Isothermal titration calorimetry studies of the binding of the antimicrobial peptide gramicidin S to phospholipid bilayer membranes

The binding of the amphiphilic, positively charged, cyclic beta-sheet antimicrobial decapeptide gramicidin S (GS) to various lipid bilayer model membrane systems was studied by isothermal titration calorimetry. Large unilamellar vesicles composed of the zwitterionic phospholipid 1-palmitoyl-2-oleoylphosphatidylcholine or the anionic phospholipid 1-palmitoyl-2-oleoylphosphatidylglycerol, or a binary mixture of the two, with or without cholesterol, were used to mimic the lipid compositions of the outer monolayers of the lipid bilayers of mammalian and bacterial membranes, respectively. Dynamic light scattering results suggest the absence of major alterations in vesicle size or appreciable vesicle fusion upon the binding of GS to the lipid vesicles under our experimental conditions. The binding isotherms can be reasonably well described by a one-site binding model. GS is found to bind with higher affinity to anionic phosphatidylglycerol than to zwitterionic phosphatidylcholine vesicles, indicating that electrostatic interactions in the former system facilitate peptide binding. However, the presence of cholesterol reduced binding only slightly, indicating that the binding of GS is not highly sensitive to the order of the phospholipid bilayer system. Similarly, the measured positive endothermic binding enthalpy (DeltaH) varies only modestly (2.6 to 4.4 kcal/mol), and the negative free energy of binding (DeltaG) also remains relatively constant (-10.9 to -12.1 kcal/mol). The relatively large but invariant positive binding entropy, reflected in relatively large TDeltaS values (13.4 to 16.4 kcal/mol), indicates that GS binding to phospholipid bilayers is primarily entropy driven. Finally, the relative binding affinities of GS for various phospholipid vesicles correlate relatively well with the relative lipid specificity for GS interactions with bacterial and erythrocyte membranes observed in vivo.     

Protein chemistry at membrane interfaces: non-additivity of electrostatic and hydrophobic interactions

Non-specific binding of proteins and peptides to charged membrane interfaces depends upon the combined contributions of hydrophobic (DeltaG(HPhi)) and electrostatic (DeltaG(ES)) free energies. If these are simply additive, then the observed free energy of binding (DeltaG(obs)) will be given by DeltaG(obs)=DeltaG(HPhi)+DeltaG(ES), where DeltaG(HPhi)=-sigma(NP)A(NP) and DeltaG(ES)=zFphi. In these expressions, A(NP) is the non-polar accessible area, sigma(NP) the non-polar solvation parameter, z the formal peptide valence, F the Faraday constant, and phi the membrane surface potential. But several lines of evidence suggest that hydrophobic and electrostatic binding free energies of proteins at membrane interfaces, such as those associated with cell signaling, are not simply additive. In order to explore this issue systematically, we have determined the interfacial partitioning free energies of variants of indolicidin, a cationic proline-rich antimicrobial peptide. The synthesized variants of the 13 residue peptide covered a wide range of hydrophobic free energies, which allowed us to examine the effect of hydrophobicity on electrostatic binding to membranes formed from mixtures of neutral and anionic lipids. Although DeltaG(obs) was always a linear function of DeltaG(HPhi), the slope depended upon anionic lipid content: the slope was 1.0 for pure, zwitterionic phosphocholine bilayers and 0.3 for pure phosphoglycerol membranes. DeltaG(obs) also varied linearly with surface potential, but the slope was smaller than the expected value, zF. As observed by others, this suggests an effective peptide valence z(eff) that is smaller than the formal valence z. Because of our systematic approach, we were able to establish a useful rule-of-thumb: z(eff) is reduced relative to z by about 20 % for each 3 kcal mol(-1) (1 kcal=4.184 kJ) favorable increase in DeltaG(HPhi). For neutral phosphocholine interfaces, we found that DeltaG(obs) could be predicted with remarkable accuracy using the Wimley-White experiment-based interfacial hydrophobicity scale.     

Thermodynamic and kinetic characterization of Co-C bond homolysis catalyzed by coenzyme B(12)-dependent methylmalonyl-CoA mutase

Methylmalonyl-CoA mutase is a member of the family of coenzyme B(12)-dependent isomerases and catalyzes the 1,2-rearrangement of methylmalonyl-CoA to succinyl-CoA. A common first step in the reactions catalyzed by coenzyme B(12)-dependent enzymes is cleavage of the cobalt-carbon bond of the cofactor, leading to radical-based rearrangement reactions. Comparison of the homolysis rate for the free and enzyme-bound cofactors reveals an enormous rate enhancement which is on the order of a trillion-fold. To address how this large rate acceleration is achieved, we have examined the kinetic and thermodynamic parameters associated with the homolysis reaction catalyzed by methylmalonyl-CoA mutase. Both the rate and the amount of cob(II)alamin formation have been analyzed as a function of temperature with the protiated substrate. These studies yield the following activation parameters for the homolytic reaction at 37 degrees C: DeltaH(f)() = 18.8 +/- 0.8 kcal/mol, DeltaS(f)() = 18.2 +/- 0.8 cal/(mol.K), and DeltaG(f)() = 13.1 +/- 0.6 kcal/mol. Our results reveal that the enzyme lowers the transition state barrier by 17 kcal/mol, corresponding to a rate acceleration of 0.9 x 10(12)-fold. Both entropic and enthalpic factors contribute to the observed rate acceleration, with the latter predominating. The substrate binding step is exothermic, with a DeltaG of -5.2 kcal/mol at 37 degrees C, and is favored by both entropic and enthalpic factors. We have employed the available kinetic and spectroscopic data to construct a qualitative free energy profile for the methylmalonyl-CoA mutase-catalyzed reaction.     

Octyl-beta-D-glucopyranoside partitioning into lipid bilayers: thermodynamics of binding and structural changes of the bilayer.

The interaction of the nonionic detergent octyl-beta-D-glucopyranoside (OG) with lipid bilayers was studied with high-sensitivity isothermal titration calorimetry (ITC) and solid-state 2H-NMR spectroscopy. The transfer of OG from the aqueous phase to lipid bilayers composed of 1-palmitoyl-2-oleoyl-sn-glycero-3-phosphocholine (POPC) can be investigated by employing detergent at concentrations below the critical micellar concentration; it can be defined by a surface partition equilibrium with a partition coefficient of K = 120 +/- 10 M-1, a molar binding enthalpy of delta H degrees D = 1.3 +/- 0.15 kcal/mol, and a free energy of binding of delta G degrees D = -5.2 kcal/mol. The heat of transfer is temperature dependent, with a molar heat capacity of delta CP = -75 cal K-1 mol-1. The large heat capacity and the near-zero delta H are typical for a hydrophobic binding equilibrium. The partition constant K decreased to approximately 100 M-1 for POPC membranes mixed with either negatively charged lipids or cholesterol, but was independent of membrane curvature. In contrast, a much larger variation was observed in the partition enthalpy. delta H degrees D increased by about 50% for large vesicles and by 75% for membranes containing 50 mol% cholesterol. Structural changes in the lipid bilayer were investigated with solid-state 2H-NMR. POPC was selectively deuterated at the headgroup segments and at different positions of the fatty acyl chains, and the measurement of the quadrupolar splittings provided information on the conformation and the order of the bilayer membrane. Addition of OG had almost no influence on the lipid headgroup region, even at concentrations close to bilayer disruption. In contrast, the fluctuations of fatty acyl chain segments located in the inner part of the bilayer increased strongly with increasing OG concentration. The 2H-NMR results demonstrate that the headgroup region is the most stable structural element of the lipid membrane, remaining intact until the disordering of the chains reaches a critical limit. The perturbing effect of OG is thus different from that of another nonionic detergent, octaethyleneglycol mono-n-dodecylether (C12E8), which produces a general disordering at all levels of the lipid bilayer. The OG-POPC interaction was also investigated with POPC monolayers, using a Langmuir trough. In the absence of lipid, the measurement of the Gibbs adsorption isotherm for pure OG solutions yielded an OG surface area of AS = 51 +/- 3 A2. On the other hand, the insertion area AI of OG in a POPC monolayer was determined by a monolayer expansion technique as AI = 58 +/- 10 A2. The similar area requirements with AS approximately AI indicate an almost complete insertion of OG into the lipid monolayer. The OG partition constant for a POPC monolayer at 32 mN/m was Kp approximately 320 M-1 and thus was larger than that for a POPC bilayer.     

Detergent-like action of the antibiotic peptide surfactin on lipid membranes

Surfactin is a bacterial lipopeptide with powerful surfactant-like properties. High-sensitivity isothermal titration calorimetry was used to study the self association and membrane partitioning of surfactin. The critical micellar concentration (CMC), was 7.5 microM, the heat of micellization was endothermic with DeltaH(w-->m)(Su) = +4.0 kcal/mol, and the free energy of micellization DeltaG(O,w-->m)(Su) = -9.3 kcal/mol (25 degrees C; 100 mM NaCl; 10 mM TRIS, 1 mM EDTA; pH 8.5). The specific heat capacity of micellization was deduced from temperature dependence of DeltaH(w-->m)(Su) as DeltaC(w-->m)(P) = -250 +/- 10 cal/(mol.K). The data can be explained by combining the hydrophobicity of the fatty acyl chain with that of the hydrophobic amino acids. The membrane partition equilibrium was studied using small (30 nm) and large (100 nm) unilamellar POPC vesicles. At 25 degrees C, the partition coefficient, K, was (2.2 +/- 0.2) x 10(4) M(-1) for large vesicles leading to a free energy of DeltaG(O, w-->b)(Su) = -8.3 kcal/mol. The partition enthalpy was again endothermic, with DeltaH(w-->b)(Su) = 9 +/- 1 kcal/mol. The strong preference of surfactin for micelle formation over membrane insertion explains the high membrane-destabilizing activity of the peptide. For surfactin and a variety of non-ionic detergents, the surfactant-to-lipid ratio, inducing membrane solubilization, R(sat)(b), can be predicted by the simple relationship R(sat)(b) approximately K. CMC.     

Protein transduction domains of HIV-1 and SIV TAT interact with charged lipid vesicles. Binding mechanism and thermodynamic analysis

Cell-penetrating peptides (CPPs) traverse cell membranes of cultured cells very efficiently by a mechanism not yet identified. Recent theories for the translocation suggest either the binding of the CPPs to extracellular glycosaminoglycans or the formation of inverted micelles with negatively charged lipids. In the present study, the binding of the protein transduction domains (PTD) of human (HIV-1) and simian immunodeficiency virus (SIV) TAT peptide (amino acid residues 47-57, electric charge z(p) = +8) to membranes containing various proportions of negatively charged lipid (POPG) is characterized. Monolayer expansion measurements demonstrate that TAT-PTD insertion between lipids requires loosely packed monolayer films. For densely packed monolayers (pi > 29 mN/m) and lipid bilayers, no insertion is possible, and binding occurs via electrostatic adsorption to the membrane surface. Light scattering experiments show an aggregation of anionic lipid vesicles when the electric surface charge is neutralized by TAT-PTD, the observed stoichiometry being close to the theoretical value of 1:8. Membrane binding was quantitated with isothermal titration calorimetry and three further methods. The reaction enthalpy is Delta H degrees approximately equal to -1.5 kcal/mol peptide and is almost temperature-independent with Delta C(p) degrees approximately 0 kcal/(mol K), indicating equal contributions of polar and hydrophobic interactions to the reaction heat capacity. The binding of TAT-PTD to the anionic membrane is described by an electrostatic attraction/chemical partition model. The electrostatic attraction energy, calculated with the Gouy-Chapman theory, accounts for approximately 80% of the binding energy. The overall binding constant, K(app), is approximately 10(3)-10(4) M(-1). The intrinsic binding constant (K(p)), corrected for electrostatic effects and describing the partitioning of the peptide between the lipid-water interface and the membrane, is small and is K(p) approximately 1-10 M(-1). Deuterium and phosphorus-31 nuclear magnetic resonance demonstrate that the lipid bilayer remains intact upon TAT-PTD binding. The NMR data provide no evidence for nonbilayer structures and also not for domain formation. This is further supported by the absence of dye efflux from single-walled lipid vesicles. The electrostatic interaction between TAT-PTD and anionic phosphatidylglycerol is strong enough to induce a change in the headgroup conformation of the anionic lipid, indicating a short-lived but distinct correlation between the TAT-PTD and the anionic lipids on the membrane outside. TAT-PTD has a much lower affinity for lipid membranes than for glycosaminoglycans, making the latter interaction a more probable pathway for CPP binding to biological membranes.     

Lipopolysaccharides in bacterial membranes act like cholesterol in eukaryotic plasma membranes in providing protection against melittin-induced bilayer lysis

Melittin is a small, cationic peptide that, like many other antimicrobial peptides, lyses cell membranes by acting on their lipid bilayers. However, the sensitivity to antimicrobial peptides varies among cell types. We have performed direct binding and vesicle leakage experiments to determine the sensitivity to melittin of bilayers composed of various physiologically relevant lipids, in particular, key components of eukaryotic membranes (cholesterol) and bacterial outer membranes (lipopolysaccharide or LPS). Melittin binds to bilayers composed of both zwitterionic and negatively charged phospholipids, as well as to the highly charged LPS bilayers. The magnitude of the free energy of binding (deltaG degrees ) increases with increasing bilayer charge density; deltaG degrees = -7.6 kcal/mol for phosphatidylcholine (PC) bilayers and -8.9 to -11.0 kcal/mol for negatively charged bilayers containing phosphatidylserine (PS), phospholipids with covalently attached polyethylene glycol (PEG-lipids), or LPS. Comparisons of these data show that binding is not markedly affected by the steric barrier produced by the PEG in PEG-lipids or by the polysaccharide core of LPS. The addition of equimolar cholesterol to PC bilayers reduces the level of binding (deltaG degrees = -6.4 kcal/mol) and reduces the extent of melittin-induced leakage by 20-fold. LPS and 1:1 PC/cholesterol bilayers have similar high resistance to melittin-induced leakage, indicating that cholesterol in eukaryotic plasma membranes and LPS in Gram-negative bacteria provide strong protection against the lytic effects of melittin. We argue that this resistance is due at least in part to the similar tight packing of the lipid acyl chains in PC/cholesterol and LPS bilayers. The addition of bacterial phospholipids to LPS bilayers increases their sensitivity to melittin, helping to explain the higher sensitivity of deep rough bacteria compared to smooth phenotypes.     

Isothermal titration calorimetry studies of the binding of a rationally designed analogue of the antimicrobial peptide gramicidin s to phospholipid bilayer membranes

The binding of the positively charged antimicrobial peptide cyclo[VKLdKVdYPLKVKLdYP] (GS14dK4) to various lipid bilayer model membranes was investigated using isothermal titration calorimetry. GS14dK4 is a diastereomeric lysine ring-size analogue of the naturally occurring antimicrobial peptide gramicidin S which exhibits enhanced antimicrobial and markedly reduced hemolytic activities compared with GS itself. Large unilamellar vesicles composed of various zwitterionic (1-palmitoyl-2-oleoyl-sn-glycero-3-phosphorylcholine [POPC]) and anionic phospholipids {1-palmitoyl-2-oleoyl-sn-glycero-3-[phospho-rac-(glycerol)] [POPG] and 1-palmitoyl-2-oleoyl-sn-glycero-3-[phosphoserine] [POPS]}, with or without cholesterol, were used as model membrane systems. Dynamic light scattering results indicate the absence of any peptide-induced major alteration in vesicle size or vesicle fusion under our experimental conditions. The binding of GS14dK4 is significantly influenced by the surface charge density of the phospholipid bilayer and by the presence of cholesterol. Specifically, a significant reduction in the degree of binding occurs when three-fourths of the anionic lipid molecules are replaced with zwitterionic POPC molecules. No measurable binding occurs to cholesterol-containing zwitterionic vesicles, and a dramatic drop in binding is observed in the cholesterol-containing anionic POPG and POPS membranes, indicating that the presence of cholesterol markedly reduces the affinity of this peptide for phospholipid bilayers. The binding isotherms can be described quantitatively by a one-site binding model. The measured endothermic binding enthalpy (DeltaH) varies dramatically (+6.3 to +26.5 kcal/mol) and appears to be inversely related to the order of the phospholipid bilayer system. However, the negative free energy (DeltaG) of binding remains relatively constant (-8.5 to -11.5 kcal/mol) for all lipid membranes examined. The relatively small variation of negative free energy of peptide binding together with a pronounced variation of positive enthalpy produces an equally strong variation of TDeltaS (+16.2 to +35.0 kcal/mol), indicating that GS14dK4 binding to phospholipids bilayers is primarily entropy driven.     

Main chain and side chain dynamics of the ubiquitin conjugating enzyme variant human Mms2 in the free and ubiquitin-bound States

Protein ubiquitination involves a cascade of enzymatic steps where ubiquitin (Ub) is sequentially transferred as a thiolester intermediate from an E1 enzyme to an E2 enzyme and finally to the protein target with the help of a Ub-protein ligase. Protein ubiquitination brought about by the Ubc13-Mms2 (E2-E2) complex has a unique role in the cell, unrelated to protein degradation. The Mms2-Ubc13 heterodimer links Ub molecules to one another through an isopeptide bond between its own C-terminus and Lys-63 on another Ub. The role of Mms2 is to orient a target-bound Ub molecule such that its Lys-63 is proximal to the C-terminus of the Ub molecule that is covalently linked to the active site of Ubc13. To gain insight into the influence of protein dynamics on the affinity of Ub for Mms2, we have determined pico- to nanosecond time scale fluctuations of the main chain and methyl side chains of human Mms2 in the free and Ub-bound states using solution state (15)N and (2)H nuclear magnetic resonance relaxation measurements. Analysis of the relaxation data allows for a semiquantitative estimation of the conformational entropy change (TDeltaS(NMR)) for the main chain and side chain methyl groups of Mms2 upon binding Ub. The value of TDeltaS(NMR) for the main chain and side chain methyl groups of Mms2 is -8 +/- 2 and -2 +/- 2 kcal mol(-)(1), respectively. The experimental DeltaG(binding) for the Mms2.Ub complex is -6 kcal mol(-)(1). Estimation of DeltaG(binding) using an empirical structure-based approach that does not account for changes in main chain entropy yields a value of -17 +/- 2 kcal mol(-)(1). However, inclusion of TDeltaS(NMR) for the main chain of Mms2 increases the estimated DeltaG(binding) to -9 +/- 3 kcal mol(-)(1). Assuming that changes in Ub main chain dynamics contribute to TDeltaS(NMR) to the same extent as Mms2, the estimated DeltaG(binding) is further reduced to -1 +/- 4 kcal mol(-)(1), a value close to the experimental DeltaG(binding).     

A quantum mechanics/molecular mechanics study of the catalytic mechanism and product specificity of viral histone lysine methyltransferase

There are three reaction steps in the S-adenosylmethionine (AdoMet) methylation of lysine-NH2 catalyzed by a methyltransferase. They are (i) combination of enzyme.Lys-NH3+ with AdoMet, (ii) substrate ionization to provide enzyme.AdoMet.Lys-NH2, and (iii) methyl transfer providing enzyme.AdoHcy.Lys-N(Me)H2+ and the dissociation of AdoHcy. In this study of the viral histone methyltransferase (vSET), we find that substrate ionization of vSET.Lys27-NH3+, vSET.Lys27-N(Me)H2+, and vSET.Lys27-N(Me)2H+ takes place upon combination with AdoMet. The presence of a water channel allows dissociation of a proton to the solvent. There is no water channel in the absence of AdoMet. That the formation of a water channel is combined with AdoMet binding was first discovered in our investigation of Rubisco large subunit methyltransferase. Via a quantum mechanics/molecular mechanics (QM/MM) approach, the calculated free energy barrier (DeltaG++) of the first methyl transfer reaction catalyzed by vSET [Lys27-NH2 + AdoMet --> Lys27-N(Me)H2+ + AdoHcy] equals 22.5 +/- 4.3 kcal/mol, which is in excellent agreement with the free energy barrier (21.7 kcal/mol) calculated from the experimental rate constant (0.047 min-1). The calculated DeltaG++ of the second methyl transfer reaction [AdoMet + Lys27-N(Me)H --> AdoHcy + Lys27-N(Me)2H+] at the QM/MM level is 22.6 +/- 3.6 kcal/mol, which is in agreement with the value of 22.4 kcal/mol determined from the experimental rate constant (0.015 min-1). The third methylation [Lys27-N(Me)2 + AdoMet --> Lys27-N(Me)3+ + AdoHcy] is associated with a DeltaG++ of 23.1 +/- 4.0 kcal/mol, which is in agreement with the value of 23.0 kcal/mol determined from the experimental rate constant (0.005 min-1). Our computations establish that the first, second, and third methyl transfer steps catalyzed by vSET are linear SN2 reactions with the bond making being approximately 50% associative.     

Catalytic mechanism and product specificity of rubisco large subunit methyltransferase: QM/MM and MD investigations

Molecular dynamics (MD) simulations and hybrid quantum mechanics/molecular mechanics (QM/MM) calculations have been carried out in an investigation of Rubisco large subunit methyltransferase (LSMT). It was found that the appearance of a water channel is required for the stepwise methylation by S-adenosylmethionine (AdoMet). The water channel appears in the presence of AdoMet (LSMT.Lys-NH3+.AdoMet), but is not present immediately after methyl transfer (LSMT.Lys-N(Me)H2+.AdoHcy). The water channel allows proton dissociation from both LSMT.AdoMet.Lys-NH3+ and LSMT.AdoMet.Lys-N(Me)H2+. The water channel does not appear for proton dissociation from LSMT.AdoMet.Lys-N(Me)2H+, and a third methyl transfer does not occur. By QM/MM, the calculated free energy barrier of the first methyl transfer reaction catalyzed by LSMT (Lys-NH2 + AdoMet --> Lys-N(Me)H2+ + AdoHcy) is DeltaG++ = 22.8 +/- 3.3 kcal/mol. This DeltaG++ is in remarkable agreement with the value 23.0 kcal/mol calculated from the experimental rate constant (6.2 x 10-5 s-1). The calculated DeltaG++ of the second methyl transfer reaction (AdoMet + Lys-N(Me)H --> AdoHcy + Lys-N(Me)2H+) at the QM/MM level is 20.5 +/- 3.6 kcal/mol, which is in agreement with the value 22.0 kcal/mol calculated from the experimental rate constant (2.5 x 10-4 s-1). The third methyl transfer (Lys-N(Me)2 + AdoMet --> Lys-N(Me)3+ + AdoHcy) is associated with an allowed DeltaG++ of 25.9 +/- 3.2 kcal/mol. However, this reaction does not occur because a water channel does not form to allow the proton dissociation of Lys-N(Me)2H+. Future studies will determine whether the product specificity of lysine (mono, di, and tri) methyltransferases is determined by the formation of water channels.     

The molecular basis for coxib inhibition of p38alpha MAP kinase

In this work, we present the results of two combined approaches, molecular docking and comparative molecular field analysis (CoMFA), to propose how the selective cyclooxygenase-2 inhibitor celecoxib could act as a p38 mitogen-activated protein (MAP) kinase inhibitor. The docking analysis revealed why celecoxib has a less favorable binding energy (DeltaG= -12.4kcal/mol) than the selective p38 MAP kinase (p38 MAPK) inhibitor, SB203580 (DeltaG= -22.2kcal/mol). The CoMFA results revealed unfavorable steric effects that can be related to the predicted lower p38 MAP kinase inhibitory activity of celecoxib. Additionally, FlexX and CoMFA results also suggested that etoricoxib, another selective COX-2 inhibitor, could inhibit p38 MAP kinase.     

The enthalpy change for the reduction of nicotinamide–adenine dinucleotide

The heat of the reaction NAD(+)+propan-2-ol=NADH+acetone+H(+) was determined to be 42.5+/-0.6kJ/mol (10.17+/-0.15kcal/mol) from equilibrium measurements at 9-42 degrees C catalysed by yeast alcohol dehydrogenase. With the aid of thermochemical data for acetone and propan-2-ol the values of DeltaH=-29.2kJ/mol (-6.99kcal/mol) and DeltaG(0)=22.1kJ/mol (5.28kcal/mol) are derived for the reduction of NAD (NAD(+)+H(2)=NADH+H(+)). These values are consistent with analogous but less accurate data for the ethanol-acetaldehyde reaction. Thermodynamic data for the reduction of NAD and NADP are summarized.     

Free energy of the binding of uridylic acid oligomers with double stranded poly(A) x poly(U)

The binding parameters (K, omega) and the free energy (DeltaG(0)) of triple helix formation have been estimated for complexes of oligo(U)(n) (n = 5, 7-10) with poly(A) . poly(U) on the basis of hypochromicity measurements. The data were treated according to the formula of McGhee and von Hippel [J. Mol. Biol. 86 (1974) 469] by a computer program ALAU [H. Schütz et al., Stud. Biophys. 104 (1984) 23] which takes absorbancies and total concentrations as input. In 1 mM cacodylate buffer pH 7.0 with 10 mM NaCl and 10 mM MgCl(2) at 5 degrees C the free energy of contiguous binding was found to be a linear function of the oligomer length with a slope of DeltaG(c,U)(0) = -0.72 (+/-0.03) kcal x mol(-1) per nucleotide. The mean cooperativity coefficient (omega) was 24.5 (+/- 5.6), and the corresponding free energy of interaction between the neighbouring oligonucleotides in the third strand was DeltaG(0(omega)) = -1.74 (+/-0.13) kcal x mol(-1).     

Thermodynamic measurements and predictions of the adsorption of short-chain peptides on nanothin polymer films

This contribution describes experimental measurements of submolecular-level interaction energies involved in the process of peptide adsorption on polymer films. The objective of this study was to use surface plasmon resonance (SPR) spectroscopy to measure the Gibbs energy change on adsorption (DeltaG(ad)) for pairs of various homopeptides on highly uniform, nanothin polymer films and to use these data, along with the principle of additivity, to predict DeltaG(ad) for homologous homopeptides, as well as for a mixed-residue peptide. By using a graft polymerization methodology, a nanothin poly(2-vinylpyridine) film was prepared and adsorption energies were measured first for a homologous series of tyrosine (Y) homopeptides on this film to determine submolecular-level interaction energies. By using SPR, adsorption isotherms were measured for YY and YYY peptides; analysis of these isotherms provided DeltaG(ad) data for a midchain tyrosine unit and a set of chain-end tyrosine units; values were -0.75 +/- 0.07 kcal/mol and -2.12 +/- 0.04 kcal/mol, respectively. Combining the thermodynamic contributions for adsorption of individual tyrosine units allowed a predictive estimate of -5.12 +/- 0.32 kcal/mol for the adsorption energy for YYYYYY; this estimate deviated by only 2.3% from its measured value of -5.24 +/- 0.06 kcal/mol. Similarly, adsorption energies were found for phenylalanine, glycine, and tyrosine-leucine peptides. Combining the thermodynamic contributions for adsorption of individual residue units allowed a predictive estimate of -3.24 +/- 0.38 kcal/mol for a pentapeptide, leucine enkephalin; this estimate deviated by only 3.0% from its measured value of -3.34 +/-0.11 kcal/mol.     

Reciprocal cooperative effects of multiple ligand binding to pyruvate kinase

The formation of multiple ligand complexes with muscle pyruvate kinase was measured in terms of dissociation constants and the standard free energies of formation were calculated. The binding of Mn2+ to the enzyme (KA = 55 +/- 5 X 10(-6) M; deltaF degrees = -5.75 +/- 0.05 kcal/mol) and to the enzyme saturated with phosphoenolpyruvate (conditional free energy) KA' = 0.8 +/- 0.4 X 10(-6) M; deltaF degrees = -8.22 +/- 0.34 kcal/mol) has been measured under identical conditions giving a free energy of coupling, delta(deltaF degrees) = -2.47 +/- 0.34 kcal/mol. Such a large negative free energy of coupling is diagnostic of a strong positively cooperative effect in ligand binding. The binding of the substrate phosphoenolpyruvate to free enzyme and the enzyme-Mn2+ complex was, by necessity, measured by different methods. The free energy of phosphoenolpyruvate binding to free enzyme (KS = 1.58 +/- 0.10 X 10(-4)M; deltaF degrees = -5.13 +/- 0.04 kcal/mol) and to the enzyme-Mn2+ complex (K3 = 0.75 +/- 0.10 X 10(-6)M; deltaF degrees = -8.26 +/- 0.07 kcal/mol) also gives a large negative free energy of coupling, delta(deltaF degrees) = -3.16 +/- 0.08 kcal/mol. Such a large negative value confirms reciprocal binding effects between the divalent cation and the substrate phosphoenolpyruvate. The binding of Mn2+ to the enzyme-ADP complex was also investigated and a free energy of coupling, delta(deltaF degrees) = -0.08 +/- 0.08 kcal/mol, was measured, indicative of little or no cooperativity in binding. The free energy of coupling with Mn2+ and pyruvate was measured as -1.52 +/- 0.14 kcal/mol, showing a significant amount of cooperativity in ligand binding but a substantially smaller effect than that observed for phosphoenolpyruvate binding. The magnitude of the coupling free energy may be related to the role of the divalent cation in the formation of the enzyme-substrate complexes. In the absence of the activating monovalent cation, the coupling free energies for phosphoenolpyruvate and pyruvate binding decrease by 40-60% and 25%, respectively, substantiating a role for the monovalent cation in the formation of enzyme-substrate complexes with phosphoenolpyruvate and with pyruvate.     

Light induces destabilization of photoactive yellow protein

To understand the effect of visible light on the stability of photoactive yellow protein (PYP), urea denaturation experiments were performed with PYP in the dark and with PYP(M) under continuous illumination. The urea concentrations at the midpoint of denaturation were 5.26 +/- 0.29 and 3.77 +/- 0.19 M for PYP and PYP(M), respectively, in 100 mM acetate buffer, and 5.26 +/- 0.24 and 4.11 +/- 0.12 M for PYP and PYP(M), respectively, in 100 mM citrate buffer. The free energy change upon denaturation (DeltaG(D)(H2O)), obtained from the denaturation curve, was 11.0 +/- 0.4 and 7.6 +/- 0.2 kcal/mol for PYP and PYP(M), respectively, in acetate buffer, and 11.5 +/- 0.3 and 7.8 +/- 0.1 kcal/mol for PYP and PYP(M), respectively, in citrate buffer. Even though the DeltaG(D)(H2O) value for PYP(M) is almost identical in the two buffer systems, the urea concentration at the midpoint of denaturation is lower in acetate buffer than in citrate buffer. Although their CD spectra indicate that the protein conformations of the denatured states of PYP and PYP(M) are indistinguishable, the configurations of the chromophores in their denatured structures are not necessarily identical. Both denatured states are interconvertible through PYP and PYP(M). Therefore, the free energy difference between PYP and PYP(M) is 3.4-3.7 kcal/mol for the protein moiety, plus the additional contribution from the difference in configuration of the chromophore.     

Complex of human apolipoprotein C-1 with phospholipid: thermodynamic or kinetic stability?

Thermal unfolding of discoidal complexes of apolipoprotein (apo) C-1 with dimyristoyl phosphatidylcholine (DMPC) reveals a novel mechanism of lipoprotein stabilization that is based on kinetics rather than thermodynamics. Far-UV CD melting curves recorded at several heating/cooling rates from 0.047 to 1.34 K/min show hysteresis and scan rate dependence characteristic of slow nonequilibrium transitions. At slow heating rates, the apoC-1 unfolding in the complexes starts just above 25 degrees C and has an apparent melting temperature T(m) approximately 48 +/- 1.5 degrees C, close to T(m) = 51 +/- 1.5 degrees C of free protein. Thus, DMPC binding may not substantially increase the low apparent thermodynamic stability of apoC-1, DeltaG(25 degrees C) < 2 kcal/mol. The scan rate dependence of T(m) and Arrhenius analysis of the kinetic data suggest an activation enthalpy E(a) = 25 +/- 5 kcal/mol that provides the major contribution to the free energy barrier for the protein unfolding on the disk, DeltaG > or = 17 kcal/mol. Consequently, apoC-1/DMPC disks are kinetically but not thermodynamically stable. To explore the origins of this kinetic stability, we utilized dynode voltage measured in CD experiments that shows temperature-dependent contribution from UV light scattering of apoC-1/DMPC complexes (d approximately 20 nm). Correlation of CD and dynode voltage melting curves recorded at 222 nm indicates close coupling between protein unfolding and an increase in the complex size and/or lamellar structure, suggesting that the enthalpic barrier arises from transient disruption of lipid packing interactions upon disk-to-vesicle fusion. We hypothesize that a kinetic mechanism may provide a general strategy for lipoprotein stabilization that facilitates complex stability and compositional variability in the absence of high packing specificity.     

Peptide binding to lipid bilayers. Nonclassical hydrophobic effect and membrane-induced pK shifts.

The binding of the cyclic peptide (+)-D-Phe1-Cys2-Phe3-D-Trp4-(+)-Lys5-Thr6- Cys7-Thr(ol)8, a somatostatin analogue (SMS 201-995), and the potential-sensitive dye 2-(p-toluidinyl)naphthalene-6-sulfonate (TNS) to lipid membranes was investigated with high-sensitivity titration calorimetry. The binding enthalpy of the peptide was found to vary dramatically with the vesicle size. For highly curved vesicles with a diameter of d congruent to 30 nm, the binding reaction was enthalpy-driven with delta H congruent to -7.0 +/- 0.3 kcal/mol; for large vesicles with more tightly packed lipids, the binding reaction became endothermic with delta H congruent to +1.0 +/- 0.3 kcal/mol and was entropy-driven. In contrast, the free energy of binding was almost independent of the vesicle size. The thermodynamic analysis suggests that the observed enthalpy-entropy compensation of about 8 kcal/mol can be related to a change in the internal tension of the bilayer and is brought about by an entropy increase of the lipid matrix. The "entropy potential" of the membrane may have its molecular origin in the excitation of the hydrocarbon chains to a more disordered configuration and may play a more important role in membrane partition equilibria than the classical hydrophobic effect. The binding of the peptide to the membrane surface induced a pK shift of the peptide terminal amino group. Neutral membranes were found to destabilize the NH3+ group, leading to a decrease in pK; negatively charged membranes, generated an apparent increase in pK due to the increase in proton concentration near the membrane surface. No pK shifts were seen for TNS. Titration calorimetry combined with the Gouy-Chapman theory can be used to determine both the reaction enthalpy and the binding constant of the membrane-binding equilibrium.     

Folding of a de novo designed native-like four-helix bundle protein

The folding of a model native-like dimeric four-helix bundle protein, (alpha(2))(2), was investigated using guanidine hydrochloride, hydrostatic pressure, and low temperature. Unfolding by guanidine hydrochloride followed by circular dichroism and intrinsic fluorescence spectroscopy revealed a highly cooperative transition between the native-like and unfolded states, with free energy of unfolding determined from CD data, DeltaG(unf) = 14.3 +/- 0.8 kcal/mol. However, CD and intrinsic fluorescence data were not superimposable, indicating the presence of an intermediate state during the folding transition. To stabilize the folding intermediate, we used hydrostatic pressure and low temperature. In both cases, dissociation of the dimeric native-like (alpha(2))(2) into folded monomers (alpha(2)) was observed. van't Hoff analysis of the low temperature experiments, assuming a two-state dimer 171-monomer transition, yielded a free energy of dissociation of (alpha(2))(2) of DeltaG(diss) = 11.4 +/- 0.4 kcal/mol, in good agreement with the free energy determined from pressure dissociation experiments (DeltaG(diss) = 10.5 +/- 0.1 kcal/mol). Binding of the hydrophobic fluorescent probe 4,4'-dianilino-1,1'-binaphthyl-5,5'-disulfonic acid (bis-ANS) to the pressure- and cold-dissociated states of (alpha(2))(2) indicated the existence of molten-globule monomers. In conclusion, we demonstrate that the folding pathway of (alpha(2))(2) can be described by a three-state transition including a monomeric molten globule-like state.