Improved frequency resolution in multidimensional constant-time experiments by multidimensional Bayesian analysis

Summary The resolution of spectral frequencies in NMR data obtained from discrete Fourier transformation (DFT) along D constant-time dimensions can be improved significantly through extrapolation of the D-dimensional free induction decay (FID) by multidimensional Bayesian analysis. Starting from Bayesian probability theory for parameter estimation and model detection of one-dimensional time-domain data [Bretthorst, (1990) J. Magn. Reson., 88, 533–551; 552–570; 571–595], a theory for the D-dimensional case has been developed and implemented in an algorithm called BAMBAM (BAyesian Model Building Algorithm in Multidimensions). BAMBAM finds the most probable sinusoidal model to account for the systematic portion of any D-dimensional stationary FID. According to the parameters estimated by the algorithm, the FID is extrapolated in D dimensions prior to apodization and Fourier transformation. Multidimensional Bayesian analysis allows for the detection of signals not resolved by the DFT alone or even by sequential one-dimensional extrapolation from mirror-image linear prediction prior to the DFT. The procedure has been tested with a theoretical two-dimensional dataset and with four-dimensional HN(CO)CAHA (Kay et al. (1992) J. Magn. Reson., 98, 443–450) data from a small protein (8 kDa) where BAMBAM was applied to the ¹³C and H constant-time dimensions.To whom correspondence should be addressed.     

Full 1H NMR assignment of a 24-nucleotide RNA hairpin: Application of the 1H 3D-NOE/2QC experiment

The subject RNA models the binding site for the coat protein of the R17 virus, as well as the ribosome recognition sequence for the R17 replicase gene. With an RNA of this size, overlaps among the sugar protons complicate assignments of the ¹H NMR spectrum. The cross peaks that overlap significantly in 2D-NOE spectra can frequently be resolved by introducing a third, in our approach the double-quantum, frequency axis. In particular the planes in a 3D-NOE/2QC spectrum perpendicular to the 2Q axis are extremely useful, showing a highly informative repeating NOE-2Q pattern. In this experiment substantial J-coupling confers special advantages. This always occurs for geminal pairs (H5/H5 for RNA plus H2/H2 for DNA), as well as for H5/H6, for H3/H4 in sugars with substantial populations of the N-pucker, for H1/H2 for S-puckered sugars, and usually for H2/H3. For the 24-mer RNA hairpin the additional information from the 3D-NOE/2QC spectrum allowed assignment of all of the non-exchangeable protons, eliminating the need for stable-isotope labeling.     

Solid-state NMR triple-resonance backbone assignments in a protein

Triple-resonance solid-state NMR spectroscopy is demonstrated to sequentially assign the 13C and 15N amide backbone resonances of adjacent residues in an oriented protein sample. The observed 13C chemical shift frequency provides an orientational constraint complementary to those measured from the 1H and 15N amide resonances in double-resonance experiments.     

Applications of tritium NMR to macromolecules: A study of two nucleic acid molecules

Summary We have tritium labeled two nucleic acid molecules, an 8 kDa DNA oligomer and a 20 kDa hammerhead RNA for tritium NMR investigations. The DNA sequence studied has been previously used in homonuclear studies of DNA-bound water molecules and tritium NMR was expected to facilitate these investigations by eliminating the need to suppress the water resonance in tritium-detected ³H-¹H NOESY experiments. We observed the anticipated through-space interactions found in B-form DNA in the NOESY experiments and an unexpected antiphase cross-peak at the water frequency. T₁ measurements on the tritiated DNA molecule indicated that relaxation rates were also accelerated for tritium and protons. Tritium NMR spectra of the hammerhead RNA molecule indicated conformational dynamics in the conserved region of the molecule in the absence of Mg²⁺ and spermine, two components necessary for cleavage. The dynamics were also investigated by ¹⁵N-correlated ¹H spectroscopy and persisted after the addition of Mg²⁺ and spermine.     

A high-resolution 1H NMR approach for structure determination of membrane peptides and proteins in non-deuterated detergent: Application to mastoparan X solubilized in n-octylglucoside

Summary Application of ¹H 2D NMR methods to solubilized membrane proteins and peptides has up to now required the use of selectively deuterated detergents. The unavailability of any of the common biochemical detergents in deuterated form has therefore limited to some extent the scope of this approach. Here a ¹H NMR method is described which allows structure determination of membrane peptides and small membrane proteins by ¹H 2D NMR in any type of non-deuterated detergent. The approach is based on regioselective excitation of protein resonances with DANTE-Z or spin-pinging pulse trains. It is shown that regioselective excitation of the amide-aromatic region of solubilized membrane proteins and peptides leads to an almost complete suppression of the two orders of magnitude higher contribution of the protonated detergent to the ¹H NMR spectrum. Consistently TOCSY, COSY and NOESY sequences incorporating such regioselective excitation in the F2 dimension yield protein ¹H 2D NMR spectra of quality comparable to those obtained in deuterated detergents. Regioselective TOCSY and NOESY spectra display all through-bond and through-space correlations within amide-aromatic protons and between these protons and aliphatic and -protons. Regioselective COSY spectra provide scalar coupling constants between amide and -protons. Application of the method to the membrane-active peptide mastoparan X, solubilized in n-octylglucoside, yields complete sequence-specific assignments and extensive secondary structure-related spatial proximities and coupling constants. It is shown that mastoparan adopts an -helical conformation when bound to nonionic detergent micelles. The present method is expected to increase the applicability of ¹H solution NMR methods to membrane proteins and peptides.Abbreviations 2D NMR two-dimensional NMR - COSY correlated spectroscopy - DANTE delays alternating nutations for tailored excitation - NOESY nuclear Overhauser enhancement spectroscopy - TOCSY total correlation spectroscopy     

Mating behaviour of Ctenomyces serratus

Nineteen isolates of Ctenomyces serratus including three pairs of tester strains were crossed in all possible combinations on diluted Pablum cereal agar with added salts, oatmeal salts agar-Medium E, and soil and hair medium. Out of 190 crosses, 18 were fertile and the remaining 172 were sterile. Of the 19 isolates, seven were– mating type, 11 were + mating type, and one (UAMH 1959) was non-fertile with the other isolates. The high degree of non-fertile crosses among the 19 isolates shows that the use of mating reactions for the identification of conidial isolates of C. serratus may not be a practical tool. unless a large number of isolates belonging to both the mating types are employed. The production of exudate droplets in the fertile crosses seemed to be correlated with the degree of mating response. Ascocarp morphology corresponded closely to that of a cleistothecium, because of the completely closed nature. Ascospores were quite alike in their size, but they differed in shape, depending on their orientation.     

Development of a method for reconstruction of crowded NMR spectra from undersampled time-domain data

NMR is a unique methodology for obtaining information about the conformational dynamics of proteins in heterogeneous biomolecular systems. In various NMR methods, such as transferred cross-saturation, relaxation dispersion, and paramagnetic relaxation enhancement experiments, fast determination of the signal intensity ratios in the NMR spectra with high accuracy is required for analyses of targets with low yields and stabilities. However, conventional methods for the reconstruction of spectra from undersampled time-domain data, such as linear prediction, spectroscopy with integration of frequency and time domain, and analysis of Fourier, and compressed sensing were not effective for the accurate determination of the signal intensity ratios of the crowded two-dimensional spectra of proteins. Here, we developed an NMR spectra reconstruction method, “conservation of experimental data in analysis of Fourier” (Co-ANAFOR), to reconstruct the crowded spectra from the undersampled time-domain data. The number of sampling points required for the transferred cross-saturation experiments between membrane proteins, photosystem I and cytochrome b ₆ f, and their ligand, plastocyanin, with Co-ANAFOR was half of that needed for linear prediction, and the peak height reduction ratios of the spectra reconstructed from truncated time-domain data by Co-ANAFOR were more accurate than those reconstructed from non-uniformly sampled data by compressed sensing.     

A maximum likelihood approach to non-linear ordination

Summary A non-linear method of ordinating vegetation samples based on the fitting of bell-shaped response curves is lescribed. For each species two Gaussian curves were itted, one to quantitative values, where the species was present, the other to probabilities of absence. A maximum likelihood approach was then used to obtain a best approximation of the positions of the samples along a one-dimensional gradient. By an iterative process successively better approximations were obtained.The method was successful in recovering gradients based on hypothetical data. With two sets of real data the gradient produced was more ecologically satisfying and far less distorted than that revealed by principal component analysis.     

1H NMR studies of the mercuric ion binding protein MerP: Sequential assignment,secondary structure and global fold of oxidized MerP

Summary The oxidized form of the mercuric ion binding protein MerP has been studied by two-dimensional NMR. MerP, which is a periplasmic water-soluble protein with 72 amino acids, is involved in the detoxification of mercuric ions in bacteria with resistance against mercury. The mercuric ions in the periplasmic space are first scavenged by the MerP protein, then transported into the cytoplasm by the membrane-bound transport protein MerT, and finally reduced to elementary (nontoxic) mercury by the enzyme mercuric reductase. In this work, the ¹H NMR spectrum of oxidized MerP (closed disulfide bridge) has been assigned by using homonuclear 2D NMR techniques. The secondary structure and global fold have been inferred from the nuclear Overhauser effect (NOE) data. The secondary structure comprises four -strands and two -helices, in the order ₁₁₂₃₂₄. The protein folds into an antiparallel -sheet, ₂₃₁₄, with the two antiparallel helices on one side of the sheet. The folding topology is similar to that of acylphosphatase, the activation domain of porcine pancreatic procarboxypeptidase B, the DNA-binding domain of bovine papillomavirus-1 E2 and the RNA-binding domains of the U1 snRNP A and hnRNP C proteins. However, there is no structural similarity between MerP and other bacterial periplasmic binding proteins.     

Microbiological synthesis of 5-ethyl- and (E)-5-(2-bromovinyl)-2′-deoxyuridine

Summary The title compounds were prepared by an enzymatic transdeoxyribosylation from 2 dGuo or 2 dThd to the respective heterocyclic bases, 5-ethyluracil and (E)-5-(2-bromovinyl)uracil, using the whole bacterial cells ofEscherichia coli as a biocatalyst.     

Backbone dynamics of the cytotoxic ribonuclease alpha-sarcin by 15N NMR relaxation methods

The cytotoxic ribonuclease -sarcin is a 150-residue protein that inactivates ribosomes by selectively cleaving a single phosphodiester bond in a strictly conserved rRNA loop. In order to gain insights on the molecular basis of its highly specific activity, we have previously determined its solution structure and studied its electrostatics properties. Here, we complement those studies by analysing the backbone dynamics of -sarcin through measurement of longitudinal relaxation rates R₁, off resonance rotating frame relaxation rates R₁, and the ¹⁵N¹HNOE of the backbone amide ¹⁵N nuclei at two different magnetic field strengths (11.7 and 17.6 T). The two sets of relaxation parameters have been analysed in terms of the reduced spectral density mapping formalism, as well as by the model-free approach. -Sarcin behaves as an axial symmetric rotor of the prolate type (D/D=1.16 ± 0.02) which tumbles with a correlation time _m of 7.54 ± 0.02 ns. The rotational diffusion properties have been also independently evaluated by hydrodynamic calculations and are in good agreement with the experimental results. The analysis of the internal dynamics reveals that -sarcin is composed of a rigid hydrophobic core and some exposed segments which undergo fast (ps to ns) internal motions. Slower motions in the s to ms time scale are less abundant and in some cases can be assigned to specific motional processes. All dynamic data are discussed in relation to the role of some particular residues of -sarcin in the process of recognition of its ribosomal target.     

Backbone dynamics of bacteriorhodopsin as studied by <Superscript>13</Superscript>C solid-state NMR spectroscopy

The surface dynamics of bacteriorhodopsin was examined by measurements of site-specific ¹³C–¹H dipolar couplings in [3-¹³C]Ala-labeled bacteriorhodopsin. Motions of slow or intermediate frequency (correlation time <50 µs) scale down ¹³C–¹H dipolar couplings according to the motional amplitude. The two-dimensional dipolar and chemical shift (DIPSHIFT) correlation technique was utilized to obtain the dipolar coupling strength for each resolved peak in the ¹³C MAS solid-state NMR spectrum, providing the molecular order parameter of the respective site. In addition to the rotation of the Ala methyl group, which scales the dipolar coupling to 1/3 of the rigid limit value, fluctuations of the C–C vector result in additional motional averaging. Typical order parameters measured for mobile sites in bacteriorhodopsin are between 0.25 and 0.29. These can be assigned to Ala103 of the C–D loop and Ala235 at the C-terminal -helix protruded from the membrane surface, and Ala196 of the F–G loop, as well as to Ala228 and Ala233 of the C-terminal -helix and Ala51 from the transmembrane -helix. Such order parameters departing significantly from the value of 0.33 for rotating methyl groups are obviously direct evidence for the presence of fluctuation motions of the Ala C–C vectors of intact preparations of fully hydrated, wild-type bacteriorhodopsin at ambient temperature. The order parameter for Ala160 from the expectantly more flexible E–F loop, however, is unavailable under highest-field NMR conditions, probably because increased chemical shift anisotropy together with intrinsic fluctuation motions result in an unresolved ¹³C NMR signal.     

Spectral properties of conformational motion in proteins

The conformational dynamics of large fragments of protein structure within the framework of a generalized model of bounded diffusion (GMBD) have been considered. This model is a development of the known ordinary model of bounded diffusion (MBD). The latter model assumes that the driving force of motion, which is at the same time a source of friction, has negligibly small correlation time (white noise). In contrast to the MBD, the GMBD takes into account the finite character of friction correlation time, i.e. memory friction effects. Two different mechanisms of friction for the fragment are considered: (1) friction by rapid density fluctuations due to the harmonic vibrational motion of atoms and (2) friction by slow encounters with surrounding fragments of protein structure. The present theory shows that at high frequencies the power decay of the spectrum which takes place in the MBD is replaced by an exponential one. In the narrow intermediate frequency range the results of the GMBD coincide with those of the MBD. At low frequencies the results of the two models differ quantitatively, though their qualitative behaviour is similar.     

Spectral characteristics of phytochrome in vivo and in vitro

The absorption maximum of the far-red absorbing form of phytochrome in the difference spectrum for phototransformation (Pfr max) was investigated in vivo and in in vitro pellets from dark grown Hordeum vulgare L. primary leaves. Exposure of pellets in Honda medium from tissue pre-irradiated with red light to far red light gave a Pfr max of 734 nm, a slightly longer wavelength than was seen in vivo (730 nm). After incubation as the red absorbing form of phytochrome (Pr) for 2 h at 0° C irradiation with red light showed that Pfr max had shifted to shorter wavelength (716 nm) in Honda medium. Further incubation as Pfr for 2 h at 0° C and irradiation with far red light showed that Pfr max had shifted to longer wavelength (726 nm). Similar shifts were also seen in other media, although the peak positions were different. Phytochrome remained pelletable throughout these experiments and Pfr max is compared to that of soluble phytochrome in similar media. The results are interpreted as indicating changes in molecular environment of the putative phytochrome membrane receptor site and that Pfr max can be used to probe the nature of this binding.Abbreviations D Dark - EDTA Ethylene diamine tetra-acetic acid - F far red light - MOPS N-morpholino-3-propane-sulphonic acid - P Phytochrome - Pr red absorbing form of P - Pfr far red absorbing form of P - Pfr max wavelength maximum of Pfr absorbance in a phototransformation difference spectrum - R red light     

Determination of the electron self-exchange rates of blue copper proteins by super-WEFT NMR spectroscopy

An NMR approach for determining the electron self-exchange (ESE) rate constants in blue copper proteins is presented. The approach uses the paramagnetic relaxation enhancement of resonances in 1D ¹H super-WEFT spectra of partly oxidized (paramagnetic) proteins. These spectra allow a more precise determination of the relevant paramagnetic linebroadenings than conventional 1D ¹H spectra and, thus, permit a more detailed investigation of the applicability of the linebroadenings for determining the electron exchange rates. The approach was used to estimate the ESE rate constant of plastocyanin from Anabaena variabilis. It was found that, although the rate constant can be determined accurately from a series of resonances, precise but erroneous constants are obtained from the resonances of the copper-bound residues, unless a narrow splitting of these resonances caused by the presence of two conformations is taken into account. As demonstrated here, this complication can be overcome by a correct analysis of the paramagnetic broadening of the combined double signals. Because of the high resolution and specific sensitivity of the approach it should be generally applicable to estimate electron transfer rates, k, if the paramagnetic relaxation enhancement R _2p of the resonances can be determined, and the conditions kR _2p or _pkR _2p are fulfilled, _p being the frequency separation between corresponding diamagnetic and paramagnetic sites.     

NMR investigation of the heme electronic structure in deoxymyoglobin possessing a fluorinated heme

The heme electronic structures of deoxymyoglobins (deoxy-Mbs) reconstituted with 13,17-bis(2-carboxylatoethyl)-3,8-diethyl-2,12,18-trimethyl-7-(trifluoromethyl)porphyrinatoiron(III) (7-PF), 13,17-bis(2-carboxylatoethyl)-3,7-difluoro-2,8,12,18-tetramethylporphyrinatoiron(III) (3,7-DF), and 13,17-bis(2-carboxylatoethyl)-3,8-diethyl-2-fluoro-7,12,18-trimethylporphyrinatoiron(III) (2-MF) have been characterized by ¹H and ¹⁹F NMR. The analysis of heme methyl proton shift patterns of the hemes in their bis-cyano forms demonstrated that, owing to the substitution of a strongly electron-withdrawing perfluoromethyl group, CF₃, to porphyrin, the porphyrin -system of 7-PF is more significantly distorted from four-fold symmetry than those of the ring-fluorinated hemes, 3,7-DF and 2-MF. The presence of the heme orientation disorder resulted in the observation of the two well-resolved ¹⁹F signals in the spectra of deoxy-Mbs possessing 7-PF and 2-MF. The ¹⁹F signals of deoxy-Mb possessing 7-PF exhibited a relatively large difference in paramagnetic shift (~30 ppm), despite their small paramagnetic shifts (~30 ppm), supporting the significant contribution of a spin delocalization mechanism in this Mb due to the d-electron configuration derived from the ⁵E ground state. On the other hand, ¹⁹F signals of deoxy-Mbs with 3,7-DF as well as 2-MF exhibited large paramagnetic shifts (~250 ppm) with a relatively small difference in the paramagnetic shift (~20 ppm), indicating the predominant contribution of spin delocalization, due to a d-electron configuration derived from the ⁵B₂ ground state. These results demonstrate for the first time that the relative contributions of the orbital ground states derived from ⁵E and ⁵B₂ states to the heme electronic structure in deoxy-Mb are affected by the distortion of the porphyrin -system exerted by chemical properties of the heme peripheral side-chains.Abbreviations 3,7-DF 13,17-bis(2-carboxylatoethyl)-3,7-difluoro-2,8,12,18-tetramethylporphyrinatoiron(III) - 2-MF 13,17-bis(2-carboxylatoethyl)-3,8-diethyl-2-fluoro-7,12,18-trimethylporphyrinatoiron(III) - 7-PF 13,17-bis(2-carboxylatoethyl)-3,8-diethyl-2,12,18-trimethyl-7-(trifluoromethyl)porphyrinatoiron(III) - Mb myoglobin - Mb(7-PF) deoxy-Mb reconstituted with 7-PF - Mb(3,7-DF) deoxy-Mb reconstituted with 3,7-DF - Mb(2-MF) deoxy-Mb reconstituted with 2-MF - NOE nuclear Overhauser effect - NOESY nuclear Overhauser effect correlated spectroscopy     

Adding teeth to wave action: the destructive effects of wave-borne rocks on intertidal organisms

Summary Observations in rocky intertidal areas demonstrate that breaking waves throw rocks and cobbles and that these missiles can damage and kill organisms. Targets in the intertidal were dented by impacts from wave-borne rocks. New dents/day in these targets was positively correlated with the daily maximum significant wave height and with new patches/day in aggregations of the barnacle Chthamalus fissus. Impact frequency was highest in the upper intertidal and varied dramatically between microhabitats on individual boulders (edges, tops and faces). These patterns were reflected in the microhabitat abundances of old and young barnacles. Comparisons were made of the survivorship and the frequency of shell damage in two populations of the limpet Lottia gigantea living in habitats which differed primarily in the number of moveable rocks (i.e. potential projectiles). The mortality rate and frequency of shell damage were significantly higher in the projectilerich habitat. In addition only in this habitat did the frequency of shell damage covary significantly with seasonal periods of high surf. Investigation of the response of limpet shells to impacts suggests that shell strength varies between species and increases with shell size. Species-specific patterns of non-fatal shell breakage may have evolved to absorb the energy of impacts. In two of the intertidal habitats studied, wave-borne rock damage was chronic and, at least in part, may have governed the faunal makeup of the community by contributing to the physical boundaries of the environment within which the inhabitants must survive.     

Fluoride transmembrane exchange in human erythrocytes measured with 19F NMR magnetization transfer

¹⁹F NMR spectra of sodium fluoride in suspensions of human erythrocytes were seen to yield separate resonances for the F^- populations inside and outside the cells. Selective saturation of the magnetization of the intracellular population gave rise to transfer of that saturation to the extracellular population. The extent of magnetization transfer was high and it was blocked by the capnophorin (band 3) anion exchange inhibitor 4,4-dini-trostilbene-2,2-disulfonic acid (DNDS). A series of magnetization-inversion transfer experiments was carried out for the range of intracellular fluoride concentrations of 11 mM to 136 mM and analysed using one-dimensional overdetermined exchange analysis. This yielded an estimate of the equilibrium exchange Michaelis constant and maximal velocity of 27 ± 3 mM and 180 ± 5 × 10^-16 mol cell^-1 s^-1, respectively. There was no alteration of exchange flux of fluoride at an intracellular concentration of 49 mM in the presence of 50 mM glucose; thus suggesting no interaction between glucose and anions in capnophorin-mediated exchange of solutes.     

Gene expression, cellular localization, and enzymatic activity of diacylglycerol kinase isozymes in rat ovary and placenta

Female reproductive organs show remarkable cyclic changes in morphology and function in response to a combination of hormones. Evidence has accumulated suggesting that phosphoinositide turnover and the consequent diacylglycerol (DG) protein kinase C (PKC) pathway are intimately involved in these mechanisms. The present study has been performed to investigate the gene expression, cellular localization, and enzymatic activity of the DG kinase (DGK) isozymes that control the DG-PKC pathway. Gene expression for DGK, -, -, and - was detected in the ovary and placenta. Intense expression signals for DGK and - were observed in the theca cells and moderate signals in the interstitium and corpora lutea of the ovary. On the other hand, signals for DGK were seen more intensely in granulosa cells. In the placenta, signals for DGK and - were observed in the junctional zone, whereas those for DGK were detected in the labyrinthine zone. At higher magnification, the signals for DGK were mainly discerned in giant cytotrophoblasts, and those for DGK were found in small cytotrophoblasts of the junctional zone. DGK signals were observed in all cellular components of the labyrinthine zone, including mesenchyme, trabecular trophoblasts, and cytotrophoblasts. DGK signals were detected in the junctional zone on day 13 and 15 of pregnancy and were diffusely distributed both in the labyrinthine and junctional zones at later stages. The present study reveals distinct patterns of mRNA localization for DGK isozymes in the rat ovary and placenta, suggesting that each isozyme plays a unique role in distinct cell types in these organs.This work was supported by Grants-in-Aids from the Ministry of Education, Culture, Sports, Science, and Technology (MEXT) of Japan, the Uehara Memorial Foundation, the ONO Medical Research Foundation, the Ciba-Geigy Foundation (Japan) for the Promotion of Science, the Kato Memorial Bioscience Foundation, and the Yamagata Health Support Foundation (to K.G.).     

Analysis of local conformation of membrane-bound and polycrystalline peptides by two-dimensional slow-spinning rotor-synchronized MAS exchange spectroscopy

2D slow-spinning, rotor-synchronized MAS exchange spectroscopy (SSRS-MASE) was applied to study local secondary structure of three structurally different peptides, two of which were membrane-bound. Each peptide was ¹³C carbonyl labeled at two adjacent residues in the peptide backbone. In general, this methodology is attractive for membrane-bound peptides because of its lenient spinning, decoupling, and RF homogeneity requirements.For a single set of raw SSRS-MASE data, two linearly independent methods exist for obtaining a 2D spectrum and each spectrum can be fit to obtain conformational constraints. An approach is described for combining the results of these two fits and this method is shown to work for spectra with both resolved and unresolved labeled site resonances. A spectrum is often fit well to a few different conformations which have somewhat different values of the fitting parameter ². A simple statistical theory is developed which relates the ² difference between a local minimum and the global minimum ² to the likelihood that the local minimum conformation is the correct structure. Because uncertainty in the simulated data can also contribute to the overall fitting uncertainty, an empirical method is described for incorporating the simulation uncertainty into the ² analysis.These data analysis methods were tested on polycrystalline Ala-Gly-Gly and then applied to the membrane-bound melittin and HIV-1 fusion peptides. Melittin gave a best-fit helical structure at Ala-4 while the fusion peptide gave a good-fit strand structure at Phe-8. The melittin analysis is in agreement with the known overall structure of this peptide.