of nonspecific complexes were summarised in a set of 68 values corresponding to the average contribution to the binding free energy of each possible of the 4 bases at each of the possible 17 bound sequence positions. These 68 values have been derived as follows. Possible substitutions are indexed from 1 to 4 for A, C, G and T, respectively. A 1000 × 68 matrix A was set where each element A(i, j) is 1.0 or 0.0 if the base at position j/4 (rounded at the closer upper integer) has index j mod 4 in sequence i. The set of 68 substitution free energies x(j) were found by solving (in a root mean square error sense) the overdetermined equation Ax = G. The resulting 68element vector x was arranged in a 17 × 4 matrix. Variants on this procedure are described in the Results section according to the level of information available included in the analysis.
Scanning of bacteriophage λ genome
The free energy matrix derived from the analysis of nonspecific proteinDNA complexes was used to score all 17mer subsequences in the bacteriophage λ genome (Accession number: NC_001416.1, 48502 basepairs) on both strands. In principle the score represents the free energy of binding of the 17mer considered.
Reference "experimental" binding free energy values, for comparison with computed data, were obtained under the hypothesis of additivity [69, 70] using experimental data on single basepair mutants.
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Acknowledgements
We wish to thank Drs. G. Tecchiolli and P. Zuccato of Exadron, the HPC Division of the Eurotech Group, for providing hardware and expert technical assistance.
Dr. M. Isola of the University of Udine is gratefully acknowledged for helpful discussions on statistical aspects of multiple regressions.
EM wishes to thank Profs. C. Destri, G. Marchesini and F. Rapuano for helpful discussions.
Part of the research was funded by FIRB grant RBNE03B8KK from the Italian Ministry for Education, University and Research.
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EM designed and performed most tests and analyses, and wrote part of the code used for the analyses. MC and FF conceived the project, supervised the work and designed some of the analyses. FF wrote part of the code used for the analyses. All authors have read and approved the final version of the manuscript.
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Keywords
 Free Energy
 Root Mean Square Deviation
 Binding Free Energy
 Solvent Accessible Surface Area
 Surface Tension Coefficient