Reversible unfolding of the major fraction of ovalbumin by guanidine hydrochloride

The guanidine hydrochloride induced unfolding of the major fraction of ovalbumin (i.e. A1 which contains two phosphate groups and constitutes about 77% of the total protein) was investigated systematically by difference spectran and viscosity measurements. As judged by the intrinsic viscosity (3.9 ml/g), the native protein conformation is compact and globular. Difference spectral results showed extensive disruption of the native structure by guanidine hydrochloride with and without 0.1 M beta-mercaptoethanol were 31.1 and 27.0 ml/g. These and optical rotation results indicated that the denatured protein existed in a cross-linked random coil conformation in 6 M guanidine hydrochloride alone. Strikingly, in contrast to whole ovalbumin, the denaturation of its A1 fraction by guanidine hydrochloride was fully reversible and obeyed first-order kinetic law under different experimental condit ions of pH, temperature, and the denaturant concentration. The monotonic variation of deltaH for the unfolding of ovalbumin A1 by guanidine hydrochloride with temperature, the coincidence of the two transition curves obtained by measuring two independent properties (namely reduced viscosity and difference in light absorption at 288 nm (or 293 nm) as a function of the denaturant concentration, and finally the adherence of the unfolding as well as refolding reactions to first-order kinetic law suggested that the transition of ovalbumin. A1 can reasonably be approximated by a two-state mode. Analysis of the equilibrium data obtained at pH 7.0 and 25 degrees C according to Aune and Tanford (Aune, K.C.,and Tanford, C. (1969), Biochemistry 8, 4586) showed that 12 additional binding sites for the denaturant with an association constant of 1.12 were freshly exposed by the unfolding process and that the native protein was marginally more stable (approximately 6 kcal/mol) than its unfolded form even under native condition. The temperature dependence of the equilibrium constant for the unfolding of ovalbumin A1 by guanidine hydrochloride which was studied in the range 10-60 degrees C at pH 7.0 can be described by assigning the following values of the thermodynamic parameters for the unfolding process: deltaH = 52 kcal/mol at 25 degrees C; deltaS = 153 cal deg-1 mol-1 at 25 degrees C; and delta Cp = 2700 +/- 400 cal deg-1 mol-1.     

Thermodynamic analysis of human plasma apolipoprotein C-1: high-temperature unfolding and low-temperature oligomer dissociation

Thermal and chemical unfolding of lipid-free apolipoprotein C-1 (apoC-1), a 6-kDa protein component of very low density and high-density lipoproteins, was analyzed by far-UV CD. In neutral 1 mM Na2HPO4 solutions containing 6-7 micrograms/mL protein, the apoC-1 monomer is approximately 30% alpha-helical at 0-22 degrees C and unfolds reversibly from about 22-80 degrees C with Tm = 51 +/- 3 degrees C and van't Hoff enthalpy delta Hv(Tm) = 19 +/- 3 kcal/mol. The apparent free energy of the monomer stabilization determined from the chemical unfolding at 0 degree C, delta G(0 degree C) = 2.8 +/- 0.8 kcal/mol, decreases by about 1 kcal/mol upon heating to 25 degrees C. A small apparent heat capacity increment suggests the absence of a substantial hydrophobic core for the apoC-1 molecule. At pH 7, increasing apoC-1 concentration above 10 micrograms/mL leads to self-association and formation of additional alpha-helices that unfold upon both heating and cooling from room temperature. The CD data indicate that the high-temperature transition reflects a complete monomer unfolding and the low-temperature transition reflects oligomer dissociation into stable monomers. This suggests the importance of hydrophobic interactions for apoC-1 self-association. Close proximity between the high- and low-temperature transitions and the absence of a plateau in the chemical unfolding curves recorded from oligomeric apoC-1 indicate marginal oligomer stability and suggest that in vivo apoC-1 transfer is mediated via the complexes with other apolipoproteins and/or lipids.     

Effect of peptide binding on amide proton exchange rates in the PDZ2 domain from human phosphatase hPTP1E

Amide hydrogen-deuterium exchange rates were measured in the PDZ2 domain from human phosphatase hPTPIE by 1H-15N heteronuclear NMR spectroscopy. Protection factors were calculated for the slowly exchanging hydrogens in both the free PDZ2 domain and its complex with an octapeptide peptide, R-N-E-I-Q-S-L-V, derived from the C-terminus of the Fas receptor. Aside from a short alpha-helical region alpha1 (amino acids A-45 to D-49), the pattern of highly protected amides correlated well with the presence of hydrogen bonds in elements of the secondary structure. Hydrogen-bonded amides showed relatively fast exchange rates with half-lives of less than 9 h at pD 7.6 and 8 degrees C. Protection factors, calculated as the ratio of theoretical (denatured) and observed exchange rates, showed less dispersion in maximal values than did the actual exchange rates. This behavior and the large pH dependence of the exchange rates suggest that amide exchange is close to the EX2 limit. In this limit, exchange of the most protected amides occurs through a global unfolding mechanism. The free energy of the unfolding calculated from the largest protection factors is 4.8 +/- 0.4 kcal/mol (1 cal = 4.184 J). This deltaG(o) closely matches the value measured by experiments with guanidine hydrochloride and fluorescence emission spectroscopy. Peptide binding to PDZ2 resulted in mostly global effects and stabilized the folded domain by 1.4 kcal/mol.     

Differential inhibition of lysophosphatidate signaling by volatile anesthetics

cAMP receptor protein (CRP) is involved in regulation of expression of several genes in Escherichia coli. The protein is a homodimer and each monomer is folded into two distinct structural domains. The mechanism of the biological activity of the protein may involve the interaction between the subunits and domains. In order to determine the interaction between the subunits or domains of CRP, we have studied the reversible denaturation of the protein by guanidine hydrochloride. The unfolding and refolding kinetics of CRP was monitored using stopped-flow fluorescence spectroscopy at 20 degrees C and pH 7.9. The results of CRP denaturation indicate that the transition can be described by a three-state model: (CRP native)2<=> 2 (CRP native)<=>2 (CRP denatured). The faster process, characterized by the relaxation time tau 2 = 80 +/- 3 ms, corresponds to the dissociation of CRP dimer into monomers. The slower process has the relaxation time tau t = 1.9 +/- 0.1 s and corresponds to the cooperative unfolding of CRP monomer. The free energy change in the absence of denaturant upon CRP dissociation is delta G dis degrees = 46.9 +/- 2.5 kJ/mol and for monomer unfolding delta G unf degrees = 30.9 +/- 1.3 kJ/mol. The thermal unfolding of CRP was studied by circular dichroism and fluorescence spectroscopy at various guanidine hydrochloride concentrations. It has been found that the native protein is maximally stable at about 21 +/- 0.3 degrees C and is denatured upon heating and cooling from this temperature. The apparent free energy change for CRP unfolding at 21 degrees C is equal to 30.5 +/- 0.4 kJ/mol and the apparent specific heat change is equal to delta Cp, app = 10.7 +/- 0.7 kJ mol-1 K-1. The predicted values of cold denaturation midpoint is equal to tau G = -18.8 +/- 1.5 degrees C and for high-temperature transition tau G = 63.1 +/- 1.5 degrees C. The predicted midpoint of high-temperature unfolding transition is about the same as determined experimentally.     

Analysis of the reaction coordinate of photosynthetic water oxidation by kinetic measurements of 355 nm absorption changes at different temperatures in photosystem II preparations suspended in either H2O or D2O

Flash-induced absorption changes at 355 nm were measured at different temperatures within the range of 2 degrees C S2) = 14 kJ/mol, EA(S2-->S3) = 35 kJ/mol, and EA(S3-->-->S0 + O2) = 21 kJ/mol for theta > 11 degrees C, 67 kJ/mol for theta < 11 degrees C in PS II core complexes dissolved in H2O; (b) replacement of exchangeable protons by deuterons causes only minor changes ( S2, S2 --> S3, and S3 -->--> S0 + O2, respectively. The corresponding values of PS II membrane fragments are 1.3, 1.3, and 1. 4. Based on these results and corresponding EA data reported in the literature for PS II membrane fragments from spinach [Renger, G., & Hanssum, B. (1992) FEBS Lett. 299, 28-32] and PS II particles from the thermophilic cyanobacterium Synechococcus vulcanus Copeland [Koike, H., Hanssum, B., Inoue, Y., & Renger, G. (1987) Biochim. Biophys. Acta 893, 524-533], the reaction coordinate of the redox sequence in the WOC is inferred to be almost invariant to the evolutionary development from cyanobacteria to higher plants. Furthermore, the rather high activation energy of the S2 --> S3 transition provides evidence for a significant structural change coupled with this reaction. Implications for the mechanism of photosynthetic water oxidation are discussed.     

Structure and stability of an immunoglobulin superfamily domain from twitchin, a muscle protein of the nematode Caenorhabditis elegans

The NMR solution structure of an immunoglobulin superfamily module of twitchin (Ig 18') has been determined and the kinetic and equilibrium folding behaviour characterised. Thirty molecular coordinates were calculated using a hybrid distance geometry-simulated annealing protocol based on 1207 distance and 48 dihedral restraints. The atomic rms distributions about the mean coordinate for the ensemble of structures is 0.55( +/- 0.09) A for backbone atoms and 1.10( +/- 0.08) A for all heavy atoms. The protein has a topology very similar to that of telokin and the titin Ig domains and thus it falls into the I set of the immunoglobulin superfamily. The close agreement between the predicted and observed structures of Ig 18' demonstrates clearly that the I set profile can be applied in the structure prediction of immunoglobulin-like domains of diverse modular proteins. Folding studies reveal that the protein has relatively low thermodynamic stability, deltaG(H2O)U-F = 4.0 kcal mol(-1) at physiological pH. Unfolding studies suggest that the protein has considerable kinetic stability, the half life of the unfolding is greater than 40 minutes in the absence of denaturant.     

Introduction of a proline residue into position 31 of the loop of the dimeric 4-alpha-helical protein ROP causes a drastic destabilization

The exchange of an alanine with a proline residue in position 31 of the loop region of the dimeric 4-alpha-helical-bundle protein ROP causes a reduction in the alpha-helix content of 7% and a reduction in stability of about 40% compared to the wild type parameters. The Gibbs energy of unfolding by denaturants extrapolated linearly to zero denaturant concentration, delta G0D (buffer, 25 degrees C), has been determined to be 43 kJ (mol dimer)-1. The corresponding ROPwt value is 72 kJ (mol dimer)-1 (Steif et al., 1993). The extrapolated delta G0D values obtained from urea and GdmHCI un- and refolding studies are identical within error limits. Deconvolution of the stability values into enthalpy and entropy terms resulted in the following parameters. At T1/2 = 43 degrees C (Cprotein = 0.05 mg.ml-1) the ROP A31P mutant is characterized by delta Hv.H.0 = 272 kJ (mol dimer)-1, delta Cp = 7.2 kJ (mol dimer)-1 K-1, delta S0 = 762 J (mol dimer)-1 K-1. These parameters are only approximately 50% as large as the corresponding values of ROPwt. We assume that the significant reduction in stability reflects the absence of at least one hydrogen bond as well as deformation of the protein structure. This interpretation is supported by the reduction in the change in heat capacity observed for the A31P mutant relative to ROPwt, by the increased aggregation tendency of the mutant and by the reduced specific CD absorption at 222 nm. All results support the view that in the case of ROP protein the loop region plays a significant role in the maintenance of native structure and conformational stability.     

Chemical denaturation: potential impact of undetected intermediates in the free energy of unfolding and m-values obtained from a two-state assumption

The chemical unfolding transition of a protein was simulated, including the presence of an intermediate (I) in equilibrium with the native (N) and unfolded (U) states. The calculations included free energies of unfolding, DeltaGuw, in the range of 1.4 kcal/mol to 10 kcal/mol and three different global m-values. The simulations included a broad range of equilibrium constants for the N left arrow over right arrow I process. The dependence of the N <--> I equilibrium on the concentration of denaturant was also included in the simulations. Apparent DeltaGuw and m-values were obtained from the simulated unfolding transitions by fitting the data to a two-state unfolding process. The potential errors were calculated for two typical experimental situations: 1) the unfolding is monitored by a physical property that does not distinguish between native and intermediate states (case I), and 2) the physical property does not distinguish between intermediate and unfolded states (case II). The results obtained indicated that in the presence of an intermediate, and in both experimental situations, the free energy of unfolding and the m-values could be largely underestimated. The errors in DeltaGuw and m-values do not depend on the m-values that characterize the global N <--> U transition. They are dependent on the equilibrium constant for the N <--> I transition and its characteristic m1-value. The extent of the underestimation increases for higher energies of unfolding. Including no random error in the simulations, it was estimated that the underestimation in DeltaGuw could range between 25% and 35% for unfolding transitions of 3-10 kcal/mol (case I). In case II, the underestimation in DeltaGuw could be even larger than in case I. In the same energy range, a 50% error in the m-value could also take place. The fact that most of the mutant proteins are characterized by both a lower m-value and a lower stability than the wild-type protein suggests that in some cases the results could have been underestimated due to the application of the two-state assumption.     

Recognition between disordered states: kinetics of the self-assembly of thioredoxin fragments

The disordered N- (1-73) and C- (74-108) fragments of oxidized Escherichia colithioredoxin (Trx) reconstitute the native structure upon association [Tasayco, M. L., & Chao, K. (1995) Proteins: Struct., Funct., Genet. 22, 41-44]. Kinetic measurements of the formation of the complex (1-73/74-108) at 20 degrees C under apparent pseudo-first-order conditions using stopped-flow far-UV CD and fluorescence spectroscopies indicate association coupled to folding, an apparent rate constant of association [kon = (1330 +/- 54) M-1 s-1], and two apparent unimolecular rate constants [k1 = (0. 037 +/- 0.007) s-1 and k2 = (0.0020 +/- 0.0005) s-1]. The refolding kinetics of the GuHCl denatured Trx shows the same two slowest rate constants. An excess of N- over C-fragment decreases the kon, and the slowest phase disappears when a P76A variant is used. Stopped-flow fluorescence measurements at 20 degrees C indicate a GuHCl-dependent biphasic dissociation/unfolding process of the complex, where the slowest phase corresponds to 90% of the total. Their rate constants, extrapolated to zero denaturant, k-1 = (9 +/- 3) x 10(-5) s-1 and k-2 = (3.4 +/- 1.2) x 10(-5) s-1, show m# values of (4.0 +/- 0.4) kcal mol-1 M-1 and (3.5 +/- 0.1) kcal mol-1 M-1, respectively. Our results indicate that: (i) a compact intermediate with trans P76 and defined tertiary structure seems to participate in both the folding and unfolding processes; (ii) not all the N-fragment is competent to associate with the C-fragment; (iii) conversion to an association competent form occurs apparently on the time scale of P76 isomerization; and (iv) the P76A variation does not alter the association competency of the C-fragment, but it permits its association with "noncompetent" forms of the N-fragment.     

Watson-Crick base-pairing properties of bicyclo-DNA

A series of sequences of the DNA analog bicyclo-DNA, 6-12 nucleotides in length and containing all four natural nucleobases, were prepared and their Watson-Crick pairing properties with complementary RNA and DNA, as well as in its own series, were analyzed by UV-melting curves and CD-spectroscopy. The results can be summarized as follows: bicyclo-DNA forms stable Watson-Crick duplexes with complementary RNA and DNA, the duplexes with RNA generally being more stable than those with DNA. Pyrimidine-rich bicyclo-DNA sequences form duplexes of equal or slightly increased stability with DNA or RNA, whereas purine-rich sequences show decreased affinity to complementary DNA and RNA when compared with wild-type (DNA-DNA, DNA-RNA) duplexes. In its own system, bicyclo-DNA prefers antiparallel strand alignment and strongly discriminates for base mismatches. Duplexes are always inferior in stability compared with the natural ones. A detailed analysis of the thermodynamic properties was performed with the sequence 5'-GGATGGGAG-3'x 5'-CTCCCATCC-3' in both backbone systems. Comparison of the pairing enthalpy and entropy terms shows an enthalpic advantage for DNA association (delta deltaH = -18 kcal x (mol)-1)) and an entropic advantage for bicyclo-DNA association (delta deltaS = 49 cal x K(-1) x mol(-1), leading to a delta deltaG 25 degrees C of -3.4 kcal x mol(-1) in favor of the natural duplex. The salt dependence of Tm for this sequence is more pronounced in the case of bicyclo-DNA due to increased counter ion screening from the solvent. Furthermore bicyclo-DNA sequences are more stable towards snake venom phosphodiesterase by a factor of 10-20, and show increased stability in fetal calf serum by a factor of 8 compared with DNA.     

Conformation and unfolding thermodynamics of epidermal growth factor and derivatives

Mouse submaxillary epidermal growth factor (EGF) is a 53-residue single chain peptide hormone of known amino acid sequence which contains three disulfides, five tyrosines, and two tryptophans. Circular dichroic (CD) spectra have been obtained and resolved for EGF, several well-characterized chemical and enzymic derivatives, and related low molecular weight model compounds. Assignments have been made to most of the resolved bands; these include the peptide, aromatic, and disulfide chromophores. From a comparison of the rotational strength of the 213-nm resolved CD band in native EGF with that of standard proteins, EGF is estimated to contain about 22% beta structure and no alpha helicity. A derivative of EGF lacking the five carboxyl-terminal residues (prepared by limited trypsin digestion) and the cyanogen bromide derivative, in which there is a single main-chain cleavage at residue 21, have spectra properties indicative of approximately 10 and 12% beta structure, respectively. The near-ultraviolet CD spectra of the derivatives are similar to, albeit not identical with, that of EGF. The rotational strengths characteristic of the side-chain chromophores in EGF and these derivatives are several-fold higher than the corresponding values in low molecular weight model compounds. Thus, it appears that EGF and these modified forms contain a stable (and similar) tertiary structure. In contrast, the S-aminoethylated derivative of EGF exhibits a drastically altered CD spectrum relative to EGF indicating a different conformation(s). Equilibrium studies on the guanidinium hydrochloride (GdmCl) mediated reversible unfolding of EGF showed that the transition midpoint is quite high (i.e., 6.89 M GdmCl at 25.0 degrees C), thus, indicating considerable stability. From these data a rough estimate of 16 kcal/mol can be made for the unfolding free energy (delta G degrees) of EGF in the absence of denaturant. Interestingly, EGF exhibits greater stability characteristics than several proteins two to four times its size. The cyanogen bromide derivative of EGF exhibited greatly reduced stability characteristics, e.g., the transition midpoint occurred at 4.19 M GdmCl (25.0 degrees C) and delta G degrees was estimated to be approximately 4 kcal/mol. Thus, a single main-chain cleavage reduced the stability of EGF by about 70%. Thermal transitions of EGF and the cyanogen bromide derivative in the presence of concentrated GdmCl are characterized by a relatively high enthalpy of about 25 kcal/mol at 40 degrees C and a low (probably zero) heat capacity. From these thermodynamic parameters one can calculate that the large reduction in delta G degrees due to scission of the single peptide bond between residues 21 and 22 can be attributed almost completely to a change in entropy; e.g., at 40 degrees C the apparent entropy of unfolding of EGF is 20.4 cal mol-1 deg-1 while that of the cyanogen bromide derivative is 66.4 cal mol-1 deg-1.     

Thermal unfolding of dodecameric glutamine synthetase: inhibition of aggregation by urea

Thermal unfolding of dodecameric manganese glutamine synthetase (622,000 M(r)) at pH 7 and approximately 0.02 ionic strength occurs in two observable steps: a small reversible transition (Tm approximately 42 degrees C; delta H approximately equal to 0.9 J/g) followed by a large irreversible transition (Tm approximately 81 degrees C; delta H approximately equal to 23.4 J/g) in which secondary structure is lost and soluble aggregates form. Secondary structure, hydrophobicity, and oligomeric structure of the equilibrium intermediate are the same as for the native protein, whereas some aromatic residues are more exposed. Urea (3 M) destabilizes the dodecamer (with a tertiary structure similar to that without urea at 55 degrees C) and inhibits aggregation accompanying unfolding at < or = 0.2 mg protein/mL. With increasing temperature (30-70 degrees C) or incubation times at 25 degrees C (5-35 h) in 3 M urea, only dodecamer and unfolded monomer are detected. In addition, the loss in enzyme secondary structure is pseudo-first-order (t1/2 = 1,030 s at 20.0 degrees C in 4.5 M urea). Differential scanning calorimetry of the enzyme in 3 M urea shows one endotherm (Tmax approximately 64 degrees C; delta H = 17 +/- 2 J/g). The enthalpy change for dissociation and unfolding agrees with that determined by urea titrations by isothermal calorimetry (delta H = 57 +/- 15 J/g; Zolkiewski M, Nosworthy NJ, Ginsburg A, 1995, Protein Sci 4: 1544-1552), after correcting for the binding of urea to protein sites exposed during unfolding (-42 J/g). Refolding and assembly to active enzyme occurs upon dilution of urea after thermal unfolding.     

Thermal denaturation of Escherichia coli thioredoxin studied by hydrogen/deuterium exchange and electrospray ionization mass spectrometry: monitoring a two-state protein unfolding transition

Thermally denatured oxidized Escherichia coli thioredoxin (TRX) in 2% acetic acid was examined by electrospray ionization mass spectrometry (ESI-MS) and circular dichroism. Conformational dynamics during thermal unfolding were probed by hydrogen/deuterium (H/D) exchange-in experiments. ESI-MS was used to determine the H/D ratios. TRX shows only a marginal change in negative ellipticity at 222 nm during thermal unfolding, but in the near-UV circular dichroism (240-350 nm) a clear transition is observed (Tm = 61 degrees C), and unfolding goes to completion. ESI mass spectra were recorded as a function of temperature, and the observed bimodal charge state distributions were analyzed assuming a two-state unfolding mechanism which allowed an estimation of the midpoint temperature, Tm = 64 degrees C. Under conditions at which the compact, folded conformational state is only marginally stable (80 degrees C, 2% acetic acid-d1), H/D exchange-in experiments in combination with ESI-MS resulted in mass spectra differing in the number of incorporated deuteriums which indicates the presence of two distinct populations of molecules after short incubation periods. As the exchange-in time increases, the population representing the unfolded state increases and the population which is protected against exchange decreases. The rate of conversion was used to estimate the rate constant of unfolding which was 2.1 +/- 0.2 min-1. The results presented here indicate that thermally denatured TRX under the conditions used may represent a collapsed unfolded state with properties often attributed to molten globule-like states, such as pronounced secondary structure but absence of rigid tertiary structure and, hence, lack of protection against H/D exchange.     

The mechanism of tubulin-colchicine recognition--a kinetic study of the binding of a bicyclic colchicine analogue with a minor modification of the A ring

2-Methoxy-5-(2',3',4'-trimethoxy)-2,4,6-cycloheptatrien-1-one (MTC) is a colchicine analogue that lacks the B ring. 2-Methoxy-5-(2',4'-dimethoxyphenyl)-2,4,6-cycloheptatrien-1-one (MD) is an A-ring analogue of MTC, in which one methoxy group is replaced by a hydrogen atom. This paper describes the kinetic features of MDC binding to tubulin, and compares its behaviour with MTC to analyse the effect of the A-ring modification on the recognition process by tubulin. Binding is accompanied by a strong enhancement of MDC fluorescence and quenching of protein fluorescence. The kinetic and thermodynamic parameters were obtained from fluorescence stopped-flow measurements. The kinetics are described by a single exponential, indicating that this drug does not discriminate between the different tubulin isotypes. The observed pseudo-first-order rate constant of the fluorescence increase upon binding increases in a non-linear way, indicating that this ligand binds with a similar overall mechanism as colchicine and MTC, consisting of a fast initial binding of low affinity followed by a slower isomerisation step leading to full affinity. The K1 and k2 values for MDC at 25 degrees C were 540 +/- 65 M(-1) and 70 +/- 6 s(-1) respectively. From the temperature dependence, a reaction enthalpy change (deltaH(o)1) of the initial binding of 49 +/- 11 kJ/mol(-1) and an activation energy for the second step of 28 +/- 9 kJ/mol(-1) were calculated. Displacement experiments of bound MDC by MTC allowed the determination of a rate constant of reverse isomerisation of 0.60 +/- 0.07 s(-1) at 25 degrees C and the activation energy of 81 +/- 6 kJ/mol(-1). The overall binding constant was (6.3 +/- 0.2) x 10(4) M(-1) at 25 degrees C. Combination of these results with the kinetic parameters for association gives a full characterisation of the enthalpy pathway for the binding of MDC. The pathway of MDC is shown to differ considerably from that of MTC binding. Since its structural difference is located in ring A, this result indicates the use of ring A in the first step. The kinetics of the binding of MDC in the presence of some A-ring colchicine analogues (podophyllotoxin, 3',4',5'-trimethoxyacetophenone and N-acetylmescaline) and a C-ring analogue (tropolone methyl ether) suggest that the A and C rings are involved in the binding of MDC.     

Recombinant human erythrocyte cytochrome b5

The gene encoding the human erythrocyte form of cytochrome b5 (97 residues in length) has been prepared by mutagenesis of an expression vector encoding lipase-solubilized bovine liver microsomal cytochrome b5 (93 residues in length) (Funk et al., 1990). Efficient expression of this gene in Escherichia coli has provided the first opportunity to obtain this protein in quantities sufficient for physical and functional characterization. Comparison of the erythrocytic cytochrome with the trypsin-solubilized bovine liver cytochrome b5 by potentiometric titration indicates that the principal electrostatic difference between the two proteins results from two additional His residues present in the human erythrocytic protein. The midpoint reduction potential of this protein determined by direct electrochemistry is -9 +/- 2 mV vs SHE at pH 7.0 (mu = 0.10 M, 25.0 degrees C), and this value varies with pH in a fashion that is consistent with the presence of a single ionizable group that changes pKa from 6.0 +/- 0.1 in the ferricytochrome to 6.3 +/- 0.1 in the ferrocytochrome with delta H degrees = -3.2 +/- 0.1 kcal/mol and delta S degrees = -11.5 +/- 0.3 eu (pH 7.0, mu = 0.10). The 1D 1H NMR spectrum of the erythrocytic ferricytochrome indicates that 90% of the protein binds heme in the "major" orientation and 10% of the protein binds heme in the "minor" orientation (pH 7.0, 25 degrees C) with delta H degrees = -2.9 +/- 0.3 kcal/mol and delta S degrees = -5.4 +/- 0.9 eu for this equilibrium.     

Hydrophobic core substitutions in calbindin D9k: effects on stability and structure

The effects of hydrophobic core mutations on the stability and structure of the four-helix calcium-binding protein, calbindin D9k, have been investigated. Eleven mutations involving eight residues distributed within the hydrophobic core of calbindin D9k were examined. Stabilities were measured by denaturant and thermal induced unfolding monitored by circular dichroism spectroscopy. The mutations were found to exert large effects on the stability with midpoints in the urea induced unfolding varying from 1.8 M for Leu23 --> Gly up to 6.6 M for Val70 --> Leu and free energies of unfolding in the absence of denaturant ranging from 6.6 to 27.4 kJ/mol for the Phe66 --> Ala mutant and the wild-type, respectively. A significant correlation was found between the difference in free energy of unfolding (Delta Delta GNU) and the change in the surface area of the side chain caused by the mutation, in agreement with other studies. Notably, both increases and decreases in side-chain surface area caused quantitatively equivalent effects on the stability. In other words, a correlation between the absolute value of the change in the surface of the side chain and Delta DeltaGNU was observed with a value of approximately 0.14 kJ M-1 A-2. The generality of this observation is discussed. Significant effects on the cooperativity of the unfolding reaction were also observed. However, a correlation between the cooperativity and Delta Delta GNU, which has been reported in other systems as an indication of effects of mutations on the unfolded state, was not observed for calbindin D9k. Despite the large effects on Delta Delta GNU and cooperativity, the structures of the mutants in the native form remained intact as indicated by circular dichroism, NMR, and fluorescence measurements. The structural response to calcium-binding was also conserved. The following paper in this issue [Kragelund, B. B., et al. (1998) Biochemistry 37, 8926-8937] examines the effects of these mutations on the calcium binding properties of calbindin D9k.     

Chemical and thermal stability of ferulic acid esterase-III from Aspergillus niger

The stability of ferulic acid esterase III (FAE-III) from Aspergillus niger was examined using chemical and thermal denaturation. Thermal denaturation was irreversible and the loss of activity was dependent on pH. At 60 degrees C and pH 6.0, the rate constant of unfolding was 0.76 10(-3)/s, and the change in free energy of irreversible inactivation, deltaG*, was 101.9 kJ/mol. Sinapic acid, a product of the reaction of methyl sinapate with FAE-III, reduced the rate of unfolding (0.66 10(-3)/s at 0.1 mM sinapic acid). Chemical denaturation was performed using guanidine hydrochloride. FAE-III was very sensitive to this denaturant, and the midpoint of unfolding was 1.38 M guanidine hydrochloride at 30 degrees C, pH 6.0. The stability of FAE-III is compared to other enzymes.     

Substrate binding to the inactive mutants of Streptomyces sp. N174 chitosanase: indirect evaluation from the thermal unfolding experiments

Oligosaccharide binding to chitosanase from Streptomyces sp. N174 was indirectly evaluated from thermal unfolding experiments of the protein. Thermal unfolding curves were obtained by fluorescence spectroscopy in the presence of D-glucosamine oligosaccharides ((GlcN)n, n = 3, 4, 5, and 6) using the inactive mutant chitosanase in which the catalytic residue, Glu22, is mutated to glutamine (E22Q), aspartic acid (E22D), or alanine (E22A). The midpoint temperature of the unfolding transition (Tm) of E22Q was found to be 44.4 degrees C at pH 7.0. However, the Tm increased upon the addition of (GlcN), by 1.3 degrees C (n = 3), 2.5 degrees C (n = 4), 5.2 degrees C (n = 5), or 7.6 degrees C (n = 6). No appreciable change in Tm was observed when (GlcNAc)6 was added to E22Q. The effect of (GlcN)n on the thermal stability was examined using the other protein, RNase T1, but the oligosaccharide did not affect Tm of the protein. Thus, we concluded that the stabilization effect of (GlcN)n on the chitosanase results from specific binding of the oligosaccharides to the substrate binding cleft. When E22D or E22A was used instead of E22Q, the increases in Tm induced by (GlcN)6 binding were 2.7 degrees C for E22D and 4.2 degrees C for E22A. In E22D or E22A, interaction with (GlcN)6 seems to be partly disrupted by a conformational distortion in the catalytic cleft.     

Luminescence and Energy Transfer Properties of Ca2Gd8(SiO4)6O2∶ A (A=Pb2+,Tm3+)Phosphors

Ca2Gd8(SiO4)6O2∶ A(A=Pb2 , Tm3 )phosphors were prepared through the sol-gel process. X-ray diffraction(XRD), scanning electron microscopy(SEM)and photoluminescence spectra were used to characterize the resulting phosphors. The results of XRD indicate that the phosphors crystallized completely at 1000 ℃. SEM study reveals that the average grain size is 300～1000 nm. In Ca2Gd8(SiO4)6O2∶ Tm3 phosphors, the Tm3 shows its characteristic blue emission at 456 nm(1D2-3F4)upon excitation into its 3H6 - 1D2(361 nm), with an optimum doping concentration of 1mol% of Gd3 in the host lattices. In Ca2Gd8(SiO4)6O2∶ Pb2 , Tm3 phosphors, excitation into the Pb2 at 266 nm(1S0-3P1)yields the emissions of Gd3 at 311 nm(6P-8S)and Tm3 at 367 nm(1D2 -3H6)and 456 nm(1D2-3F4), indicating that energy transfer processes of Pb2 - Gd3 and Pb2 - Tm3 have occurred in the host lattices.