Microcalorimetric method to determine competitive binding. Action of a psychotropic drug (dipotassium chlorazepate) on L-tryptophan . human serum albumin complex.

A mathematical treatment and an original microcalorimetric method are developed to verify an eventual competitive binding between any two substances for the same macromolecule. To apply this method, a competitive binding of L-tryptophan and one benzodiazepin (dipotassium chlorazepate) for human serum albumin is perfectly demonstrated. The association constants and the enthalpy variations are equal to 14 000 +/- 2000 M-1 and --6.6 +/- 0.2 kcal/mol for human serum albumin . tryptophan complex and 13 000 +/- 1000 M-1 and --10.0 +/- 0.2 kcal/mol for human serum albumin . chlorazepate complex. In all cases the stoichiometry is equal to one. The binding of tryptophan to human serum albumin is partially stereospecific; the association constant and the enthalpy variation for D-tryptophan complex are equal, respectively, to 1000 +/- 200 M-1 and --2.6 +/- 0.3 kcal/mol.     

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.     

Time-resolved thermodynamic profiles for CO photolsysis from the mixed valence form of bovine heart cytochrome c oxidase.

Photoacoustic calorimetry has been utilized to probe the thermodynamics accompanying photodissociation of the CO mixed valence form of bovine heart cytochrome c oxidase (COMV CcO). At pH's below 9 photolysis of the COMV CcO results in three kinetic phases with the first phase occurring faster than the time resolution of the instrument (i.e., < approximately 50 ns), a second phase occurring with a lifetime of approximately 100 ns and a third phase occurring with a lifetime of approximately 2 micros. The corresponding volume and enthalpy changes for these processes are: DeltaH1, DeltaV1 = +79 +/- 10 kcal mol(-1), +9 +/- 1 mL mol(-1); DeltaH2, DeltaV2 = -79 +/- 5 kcal mol(-1), -9 +/- 2 mL mol(-1); DeltaH3, DeltaV3 = +54 +/- 7 kcal mol(-1), +8 +/- 1 mL mol(-1). At pH's above 9 only one phase is observed, a prompt phase occurring in < 50 ns. The overall volume change is negligible above pH 9 and the enthalpy change is +29 +/- 5 kcal mol(-1). The data are consistent with the prompt phase being associated with CO-Fe(a3) bond cleavage, CO-CuB+ bond formation, Fe(a3) low-spin to high-spin transition and fast electron transfer (ET) from heme a3 to heme a followed by proton transfer from Glu242 to Arg38 on an approximately 100 ns timescale. The slow phase is likely a combination of CO thermal dissociation from CuB and additional ET between heme a3 to heme a. Interestingly, this phase is not evident above pH 9 suggesting linkage between CO dissociation/ET and the protonation state of a group or groups near the binuclear center.     

Thermodynamic analysis of inducer binding to the lactose repressor protein: contributions of galactosyl hydroxyl groups and beta substituents

Kinetic and equilibrium studies of the binding of modified beta-D-galactoside sugars to the lac repressor were carried out to generate thermodynamic data for protein-inducer interactions. The energetic contributions of the galactosyl hydroxyl groups to binding were assessed by using a series of methyl deoxyfluoro-beta-D-galactosides. The C-3 and C-6 hydroxyls contributed less than or equal to -2.3 and -1.7 +/- 0.3 kcal/mol to the binding free energy change, respectively, whereas the C-4 hydroxyl provided only a nominal contribution (-0.1 +/- 0.2 kcal/mol). Favorable contributions to the total binding free energy change were observed for replacement of O-methyl by S-methyl at the beta-anomeric position and for S-methyl by S-isopropyl. Negative delta H degrees values characteristic of protein-sugar complexes [Quiocho, F. A. (1986) Annu. Rev. Biochem. 55, 287-315] were observed for a series of beta-D-galactosides differing at the beta-glycosidic position. A decrease in delta H degrees of approximately 6 kcal/mol upon replacement of the O-methyl substituent by S-methyl indicates a substantial increase in van der Waals' interactions and/or hydrogen bonding in this region of the ligand binding site. The more favorable free energy change for the binding of the S-isopropyl vs S-methyl compound is due mainly to more positive entropic contributions, consistent with an increase in apolar interactions.(ABSTRACT TRUNCATED AT 250 WORDS)     

The promotion of collagen polymerization by lanthanide and calcium ions.

Ca2+ (1-5 mM) and lanthanide (20-250 microM) ions enhance the rate of polymerization of purified calf skin collagen (1.5 mg/ml) at pH 7.0 in the presence of 30mM-Tris/HCl and 0.2 M-NaCl. Both the nucleation phase and the growth phase of polymerization are accelerated. The activation energy of the growth phase, 239.3 +/- 24.3 kJ/mol (57.2 +/- 5.8 kcal/mol), is decreased to 145.6 +/- 9.6 kJ/mol (34.8 +/- 2.3 kcal/mol) by 5 mM-Ca2+ and to 75.3 +/- 4.6 kJ/mol (18.0 +/- 1.1 kcal/mol) by 25 microM-Sm3+. In contrast, the activation energy of the nucleation phase, 191.6 +/- 23.4 kJ/mol (45.8 +/- 5.6 kcal/mol), is only slightly decreased by Ca2+ or Sm3+. Collagen fibrils formed in the presence of Sm3+ are thinner than control fibrils, and more thermoresistant.     

Kinetics and thermodynamics of mandelate racemase catalysis

Mandelate racemase (EC 5.1.2.2) from Pseudomonas putida catalyzes the interconversion of the two enantiomers of mandelic acid with remarkable proficiency, producing a rate enhancement exceeding 15 orders of magnitude. The rates of the forward and reverse reactions catalyzed by the wild-type enzyme and by a sluggish mutant (N197A) have been studied in the absence and presence of several viscosogenic agents. A partial dependence on relative solvent viscosity was observed for values of kcat and kcat/Km for the wild-type enzyme in sucrose-containing solutions. The value of kcat for the sluggish mutant was unaffected by varying solvent viscosity. However, sucrose did have a slight activating effect on mutant enzyme efficiency. In the presence of the polymeric viscosogens poly(ethylene glycol) and Ficoll, no effect on kcat or kcat/Km for the wild-type enzyme was observed. These results are consistent with both substrate binding and product dissociation being partially rate-determining in both directions. The viscosity variation method was used to estimate the rate constants comprising the steady-state expressions for kcat and kcat/Km. The rate constant for the conversion of bound (R)-mandelate to bound (S)-mandelate (k2) was found to be 889 +/- 40 s(-1) compared with a value of 654 +/- 58 s(-1) for kcat in the same direction. From the temperature dependence of Km (shown to equal K(S)), k2, and the rate constant for the uncatalyzed reaction [Bearne, S. L., and Wolfenden, R. (1997) Biochemistry 36, 1646-1656], we estimated the enthalpic and entropic changes associated with substrate binding (DeltaH = -8.9 +/- 0.8 kcal/mol, TDeltaS = -4.8 +/- 0.8 kcal/mol), the activation barrier for conversion of bound substrate to bound product (DeltaH# = +15.4 +/- 0.4 kcal/mol, TDeltaS# = +2.0 +/- 0.1 kcal/mol), and transition state stabilization (DeltaH(tx) = -22.9 +/- 0.8 kcal/mol, TDeltaS(tx) = +1.8 +/- 0.8 kcal/mol) during mandelate racemase-catalyzed racemization of (R)-mandelate at 25 degrees C. Although the high proficiency of mandelate racemase is achieved principally by enthalpic reduction, there is also a favorable and significant entropic contribution.     

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.     

Use of MM-PB/SA in estimating the free energies of proteins: application to native, intermediates, and unfolded villin headpiece

We investigated the stability of three different ensembles of the 36-mer villin headpiece subdomain, the native, a compact folding intermediate, and the random coil. Structures were taken from a 1-micros molecular dynamics folding simulation and a 100-ns control simulation on the native structure. Our approach for each conformation is to first determine the solute internal energy from the molecular mechanics potential and then to add the change resulting from solvation (DeltaG(solv)). Explicit water was used to run the simulation, and a continuum model was used to estimate DeltaG(solv) with the finite difference Poisson-Boltzmann model accounting for the polarization part and a linearly surface area-dependent term for the non-polar part. We leave out the solute vibrational entropy from these values but demonstrate that there is no statistical difference among the native, folding intermediate, and random coil ensembles. We find the native ensemble to be approximately 26 kcal/mol more stable than the folding intermediate and approximately 39 kcal/mol more stable than the random coil ensemble. With an experimental estimate for the free energy of denaturation equal to 3 kcal/mol, we approximate the non-native degeneracy to lie between 10(16) and 10.(25) We also present a possible scheme for the mechanism of folding, first-order exponential decay of a putative transition state, with an estimate for the t(1/2) of folding of approximately 1 micros.     

Laser-induced time-resolved photoacoustic calorimetry study on photo-dissociation of human and bovine oxyhemoglobin

The dynamics of the enthalpy and volume changes related to the photo-dissociation of oxygen from human and bovine oxyhemoglobin are investigated by nanosecond time-resolved photoacoustic calorimetry (PAC). The values of enthalpy and volume change associated with the above process are deltaH = 37.8 +/- 3 kcal/mol, deltaV = 5.0 +/- 1 ml/mol for human HbO(2); and deltaH = 35.7 +/- 3.5 kcal/mol, deltaV = 4.8 +/- 1 ml/mol for bovine HbO(2), respectively. A possible explanation for the similar values between both human and bovine oxyhemoglobin is proposed. In addition, the PAC results for human HbO(2) and HbCO are compared and discussed.     

Ser45 plays an important role in managing both the equilibrium and transition state energetics of the streptavidin-biotin system

The contribution of the Ser45 hydrogen bond to biotin binding activation and equilibrium thermodynamics was investigated by biophysical and X-ray crystallographic studies. The S45A mutant exhibits a 1,700-fold greater dissociation rate and 907-fold lower equilibrium affinity for biotin relative to wild-type streptavidin at 37 degrees C, indicating a crucial role in binding energetics. The crystal structure of the biotin-bound mutant reveals only small changes from the wild-type bound structure, and the remaining hydrogen bonds to biotin retain approximately the same lengths. No additional water molecules are observed to replace the missing hydroxyl, in contrast to the previously studied D128A mutant. The equilibrium deltaG degrees, deltaH degrees, deltaS degrees, deltaC degrees(p), and activation deltaG++ of S45A at 37 degrees C are 13.7+/-0.1 kcal/mol, -21.1+/-0.5 kcal/mol, -23.7+/-1.8 cal/mol K, -223+/-12 cal/mol K, and 20.0+/-2.5 kcal/mol, respectively. Eyring analysis of the large temperature dependence of the S45A off-rate resolves the deltaH++ and deltaS++ of dissociation, 25.8+/-1.2 kcal/mol and 18.7+/-4.3 cal/mol K. The large increases of deltaH++ and deltaS++ in the mutant, relative to wild-type, indicate that Ser45 could form a hydrogen bond with biotin in the wild-type dissociation transition state, enthalpically stabilizing it, and constraining the transition state entropically. The postulated existence of a Ser45-mediated hydrogen bond in the wild-type streptavidin transition state is consistent with potential of mean force simulations of the dissociation pathway and with molecular dynamics simulations of biotin pullout, where Ser45 is seen to form a hydrogen bond with the ureido oxygen as biotin slips past this residue after breaking the native hydrogen bonds.     

Na+ and K+ binding by glycerinated muscle fibers at equal concentrations of the chlorides of these cations in the medium

The Na+ and K+ equilibrium distribution between the medium and glycerinated muscle fibres of the frog has been investigated under equal concentrations of NaCl and KCl in solutions. Concentrations of NaCl and KCl varied from 0.5-1.5 mkM till 50 mM. Ion strength (0.11) was constant owing to the imidazol--HCl buffer. The binding of Na+ and K+ by model fibres occurred in accordance with the Langmur equation. Two kinds of cation-binding sites were found. The one with a low limiting ion sorption (A infinity approximately 1.3 mmol/kg dry weight of fibres) and high affinities (-delta F0 approximately 4.3 kcal/mol) was saturated at 0.5 mM concentrations (Na+ = K+) in the medium, and the other--with A infinity exceeding the previous one by an order and low -delta F0 (2.5 kcal/mol) was discovered at Na+, K+-1-10 mM. At ion concentrations equal to 0.5-1 mM the Langmur-binding is disturbed. At Na+-K+ less than or equal to 1 mM Na+ bound:K+ bound approximately to 1:1. At higher concentrations of cations Na+ bound:K+ bound approximately equal to 3:2. It is concluded that at least part of the sites in model fibres is capable of interacting only with Na+, but not with K+. It is supposed that at equal concentrations of Na+ and K+ in the medium the cations are bound by Na+, K+-ATPase of glycerinated muscle fibres.     

In vivo non-specific binding of lambda CI and Cro repressors is significant

We propose a thermodynamic model that includes the non-specific binding of the lambda phage regulatory proteins CI and Cro. By fitting the model to experimental in vivo data on activities of the two promoters P(RM) and P(R) versus concentration, we estimate the free energy upon non-specific binding to be -4.1+/-0.9 kcal/mol for CI and -4.2+/-0.8 kcal/mol for Cro. For concentrations >100 nM of CI or Cro, we find that >50% of these proteins are non-specifically bound. In particular, in a lysogen (approximately 250 CI monomeric equivalents per cell) nearly 90% of CI is non-specifically bound.     

The vnd/NK-2 homeodomain: thermodynamics of reversible unfolding and DNA binding for wild-type and with residue replacements H52R and H52R/T56W in helix III

The conformational stabilities of the vnd (ventral nervous system defective)/NK-2 homeodomain [HD(wt); residues 1-80 that encompass the 60-residue homeodomain] and those harboring mutations in helix III of the DNA recognition site [HD(H52R) and HD(H52R/T56W)] have been investigated by differential scanning calorimetry (DSC) and ellipticity changes at 222 nm. Thermal unfolding reactions at pH 7.4 are reversible and repeatable in the presence of 50-500 mM NaCl with DeltaC(p) = 0.52 +/- 0.04 kcal K(-1) mol(-1). A substantial stabilization of HD(wt) is produced by 50 mM phosphate or by the addition of 100-500 mM NaCl to 50 mM Hepes, pH 7.4, buffer (from T(m) = 35.5 degrees C to T(m) 43-51 degrees C; DeltaH(vH) congruent with 47 +/- 5 kcal mol(-1)). The order of stability is HD(H52R/T56W) > HD(H52R) > HD(wt), irrespective of the anions present. Progress curves for ellipticity changes at 222 nm as a function of increasing temperature are fitted well by a two-state unfolding model, and the cooperativity of secondary structure changes is greater for mutant homeodomains than for HD(wt) and also is increased by adding 100 mM NaCl to Hepes buffer. A 33% quench of the intrinsic tryptophanyl residue fluorescence of HD(wt) by phosphate binding (K(D)' = 2.6 +/- 0.3 mM phosphate) is reversed approximately 60% by DNA binding. Thermodynamic parameters for vnd/NK-2 homeodomain proteins binding sequence-specific 18 bp DNA have been determined by isothermal titration calorimetry (10-30 degrees C). Values of DeltaC(p) are +0.25, -0.17, and -0.10 +/- 0.04 kcal K(-1) mol(-1) for HD(wt), HD(H52R), and HD(H52R/T56W) binding duplex DNA, respectively. Interactions of homeodomains with DNA are enthalpically controlled at 298 K and pH 7.4 with corresponding DeltaH values of -6.6 +/- 0.5, -10.8 +/- 0.1, and -9.0 +/- 0.6 kcal mol(-1) and DeltaG' values of -11.0 +/- 0.1, -11.0 +/- 0.1, and -11.3 +/- 0.3 kcal mol(-1) with a binding stoichiometry of 1.0 +/- 0.1. Thermodynamic parameters for DNA binding are not predicted from homeodomain structural changes that occur upon complexing to DNA and must reflect also solvent and possibly DNA rearrangements.     

Tryptophan-47 rotational isomerization in variant-3 scorpion neurotoxin. A combination thermodynamic perturbation and umbrella sampling study.

A combination thermodynamic perturbation and umbrella sampling study predicts two free energy wells for the rotational isomerization of the variant-3 scorpion neurotoxin tryptophan-47 indole side chain. One well has the indole side chain in the crystallographic orientation; the other has the indole rotated approximately 220 degrees to form a new conformation with a relative free energy of 3 +/- 2 kcal/mol. The activation barrier is 8.5 kcal/mol from the crystallographic well, from which transition state theory predicts a rate of escape of 2 x 10(5) s-1. Correlations in the displacements of side chains neighboring tryptophan-47 and the isomerization reaction coordinate last up to 20 ps. Favorable conditions of experimental verification are discussed.     

Ab initio modeling of glycosyl torsions and anomeric effects in a model carbohydrate: 2-ethoxy tetrahydropyran

A range of ab initio calculations were carried out on the axial and equatorial anomers of the model carbohydrate 2-ethoxy tetrahydropyran to evaluate the level of theory required to accurately evaluate the glycosyl dihedral angle and the anomeric ratio. Vacuum CCSD(T)/CBS extrapolations at the global minimum yield DeltaE = E(equatorial) - E(axial) = 1.42 kcal/mol. When corrected for solvent (by the IEFPCM model), zero-point vibrations and entropy, DeltaG(298) = 0.49 kcal/mol, in excellent agreement with the experimental value of 0.47 +/- 0.3 kcal/mol. A new additivity scheme, the layered composite method (LCM), yields DeltaE to within 0.1 kcal/mol of the CCSD(T)/CBS result at a fraction of the computer requirements. Anomeric ratios and one-dimensional torsional surfaces generated by LCM and the even more efficient MP2/cc-pVTZ level of theory are in excellent agreement, indicating that the latter is suitable for force-field parameterization of carbohydrates. Hartree-Fock and density functional theory differ from CCSD(T)/CBS for DeltaE by approximately 1 kcal/mol; they show similar deviations in torsional surfaces evaluated from LCM. A comparison of vacuum and solvent-corrected one- and two-dimensional torsional surfaces indicates the equatorial form of 2-ethoxy tetrahydropyran is more sensitive to solvent than the axial.     

Relationship between lipid fluidity and water permeability of bovine tracheal epithelial cell apical membranes

Apical membrane vesicles were prepared from bovine tracheal epithelial cells. These membranes were enriched in alkaline phosphatase specific activity 35-fold compared to cellular homogenates. Steady-state fluorescence polarization studies of these membranes, using three fluorophores, demonstrated that they possessed a relatively low fluidity. Studies using the probe 1,6-diphenyl-1,3,5-hexatriene detected thermotropic transitions at 25.7 +/- 0.4 and 26.8 +/- 0.6 degrees C in these membranes and their liposomes, respectively. Analysis of the composition of these membranes revealed a fatty acyl saturation index of 0.59 +/- 0.02, a protein/lipid ratio (w/w) of 0.60 +/- 0.06, a cholesterol/phospholipid ratio (mol/mol) of 0.83 +/- 0.11, and a sphingomyelin/lecithin ratio (mol/mol) of 0.64 +/- 0.10. Membrane vesicles were osmotically active when studied by a stopped-flow nephelometric technique. Arrhenius plots of rates of osmotic water efflux demonstrated break points at approximately 28 and 18 degrees C, with activation energies of 16.7 +/- 0.2 kcal mol-1 from 35 to 28 degrees C, 8.3 +/- 0.5 kcal mol-1 from 28 to 18 degrees C, and approximately 3.0 kcal mol-1 below 18 degrees C. Treatment of membrane vesicles with benzyl alcohol, a known fluidizer, decreased lipid order (increased fluidity) and increased the rate of osmotic water efflux. The present results suggest that water crosses tracheal epithelial cell apical membranes by solubility-diffusion across the lipid domain and that increases in fluidity correlate with increases in the water permeability of these membranes.     

Thermodynamic and base-pairing studies of matched and mismatched DNA dodecamer duplexes containing cis-syn, (6-4) and Dewar photoproducts of TT.

Cis-syn dimers, (6-4) products and their Dewar valence isomers are the major photoproducts of DNA and have different mutagenic properties and rates of repair. To begin to understand the physical basis for these differences, the thermal stability and base pairing properties of the corresponding photoproducts of the TT site in d(GAGTATTATGAG) were investigated. The (6-4) and Dewar products destabilize the duplex form by approximately 6 kcal/mol of free energy at 37 degreesC relative to the parent, whereas a cis-syn dimer only destabilizes the duplex form by 1.5 kcal/mol. Duplexes with G opposite the 3'-T of the (6-4) and Dewar products are more stable than those with A by approximately 0.4 kcal/mol, whereas the cis-syn dimer prefers A over G by 0.7 kcal/mol. Proton NMR suggests that wobble base pairing takes place between the 3'-T of the cis-syn dimer and an opposed G, whereas there is no evidence of significant H-bonding between these two bases in the (6-4) product. The thermodynamic and H-bonding data for the (6-4) product are consistent with a 4 nt interior loop structure which may facilitate flipping of the photoproduct in and out of the helix.     

Thermodynamic and structural characterization of Asn and Ala residues in the disallowed II' region of the Ramachandran plot

Residue Asn47 at position L1 of a type II' beta-turn of the alpha-spectrin SH3 domain is located in a disallowed region of the Ramachandran plot (phi = 56 +/- 12, psi = -118 +/- 17). Therefore, it is expected that replacement of Asn47 by Gly should result in a considerable stabilization of the protein. Thermodynamic analysis of the N47G and N47A mutants shows that the change in free energy is small (approximately 0.7 kcal/mol; approximately 3 kJ/mol) and comparable to that found when mutating a Gly to Ala in a alpha-helix or beta-sheet. X-ray structural analysis of these mutants shows that the conformation of the beta-turn does not change upon mutation and, therefore, that there is no relaxation of the structure, nor is there any gain or loss of interactions that could explain the small energy change. Our results indicate that the energetic definition of II' region of the Ramachandran plot (phi = 60 +/- 30, psi = -115 +/- 15) should be revised for at least Ala and Asn in structure validation and protein design.     

Response of murine bone marrow granulocyte-macrophage colony-forming units to hyperthermia in situ

A detailed understanding of how bone marrow stem cell progenitors are affected by heat is prerequisite to predicting how whole-body or regional hyperthermia protocols may affect bone marrow function. This investigation reports the reproductive integrity of murine tibial bone marrow granulocyte-macrophage colony-forming units (CFU-GM) after in situ hyperthermia. Heat was applied by water bath immersion of the leg of male BALB/c mice anesthetized with 90 mg/kg pentobarbital given subcutaneously. Tibial and rectal temperatures were monitored in representative animals by microthermocouples (tip diameter approximately 100 microns). By approximately 3 min after immersion of the limb, marrow temperature was within 0.3 degree C of water bath temperature (O'Hara et al., Int. J. Hyperthermia 5, 589-601, 1989) and was within 0.1 degree C by 5 min after immersion. The CFU-GM were cultured in "lung-conditioned" McCoy's 5A medium supplemented with 15% fetal calf serum and 0.3% Bacto agar. In situ heating of tibial marrow to exposure temperatures of 42, 42.5, 43, 44, and 45 degrees C gave D0's (+/- 95% CI) of 91 +/- 44, 44 +/- 27, 27 +/- 2.2, 16 +/- 6, and 7 +/- 4 min, respectively. Heating to 41.5 degrees C for up to 180 min did not result in cytotoxicity. Development of thermotolerance after approximately 100 min of heating was apparent by the presence of a "resistant tail" of the 42 degrees C survival curve. A plot of D0 vs water bath temperature was bimodal with an inflection point at approximately 42.5 degrees C. The inactivation enthalpy for temperatures above 42.5 degrees C was 586 kJ/mol (140 kcal/mol) and for temperatures below 42.5 degrees C was estimated to be 1205 kJ/mol (288 kcal/mol). These results show that CFU-GM can be heated predictably in situ, can be inactivated with thermal exposures as low as 42 degrees C, and are capable of developing thermotolerance. These findings underscore the necessity to understand stem cell inactivation by hyperthermia in situ prior to widespread implementation of clinical hyperthermia protocols where bone marrow may be included in the treatment field.