Secondary structure of the membrane-bound form of the pore-forming domain of colicin A. An attenuated total-reflection polarized Fourier-transform infrared spectroscopy study.

The structure of the pore-forming domain of the bacterial toxin colicin A was studied by attenuated total-reflection polarized Fourier-transform infrared spectroscopy. This channel-forming fragment interacts with dimyristoylglycerophosphoglycerol (Myr2GroPGro) vesicles and forms disk-like complexes. Analysis of the shape of the amide I' band indicates that its secondary structure is not affected by the pH 5.0-7.2. However, 5-10% of the peptide amino acids adopt an alpha-helical structure upon complex formation with Myr2GroPGro, while the random-coil and beta-sheet structure contents decrease. Interestingly, the increase in alpha-helical content is essentially due to an increase in the high-frequency component of the alpha-helical domain of amide I'. The fact that only this component was 90 degrees polarized (i.e. the helix is parallel to the acyl chain) suggests that only this particular type of helix is associated with the Myr2GroPGro bilayer.     

Conformational analysis of melittin in solution phase: vibrational circular dichroism study

The vibrational absorption and vibrational circular dichroism (VCD) spectra of melittin in D(2)O solutions at different pH values, different salt concentrations, or different 2,2,2-trifluoroethanol (TFE) concentrations are recorded in the amide I' (1850-1600 cm(-1)) region. Two models are used to simulate this peptide in different conditions, and a coupled oscillator program is used to obtain the calculated absorption and VCD spectra. This study indicates that melittin adopts a mixed structure in D(2)O solution at low pH, low salt concentration, or low TFE concentration. With an increase in pH, salt concentration, or TFE concentration, the structure changes to alpha-helix and further increases lead to aggregation. These results demonstrate the versatility of VCD in probing the conformations of peptides under different environmental perturbations.     

Estimation of beta-structure content of proteins by means of deconvolved FTIR spectra

Fourier self-deconvolution was applied to the infrared spectra of five globular proteins with a high beta-structure content and to the essentially alpha-helical protein hemoglobin. The featureless amide I' bands around 1650 cm-1 were thereby resolved into six to nine components, depending on the protein. Specific components were assigned to the beta-structure segments in each protein. The frequencies and the number of 'beta-bands' differ from one protein to another. The areas of the components were evaluated by means of a Gauss-Newton iteration procedure. It appears that the total area of the beta-bands, as a fraction of the total amide I' band area, reflects the relative beta-structure content of each protein studied.     

Redox-induced conformational changes in plastocyanin: an infrared study.

The conformational changes associated with the redox transition of plastocyanin (PC) were investigated by absorption and reaction-induced infrared spectroscopy. In addition to spectral features readily ascribed to beta and turn protein secondary structures, the amide I band shows a major component band at 1647 cm(-1) in both redox states of the protein. The sensitivity of this component to deuteration and increasing temperature suggests that PC adopts an unusual secondary structure in solution, which differs from those described for other type I copper proteins, such as azurin and halocyanin. The conformations of oxidized and reduced PC are different, as evidenced (1) by analysis of their amide I band contour and the electrochemically induced oxidized-minus-reduced difference spectrum and (2) by their different thermal stability. The redox-induced difference spectrum exhibits a number of difference bands within the conformationally sensitive amide I band that could be assigned to peptide C=O modes, in light of their small shift upon deuteration, and to signals attributable to side chain vibrational modes of Tyr residues. Lowering the pH to 4.8 induces destabilization of both redox states of the protein, more pronounced for reduced PC, without significantly affecting their secondary structure. Besides the conformational differences obtained at neutral pH, the oxidized-minus-reduced difference spectrum shows two broad and strong negative bands at 1405 and 1571 cm(-1), assigned to COO(-) vibrations, and a broad positive band at 1710 cm(-1), attributed to the C=O vibration of a COOH group(s). These bands are indicative of a protonation of (an) Asp or Glu side chain(s) upon plastocyanin oxidation at acidic pH.     

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.     

Pressure-induced transformation of alpha-helix to beta-sheet in the secondary structures of amyloid beta (1-40) peptide exacerbated by temperature

The effect of pressure on the conformational structure of amyloid beta (1-40) peptide (A beta(1-40)), exacerbated with or without temperature, was determined by Fourier transform infrared (FT-IR) microspectroscopy. The result indicates the shift of the maximum peak of amide I band of intact solid A beta(1-40) from 1655 cm(-1) (alpha-helix) to 1647-1643 cm(-1) (random coil) with the increase of the mechanical pressure. A new peak at 1634 cm(-1) assigned to beta-antiparallel sheet structure was also evident. Furthermore, the peak at 1540 cm(- 1) also shifted to 1527 (1529) cm(-1) in amide II band. The former was assigned to the combination of alpha-helix and random coil structures, and the latter was due to beta-sheet structure. Changes in the composition of each component in the deconvoluted and curve-fitted amide I band of the compressed A beta(1-40) samples were obtained from 33% to 22% for alpha-helix/random coil structures and from 47% to 57% for beta-sheet structure with the increase of pressure, respectively. This demonstrates that pressure might induce the conformational transition from alpha-helix to random coil and to beta- sheet structure. The structural transformation of the compressed A beta(1-40) samples was synergistically influenced by the combined effects of pressure and temperature. The thermal-induced formation of beta-sheet structure was significantly dependent on the pressures applied. The smaller the pressure applied the faster the beta-sheet structure transformed. The thermal-dependent transition temperatures of solid A beta(1-40) prepared by different pressures were near 55-60 degrees C.     

Salmon calcitonin and amyloid beta: two peptides with amyloidogenic capacity adopt different conformational manifolds in their unfolded states

The molecular conformations of salmon calcitonin in aqueous solution have been investigated by exploiting the different influences of excitonic coupling on the amide I band profile in the isotropic and anisotropic Raman, FTIR, and vibrational circular dichroism spectra of a polypeptide. The N-terminal loop, caused by a disulfide bridge between cysteines at positions 1 and 7, was modeled by performing a conformational search by molecular mechanics calculations. The remaining part of the peptide chain was modeled as a mixture of three sequences containing different fractions of residues adopting poly-l-proline II (PPII), extended beta-strand, and alpha-helix-like conformations. This yielded an excellent reproduction of the experimentally observed amide I' band profiles. A comparison with recent data on the beta-amyloid fragment Abeta(1)(-)(28) revealed a lower PPII content and more conformational heterogeneity for calcitonin. Thus, our results underscore the notion that individual structural propensities of amino acid residues give rise to structural differences between the unfolded states of even long peptide chains, at variance with expectations based on a random or statistical coil model.     

Centrin: its secondary structure in the presence and absence of cations

Centrin is a low molecular mass (20 kDa) protein that belongs to the EF-hand superfamily of calcium-binding proteins. Local and overall changes were investigated for interactions between cations and Chlamydomonas centrin using Fourier transform infrared (FT-IR) and circular dichroic (CD) spectroscopies. FT-IR spectral features studied included the amide I' band and the side-chain absorbances for aspartate residues located almost exclusively at the calcium-binding sites in the spectral region of 1700-1500 cm(-1). The amide I' band is exquisitely sensitive to changes in protein secondary structure and is observed to shift from 1626.5 to 1642.7 cm(-1) in the presence and absence of calcium. These spectral bands are complex and were further studied using two-dimensional Fourier transform infrared (2D-FT-IR) correlation along with curve-fitting routines. Using these methods the secondary structure contributions were determined for holocentrin and apocentrin. The alpha-helical content in centrin was determined to be 60%-53% in the presence and absence of cations, respectively. Furthermore, the beta-strand content was determined to be 12%-36%, while the random coil component remained almost constant at 7%-13.5% in the presence and absence of cations, respectively. Changes in the side-chain band are mostly due to the monodentate coordination of aspartate to the cation. A shift of approximately 4 cm(-1) (for the COO- antisymmetric stretch in Asp) from 1565 to 1569 cm(-1) is observed for apocentrin and holocentrin, respectively. Thermal dependence revealed reversible conformational transition temperatures for apocentrin at 37 degrees C and holocentrin at 45 degrees C, suggesting greater stability for holocentrin.     

Fourier transform infrared spectroscopy for the characterization of a model peptide-DNA interaction

To better understand the structural basis of protein-DNA interactions, the conformational changes that accompany these interactions need to be described. In order to develop a methodological approach to this problem, Fourier transform infrared spectroscopy (FTIR) with derivative resolution enhancement has been used to identify conformational changes that occur when a 29-residue synthetic peptide binds nonspecifically to heterogeneous cellular DNA in aqueous solution. The peptide sequence was chosen de novo, in order to rationally design a peptide model that would allow the relationship between DNA binding and the stability of protein secondary structure to be studied. Peptide at a concentration of 100-200 microM produces 50% saturation of heterogeneous phage DNA sequences as well as of short synthetic oligonucleotides. FTIR spectra reveal significant changes in peptide and DNA upon binding. Second-derivative spectra resolve the amide I band of native peptide into components located at 1627 (beta-strand), 1658 (alpha-helix), and 1681 (turn or beta-strand) cm-1, with a distinct shoulder at 1647 cm-1 (disordered structure). Assignment of the 1681 cm-1 vibration to a turn conformation is supported by uv CD studies, which indicate significant amounts of turn structure in unbound peptide. Ultraviolet CD also confirms the existence of disordered and beta-strand regions in the free peptide. Upon interacting with DNA the band at 1681 cm-1 (turn) is no longer seen; a new band appears at 1675 cm-1; the 1627 cm-1 band (beta-strand) is considerably reduced in intensity; the position of the alpha-helical (1658 cm-1) component remains unchanged; the shoulder at 1647 cm-1 (disorder) disappears. The new vibration at 1675 cm-1 is characteristic of beta-strand structures. The asymmetric stretch (vAS) of the DNA phosphates shifts from 1223 (unbound) to 1229 cm-1 (bound); the relative intensities of vAS and the PO2- symmetric stretch (vS) are altered upon peptide binding.(ABSTRACT TRUNCATED AT 400 WORDS)     

Study of the secondary structure of the C-terminal domain of the antiapoptotic protein bcl-2 and its interaction with model membranes

Bcl-2 is a protein which inhibits programmed cell death. It is associated to many cell membranes such as mitochondrial outer membrane, endoplasmic reticulum, and nuclear envelope, apparently through a C-terminal hydrophobic domain. We have used infrared spectroscopy to study the secondary structure of a synthetic peptide (a 23mer) with the same sequence as this C-terminal domain (residues 217-239) of Bcl-2. The spectrum of this peptide in D(2)O buffer shows an amide I' band with a maximum at 1622 cm(-1), which clearly indicates its tendency to aggregate in aqueous solvent. However, the peptide incorporated in multilamellar phosphatidylcholine membranes shows a totally different spectrum of the amide I' band, with a maximum at 1655 cm(-)(1), indicating a predominantly alpha-helical structure. Addition of the peptide to unilamellar vesicles destabilized them and released encapsulated carboxyfluorescein. Differential scanning calorimetry of dimyristoylphosphatidylcholine multilamellar vesicles in which the peptide was incorporated revealed that increasing concentrations of the peptide progressively broadened the pretransition and the main transition, as is to be expected for a membrane integral molecule. Fluorescence polarization of 1,6-diphenyl-1,3,5-hexatriene in fluid phosphatidylcholine vesicles showed that increasing concentrations of the peptide produced increased polarization values, pointing to an increase in the apparent order of the membrane and indicating that high concentrations of the peptide considerably broaden the phase transition of dimyristoylphosphatidylcholine multilamellar vesicles. Quenching the intrinsic fluorescence of the Tyr-235 of the peptide, by KI, indicated that this aminoacyl residue is highly exposed to aqueous solvent when incorporated in phospholipid vesicles. The results are discussed in terms of their relevance to the proposed topology of insertion of Bcl-2 into biological membranes.     

Synthesis and spectroscopy of membrane receptor proteins. The gamma subunit of the IgE receptor.

The high-affinity receptor for IgE is a tetrameric complex of subunits of the type alpha beta gamma 2. We report here conformational studies of the intact gamma subunit in trifluoroethanol and water/liposomes by circular dichroism and Fourier-transform infrared (FTIR) spectroscopy. In trifluoroethanol, the FTIR amide I' frequencies were consistent with two predominant conformational components, the beta-turn and alpha-helix, whilst in liposomes consisting of D2O and dimyristoylglycerophosphocholine (Myr2GroPCho), three components were observed. The third component present may contain some left-handed extended helix. Spectral simulation was carried out to demonstrate that the CD spectra were consistent with the component conformations identified from FTIR spectroscopy. The stimulated CD spectra were in excellent agreement with the experimental spectra. The intact gamma subunit conformation in trifluoroethanol was shown to possess 72% alpha-helical and 28% beta-turn conformations. In water/Myr2GroPCho liposomes the percentage of each conformational component present is 37%, 38% and 25% for the alpha-helix, beta-turn and extended structures, respectively. Assuming that the transmembrane fragment was alpha-helical, an excellent correlation was found between this derived alpha-helical content in water/liposomes (37%) and from hydrophobicity plots where the percentage of amino acids in the transmembrane domain is predicted by others to be 34%. It is suggested that the beta-turn detected by CD and FTIR was attributable to a 3(10) helix rather than a type I or type III reverse turn.     

Conformational analysis of a mitochondrial presequence derived from the F1-ATPase beta-subunit by CD and NMR spectroscopy.

Previous studies on mitochondrial targeting presequences have indicated that formation of an amphiphillic helix may be required for efficient targeting of the precursor protein into mitochondria, but the structural details are not well understood. We have used CD and NMR spectroscopy to characterize in detail the structure of a synthetic peptide corresponding to the presequence for the beta-subunit of F1-ATPase, a mitochondrial matrix protein. Although this peptide is essentially unstructured in water, alpha-helix formation is induced when the peptide is placed in structure-promoting environments, such as SDS micelles or aqueous trifluoroethanol (TFE). In 50% TFE (by volume), the peptide is in dynamic equilibrium between random coil and alpha-helical conformations, with a significant population of alpha-helix throughout the entire peptide. The helix is somewhat more stable in the N-terminal part of the presequence (residues 4-10), and this result is consistent with the structure proposed previously for the presequence of another mitochondrial matrix protein, yeast cytochrome oxidase subunit IV. Addition of increasing amounts of TFE causes the alpha-helical content to increase even further, and the TFE titration data for the presequence peptide of the F1-ATPase beta-subunit are not consistent with a single, cooperative transition from random coil to alpha-helix. There is evidence that helix formation is initiated in two different regions of the peptide. This result helps to explain the redundancy of the targeting information contained in the presequence for the F1-ATPase beta-subunit.     

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.     

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).     

Synthesis and secondary structural studies of penta(acetyl-Hmb)A beta(1-40).

The Fmoc solid phase synthesis of A beta(1-40), a strongly aggregating peptide found in Alzheimer's disease brain, was performed using 2-hydroxy-4-methoxybenzyl (Hmb) backbone amide protection. Hmb-Gly residues were incorporated using N(alpha)-Fmoc-Hmb-Gly-OH rather than N,O-bisFmoc-Hmb-Gly-OPfp. Amino acid acylation of the sterically hindered Hmb-amino acids was monitored using 'semi-on-line' MALDI-TOF-MS in a novel application of this technique which significantly simplified the successful incorporation of these residues. Standard coupling conditions in N,N-dimethylformamide (DMF) were used throughout the synthesis. Comparative structural studies of acetyl-Hmb-protected and native A beta(1-40) were performed to investigate the structural basis of Hmb-mediated disaggregation. The incorporation of backbone amide protection was observed by circular dichroism spectroscopy and gel electrophoresis to strongly affect the solution structure of A beta(1-40). Despite the reported structure-breaking activity of Hmb groups, penta(acetyl-Hmb)A beta(1-40) was found to adopt both alpha-helix and intermolecular beta-sheet conformations. In 100% TFE a mixed alpha-helix/random coil structure was formed by the protected peptide indicating reduced alpha-helical propensity relative to A beta(1-40). The protected peptide formed beta-sheet structures in aqueous buffer. Gel electrophoresis indicated that, unlike native A beta(1-40), penta(acetyl-Hmb)A beta(1-40) did not form large aggregate species.     

Spectroscopic evidence for backbone desolvation of helical peptides by 2,2,2-trifluoroethanol: an isotope-edited FTIR study

2,2,2-Trifluoroethanol (TFE) is widely used to induce helix formation in peptides and proteins, but the mechanism behind this effect is still poorly understood. Several recent papers have proposed that TFE acts by selectively desolvating the peptide backbone groups of the helix state. Infrared (IR) spectroscopy of the amide I band of polypeptides can be used to probe both secondary structure and backbone solvation, making this technique well suited for addressing the effect of TFE on polypeptide conformation. In this paper, we report the IR spectra as a function of TFE concentration for an alanine-rich peptide based on the repeat (AAKAA)(n)(). The IR spectra confirm that TFE desolvates the helical state of the peptide to a greater extent than the random coil state. Moreover, using a series of specifically (13)C-labeled peptides, the precise residues desolvated in the presence of TFE were identified. The residues most desolvated by TFE are the alanines located at position i - 4 in the sequence, where i is a lysine residue. This pattern of desolvation is consistent with molecular dynamics simulations which predict strong interactions between the lysine side chain at position n and the backbone carbonyl of the alanine at position i - 4. This is the first direct spectroscopic evidence of specific desolvation of helix backbone atoms in model alanine-rich peptides.     

Abeta(1-28) fragment of the amyloid peptide predominantly adopts a polyproline II conformation in an acidic solution

To structurally characterize the nonaggregated state of the amyloid beta peptide, which assembles into the hallmark fibrils of Alzheimer disease, we investigated the conformation of the N-terminal extracellular peptide fragment Abeta(1-28) in D(2)O at acidic pD by utilizing combined FTIR and isotropic and anisotropic Raman spectra measured between 1550 and 1750 cm(-1). Peptide aggregation is avoided under the conditions chosen. The amide I' band was found to exhibit a significant noncoincidence effect in that the first moment of the anisotropic Raman and of the IR band profile appears red-shifted from that of the isotropic Raman scattering. A simulation based on a coupled oscillator model involving all 27 amide I' modes of the peptide reveals that the peptide adopts a predominantly polyproline II conformation. Our results are inconsistent with the notion that the monomeric form of Abeta(1-28) is a totally disordered, random-coil structure. Generally, they underscore the notion that polyproline II is a characteristic motif of the unfolded state of proteins and peptides.     

FTIR spectra of solid poly-l-lysine in the stretching NH mode range

Three bands at 3270 cm(-1), 3200 cm(-1) and 3030 cm(-1) are found in the IR stretching proton (nu(1)) mode spectral range in spectra of solid poly-l-lysine (PLL). Strong quantitative changes of these bands are observed in samples dried from water solutions with different pH. The narrow band at 3270 cm(-1), which is strong in the spectrum of PLL precipitated from pH=12 alkaline medium, is assigned to the nu(1) peptide proton mode of NH-CO (amide A) of the beta-sheet structure type. The band at 3200 cm(-1), which is intensified in PLL precipitated from pH=1 acidic medium, relates to the nu(1) peptide mode in the random coil structure. The band at 3030 cm(-1), whose peak intensity increases two-fold in going from alkaline to acidic medium, is assigned to the nu(1) modes of protonated NH(3)(+) side chain groups. The frequencies of all bands were used for estimating H-bond energy relying on an empirical correlation between this property and the red shift of the nu(1) band. The enthalpy of the secondary structure transition from beta-sheet to the random coil, which is observed in PLL at the change of pH from 11 to 1 amounts to 4.7 kJ mol(-1).     

A helix-turn motif in the C-terminal domain of histone H1

The structural study of peptides belonging to the terminal domains of histone H1 can be considered as a step toward the understanding of the function of H1 in chromatin. The conformational properties of the peptide Ac-EPKRSVAFKKTKKEVKKVATPKK (CH-1), which belongs to the C-terminal domain of histone H1(o) (residues 99-121) and is adjacent to the central globular domain of the protein, were examined by means of 1H-NMR and circular dichroism. In aqueous solution, CH-1 behaved as a mainly unstructured peptide, although turn-like conformations in rapid equilibrium with the unfolded state could be present. Addition of trifluoroethanol resulted in a substantial increase of the helical content. The helical limits, as indicated by (i,i + 3) nuclear Overhauser effect (NOE) cross correlations and significant up-field conformational shifts of the C(alpha) protons, span from Pro100 to Val116, with Glu99 and Ala117 as N- and C-caps. A structure calculation performed on the basis of distance constraints derived from NOE cross peaks in 90% trifluoroethanol confirmed the helical structure of this region. The helical region has a marked amphipathic character, due to the location of all positively charged residues on one face of the helix and all the hydrophobic residues on the opposite face. The peptide has a TPKK motif at the C-terminus, following the alpha-helical region. The observed NOE connectivities suggest that the TPKK sequence adopts a type (I) beta-turn conformation, a sigma-turn conformation or a combination of both, in fast equilibrium with unfolded states. Sequences of the kind (S/T)P(K/R)(K/R) have been proposed as DNA binding motifs. The CH-1 peptide, thus, combines a positively charged amphipathic helix and a turn as potential DNA-binding motifs.     

DNA-induced alpha-helical structure in the NH2-terminal domain of histone H1

It is important to establish the structural properties of linker histones to understand the role they play in chromatin higher order structure and gene regulation. Here, we use CD, NMR, and IR spectroscopy to study the conformation of the amino-terminal domain of histone H1 degrees, free in solution and bound to the DNA. The NH(2)-terminal domain has little structure in aqueous solution, but it acquires a substantial amount of alpha-helical structure in the presence of trifluoroethanol (TFE). As in other H1 subtypes, the basic residues of the NH(2)-terminal domain of histone H1 degrees are clustered in its COOH-terminal half. According to the NMR results, the helical region comprises the basic cluster (Lys(11)-Lys(20)) and extends until Asp(23). The fractional helicity of this region in 90% TFE is about 50%. His(24) together with Pro(25) constitute the joint between the NH(2)-terminal helix and helix I of the globular domain. Infrared spectroscopy shows that interaction with the DNA induces an amount of alpha-helical structure equivalent to that observed in TFE. As coulombic interactions are involved in complex formation, it is highly likely in the complexes with DNA that the minimal region with alpha-helical structure is that containing the basic cluster. In chromatin, the high positive charge density of the inducible NH(2)-terminal helical element may contribute to the binding stability of the globular domain.