Infrared reflection-absorption of melittin interaction with phospholipid monolayers at the air/water interface.

The interaction of melittin with monolayers of 1,2-dipalmitoylphosphatidylcholine and 1,2-dipalmitoylphosphatidylserine has been investigated with infrared external reflection-absorption spectroscopy. Improved instrumentation permits determination of acyl chain conformation and peptide secondary structure in situ at the air/water interface. The IR frequency of the 1,2-dipalmitoylphosphatidylcholine antisymmetric acyl chain CH2 stretching vibration decreases by 1.3 cm-1 upon melittin insertion, consistent with acyl chain ordering, whereas the same vibrational mode increases by 0.5 cm-1 upon peptide interaction with the 1,2-dipalmitoylphosphatidylserine monolayer, indicative of chain disordering. Thus the peptide interacts quite differently with zwitterionic compared with negatively charged monolayer surfaces. Melittin in the monolayer adopted a secondary structure with an amide l(l') frequency (1635 cm-1) dramatically different from the alpha-helical motif (amide l frequency 1656 cm-1 in a dry or H2O hydrated environment, amide l' frequency 1645 cm-1 in an H-->D exchanged alpha-helix) assumed in bilayer or multibilayer environments. This work represents the first direct in situ spectroscopic indication that peptide secondary structure in lipid monolayers may differ from that in bilayers.     

The structural properties of magainin in water, TFE/water, and aqueous urea solutions: molecular dynamics simulations

Here, the MD simulations and comparative structural analysis of Magainin in water, TFE/water, and 2M, 4M, and BM urea solutions is reported. For MAG-TFE/water and MAG-2M urea the largely alpha helical conformation of the peptide is maintained throughout the 9-ns simulation. While in water, 4M urea, and 8M urea, the helix length decreases and at the same time helix radius increases. This suggests a more destabilized magainin secondary structure. Our simulation data reveals that the stabilizing effect of TFE is induced by preferential accumulation of TFE molecules around the alpha helical peptide. These results indicate that an aqueous urea solution solvates the surface of polypeptide chain more favorably than pure water. Urea molecules interact more favorably with nonpolar groups of the peptide in comparison with water, and the presence of urea improves the interactions of water molecules with the hydrophilic groups of the peptide. At 8M urea, there are more direct interactions between the urea and solute, and the helix is destabilized. At 2M urea, the interaction of urea molecules and nonpolar residues are weak, therefore, the presence of urea molecules decreases the interactions of water molecules with hydrophilic groups. Urea could not deteriorate the peptide secondary structure with time from an initial helix structure.     

Internal dynamics of the nicotinic acetylcholine receptor in reconstituted membranes

The structure and 1H/2H exchange kinetics of affinity-purified nAChR reconstituted into egg phosphatidylcholine membranes with increasing levels of either dioleoylphosphatidic acid (DOPA) or cholesterol (Chol) have been examined using infrared spectroscopy. All spectra of the reconstituted nAChR membranes recorded after 72 h in 2H2O exhibit comparable amide I band shapes, suggesting a similar secondary structure for the nAChR in each lipid environment. Increasing levels of either DOPA or Chol, however, lead to an increasing intensity of the amide II band, indicating a decreasing proportion of nAChR peptide hydrogens that have exchanged for deuterium. Spectra recorded as a function of time after exposure of the nAChR to 2H2O show that the presence of either lipid slows down the 1H/2H exchange of those peptide hydrogens that normally exchange on the minutes to hours time scale. The slowing of peptide 1H/2H exchange correlates with both an increasing ability of the nAChR to undergo agonist-induced conformational change [Baenziger, J. E., Morris, M.-L., Darsaut, T. E., and Ryan, S. E. (1999) in preparation] and possibly a decreasing membrane fluidity. Our data suggest that lipid composition dependent changes in nAChR peptide 1H/2H exchange kinetics reflect altered internal dynamics of the nAChR. Lipids may influence protein function by changing the internal dynamics of integral membrane proteins.     

Infrared spectroscopic study of photoreceptor membrane and purple membrane. Protein secondary structure and hydrogen deuterium exchange

Infrared spectroscopy in the interval from 1800 to 1300 cm-1 has been used to investigate the secondary structure and the hydrogen/deuterium exchange behavior of bacteriorhodopsin and bovine rhodopsin in their respective native membranes. The amide I' and amide II' regions from spectra of membrane suspensions in D2O were decomposed into constituent bands by use of a curve-fitting procedure. The amide I' bands could be fit with a minimum of three theoretical components having peak positions at 1664, 1638, and 1625 cm-1 for bacteriorhodopsin and 1657, 1639, and 1625 cm-1 for rhodopsin. For both of these membrane proteins, the amide I' spectrum suggests that alpha-helix is the predominant form of peptide chain secondary structure, but that a substantial amount of beta-sheet conformation is present as well. The shape of the amide I' band was pH-sensitive for photoreceptor membranes, but not for purple membrane, indicating that membrane-bound rhodopsin undergoes a conformation change at acidic pH. Peptide hydrogen exchange of bacteriorhodopsin and rhodopsin was monitored by observing the change in the ratio of integrated absorbance (Aamide II'/Aamide I') during the interval from 1.5 to 25 h after membranes were introduced into buffered D2O. The fraction of peptide groups in a very slowly exchanging secondary structure was estimated to be 0.71 for bacteriorhodopsin at pD 7. The corresponding fraction in vertebrate rhodopsin was estimated to be less than or equal to 0.60. These findings are discussed in relationship to previous studies of hydrogen exchange behavior and to structural models for both proteins.     

Structure of cytochrome b5 in solution by Fourier-transform infrared spectroscopy

Fourier-transform infrared spectroscopy was used to examine the secondary structure of rabbit liver cytochrome b5 and the polar and nonpolar domains of the protein. The data for both the polar and nonpolar domains agree well with those previously obtained by other physical techniques. In particular it was found that the nonpolar membrane-binding domain was predominantly alpha helix and that the polar domain was also highly helical, but not all alpha helix. The independence of the two domains in the whole molecule was, in general, confirmed by the additivity of the spectra of the two domains. The small differences that were seen indicate that there is a loss of alpha helix when the protein is cut into the two domains. In addition, there appeared to be a slight difference in the exposure to solvent of the amide NH groups in the alpha-helical portion of the nonpolar domain when it was examined in isolation.     

5,5-Dimethylthiazolidine-4-carboxylic acid (DTC) as a proline analog with restricted conformation

Spectroscopic evidence is presented for the lack of intramolecular hydrogen bonding in a simple peptide derivative of 5,5-dimethylthiazolidine-4-carboxylic acid (Dtc). The infrared spectrum of Boc-Pro-Ile-OMe 1 in nonpolar solvents displays two N-H stretching bands at 3419 and 3330 cm-1 in CCl4 and one at 3417 and 3328 cm-1 in CHCl3. The low frequency band at 3328-3330 cm-1 may be assigned to conformations with an intramolecular hydrogen bond between the Ile N-H and Boc C = O. The band at 3417-3419 cm-1 is the normal Ile N-H stretch. In the polar solvent CH3CN only one NH stretching band at 3365 cm-1 is observed. The IR spectrum of Boc-Dtc-Ile-OMe 2, on the other hand, displays one N-H stretching band at 3423 cm-1 in CCl4 and one at 3418 cm-1 in CHCl3. The IR spectrum of 2 does not display the N-H stretching band that would arise from intramolecular hydrogen bonding between the Boc C = O and Ile N-H. The lack of intramolecular hydrogen bonding for Boc-Dtc-Ile-OMe 2 was evident also in the NMR spectra in nonpolar solvents. The 1H-NMR spectrum of the Pro dipeptide 1 in 50% CDCl3/C6D6 at 20 degrees displayed two Ile-NH signals at 6.58 and 7.74 ppm. The latter signal corresponds to the intramolecularly hydrogen bonded Ile-NH in the trans-Boc isomer of 1 (60% of the total population), while the former signal corresponds to the nonhydrogen bonded Ile-NH in the cis-Boc isomer.(ABSTRACT TRUNCATED AT 250 WORDS)     

A left-handed 3(1) helical conformation in the Alzheimer Abeta(12-28) peptide

We show for the first time that the secondary structure of the Alzheimer beta-peptide is in a temperature-dependent equilibrium between an extended left-handed 3(1) helix and a flexible random coil conformation. Circular dichroism spectra, recorded at 0.03 mM peptide concentration, show that the equilibrium is shifted towards increasing left-handed 3(1) helix structure towards lower temperatures. High resolution nuclear magnetic resonance (NMR) spectroscopy has been used to study the Alzheimer peptide fragment Abeta(12-28) in aqueous solution at 0 degrees C and higher temperatures. NMR translation diffusion measurements show that the observed peptide is in monomeric form. The chemical shift dispersion of the amide protons increases towards lower temperatures, in agreement with the increased population of a well-ordered secondary structure. The solvent exchange rates of the amide protons at 0 degrees C and pH 4.5 vary within at least two orders of magnitude. The lowest exchange rates (0.03-0.04 min(-1)) imply that the corresponding amide protons may be involved in hydrogen bonding with neighboring side chains.     

Peptide-chain secondary structure of bacteriorhodopsin.

Ultraviolet circular dichroism spectroscopy in the interval from 190 to 240 nm and infrared spectroscopy in the region of the amide I band (1,600 cm-1 to 1,700 cm-1) has been used to estimate the alpha-helix content and the beta-sheet content of bacteriorhodopsin. Circular dichroism spectroscopy strongly suggests that the alpha-helix content is sufficient for only five helices, if each helix is composed of 20 or more residues. It also suggests that there is substantial beta-sheet conformation in bacteriorhodopsin. The presence of beta-sheet secondary structure is further suggested by the presence of a 1,639 cm-1 shoulder on the amide I band in the infrared spectrum. Although a structural model consisting of seven alpha-helical rods has been generally accepted up to this point, the spectroscopic data are more consistent with a model consisting of five alpha-helices and four strands of beta-sheet. We note that the primary amino acid sequence can be assigned to segments of alpha-helix and beta-sheet in a way that does not require burying more than two charged groups in the hydrophobic membrane interior, contrary to the situation for any seven-helix model.     

Beware of proteins in DMSO

The effect on the secondary structure of representative alpha-helical, beta-sheet and disordered proteins by varying concentrations of dimethyl sulphoxide (DMSO) in 2H2O has been investigated by Fourier transform infrared spectroscopy. Significant perturbations of protein secondary structure are induced by DMSO and DMSO/2H2O mixtures. For highly structured proteins, such as myoglobin and concanavalin A, the infrared spectra point to a progressive destabilisation of the secondary structure until at moderate DMSO concentrations (around 0.33 mol fraction) intermolecular beta-sheet formation and aggregation are induced, as indicated by the appearance of a strong band at 1621 cm-1. This is a direct consequence of the disruption of intramolecular peptide group interactions by DMSO (partial unfolding). At higher DMSO concentrations (above 0.75 mol fraction), such aggregates are dissociated by disruption of the intermolecular C = O...2H-N deuterium bonds. The presence of a single amide I band at 1662 cm-1 corresponding to free amide C = O groups indicates that at high concentrations and in pure DMSO the proteins are completely unfolded, lacking any secondary structure. While low concentrations of DMSO showed no detectable effect upon the gross secondary structure of myoglobin and concanavalin A, the thermal stability of both proteins was markedly reduced. In alpha-casein, a highly unstructured protein, the situation is one of direct competition. The amide I maximum in 2H2O, at 1645 cm-1, is typical of unordered proteins with C = O groups deuterium-bonded predominantly to 2H2O. Addition of DMSO disrupts such interactions by competing with the peptide C = O group for the deuterium bond donor capacity of the 2H2O, and so progressively increases the amide I maximum until it stabilizes at 1663 cm-1, a position indicative of free C = O groups.     

Conformational states of the bacteriophage P22 capsid subunit in relation to self-assembly

The formation of closed icosahedral capsids from a single species of coat protein subunit requires that the subunits assume different conformations at different lattice positions. In the double-stranded DNA bacteriophage P22, formation of correctly dimensioned capsids is mediated by interaction between coat protein subunits and scaffolding protein. Raman spectroscopy has been employed to compare the conformations of coat protein subunits which have been polymerized to form capsids in the presence and absence of the of scaffolding protein display a Raman spectrum characterized by a broad amide I band centered at 1665 cm-1 with a discernible shoulder near 1653 cm-1, and a broad amide III profile centered at 1238 cm-1 but asymmetrically skewed to higher frequency. These spectral features indicate that the protein conformation in procapsid shells is rich in beta-sheet secondary structure but contains also a significant distribution of alpha-helix. When biologically active, purified subunits assemble in the absence of scaffolding protein, they form polydisperse multimers lacking the proper dimensions of procapsid closed shells. We designate these multimers as "associated subunits" (AS). The Raman spectrum of associated subunits indicates a narrower distribution of secondary structure. The associated subunits are characterized by a sharper and more intense Raman amide I band at 1666 cm-1, with no prominent amide I shoulder of lower frequency. An analogous narrowing of the Raman amide III profile is also observed for AS particles, with an accompanying shift of the amide III band center to 1235 cm-1.(ABSTRACT TRUNCATED AT 250 WORDS)     

Fourier transform infrared investigation of the Escherichia coli methionine aporepressor

This study represents the first physicochemical analysis of the recently cloned methionine repressor protein (Met aporepressor) from Escherichia coli. Infrared spectrometry was used to investigate the secondary structure and the hydrogen-deuterium exchange behavior of the E. coli Met aporepressor. The secondary structure of the native bacterial protein was derived by analysis of the amide I mode. The amide I band contour was found to consist of five major component bands (at 1625, 1639, 1653, 1665, and 1676 cm-1) which reflect the presence of various substructures. The relative areas of these component bands are consistent with a high alpha-helical content of the peptide chain secondary structure in solution (43%) and a small amount of beta-sheet structure (7%). The remaining substructure is assigned to turns (10%) and to unordered (or less ordered) structures (40%). The temperature dependence of the infrared spectra of native Met aporepressor in D2O medium over the temperature interval 20-80 degrees C indicates that there are two discrete thermal events: the first thermal event, centered at 42 degrees C, is associated with the hydrogen-deuterium exchange of the hard-to-exchange alpha-helical peptide bonds accompanied by a partial denaturation of the protein, while the second event, centered around 50 degrees C, represents the irreversible thermal denaturation of the protein.     

Enhanced catalytic action of HLA-DM on the exchange of peptides lacking backbone hydrogen bonds between their N-terminal region and the MHC class II alpha-chain

The class II MHC homolog HLA-DM catalyzes exchange of peptides bound to class II MHC proteins, and is an important component of the Ag presentation machinery. The mechanism of HLA-DM-mediated catalysis is largely obscure. HLA-DM catalyzes exchange of peptides of varying sequence, suggesting that a peptide sequence-independent component of the MHC-peptide interaction could be involved in the catalytic process. Twelve conserved hydrogen bonds between the peptide backbone and the MHC are a prominent sequence-independent feature of the MHC-peptide interaction. To evaluate the relative importance of these hydrogen bonds toward HLA-DM action, we prepared peptide variants that lacked the ability to form one or more of the hydrogen bonds as a result of backbone amide N-methylation or truncation, and tested their ability to be exchanged by HLA-DM. We found that disruption of hydrogen bonds involving HLA-DR1 residues alpha51-53, a short extended segment at the N terminus of the alpha subunit helical region, led to heightened HLA-DM catalytic efficacy. We propose that those bonds are disrupted in the MHC conformation recognized by HLA-DM to allow structural transitions in that area during DM-assisted peptide release. These results suggest that peptides or compounds that bind MHC but cannot form these interactions would be preferentially edited out by HLA-DM.     

Intrinsic helical propensities and stable secondary structure in a membrane-bound fragment (S4) of the shaker potassium channel.

The location and stability of helical secondary structure in a fragment comprising an extended sequence of the S4 transmembrane segment of the Shaker potassium channel was determined in methanol, and when bound to vesicles composed of egg phosphatidylcholine: egg phosphatidylglycerol (4:1; mol:mol) in water. The N-acetylated, C-amidated peptide corresponds to the sequence comprising residues A355-I384 in the Shaker potassium channel. Although NOEs characteristic of helical structure encompass essentially the full peptide sequence in methanol, analysis of amide and CH(alpha) chemical shifts, and amide exchange protection factors establish that stable helical structure comprises only around the first 22 amino acids of the 30 residue peptide. This sequence corresponds to that predicted to have the highest helical stability in water, indicating that while helical structure is considerably stabilised in methanol, the relative helical propensities of amino acids in methanol may be similar to those in water.In the presence of vesicles containing negatively charged lipids, helical structure corresponding to a maximum of around 40 % of the extended S4 peptide is induced; no helical structure is induced in the presence of vesicles composed only of neutral lipids. The location of stable helical structure in the membrane-bound peptide was determined by amide hydrogen-deuterium exchange trapping, and was shown to encompass the sequence between residues near M2 and I18. This sequence is similar to that having high helix propensity in water and methanol, supporting the idea that intrinsic helical propensities are important in defining the location of stable helical structure in polypeptides bound in the interfacial region of lipid bilayers. The study defines an approach to determining the location of, and contributions to, the stability of helical secondary structure in membrane-reconstituted polypeptides.     

Aggregation of chymotrypsinogen: portrait by infrared spectroscopy.

Changes in the secondary structure and aggregation of chymotrypsinogen were investigated by infrared difference spectroscopy in conjunction with temperature and pressure tuning IR spectroscopy; both the amide I' band and side chain bands were studied. A prominent component of the amide I' band in the difference spectrum obtained upon cooling a chymotrypsinogen solution, or increasing the hydrostatic pressure, was observed in the region between 1627 and 1622 cm-1. Under denaturing conditions a white gel was formed, which is attributed to irreversible self-association or aggregation. This process was accompanied by the appearance of two new amide I' bands in the infrared spectrum of the protein: a very strong band at 1618 cm-1 and a weak band at 1685 cm-1. These bands are assigned to peptide segments with anti-parallel aligned beta-strands.     

Preliminary identification of the secondary structure of the trp repressor from Escherichia coli

The probable secondary structure content of the trp repressor from Escherichia coli has been inferred from NMR and circular dichroic measurements; the results are compared with those of prediction algorithms. 70% of the amide protons have exchange rate constants orders of magnitude smaller than the intrinsic rate constants, identifying them as participating in hydrogen bonds. The exchange rate constants fall into two distinct classes, one having half-lives of 20 min and the other more than 24 h. The latter class, consisting of 50% of all amide protons, indicates a stable core. The exchange data are consistent with circular dichroism and predictions that suggest that about 55% of the peptides from alpha helix, and 20% form beta sheets and turns. The NMR spectrum further indicates that there is little beta sheet, suggesting that the secondary structure class is alpha.     

Fourier transform infrared spectroscopy and site-directed isotope labeling as a probe of local secondary structure in the transmembrane domain of phospholamban.

Phospholamban is a 52-amino acid residue membrane protein that regulates Ca(2+)-ATPase activity in the sarcoplasmic reticulum of cardiac muscle cells. The hydrophobic C-terminal 28 amino acid fragment of phospholamban (hPLB) anchors the protein in the membrane and may form part of a Ca(2+)-selective ion channel. We have used polarized attenuated total reflection-Fourier transform infrared (ATR-FTIR) spectroscopy along with site-directed isotope labeling to probe the local structure of hPLB. The frequency and dichroism of the amide I and II bands appearing at 1658 cm-1 and 1544 cm-1, respectively, show that dehydrated and hydrated hPLB reconstituted into dimyristoylphosphatidycholine bilayer membranes is predominantly alpha-helical and has a net transmembrane orientation. Specific local secondary structure of hPLB was probed by incorporating 13C at two positions in the protein backbone. A small band seen near 1614 cm-1 is assigned to the amide I mode of the 13C-labeled amide carbonyl group(s). The frequency and dichroism of this band indicate that residues 39 and 46 are alpha-helical, with an axial orientation that is approximately 30 degrees relative to the membrane normal. Upon exposure to 2H2O (D2O), 30% of the peptide amide groups in hPLB undergo a slow deuterium/hydrogen exchange. The remainder of the protein, including the peptide groups of Leu-39 and Leu-42, appear inaccessible to exchange, indicating that most of the hPLB fragment is embedded in the lipid bilayer. By extending spectroscopic characterization of PLB to include hydrated, deuterated as well as site-directed isotope-labeled hPLB films, our results strongly support models of PLB that predict the existence of an alpha-helical hydrophobic region spanning the membrane domain.     

Fourier transform infrared evidence for a predominantly alpha-helical structure of the membrane bound channel forming COOH-terminal peptide of colicin E1.

The structure of the membrane bound state of the 178-residue thermolytic COOH-terminal channel forming peptide of colicin E1 was studied by polarized Fourier transform infrared (FTIR) spectroscopy. This fragment was reconstituted into DMPC liposomes at varying peptide/lipid ratios ranging from 1/25-1/500. The amide I band frequency of the protein indicated a dominant alpha-helical secondary structure with limited beta- and random structures. The amide I and II frequencies are at 1,656 and 1,546 cm-1, close to the frequency of the amide I and II bands of rhodopsin, bacteriorhodopsin and other alpha-helical proteins. Polarized FTIR of oriented membranes revealed that the alpha-helices have an average orientation less than the magic angle, 54.6 degrees, relative to the membrane normal. Almost all of the peptide groups in the membrane-bound channel protein undergo rapid hydrogen/deuterium (H/D) exchange. These results are contrasted to the alpha-helical membrane proteins, bacteriorhodopsin, and rhodopsin.