Salt effects on protein-DNA interactions. The lambda cI repressor and EcoRI endonuclease

In this paper, finite-difference solutions to the nonlinear Poisson-Boltzmann (NLPB) equation are used to calculate the salt dependent contribution to the electrostatic DNA binding free energy for both the lambda cI repressor and the EcoRI endonuclease. For the protein-DNA systems studied, the NLPB method describes nonspecific univalent salt dependent effects on the binding free energy which are in excellent agreement with experimental results. In these systems, the contribution of the ion atmosphere to the binding free energy substantially destabilizes the protein-DNA complexes. The magnitude of this effect involves a macromolecular structure dependent redistribution of both cations and anions around the protein and the DNA which is dominated by long range electrostatic interactions. We find that the free energy associated with global ion redistribution upon binding is more important than changes associated with local protein-DNA interactions (ion-pairs) in determining salt effects. The NLPB model reveals how long range salt effects can play a significant role in the relative stability of protein-DNA complexes with different structures.     

Electrostatic contributions to the binding free energy of the lambdacI repressor to DNA

A model based on the nonlinear Poisson-Boltzmann (NLPB) equation is used to study the electrostatic contribution to the binding free energy of the lambdacI repressor to its operator DNA. In particular, we use the Poisson-Boltzmann model to calculate the pKa shift of individual ionizable amino acids upon binding. We find that three residues on each monomer, Glu34, Glu83, and the amino terminus, have significant changes in their pKa and titrate between pH 4 and 9. This information is then used to calculate the pH dependence of the binding free energy. We find that the calculated pH dependence of binding accurately reproduces the available experimental data over a range of physiological pH values. The NLPB equation is then used to develop an overall picture of the electrostatics of the lambdacI repressor-operator interaction. We find that long-range Coulombic forces associated with the highly charged nucleic acid provide a strong driving force for the interaction of the protein with the DNA. These favorable electrostatic interactions are opposed, however, by unfavorable changes in the solvation of both the protein and the DNA upon binding. Specifically, the formation of a protein-DNA complex removes both charged and polar groups at the binding interface from solvent while it displaces salt from around the nucleic acid. As a result, the electrostatic contribution to the lambdacI repressor-operator interaction opposes binding by approximately 73 kcal/mol at physiological salt concentrations and neutral pH. A variety of entropic terms also oppose binding. The major force driving the binding process appears to be release of interfacial water from the protein and DNA surfaces upon complexation and, possibly, enhanced packing interactions between the protein and DNA in the interface. When the various nonelectrostatic terms are described with simple models that have been applied previously to other binding processes, a general picture of protein/DNA association emerges in which binding is driven by the nonpolar interactions, whereas specificity results from electrostatic interactions that weaken binding but are necessary components of any protein/DNA complex.     

Thermodynamics of gamma-aminobutyric acid type A receptor binding differentiate agonists from antagonists

Specific binding of the gamma-aminobutyric acid (GABA)A antagonist [3H]SR 95531 to synaptosomal membranes of rat whole brain was examined between 0 degrees and 37 degrees. Scatchard analysis revealed two (high and low affinity) populations of [3H]SR 95531 binding sites. The Kd values increased with increasing temperature. Ki values for GABAA agonists and antagonists were determined from the displacement of [3H]SR 95531 binding at a low concentration (1.8 nM) of [3H]SR 95531, which binds predominantly to high affinity sites. For most compounds van't Hoff plots (--In Ki, i.e., In Ka, versus 1/T) were linear between 0 degrees and 37 degrees. Curvilinear van't Hoff plots for the antagonists R 5135 and bicuculline methiodide can be attributed to their hydrophobic binding interactions. The enthalpy changes of binding (delta H degrees) were positive for the agonists (muscimol, isoguvacine, GABA, 4,5,6,7-tetrahydroisoxazolo[4,5-c]pyridin-3-ol hydrochloride, and imidazole-4-acetic acid) and negative for the antagonists (pitrazepin, bicuculline methiodide, R 5135, SR 95531, and SR 95103). Separation of the enthalpic and entropic components of the Gibbs free energy changes of binding (delta G degrees) revealed that binding of the antagonists is driven by both the enthalpic and entropic terms, whereas that of the agonists is driven entirely by entropy changes. A plot of the entropic term (-T delta S degrees) versus the enthalpic term (delta H degrees) showed separate patterns for GABAA agonists and antagonists, with the partial agonists [5-(4-piperidyl)isoxazol-3-ol, imidazole-4-acetic acid, and 4,5,6,7-tetrahydroisoxazolo[4,5-c]pyridin-3-ol hydrochloride] between them. It is proposed that the entropic term is partly determined by a transition from antagonist to agonist conformation of the GABAA binding sites.     

Calorimetric studies of E. coli SSB protein-single-stranded DNA interactions. Effects of monovalent salts on binding enthalpy

Isothermal titration calorimetry (ITC) was used to examine the effects of monovalent salts (NaCl, NaBr, NaF and ChCl) on the binding enthalpy (DeltaHobs) for E. coli SSB tetramer binding to the single-stranded oligodeoxythymidylates, dT(pT)69 and dT(pT)34 over a wide range of salt concentrations from 10 mM to 2.0 M (25 degrees C, pH 8.1), and when possible, the binding free energy and entropy (DeltaG degrees obs, DeltaS degrees obs). At low monovalent salt concentrations (<0.1 M), the total DeltaHobs for saturating all sites on the SSB tetramer with ssDNA shows little dependence on salt concentration, but is extremely large and exothermic (DeltaHobs=-150(+/-5) kcal/mol). This is much larger than any DeltaHobs previously reported for a protein-nucleic acid interaction. However, at salt concentrations above 0.1 M, DeltaHobs is quite sensitive to NaCl and NaBr concentration, becoming less negative with increasing salt concentration (DeltaHobs=-70(+/-1)-kcal/mol in 2 M NaBr). These salt effects on DeltaHobs were mainly a function of anion type and concentration, with the largest effects observed in NaBr, and then NaCl, with little effect of [NaF]. These large effects of salt on DeltaHobs appear to be coupled to a net release of weakly bound anions (Br- and Cl-) from the SSB protein upon DNA binding. However, at lower salt concentrations (相似文献   

The binding of cyclosporin A to human plasma: an in vitro microdialysis study

PURPOSE: The human plasma binding of cyclosporin A was studied in vitro using the technique of microdialysis. The effect of temperature on the overall binding interaction between cyclosporin A and human plasma was also investigated. METHODS: Flow-through loop-type microdialysis probes were constructed from fused silica tubing and regenerated cellulose tubing with a MWCO of 13000 daltons. Probes were perfused with phosphate buffer (0.5 microliters/min) and the concentration of 3H-cyclosporin A in the well-mixed medium (plasma or buffer) was 1200 ng/ml. Relative recoveries of cyclosporin A from plasma or buffer were determined for each probe by separate experiments to measure the solute gain or loss with reference to the perfusate. RESULTS: Recoveries determined by loss were significantly greater than those determined by gain and in each case temperature dependent, with higher recoveries at higher temperatures. The plasma free fraction of cyclosporin A calculated from the recovery data and the perfusate to plasma concentration ratios was dependent on temperature in a log-linear fashion. Mean +/- s.d. plasma free fractions expressed in percent were 33.5 +/- 4.6, 17.9 +/- 3.6, 6.2 +/- 0.8, 3.0 +/- 0.6, and 1.5 +/- 0.2 at temperatures of 4, 10, 20, 30, and 37 degrees C, respectively. Assuming that the enthalpy of binding is constant over the temperature range studied and pseudo-first order conditions exist, the binding reaction at these temperatures was spontaneous, endothermic (delta H = 74.0 kJ/mole), and entropically driven (delta S = 0.274 kJ/mole/deg). CONCLUSIONS: These results show that the free fraction of cyclosporin A in human plasma is dependent on temperature with the fraction unbound decreasing with temperature in the range of 4 to 37 degrees C. The thermodynamic parameters for the binding of cyclosporin A to plasma components indicate that the reaction is a spontaneous endothermic reaction that is mainly entropy driven, similar to the partitioning of lipophilic molecules from an aqueous to a hydrophobic phase. Moreover, these results show that microdialysis is a feasible method to determine the binding interactions between plasma and cyclosporin A, which indicates the method may be suitable for other difficult binding studies where the solutes have nonspecific binding to separation devices.     

Thermodynamics of antigen-antibody binding using specific anti-lysozyme antibodies

Titration calorimetry measurements on the binding of hen lysozyme to the specific monoclonal IgG antibodies D1.3, D11.15, D44.1, F9.13.7, F10.6.6, their papain-cleaved antigen binding fragments (Fab) and their protein-engineered fragments consisting of non-covalently linked heavy variable chain and light variable chain domains (Fv) were performed between 6-50 degrees C in 0.15 M NaCl, 0.01 M sodium phosphate pH 7.1. The binding thermodynamic free energy change (delta G degrees b), enthalpy change (delta Hb), and entropy change (delta Sb) were the same for the whole IgG and its Fv and Fab fragments. With the exception of F9.13.7 at 13 degrees C, all the binding reactions were enthalpically driven with enthalpy changes ranging from -129 +/- 7 kJ mol-1 (D1.3 at 49.8 degrees C) to -26.2 +/- 0.6 kJ mol-1 (D44.1 at 8.0 degrees C). The heat capacity changes for the binding reaction (delta Cp) ranged from -2.72 +/- 0.16 kJ mol-1 K-1 (F9.13.7) to -0.95 +/- 0.06 kJ mol-1 K-1 (F10.6.6). The apolar surface areas buried at the binding sites estimated from the heat capacity changes indicate that the binding reactions are primarily hydrophobic, contrary to the mainly observed enthalpy-driven nature of the reactions. Conformational stabilization and the presence of water at the antigen-antibody interface may account for this discrepancy.     

Counterion condensation revisited

We review some of the characteristic properties of the structure of polyelectrolyte solutions: the condensed layer of counterions that forms abruptly at a critical threshold charge density on the polymer chain; the more diffuse Debye-Hückel cloud, which is spatially distinct from the condensed layer; and the entropic release of counterions from the condensed layer as a driving force for the binding of oppositely charged ligands. We present a reminder of the basis of our current understanding in a variety of experiments, simulations, and theories; and we attempt as well to clarify some misunderstandings. We present a new analysis of a lattice model that suggests why the limiting laws for polyelectrolyte thermodynamics have proved to be accurate despite the neglect of polymer-polymer interactions in their original derivation. We sketch recent progress in constructing a potential between counterion and polyion. A counterion located in the interface between condensed layer and Debye cloud is repelled from the polyion, creating a sharp boundary between the two counterion populations.     

Isothermal titration microcalorimetric studies for the binding of octenoyl-CoA to medium chain acyl-CoA dehydrogenase

We investigated the binding of octenoyl-CoA to pig kidney medium chain acyl-CoA dehydrogenase (MCAD) by isothermal titration microcalorimetry under a variety of experimental conditions. At 25 degrees C in 50 mM phosphate buffer at pH 7.6 (ionic strength of 175 mM), the binding is characterized by the stoichiometry (n) of 0.89 mole of octenoyl-CoA/(mole of MCAD subunit), delta G = -8.75 kcal/mol, delta H = -10.3 kcal/mol, and delta S = -5.3 cal mol(-1) K(-1), suggesting that formation of MCAD-octenoyl-CoA is enthalpically driven. By employing buffers with various ionization enthalpies, we discerned that formation of the MCAD-octenoyl-CoA complex, at pH 7.6, accompanies abstraction (consumption) of 0.52 +/- 0.15 proton/(MCAD subunit) from the buffer media. We studied the effects of pH, ionic strength, and temperature on the thermodynamics of MCAD-octenoyl-CoA interaction. Whereas the ionic strength does not significantly influence the above interaction, the pH of the buffer media exhibits a pronounced effect. The pH dependence of the association constant of MCAD +octenoyl-CoA <==> MCAD-octenoyl-CoA yields a pKa for the free enzyme of 6.2. Among thermodynamic parameters, whereas delta G remains invariant as a function of temperature, delta H and deltaS(standard) both decrease with an increase in temperature. At temperatures of < 25 degrees C, delta G is dominated by favorable entropic contributions. As the temperature increases, the entropic contributions progressively decrease, attain a value of zero at 23.8 degrees C, and then becomes unfavorable. During this transition, the enthalpic contributions become progressively favorable, resulting in an enthalpy-entropy compensation. The temperature dependence of delta H yields the heat capacity change (delta Cp(0)) of -0.37 +/- 0.05 kcal mol(-1) K(-1), attesting to the fact that the binding of octenoyl-CoA to MCAD is primarily dominated by the hydrophobic forces. The thermodynamic data presented herein are rationalized in light of structural-functional relationships in MCAD catalysis.     

Comparison of the DNA binding characteristics of the related zinc finger proteins WT1 and EGR1

The interactions of the related zinc finger proteins WT1 and EGR1 with DNA have been investigated using a quantitative binding assay. A recombinant peptide containing the four zinc fingers of WT1 binds to the dodecamer DNA sequence GCG-TGG-GCG-TGT with an apparent dissociation constant (Kd) of (1.14 +/- 0.09) x 10(-9) M under conditions of 0.1 M KCl, pH 7.5, at 22 degrees C. Under the same conditions, a recombinant peptide containing the three zinc fingers of EGR1 binds to the dodecamer sequence, the first nine bases comprising the EGR consensus binding site, with an apparent Kd of (3.55 +/- 0.24) x 10(-9) M. The nature of the equilibrium binding of each peptide to DNA was investigated as a function of temperature, pH, monovalent salt concentration, and divalent salt concentration. The interaction of WT1 with DNA is an entropy-driven process, while the formation of the EGR1-DNA complex is favored by enthalpy and entropy. The DNA binding activities of both proteins have broad pH optima centered at pH 8.0. The binding of both proteins to DNA shows similar sensitivity to ionic strength, with approximately 7.7 +/- 0.8 ion pairs formed in the EGR1-DNA complex and 9.2 +/- 1.8 ion pairs formed in the WT1-DNA complex. Results of measuring the effects of point mutations in the DNA binding site on the affinity of WT1 and EGR1 indicates a significant difference in the optimal binding sites: for EGR1, the highest affinity binding site has the sequence GNG-(T/G)GG-G(T/C)G, while for WT1 the highest affinity binding site has the sequence G(T/C)G-(T/G)GG-GAG-(T/C)G(T/C).     

Protein surface-distribution and protein-protein interactions in the binding of peripheral proteins to charged lipid membranes

The binding of native cytochrome c to negatively charged lipid dispersions of dioleoyl phosphatidylglycerol has been studied over a wide range of ionic strengths. Not only is the strength of protein binding found to decrease rapidly with increasing ionic strength, but also the binding curves reach an apparent saturation level that decreases rapidly with increasing ionic strength. Analysis of the binding isotherms with a general statistical thermodynamic model that takes into account not only the free energy of the electrostatic double layer, but also the free energy of the surface distribution of the protein, demonstrates that the apparent saturation effects could arise from a competition between the out-of-plane binding reaction and the lateral in-plane interactions between proteins at the surface. It is found that association with nonlocalized sites results in binding isotherms that display the apparent saturation effect to a much more pronounced extent than does the Langmuir adsorption isotherm for binding to localized sites. With the model for nonlocalized sites, the binding isotherms of native cytochrome c can be described adequately by taking into account only the entropy of the surface distribution of the protein, without appreciable enthalpic interactions between the bound proteins. The binding of cytochrome c to dioleoyl phosphatidylglycerol dispersions at a temperature at which the bound protein is denatured on the lipid surface, but is nondenatured when free in solution, has also been studied. The binding curves for the surface-denatured protein differ from those for the native protein in that the apparent saturation at high ionic strength is less pronounced. This indicates the tendency of the denatured protein to aggregate on the lipid surface, and can be described by the binding isotherms for nonlocalized sites only if attractive interactions between the surface-bound proteins are included in addition to the distributional entropic terms. Additionally, it is found that the binding capacity for the native protein is increased at low ionic strength to a value that is greater than that for complete surface coverage, and that corresponds more closely to neutralization of the effective charge (determined from the ionic strength dependence), rather than of the total net charge, on the protein. Electron spin resonance experiments with spin-labeled lipids indicate that this different mode of binding arises from a penetration or disturbance of the bilayer surface by the protein that may alleviate the effects of in-plane interactions under conditions of strong binding.     

Thermodynamic studies of tyrosyl-phosphopeptide binding to the SH2 domain of p56lck

The interaction between SH2 domains and tyrosine-phosphorylated proteins is essential in several cytosolic signal transduction pathways. Here we report thermodynamic studies of the interaction of the p56lck (lck) SH2 domain with several phosphopeptides, using the technique of isothermal titration calorimetry (ITC). This is the first report of the use of ITC to study SH2 domain binding reactions. The free energy of binding of the SH2 domain of lck to a phosphopeptide corresponding to the autoregulatory C-terminus of the protein (pY505) was found to be similar to that measured for a phosphopeptide modeled on the C-terminus of the epidermal growth-factor receptor (delta G degrees approximately -7.0 kcal mol-1 at pH 6.8), although significant differences in the enthalpy and entropy were observed. Binding of a phosphopeptide modeled on the C-terminus of p185neu was weaker (delta G degrees approximately -5.4 kcal mol-1 at pH 6.8). Lowering the pH to 5.5 reduced the binding affinity of pY505 by approximately 1 order of magnitude. We ascribe this to the protonation of a histidine side chain in the SH2 domain (H180), which is involved in a hydrogen-bonding network that optimizes the binding site geometry. No difference in affinity was observed between portions of lck corresponding to the SH3-SH2 (residues 63-228) and SH2 (residues 123-228) domains for the pY505 peptide. We also studied the effect upon pY505 peptide binding of mutations at two highly conserved arginine residues in the lck SH2 domain (R134 and R154).(ABSTRACT TRUNCATED AT 250 WORDS)     

Thermodynamic characterization of daunomycin-DNA interactions: comparison of complete binding profiles for a series of DNA host duplexes

Using a combination of spectroscopic and calorimetric techniques, we have determined complete thermodynamic binding profiles (delta G degree, delta H degree, and delta S degree) for the complexation of daunomycin to a series of 10 polymeric DNA duplexes. We find the resulting drug binding data to be sensitive to the base composition and sequence of the host duplex, with the binding free energies ranging from -7.5 to -10.8 kcal/mol of bound drug and the binding enthalpies ranging from +4.11 to -10.76 kcal/mol of bound drug at 25 degrees C. The smaller range in the free energy term reflects the impact of large enthalpy-entropy compensations. We observe that the three synthetic duplexes which exhibit the highest daunomycin binding affinities all contain GC (or IC) base pairs as part of alternating purine/pyrimidine sequence motifs, with these high binding affinities being strongly enthalpy driven at 25 degrees C. Specific comparisons between the binding profiles for daunomycin complexation with select pairs of host duplexes lead to the following observations: (1) The presence or absence of a major-groove methyl group does not alter daunomycin binding thermodynamics. (2) The presence or absence of a minor-groove amino group does alter daunomycin binding thermodynamics. (3) Duplexes with different base compositions but identical minor-groove functionality exhibit similar daunomycin binding thermodynamics. (4) Homopolymeric duplexes composed of either AT or AU base pairs, but not GC base pairs, exhibit large enthalpy-entropy compensations in their daunomycin binding profiles. We propose interpretations of these and other features of our thermodynamic data in terms of specific daunomycin-DNA interactions deduced from available structural data.     

Ultratight DNA binding of a new bisintercalating anthracycline antibiotic

Differential scanning calorimetry and absorption spectroscopy were used to characterize the interaction of the new bisintercalating anthracycline antibiotic, WP631, with DNA. The method of continuous variations revealed five distinct binding modes for WP631, corresponding to 6, 3, 1.3, 0.5, and 0.25 mol of base pairs (bp) per mole of ligand. The binding of one drug to 6 bp corresponds to the bisintercalative binding mode determined previously, and was the mode studied in detail. UV melting experiments and differential scanning calorimetry were used to measure the ultratight binding of WP631 to DNA. The binding constant for the interaction of WP631 with herring sperm DNA was determined to be 3.1 (+/- 0.2) x 10(11) M-1 at 20 degrees C. The large, favorable binding free energy of -15.3 kcal mol-1 was found to result from a large, negative enthalpic contribution of -30.2 kcal mol-1. DNA melting curves at different concentrations of WP631 were fitted to McGhee's model of DNA melting in the presence of ligands, yielding an independent estimate of DNA binding parameters. The salt dependence of the WP631 binding constant was examined, yielding a slope SK = delta (log K)/delta (log[Na+]) = 1.63. The observed salt dependence of the equilibrium constant, interpreted according to polyelectrolyte theory, indicates that there is a significant nonpolyelectrolyte contribution to the binding free energy. DNA melting studies using a homogeneous 214 bp DNA fragment showed that WP631 binds preferentially to the GC-rich region of the DNA.     

Toward an estimation of binding constants in aqueous solution: studies of associations of vancomycin group antibiotics

An approach toward the estimation of binding constants for organic molecules in aqueous solution is presented, based upon a partitioning of the free energy of binding. Consideration is given to polar and hydrophobic contributions and to the entropic cost of rotor restrictions and bimolecular associations. Several parameters (derived from an analysis of entropy changes upon the melting of crystals and from the binding of cell wall peptide analogues to the antibiotic ristocetin A) which may be useful guides to a crude understanding of binding phenomena are presented: (i) amide-amide hydrogen bond strengths of -(1 to 7) +/- 2 kJ.mol-1, (ii) a hydrophobic effect of -0.2 +/- 0.05 kJ.mol-1.A-2 of hydrocarbon removed from exposure to water in the binding process, and (iii) free energy costs for rotor restrictions of 3.5-5.0 kJ.mol-1. The validity of the parameters for hydrogen bond strengths is dependent on the validity of the other two parameters. The phenomenon of entropy/enthalpy compensation is considered, with the conclusion that enthalpic barriers to dissociations will result in larger losses in translational and rotational entropy in the association step. The dimerization of some vancomycin group antibiotics is strongly exothermic (-36 to -51 kJ.mol-1) and is promoted by a factor of 50-100 by a disaccharide attached to ring 4 (in vancomycin and eremomycin) and by a factor of ca. 1000 by an amino-sugar attached to the benzylic position of ring 6 in eremomycin. The dimerization process (which, as required for an exothermic association, appears to be costly in entropy) may be relevant to the mode of action of the antibiotics.     

Evaluation of the counterion condensation theory of polyelectrolytes

We compare free energies of counterion distributions in polyelectrolyte solutions predicted from the cylindrical Poisson-Boltzmann (PB) model and from the counterion condensation theories of Manning: CC1 (Manning, 1969a, b), which assumes an infinitely thin region of condensed counterions, and CC2 (Manning, 1977), which assumes a region of finite thickness. We consider rods of finite radius with the linear charge density of B-DNA in 1-1 valent and 2-2 valent salt solutions. We find that under all conditions considered here the free energy of the CC1 and the CC2 models is higher than that of the PB model. We argue that counterion condensation theory imposes nonphysical constraints and is, therefore, a poorer approximation to the underlying physics based on continuum dielectrics, point-charge small ions, Poisson electrostatics, and Boltzmann distributions. The errors in counterion condensation theory diminish with increasing distance from, or radius of, the polyion.     

The folding of centromeric DNA strands into intercalated structures: a physicochemical and computational study

We have carried out a physicochemical and computational analysis on the stability of the intercalated structures formed by cytosine-rich DNA strands. In the computational study, the electrostatic energy components have been calculated using a Poisson-Boltzmann model, and the non-polar energy components have been computed with a van der Waals function and/or a term dependent on the solvent-accessible surface area of the molecules. The results have been compared with those obtained for Watson-Crick duplexes and with thermodynamic data derived from UV experiments. We have found that intercalated DNA is mainly stabilized by very favorable electrostatic interactions between hydrogen-bonded protonated and neutral cytosines, and by non-polar forces including the hydrophobic effect and enhanced van der Waals contacts. Cytosine protonation electrostatically promotes the association of DNA strands into a tetrameric structure. The electrostatic interactions between stacked C.C+ pairs are strongly attenuated by the reaction field of the solvent, and are modulated by a complex interplay of geometric and protonation factors. The forces stabilizing intercalated DNA must offset an entropic penalty due to the uptake of protons for cytosine protonation, at neutral pH, and also the electrostatic contribution to the solvation free energy. The latter energy component is less favorable for protonated DNA due to the partial neutralization of the negative charge of the molecule, and probably affects other protonated DNA and RNA structures such as C+-containing triplexes.     

Comparison between antigen-antibody binding energies and interfacial free energies

Antigen-antibody binding energies derived from equilibrium data are compared with the binding energies resulting from the interfacial free energies obtained from contact angle measurements of antigens and antibodies. From these interfacial free energies two sorts of theoretical antigen-antibody binding energies can be derived, as well as the Hamaker constants for most antigen-antibody systems. For interaction in vacuo the Hamaker constants obtained are between 4 and 6 X 10(-13) ergs, while these constants for hydrated antigen antibody interactions are less than 10(-14) ergs. For interactions in vacuo, interfacial free energies yield binding energies (delta Fa) that lie between -120 and -140 ergs/cm2. For interactions in the aqueous phase (with interstitial water still present), much lower binding energies (delta Fb) are derived, of the order of -.01 and -1 ergs/cm2. In comparison, dextran-anti-dextran interactions show a binding energy derived from equilibrium data (delta Feq) of the order of -10 ergs/cm2. In general the equilibrium binding energies delta Feq of most antigen-antibody systems would vary between -1 and -20 ergs/cm2. The implications of this comparison are discussed in the light of the influence of residual water between antigenic determinant and antibody-active site, as well as in the light of the degree of perfection of fit between these sites.     

Energetics of drug-DNA interactions

Understanding the thermodynamics of drug binding to DNA is of both practical and fundamental interest. The practical interest lies in the contribution that thermodynamics can make to the rational design process for the development of new DNA targeted drugs. Thermodynamics offer key insights into the molecular forces that drive complex formation that cannot be obtained by structural or computational studies alone. The fundamental interest in these interactions lies in what they can reveal about the general problems of parsing and predicting ligand binding free energies. For these problems, drug-DNA interactions offer several distinct advantages, among them being that the structures of many drug-DNA complexes are known at high resolution and that such structures reveal that in many cases the drug acts as a rigid body, with little conformational change upon binding. Complete thermodynamic profiles (delta G, delta H, delta S, delta Cp) for numerous drug-DNA interactions have been obtained, with the help of high-sensitivity microcalorimetry. The purpose of this article is to offer a perspective on the interpretation of these thermodynamics parameters, and in particular how they might be correlated with known structural features. Obligatory conformational changes in the DNA to accommodate intercalators and the loss of translational and rotational freedom upon complex formation both present unfavorable free energy barriers for binding. Such barriers must be overcome by favorable free energy contributions from the hydrophobic transfer of ligand from solution into the binding site, polyelectrolyte contributions from coupled ion release, and molecular interactions (hydrogen and ionic bonds, van der Waals interactions) that form within the binding site. Theoretical and semiempirical tools that allow estimates of these contributions to be made will be discussed, and their use in dissecting experimental data illustrated. This process, even at the current level of approximation, can shed considerable light on the drug-DNA binding process.     

Quality of life and pain in patients with recurrent breast and gynecologic cancer

The kinetic mechanisms of the binding to tubulin of colchicine and eight different analogues have been studied to elucidate details of the recognition mechanism. All of the analogues follow a two step binding mechanism i.e. binding occurs via an initial step with low affinity, followed by an isomerisation of the initial complex leading to the final high affinity state. For several analogues the kinetic and thermodynamic data of both processes are compared here. For all the analogues the delta G1 degree of initial binding at 25 degrees C varies between -13.3 and -28.8 kJ. mol-1. For the second step delta G2 degrees varies between -2.4 and -27 kJ. mol-1. These limited ranges of free energy change are, however, obtained by a great variety of enthalpy changes and compensatory entropy changes. Comparison of the data for the first and second steps indicates that structural alterations of the drugs always change the thermodynamic parameters of the two steps, and the changes in the first and the second steps are in opposite directions. The fact that this range of experimental behaviour can be incorporated into a general mechanism encourages the extension of these investigations to other colchicine analogues and related compounds with potential pharmaceutical applications.