The secondary structure of the inhibited mitochondrial ADP/ATP transporter from yeast analyzed by FTIR spectroscopy

Fourier transform infrared spectroscopy has been applied to the study of the carboxyatractyloside-inhibited mitochondrial ADP/ATP transporter from the yeast Saccharomyces cerevisiae, either solubilized in dodecyl maltoside or reconstituted in phosphatidylcholine liposomes. Its secondary structure has been estimated by means of Fourier self-deconvolution followed by curve fit. A Voigt function was used to fit the components of the deconvoluted spectrum, aiming to account for any distortions introduced by deconvolution. For any of the states analyzed, reconstituted or solubilized, in solution or in dry films, 60-70% of the amino acids are found to adopt alpha-helix plus unordered structures, coherent with the six transmembrane spanning helix model. Moreover, the problem of structure preservation on drying was addressed, and several observations pointed to a maintenance of the protein structure in dry films. Comparison of reconstituted and solubilized samples indicated the presence of both lipid-induced changes in the protein (decrease of the beta-sheets and increase of unordered structures) and protein-induced changes in the lipids (strong hydrogen bonding of lipid C=O groups). To obtain a better discrimination of alpha-helix and unordered structure contributions for the reconstituted form, H/D exchange experiments were performed. Between 35% and 45% of the amino acids were finally assigned to alpha-helix structures, compatible with the existence of five or six transmembrane spanning helices in the transporter. The level of H/D exchange was determined after 15 h of exposure to D(2)O vapor to be 85%, reflecting a high accessibility of the amide hydrogens even for the carboxyatractyloside-inhibited state.     

Fourier transform infrared spectrometric analysis of protein conformation: effect of sampling method and stress factors.

Changes in the amide bands in Fourier transform infrared spectra of proteins are generally attributed to alterations in protein secondary structure. In this study spectra of five different globular proteins were compared in the solid and solution states recorded with several sampling techniques. Spectral differences for each protein were observed between the various sampling techniques and physical states, which could not all be explained by a change in protein secondary structure. For example, lyophilization in the absence of lyoprotectants caused spectral changes that could (partially) have been caused by the removal of hydrating water molecules rather than secondary structural changes. Moreover, attenuated total reflectance spectra of proteins in H2O were not directly comparable to transmission spectra due to the anomalous dispersion effect. Our study also revealed that the amide I, II, and III bands differ in their sensitivities to changes in protein conformation: For example, strong bands in the region 1620-1630 and 1685-1695 cm(-1) were seen in the amide I region of aggregated protein spectra. Surprisingly, absorbance of such magnitudes was not observed in the amide II and III region. It appears, therefore, that only the amide I can be used to distinguish between intra- and intermolecular beta-sheet formation. Considering the differing sensitivity of the different amide modes to structural changes, it is advisable to utilize not only the amide I band, but also the amide II and III bands, to determine changes in protein secondary structure. Finally, it is important to realize that changes in these bands may not always correspond to secondary structural changes of the proteins.     

Evolutionary plasticity of protein families: coupling between sequence and structure variation

In this work we examine how protein structural changes are coupled with sequence variation in the course of evolution of a family of homologs. The sequence-structure correlation analysis performed on 81 homologous protein families shows that the majority of them exhibit statistically significant linear correlation between the measures of sequence and structural similarity. We observed, however, that there are cases where structural variability cannot be mainly explained by sequence variation, such as protein families with a number of disulfide bonds. To understand whether structures from different families and/or folds evolve in the same manner, we compared the degrees of structural change per unit of sequence change ("the evolutionary plasticity of structure") between those families with a significant linear correlation. Using rigorous statistical procedures we find that, with a few exceptions, evolutionary plasticity does not show a statistically significant difference between protein families. Similar sequence-structure analysis performed for protein loop regions shows that evolutionary plasticity of loop regions is greater than for the protein core.     

Infrared spectroscopic discrimination between the loop and alpha-helices and determination of the loop diffusion kinetics by temperature-jump time-resolved infrared spectroscopy for cytochrome c

The infrared (IR) absorption of the amide I band for the loop structure may overlap with that of the alpha-helices, which can lead to the misassignment of the protein secondary structures. A resolution-enhanced Fourier transform infrared (FTIR) spectroscopic method and temperature-jump (T-jump) time-resolved IR absorbance difference spectra were used to identify one specific loop absorption from the helical IR absorption bands of horse heart cytochrome c in D2O at a pD around 7.0. This small loop consists of residues 70-85 with Met-80 binding to the heme Fe(III). The FTIR spectra in amide I' region indicate that the loop and the helical absorption bands overlap at 1653 cm(-1) at room temperature. Thermal titration of the amide I' intensity at 1653 cm(-1) reveals that a transition in loop structural change occurs at lower temperature (Tm=45 degrees C), well before the global unfolding of the secondary structure (Tm approximately 82 degrees C). This loop structural change is assigned as being triggered by the Met-80 deligation from the heme Fe(III). T-jump time-resolved IR absorbance difference spectra reveal that a T-jump from 25 degrees C to 35 degrees C breaks the Fe-S bond between the Met-80 and the iron reversibly, which leads to a loop (1653 cm(-1), overlap with the helical absorption) to random coil (1645 cm(-1)) transition. The observed unfolding rate constant interpreted as the intrachain diffusion rate for this 16 residue loop was approximately 3.6x10(6) s(-1).     

Probing the Dynamic Distribution of Bound States for Methylcytosine-binding Domains on DNA

Although highly homologous to other methylcytosine-binding domain (MBD) proteins, MBD3 does not selectively bind methylated DNA, and thus the functional role of MBD3 remains in question. To explore the structural basis of its binding properties and potential function, we characterized the solution structure and binding distribution of the MBD3 MBD on hydroxymethylated, methylated, and unmethylated DNA. The overall fold of this domain is very similar to other MBDs, yet a key loop involved in DNA binding is more disordered than previously observed. Specific recognition of methylated DNA constrains the structure of this loop and results in large chemical shift changes in NMR spectra. Based on these spectral changes, we show that MBD3 preferentially localizes to methylated and, to a lesser degree, unmethylated cytosine-guanosine dinucleotides (CpGs), yet does not distinguish between hydroxymethylated and unmethylated sites. Measuring residual dipolar couplings for the different bound states clearly shows that the MBD3 structure does not change between methylation-specific and nonspecific binding modes. Furthermore, residual dipolar couplings measured for MBD3 bound to methylated DNA can be described by a linear combination of those for the methylation and nonspecific binding modes, confirming the preferential localization to methylated sites. The highly homologous MBD2 protein shows similar but much stronger localization to methylated as well as unmethylated CpGs. Together, these data establish the structural basis for the relative distribution of MBD2 and MBD3 on genomic DNA and their observed occupancy at active and inactive CpG-rich promoters.     

Structural comparison of monomeric variants of the chemokine MIP-1beta having differing ability to bind the receptor CCR5

MIP-1beta, a member of the chemokine family of proteins, tightly binds the receptor CCR5 as part of its natural function in the immune response, and in doing so also blocks the ability of many strains of HIV to enter the cell. The single most important MIP-1beta residue known to contribute to its interaction with the receptor is Phe13, which when mutated reduces the ability of MIP-1beta to bind to CCR5 by more than 1000-fold. To obtain a structural understanding of the dramatic effect of the absence of Phe13 in MIP-1beta, we used multidimensional heteronuclear NMR to determine the three-dimensional structure of the MIP-1beta F13A variant. We had previously shown that, unlike the wild-type protein which has been shown to be a tight dimer, the F13A mutant is monomeric even at high concentrations [Laurence, J. S., Blanpain, C., Burgner, J. W., Parmentier, M., and LiWang, P. J. (2000) Biochemistry 39, 3401-3409], leading to significant changes in the NMR spectra of F13A and the wild-type protein. We have obtained a total of 940 structural restraints for MIP-1beta F13A, and have calculated a family of structures having a backbone rmsd from the average of 0.55 A (residues 12-67). A structural comparison of the F13A mutant with a fully active monomeric variant, P8A, shows that despite some differences in the (1)H-(15)N HSQC spectra the two are nearly identical in NOE distance restraints and in backbone conformation. A comparison of F13A with the wild-type protein shows largely the same fold, although differences exist in the N-terminal and loop regions for which the loss of the dimer in F13A can mainly account. A dynamics comparison confirms greater flexibility in F13A than in the wild-type protein in regions of dimer contact in the wild-type protein. In an analysis to determine if the large functional effect resulting from the loss of Phe13 is due to the local side chain change or due to more global structural changes, we conclude that local effects predominate. This suggests that a strategy for designing tight binding anti-CCR5 therapeutics should include a Phe-like component.     

Dependence of the conformational state of the isolated adenine nucleotide carrier protein on the detergent used for solubilization

The mitochondrial adenine nucleotide (AdN) carrier can assume two conformational states that are trapped by the specific inhibitors of AdN transport carboxyatractyloside (CATR) and bongkrekic acid (BA). When the AdN carrier protein was extracted from beef heart mitochondria by the zwitterionic detergent 3-[(3-cholamidopropyl)dimethylammonio)]-1-propanesulfonate (CHAPS) and purified in the same detergent, the fluorescence of the tryptophanyl residue(s) of the protein was partially quenched by ATP (or ADP), but not by nontransportable nucleotides; CATR, which alone was ineffective, was able in the presence of ATP (ADP) to further quench the fluorescence, and BA reversed the quenched fluorescence to the original level. With 3'-O-naphthoyl-ATP (N-ATP) as an extrinsic fluorescence probe, it was shown that BA could release bound N-ATP but that CATR was ineffective. These results indicate that the AdN carrier in CHAPS is able to react readily with BA, but not with CATR. The opposite situation occurs with the carrier solubilized and purified in (laurylamido)-N,N-dimethylpropylamine oxide (LAPAO) [Brandolin, G., Dupont, Y., & Vignais, P.V. (1985) Biochemistry 24, 1991-1997]. These data taken together were interpreted to mean that the CATR and BA conformations of the isolated AdN carrier depend on the micellar structure in which it is embedded; the carrier in LAPAO is in the CATR conformation, and the carrier in CHAPS is in the BA conformation. For the transition between the CATR and BA conformations to occur in the carrier in CHAPS and in the carrier in LAPAO, ATP or ADP is required; nontransportable nucleotides were ineffective.(ABSTRACT TRUNCATED AT 250 WORDS)     

Vibrational spectrum of the unordered polypeptide chain: A Raman study of feather keratin

Raman spectra of native and solubilized feather keratin have been obtained, and the amide I and amide III regions have been analyzed by band resolution techniques. The amide I region of the native form indicates that at least 64% of the protein has an antiparallel chain pleated sheet structure, the remainder being unordered. For the solubilized keratin all of the protein is in an unordered state. The amide III region is not as easily analyzed into component contributions. Normal vibration analyses on N-acetyl-L -alanine-N-methylamide support the conclusion that the amide III region is not as satisfactory as the amide I region in characterizing unordered structures. Even in the latter case caution must be used, since the observed amide I band is an average over the conformational distribution in the particular unordered system.     

Water structural changes involved in the activation process of photoactive yellow protein

Fourier transform infrared (FTIR) spectroscopy was applied to the blue-light photoreceptor photoactive yellow protein (PYP) to investigate water structural changes possibly involved in the photocycle of PYP. Photointermediates were stabilized at low temperature, and difference IR spectra were obtained between intermediate states and the original state of PYP (pG). Water structural changes were never observed in the >3570 cm(-)(1) region for the intermediates stabilized at 77-250 K, such as the red-shifted pR and blue-shifted pB intermediates. In contrast, a negative band was observed at 3658 cm(-)(1) in the pB minus pG spectrum at 295 K, which shifts to 3648 cm(-)(1) upon hydration with H(2)(18)O. The high frequency of the O-H stretch of water indicates that the water O-H group does not form hydrogen bonds in pG, and newly forms these upon pB formation at 295 K, but not at 250 K. Among 92 water molecules in the crystal structure of PYP, only 1 water molecule, water-200, is present in a hydrophobic core inside the protein. The amide N-H of Gly-7 and the imidazole nitrogen atom of His-108 are its possible hydrogen-bonding partners, indicating that one O-H group of water-200 is free to form an additional hydrogen bond. The water band at 3658 cm(-)(1) was indeed diminished in the H108F protein, which strongly suggests that the water band originates from water-200. Structural changes of amide bands in pB were much greater in the wild-type protein at 295 K than at 250 K or in the H108F protein at 295 K. The position of water-200 is >15 A remote from the chromophore. Virtually no structural changes were reported for regions larger than a few angstroms away from the chromophore, in the time-resolved X-ray crystallography experiments on pB. On the basis of the present results, as well as other spectroscopic observations, we conclude that water-200 (buried in a hydrophobic core in pG) is exposed to the aqueous phase upon formation of pB in solution. In neither crystalline PYP nor at low temperature is this structural transition observed, presumably because of the restrictions on global structural changes in the protein under these conditions.     

Infrared spectroscopic study of the structural and functional properties of the Na/H antiporter MjNhaP1 from Methanococcus jannaschii

In this study, structural, functional, and mechanistic properties of the Na⁺/H⁺ antiporter MjNhaP1 from Methanococcus jannaschii were analyzed by infrared spectroscopic techniques. Na⁺/H⁺ antiporters are generally responsible for the regulation of cytoplasmic pH and Na⁺ concentration. MjNhaP1 is active in the pH range between pH 6 and pH 6.5; below and above it is inactive.The secondary structure analysis on the basis of ATR-IR spectra provides the first insights into the structural changes between inactive (pH 8) and active (pH 6) state of MjNhaP1. It results in decreased ordered structural elements with increasing the pH-value i.e. with inactivation of the protein. Analysis of temperature-dependent FTIR spectra indicates that MjNhaP1 in the active state exhibits a much higher unfolding temperature in the spectral region assigned to α-helical segments. In contrast, the temperature-induced structural changes for β-sheet structure are similar for inactive and active state. Consequently, this structure element is not the part of the activation region of the protein. The surface accessibility of the protein was analyzed by following the extent of H/D exchange. Due to higher content of unordered structural elements a higher accessibility for amide protons is observed for the inactive as compared to the active state of MjNhaP1. Altogether, the results present the active state of MjNhaP1 as the state with ordered structural elements which exhibit high thermal stability and increased hydrophobicity.     

Exploration of the nucleotide binding sites of the isolated ADP/ATP carrier protein from beef heart mitochondria. 1. Probing of the nucleotide sites by Naphthoyl-ATP, a fluorescent nontransportable analogue of ATP

The ADP/ATP carrier protein was extracted and purified from beef heart mitochondria, and its binding parameters with respect to 3'-O-naphthoyladenosine 5'-triphosphate (N-ATP), a fluorescent nontransportable analogue of ATP, were studied. The binding of N-ATP to the isolated carrier protein was accompanied by a decrease in fluorescence. Conversely, the release of bound N-ATP upon addition of carboxyatractyloside (CATR) or ATP resulted in a fluorescence increase. The bound N-ATP that was released upon addition of an excess of CATR or ATP was referred to as specifically bound N-ATP, i.e., N-ATP bound to the nucleotide sites of the carrier protein. Two classes of binding sites for N-ATP could be identified; the number of high-affinity sites (Kd less than 10 nM) was equal to the number of low-affinity sites (Kd = 0.45 microM). CATR behaved apparently as a noncompetitive inhibitor of the binding of N-ATP. The amount of N-ATP released increased linearly with the amount of CATR added, indicating an extremely high affinity of the carrier protein for CATR. The number of CATR binding sites was equal to half the total number of N-ATP binding sites (high- and low-affinity sites); at saturating concentrations of N-ATP, the binding of 1 mol of CATR resulted in the release of 2 mol of bound N-ATP, one from the high-affinity site and the other from the low-affinity site, showing unambiguously that each CATR site is interacting with a pair of probably interdependent N-ATP sites. A clear competition between N-ATP and ATP for binding to the carrier protein was demonstrated. The Kd values of the high- and low-affinity sites for ATP were less than 50 nM and 5 microM, respectively. In the presence of high concentrations of ATP, the two classes of N-ATP binding sites became indistinguishable, suggesting interconversion. It is proposed that the asymmetry in affinity for N-ATP binding is induced by the binding step itself, the carrier protein exhibiting a negative cooperativity for N-ATP binding.     

Probing the pH sensitivity of R-phycoerythrin: Investigations of active conformational and functional variation

Crystal structures of phycobiliproteins have provided valuable information regarding the conformations and amino acid organizations of peptides and chromophores, and enable us to investigate their structural and functional relationships with respect to environmental variations. In this work, we explored the pH-induced conformational and functional dynamics of R-phycoerythrin (R-PE) by means of absorption, fluorescence and circular dichroism spectra, together with analysis of its crystal structure. R-PE presents stronger functional stability in the pH range of 3.5-10 compared to the structural stability. Beyond this range, pronounced functional and structural changes occur. Crystal structure analysis shows that the tertiary structure of R-PE is fixed by several key anchoring points of the protein. With this specific association, the fundamental structure of R-PE is stabilized to present physiological spectroscopic properties, while local variations in protein peptides are also allowed in response to environmental disturbances. The functional stability and relative structural sensitivity of R-PE allow environmental adaptation.     

Structure and dynamics of the phospholipase C-delta1 pleckstrin homology domain located at the lipid bilayer surface

Despite the importance of signal transduction pathways at membrane surfaces, there have been few means of investigating their molecular mechanisms based on the structural information of membrane-bound proteins. We applied solid state NMR as a novel method to obtain structural information about the phospholipase C-delta1 (PLC-delta1) pleckstrin homology (PH) domain at the lipid bilayer surface. NMR spectra of the alanine residues in the vicinity of the beta5/beta6 loop in the PH domain revealed changes in local conformations due to the membrane localization of the protein. We propose that these conformational changes originate from a hydrophobic interaction between the amphipathic alpha-helix located in the beta5/beta6 loop and the hydrophobic layer of the membrane and contribute to the membrane binding affinity, interdomain interactions and intermolecular interactions of PLC-delta1.     

IR spectroscopic studies of major cellular components. III. Hydration of protein,nucleic acid,and phospholipid films

The IR absorption spectra of protein, DNA, RNA, and phospholipid films as a function of the water content are reported. We find that the hydration of protein films affects the peak intensity of amide I and amide II bands and the shape of the amide III band. For nucleic acids, the symmetric (nu(S) PO(2) (-)) and antisymmetric (nu(AS) PO(2) (-)) stretching vibrations of the phosphate linkage are the most affected by hydration, because both intensity changes and frequency shifts are observed. The spectra of phospholipid films are also sensitive to hydration, and they exhibit changes in the peak intensities and frequencies of both nu(S) PO(2) (-) and nu(AS) PO(2) (-) vibrations. We interpret the spectral differences between water saturated and dried films both in terms of structural changes and the change in the local dielectric in the vicinity of the polar and solvent exposed groups. In addition, we observe that the most significant change in the absorption intensity, frequency, and shape of the water sensitive vibrations occurs at high hydration levels. The principal component analysis of hydration results and the kinetics of water removal from sample films are also discussed. In addition, protein spectra acquired using film and KBr pellet sampling techniques are compared.     

Cell-free co-expression of functional membrane proteins and apolipoprotein, forming soluble nanolipoprotein particles

Here we demonstrate rapid production of solubilized and functional membrane protein by simultaneous cell-free expression of an apolipoprotein and a membrane protein in the presence of lipids, leading to the self-assembly of membrane protein-containing nanolipoprotein particles (NLPs). NLPs have shown great promise as a biotechnology platform for solubilizing and characterizing membrane proteins. However, current approaches are limited because they require extensive efforts to express, purify, and solubilize the membrane protein prior to insertion into NLPs. By the simple addition of a few constituents to cell-free extracts, we can produce membrane proteins in NLPs with considerably less effort. For this approach an integral membrane protein and an apolipoprotein scaffold are encoded by two DNA plasmids introduced into cell-free extracts along with lipids. For this study reported here we used plasmids encoding the bacteriorhodopsin (bR) membrane apoprotein and scaffold protein Delta1-49 apolipoprotein A-I fragment (Delta49A1). Cell free co-expression of the proteins encoded by these plasmids, in the presence of the cofactor all-trans-retinal and dimyristoylphosphatidylcholine, resulted in production of functional bR as demonstrated by a 5-nm shift in the absorption spectra upon light adaptation and characteristic time-resolved FT infrared difference spectra for the bR --> M transition. Importantly the functional bR was solubilized in discoidal bR.NLPs as determined by atomic force microscopy. A survey study of other membrane proteins co-expressed with Delta49A1 scaffold protein also showed significantly increased solubility of all of the membrane proteins, indicating that this approach may provide a general method for expressing membrane proteins enabling further studies.     

Unraveling a phosphorylation event in a folded protein by NMR spectroscopy: phosphorylation of the Pin1 WW domain by PKA

The Pin1 protein plays a critical role in the functional regulation of the hyperphosphorylated neuronal Tau protein in Alzheimer’s disease and is by itself regulated by phosphorylation. We have used Nuclear Magnetic Resonance (NMR) spectroscopy to both identify the PKA phosphorylation site in the Pin1 WW domain and investigate the functional consequences of this phosphorylation. Detection and identification of phosphorylation on serine/threonine residues in a globular protein, while mostly occurring in solvent-exposed flexible loops, does not lead to chemical shift changes as obvious as in disordered proteins and hence does not necessarily shift the resonances outside the spectrum of the folded protein. Other complications were encountered to characterize the extent of the phosphorylation, as part of the ¹H,¹⁵N amide resonances around the phosphorylation site are specifically broadened in the unphosphorylated state. Despite these obstacles, NMR spectroscopy was an efficient tool to confirm phosphorylation on S16 of the WW domain and to quantify the level of phosphorylation. Based on this analytical characterization, we show that WW phosphorylation on S16 abolishes its binding capacity to a phosphorylated Tau peptide. A reduced conformational heterogeneity and flexibility of the phospho-binding loop upon S16 phosphorylation could account for part of the decreased affinity for its phosphorylated partner. Additionally, a structural model of the phospho-WW obtained by molecular dynamics simulation and energy minimization suggests that the phosphate moiety of phospho-S16 could compete with the phospho-substrate.     

Solubilization of active GLP-1 (7–36)amide receptors from RINm5F plasma membranes

Glucagon-like peptide-1 (7–36)amide (GLP-1 (7–36)amide) represents a physiologically important incretin in mammals including man. Receptors for GLP-1 (7–36)amide have been described in RINm5F cells. We have solubilized active GLP-1 (7–36)amide receptors from RINm5F cell membranes utilizing the detergents octyl-β-glucoside and CHAPS; Triton X-100 and Lubrol PX were ineffective. Binding of radiolabeled GLP-1(7–36)amide to the solubilized receptor was inhibited conentration-dependently by addition of unlabeled peptide. Scatchard analysis of binding data revealed a single class of binding sites with K_a= 0.26 ± 0.03 nM and B_max= 65.4 ± 21.24 fmol/mg of protein for the membrane-bound receptor and K_a= 22.54 ± 4.42 μM and B_max= 3.9 ± 0.79 pmol/mg of protein for the solubilized receptor. The binding of the radiolabel to the solubilized receptor was dependent both on the concentrations of mono- and divalent cations and the protein/detergent ratio in the incubation buffer. The membrane bound receptor is sensitive to guanine-nucleotides, however neither GTP-γ-S nor GDP-β-S affected binding or labeled peptide to solubilized receptor. These data indicate that the solubilized receptor may have lost association with its G-protein. In conclusion, the here presented protocol allows solubilization of the GLP-1(7–36)amide receptor in a functional state and opens up the possibility for further molecular characterization of the receptor protein.     

Analysis of the Secondary Structure of the Cys-Less Yeast Mitochondrial Citrate Transport Protein and Four Single-Cys Variants by Circular Dichroism

Utilizing cysteine scanning mutagenesis, with functional Cys-less citrate transport protein (CTP) serving as the starting template, we previously demonstrated that four single-Cys mutants located in transmembrane domains III and IV, rendered the CTP nonfunctional. The present investigations assess and quantify the secondary structure of the Cys-less CTP and the four single-Cys mutants, both in the absence and presence of citrate, via circular dichroism (CD) spectroscopy. In detergent micelles, highly purified Cys-less CTP contained approximately 50% alpha-helix and approximately 20% beta-sheet. The CD spectra of the G119C, E122C, R181C, and R189C mutants in detergent micelles were virtually superimposable with that of the functional Cys-less CTP, thereby suggesting that the wild-type residues, rather than affecting structure, may assume important mechanistic roles. Exogenously added citrate caused a significant change in the CD spectra of all solubilized CTP samples. Analyses of the spectra of the Cys-less CTP indicated an approximately 10% increase in its alpha-helical content in the presence of citrate. The conformational changes effected by the addition of substrate were less pronounced with the single-Cys mutants. Studies of the Cys-less CTP reconstituted in liposomes indicated that while the CD spectra was red-shifted, the net secondary structure of the reconstituted carrier is approximately equivalent to that of the transporter in detergent micelles, and displayed a response to added citrate. In combination, the above studies indicate that purified Cys-less CTP in either sarkosyl micelles or in liposomes, and the four inactive single-Cys mutants in sarkosyl micelles, retain native-like structure, and thus represent ideal material for detailed structural characterization.     

Spectroscopic study on structure of horseradish peroxidase in water and dimethyl sulfoxide mixture

The structure of horseradish peroxidase (HRP) in phosphate buffered saline (PBS)/dimethyl sulfoxide (DMSO) mixed solvents at different compositions is investigated by IR, electronic absorption, and fluorescence spectroscopies. The fluorescence spectra and the amide I spectra of ferric HRP [HRP(Fe3+)] show that overall structural changes are relatively small up to 60% DMSO. Although the amide I band of HRP(Fe3+) shows a gradual change in the secondary structure and a decrease in the contents of a helices, its fluorescence spectra indicate that the distance between the heme and Trp173 is almost constant. In contrast, the changes in the positions of the Soret bands for resting HRP(Fe3+) and catalytic intermediates (compounds I and II) and the IR spectra at the C-O stretching vibration mode of carbonyl ferrous HRP [HRP(Fe2+)-CO] show that the microenvironment in the distal heme pocket is altered, even with low DMSO contents. The large reduction of the catalytic activity of HRP even at low DMSO contents can be attributed to the structural transition in the distal heme pocket. In PBS/DMSO mixtures containing more than 70 vol % DMSO, HRP undergoes large structural changes, including a large loss of the secondary structure and a dissociation of the heme from the apoprotein. The presence of the components of the amide I band that can be assigned to strongly hydrogen bonding amide C=O groups at 1616 and 1684 cm(-1) suggests that the denatured HRP may aggregate through strong hydrogen bonds.