Base dynamics of local Z-DNA conformations as detected by electron paramagnetic resonance with spin-labeled deoxycytidine analogues

Conformation detection and base dynamics of spin-labeled Z-DNA have been investigated by electron paramagnetic resonance (EPR) spectroscopy. The two synthesized and characterized probes used in this study were C(5)-nitroxide-labeled 2'-deoxycytidine 5'-triphosphates, pppDCAT and pppDCAVAT, which serve as suitable substrates for Micrococcus luteus DNA polymerase. Enzymatic incorporation of these probes into (dG-dC)n yields the EPR-active alternating copolymers (dG-dC,DCAT)n and (dG-dC,-DCAVAT)n. These polymers assume typical B- and Z-DNA conformations under respective low (0.1 M NaCl) and high (4.5 M NaCl) salt conditions, as evidenced by their UV-circular dichroism spectra. The EPR line shape of (dG-dC,DCAT)n in Z-form is unique and significantly different from the B-form EPR spectrum. A similar observation is made for (dG-dC,DCAVAT)n. Thus, the EPR line shapes of these spin-labeled DNAs are indicative of their local conformations. The EPR spectra, analyzed with a previously published motional model [Kao, S.-C., Polnaszek, C.F., Toppin, C.R., & Bobst, A.M. (1983) Biochemistry 22, 5563-5568], indicate tau perpendicular values of 4 and 7 ns for the B- and Z-forms, respectively. Therefore, the base dynamics of Z-DNA are about two times slower than in B-DNA.     

Preparation and characterization of spin-labeled oligonucleotides for DNA hybridization.

Sequence-specific spin-labeled oligodeoxynucleotides with conformation-sensitive electron paramagnetic resonance (EPR) signals are synthesized and examined as solution-phase nucleic acid hybridization probes. Either a proxyl or tempo ring linked to the C(5) position of deoxyuridine (dU) by a nonrigid two-atom methylamino tether is incorporated within 15-mers by phosphotriester chemistry yielding stable spin-labeled probes with distinctive EPR specific activity (AEPR) values. The AEPR is greater for a proxyl-labeled than for a tempo-labeled probe and is consistent with EPR data of enzymatically labeled 26-mers [Bobst, A. M., Pauly, G. T., Keyes, R. S., and Bobst, E. V. (1988) FEBS Lett. 228, 33-36], after normalizing for percent labeling. The spectral characteristics of the free probes and the probe/target complexes are similar to those of enzymatically spin-labeled nucleic acids containing a different nonrigid two-atom-tethered spin label [Bobst, A. M., Kao, S.-C., Toppin, R. C., Ireland, J. C., and Thomas, I. E. (1984) J. Mol. Biol. 173, 63-70]. The presence of target DNA is detected in solution by EPR spectroscopy and the assay is based on the characteristic line-shape change associated with hybridization. The EPR spectra of free and bound probe reflect little interference from changes in global dynamics of the probe, and the line-shape change upon complexation results primarily from a change in local base dynamics. The presence or absence of hybridization can be detected in a loop-gap resonator with about 1 pmol of spin-labeled 15-mer within minutes.     

An electron paramagnetic resonance probe to detect local Z-DNA conformations

We present spectroscopic evidence for an electron paramagnetic resonance (EPR) probe to detect local Z-DNA conformations in synthetic DNA. A spin labeled deoxycytidine-5'-triphosphate (pppDCAT) was co-polymerized with Micrococcus luteus DNA polymerase to yield the spin active alternating co-polymer (dG-dC,DCAT)n. The EPR spectrum of (dG-dC,DCAT)n in the Z-DNA conformation indicates a decrease in the local base dynamics by about a factor of two as compared to that computed for B-DNA. A control experiment conducted with (dA-dT, DUAT)n under similar salt conditions rules out the possibility of observing salt induced artifacts.     

Spin label method reveals barnase-barstar interaction: a temperature and viscosity dependence approach

Spin labeling was used to study the protein-protein interaction between the enzyme barnase (Bn) and its inhibitor barstar (Bs). A mutant of barstar (C40A), which contains only one cysteine, C82, located near the Bn-Bs contact region, was selectively modified by two spin labels having different lengths and structures of the flexible tether. The formation of a strong protein complex resulted in significant restriction of spin label mobility at the C82 residue of barstar, as indicated by notable changes in the recorded EPR spectra. The dependence of the separation between broad outer peaks of the EPR spectra on viscosity at constant temperature was used to evaluate the order parameter S and the rotational correlation time tau (a temperature-viscosity dependence approach). The order parameter S, which characterizes fast reorientation of a spin label relative to the protein molecule, sharply increases and approaches unity when Bs binds to Bn. In addition, formation of a Bs-Bs complex was observed; it is also accompanied by restriction of spin label mobility. At the same time, the rotational correlation times tau of spin-labeled Bs, its complex with Bn, and the Bs dimer in solution agree well with their molecular masses. This indicates that barstar, its complex with barnase, and barstar dimer are rigid protein entities. The described approach is suitable for studying any spin-labeled macromolecular complexes.     

Melting studies on spin-labeled polyadenylic–polyuridylic complexes

Temperature-dependent conformational transitions of spin-labeled poly rA, spin-labeled poly rU and the two-stranded helical complexes consisting either of spin-labeled rA·poly rU or spin-labeled poly rU·poly rA have been measured by electron spin resonance spectrocopy. The polynucleotides were spin labeled with 4-(2-iodoacetamido)2,2,6,6-tetramethylpiperidinooxyl and the spin label to nucleotide base ratio was approximately 1:600. The relationship between the log of tumbling time τ and the reciprocal absolute temperature for the spin-labeled single and double-stranded polynucleotides is presented. An agreement between T_m^OD (optical density melting) and T_m^sp (spin melting) is found for the complexes, which strongly supports the conclusion that the same temperature-dependent structural changes are monitored with both techniques.     

Probing iso-1-cytochrome c structure by site-directed spin labeling and electron paramagnetic resonance techniques

A cysteine-specific methanethiosulfonate spin label was introduced into yeast iso-1-cytochrome c at three different positions. The modified forms of cytochrome c included: the wild-type protein labeled at naturally occurring C102, and two mutated proteins, S47C and L85C, labeled at positions 47 and 85, respectively (both S47C and L85C derived from the protein in which C102 had been replaced by threonine). All three spin-labeled protein derivatives were characterized using electron paramagnetic resonance (EPR) techniques. The continuous wave (CW) EPR spectrum of spin label attached to L85C differed from those recorded for spin label attached to C102 or S47C, indicating that spin label at position 85 was more immobilized and exhibited more complex tumbling than spin label at two other positions. The temperature dependence of the CW EPR spectra and CW EPR power saturation revealed further differences of spin-labeled L85C. The results were discussed in terms of application of the site-directed spin labeling technique in probing the local dynamic structure of iso-1-cytochrome c.     

Is the Fab-fragment from monoclonal rheumatoid IgM flexible? A spin label dynamics study

A comparative study of the Fab- and Fab-RF-fragments in the molecules of monoclonal IgM and IgM-RF, respectively, was performed by the spin label method. The spin label, 2,2,6,6-tetramethyl-4-dichloro-triazinylaminopiperidine-1-oxyl, was introduced into the peptide part of the protein. On the basis of the data on the temperature-viscosity dependences of the EPR spectral parameters of the resultant spin-labeled proteins, the rotational correlation time tau of the spin carrier was determined. It turned out that the reduced to normal conditions tau values for the molecules of the Fab- and Fab-RF-fragments were 21+/-2 and 11+/-1 ns, respectively. Analysis of the resultant data provides sufficient grounds for assuming that such a sharp decrease in the tau value for the molecule of the Fab-RF fragment is due to local flexibility of its globular structure, which, in turn, can determine the specific features of the IgM-RF functioning as an autoantibody.     

A simple method for determination of rotational correlation times and separation of rotational and polarity effects from EPR spectra of spin-labeled biomolecules in a wide correlation time range

A method using nitroxide radical spin labels for determining both the isotropic rotational correlation time tau R and the environmental polarity of the label is described. By means of a least square fitting method, the values of an effective hyperfine tensor A' and of an effective g value tensor g' of randomly oriented spin labels are determined from X-band EPR spectra on the basis of an effective time-independent Hamiltonian. The traces of the tensors deliver the information about the environmental polarity of the label and are not dependent on the rotational correlation time tau R. A new averaging parameter S (tau R), calculated on the basis of the principal values of the tensor A', permits the evaluation of the rotational correlation time tau R in a very wide time range between 10(-10) and 10(-6) s. An application of this method to spin-labeled methemoglobin over a large temperature range and in environments of different polarity is discussed.     

Reaction path ensemble of the B–Z-DNA transition: a comprehensive atomistic study

Since its discovery in 1979, left-handed Z-DNA has evolved from an in vitro curiosity to a challenging DNA structure with crucial roles in gene expression, regulation and recombination. A fundamental question that has puzzled researchers for decades is how the transition from B-DNA, the prevalent right-handed form of DNA, to Z-DNA is accomplished. Due to the complexity of the B–Z-DNA transition, experimental and computational studies have resulted in several different, apparently contradictory models. Here, we use molecular dynamics simulations coupled with state-of-the-art enhanced sampling techniques operating through non-conventional reaction coordinates, to investigate the B–Z-DNA transition at the atomic level. Our results show a complex free energy landscape, where several phenomena such as over-stretching, unpeeling, base pair extrusion and base pair flipping are observed resulting in interconversions between different DNA conformations such as B-DNA, Z-DNA and S-DNA. In particular, different minimum free energy paths allow for the coexistence of different mechanisms (such as zipper and stretch–collapse mechanisms) that previously had been proposed as independent, disconnected models. We find that the B–Z-DNA transition—in absence of other molecular partners—can encompass more than one mechanism of comparable free energy, and is therefore better described in terms of a reaction path ensemble.     

ESR spectral analysis of the molecular motion of spin labels in lipid bilayers and membranes based on a model in terms of two angular motional parameters and rotational correlation times

Electron spin resonance (ESR) spectral line shapes are calculated for a nitroxide spin-labeled molecule undergoing rapid restricted rotations (twisting) about its long molecular axis while simultaneously tumbling within a cone. Explicit expressions are derived for the hyperfine splittings and $\text{g-}\text{values}$, as well as for the secular contributions to the motionally modulated linewidths. The present model is useful for analyzing the restricted twisting and tumbling motions, and rotational correlation times, of spin-labeled molecules in bilayers. Simulated spectra compare well with experimental spectra of lecithin bilayers marked with cholestane spin label, over a wide temperature range.     

23Na NMR relaxation study of the effects of conformation and base composition on the interactions of counterions with double-helical DNA

NMR relaxation rates (T1(-1) and T2(-1)) have been determined for 23Na in aqueous salt solutions containing various types of helical double-stranded deoxyribonucleic acids. These measurements were performed on three synthetic polynucleotides having different overall conformations, poly-(dA-dT).poly(dA-dT) (alternating B-DNA), poly(dG-dC).poly(dG-dC) at low salt (B-DNA), and Br-poly(dG-dC).Br-poly(dG-dC) (left-handed Z-DNA), and on four types of natural DNA differing in base composition, Clostridium perfringens (26% GC), calf thymus (40% GC), Escherichia coli (50% GC), and Micrococcus lysodeikticus (72% GC). For all types of DNA investigated, except poly(dA-dT).poly(dA-dT), the 23Na NMR spectra measured at 21 degrees C and an applied field of 4.7 T are non-Lorentzian. These non-Lorentzian spectra were analyzed on the basis of the two-state model and the standard theory of nonexponential quadrupolar relaxation processes in order to obtain estimates of the correlation times (tau c) characteristic of the sodium nuclei associated with the various nucleic acids. All of the correlation times estimated in this way are in the range of nanoseconds. The magnitudes of these correlation times show a significant dependence on the overall conformation of the nucleic acid (B vs. Z) but not on its base composition. To investigate the concentration dependence of tau c, sodium or magnesium salts were added to solutions of Br-poly(dG-dC).Br-poly(dG-dC) (Z-DNA).(ABSTRACT TRUNCATED AT 250 WORDS)     

Probing triplex formation by EPR spectroscopy using a newly synthesized spin label for oligonucleotides

Spin labels have been extensively used to study the dynamics of oligonucleotides. Spin labels that are more rigidly attached to a base in an oligonucleotide experience much larger changes in their range of motion than those that are loosely tethered. Thus, their electron paramagnetic resonance spectra show larger changes in response to differences in the mobility of the oligonucleotides to which they are attached. An example of this is 5-(2,2,5,5-tetramethyl-3-ethynylpyrrolidine-1-oxyl)-uridine (1). How ever, the synthesis of this modified DNA base is quite involved and, here, we report the synthesis of a new spin-labeled DNA base, 5-(2,2,6,6-tetramethyl-4-ethynylpiperidyl-3-ene-1-oxyl)-uridine (2). This spin label is readily prepared in half the number of steps required for 1, and yet behaves in a spectroscopically analogous manner to 1 in oligonucleotides. Finally, it is shown here that both spin labels 1 and 2 can be used to detect the formation of both double-stranded and triplex DNA.     

An EPR study to determine the relative nucleic acid binding affinity of single-stranded DNA-binding protein from Escherichia coli.

A direct quantitative determination by EPR of the nucleic acid binding affinity relationship of the single-stranded DNA-binding protein (SSB) from Escherichia coli at close to physiological NaCl concentration is reported. Titrations of (DUAP, dT)n, an enzymatically spin-labeled (dT)n, with SSB in 20 mM Tris-HCl (pH 8.1), 1 mM sodium EDTA, 0.1 mM dithiothreitol, 10% (w/v) glycerol, 0.05% Triton with either low (5 mM), intermediate (125 mM) or high 200 mM) NaCl content, reveal the formation of a high nucleic acid density complex with a binding stoichiometry (s) of 60 to 75 nucleotides per SSB tetramer. Reverse titrations, achieved by adding (DUAP, dT)n to SSB-containing solutions, form a low nucleic acid density complex with an s = 25 to 35 in the buffer with low NaCl content (5 mM NaCl). The complex with an s = 25 to 35 is converted to the high nucleic acid density complex by increasing the NaCl content to 200 mM. It is, therefore, metastable and forms only under reverse titration conditions in low NaCl. The relative apparent affinity constant Kapp of SSB for various unlabeled single-stranded nucleic acids was determined by EPR competition experiments with spin-labeled nucleic acids as macromolecular probes in the presence of the high nucleic acid density complex. The Kapp of SSB exhibits the greatest affinity for (dT)n as was previously found for T4 gene 32 protein (Bobst, A.M., Langemeier, P.W., Warwick-Koochaki, P.E., Bobst, E.V. and Ireland, J.C. (1982) J. Biol. Chem. 257, 6184) and gene 5 protein (Bobst, A.M., Ireland, J.C. and Bobst, E.V. (1984) J. Biol. Chem. 259, 2130) by EPR competition assays. In contrast, however, SSB does not display several orders of magnitude greater affinity for (dT)n than for other single stranded DNAs as is the case with both gene 5 and T4 gene 32 protein. The relative Kapp values for SSB in the above buffer with 125 mM NaCl are: Kapp(dT)n = 4KappfdDNA = 40Kapp(dA)n = 200Kapp(A)n.     

ESR spectral analysis of the molecular motion of spin labels in lipid bilayers and membranes based on a model in terms of two angular motional parameters and rotational correlation times.

Electron spin resonance (ESR) spectral line shapes are calculated for a nitroxide spin-labeled molecule undergoing rapid restricted rotations (twisting) about its long molecular axis while simultaneously tumbling within a cone. Explicit expressions are derived for the hyperfine splittings and g-values, as well as for the secular contributions to the motionally modulated linewidths. The present model is useful for analyzing the restricted twisting and tumbling motions, and rotational correlation times, of spin-labeled molecules in bilayers. Simulated spectra compare well with experimental spectra of lecithin bilayers marked with cholestane spin label, over a wide temperature range.     

Low-frequency dynamics and Raman scattering of crystals, of B-, A-, and Z-DNA, and fibers of C-DNA

Normal modes of vibration of DNA in the low-frequency region (10-300 cm-1 interval) have been identified from Raman spectra of crystals of B-DNA [d(CGCAAATTTGCG)], A-DNA [r(GCG)d(CGC) and d(CCCCGGGG)], and Z-DNA [d(CGCGCG) and d(CGCGTG)]. The lowest vibrational frequencies detected in the canonical DNA structures--at 18 +/- 2 cm-1 in the B-DNA crystal, near 24 +/- 2 cm-1 in A-DNA crystals, and near 30 +/- 2 cm-1 in Z-DNA crystals--are shown to correlate well with the degree of DNA hydration in the crystal structures, as well as with the level of hydration in calf thymus DNA fibers. These findings support the assignment [H. Urabe et al. (1985) J. Chem. Phys. 82, 531-535; C. Demarco et al. (1985) Biopolymers 24, 2035-2040] of the lowest frequency Raman band of each DNA to a helix mode, which is dependent primarily upon the degree of helix hydration, rather than upon the intrahelical conformation. The present results show also that B-, A-, C-, and Z-DNA structures can be distinguished from one another on the basis of their characteristic Raman intensity profiles in the region of 40-140 cm-1, even though all structures display two rather similar and complex bands centered within the intervals of 66-72 and 90-120 cm-1. The similarity of Raman frequencies for B-, A-, C-, and Z-DNA suggests that these modes originate from concerted motions of the bases (librations), which are not strongly dependent upon helix backbone geometry or handedness. Correlation of the Raman frequencies and intensities with the DNA base compositions suggests that the complex band near 90-120 cm-1 in all double-helix structures is due to in-plane librational motions of the bases, which involve stretching of the purine-pyrimidine hydrogen bonds. This would explain the centering of the band at higher frequencies in structures containing G.C pairs (greater than 100 cm-1) than in structures containing A.T pairs (less than 100 cm-1), consistent with the strengths of G.C and A.T hydrogen bonding.     

Backbone dynamics of the calcium-signaling protein apo-S100B as determined by 15N NMR relaxation

Backbone dynamics of homodimeric apo-S100B were studied by (15)N nuclear magnetic resonance relaxation at 9.4 and 14.1 T. Longitudinal relaxation (T(1)), transverse relaxation (T(2)), and the (15)N-[(1)H] NOE were measured for 80 of 91 backbone amide groups. Internal motional parameters were determined from the relaxation data using the model-free formalism while accounting for diffusion anisotropy. Rotational diffusion of the symmetric homodimer has moderate but statistically significant prolate axial anisotropy (D( parallel)/D( perpendicular) = 1.15 +/- 0.02), a global correlation time of tau(m) = 7.80 +/- 0.03 ns, and a unique axis in the plane normal to the molecular symmetry axis. Of 29 residues at the dimer interface (helices 1 and 4), only one has measurable internal motion (Q71), and the order parameters of the remaining 28 were the highest in the protein (S(2) = 0.80 to 0.91). Order parameters in the typical EF hand calcium-binding loop (S(2) = 0.73 to 0.87) were slightly lower than in the pseudo-EF hand (S(2) = 0.75 to 0.89), and effective internal correlation times, tau(e), distinct from global tumbling, were detected in the calcium-binding loops. Helix 3, which undergoes a large, calcium-induced conformational change necessary for target-protein binding, does not show evidence of interchanging between the apo and Ca(2+)-bound orientations in the absence of calcium but has rapid motion in several residues throughout the helix (S(2) = 0.78 to 0.88; 10 < or = tau(e) < or = 30 ps). The lowest order parameters were found in the C-terminal tail (S(2) = 0.62 to 0.83). Large values for chemical exchange also occur in this loop and in regions nearby in space to the highly mobile C-terminal loop, consistent with exchange broadening effects observed.     

Simulation of nitroxide electron paramagnetic resonance spectra from brownian trajectories and molecular dynamics simulations

A simulated continuous wave electron paramagnetic resonance spectrum of a nitroxide spin label can be obtained from the Fourier transform of a free induction decay. It has been previously shown that the free induction decay can be calculated by solving the time-dependent stochastic Liouville equation for a set of Brownian trajectories defining the rotational dynamics of the label. In this work, a quaternion-based Monte Carlo algorithm has been developed to generate Brownian trajectories describing the global rotational diffusion of a spin-labeled protein. Also, molecular dynamics simulations of two spin-labeled mutants of T4 lysozyme, T4L F153R1, and T4L K65R1 have been used to generate trajectories describing the internal dynamics of the protein and the local dynamics of the spin-label side chain. Trajectories from the molecular dynamics simulations combined with trajectories describing the global rotational diffusion of the protein are used to account for all of the dynamics of a spin-labeled protein. Spectra calculated from these combined trajectories correspond well to the experimental spectra for the buried site T4L F153R1 and the helix surface site T4L K65R1. This work provides a framework to further explore the modeling of the dynamics of the spin-label side chain in the wide variety of labeling environments encountered in site-directed spin labeling studies.     

Role of rapid movement of spin labels in interpreting EPR spectra for spin-labelled macromolecules

The method of spin labeling was used to monitor quick movements of side residues in protein monocrystals. The EPR spectra of monocrystals of spin-labeled lysozyme at different orientations of the tetrahonal crystal relative to the direction of the magnetic field were interpreted using the molecular dynamics method. A simple model was proposed, which enables one to calculate the trajectory of movements of the spin label by the molecular dynamic method over a relatively short period of time. The entire "frozen" protein molecule and a "defrozen" spin-labeled amino acid residue were considered in the framework of the model. To calculate the trajectories in vacuum, a model of spin-labeled lysozyme was constructed, and the parameters of force potentials for the atoms of the protein molecule and the spin label were specified. It follows from the calculations that the protein environment sterically hinders the range of eventual angular reorientations of the reporter NO-group of nitroxyl incorporated into the spin label, thereby affecting the shape of the EPR spectrum. However, the scatter in the positions of the reporter group in the angular space turned out to correspond to the Gauss distribution. Using the atomic coordinates of the spin label, obtained in a chosen time interval by the method of molecular dynamics, and taking into account the distribution of the states of the spin label in the ensemble of spin-labeled macromolecules in the crystal, we simulated the EPR spectra of monocrystals of spin-labeled lysozyme. The theoretical EPR spectra coincide well with the experimental.     

The role of the fast motion of the spin label in the interpretation of EPR spectra for spin-labeled macromolecules

The spin label method was used to observe the nature of the fast motions of side chains in protein monocrystals. The EPR spectra of spin-labeled lysozyme monocrystals (with different orientations of the tetragonal protein crystal in relation to the direction of the magnetic field) were interpreted using the method of molecular dynamics (MD). Within the proposed simple model, MD calculations of the spin label motion trajectories are performed in a reasonable real time. The model regards the protein molecule as frozen as a whole and the spin-labeled amino acid residue as unfrozen. To calculate the trajectories in vacuum, a model of spin-labeled lysozyme was assembled, and the parameters of the force fields were specified for atoms of the protein molecule, including the spin label. The calculations show that the protein environment sterically limits the area of the possible angular reorientations for the NO reporter group of the nitroxide (within the spin label), and this, in turn, affects the shape of the EPR spectrum. However, it turned out that the spread in the positions of the reporter group in the angle space strictly adheres to the Gaussian distribution. Using the coordinates of the spin label atoms obtained by the MD method within a selected time range and considering the distribution of the spin label states over the ensemble of spin-labeled macromolecules in a crystal, the EPR spectra of spin-labeled lysozyme monocrystals were simulated. The resultant theoretical EPR spectra appeared to be similar to experimental ones.     

Spin-Labeled Nucleotide Mobility in the Boundary of the EcoRI Endonuclease Binding Site

Abstract

A complex consisting of the EcoRI endonuclease site-specifically bound to spin-labeled DNA 26mers was prepared to provide a model system for studying possible conformational changes resulting from protein binding. EPR was used to monitor the mobility of the spin labels that were strategically placed in position 6, 9, or 11 with respect to the dyad axis of the 26mer. These positions are located within the flanking region on either side of the EcoRI hexamer binding site. This allows the monitoring of potential distal structural changes in the DNA helix caused by protein binding. The spectral line shapes indicate that the spin label closest to the EcoRI endonuclease binding site, i.e., in position 6, is most influenced by the binding event. The EPR data are analyzed according to a model that distinguishes between spectral effects due to a change in the hydrodynamic shape of the complex and those resulting from local variations in the spin-label mobility as characterized by a local order parameter S. S reflecting the motional restriction of the spin-labeled base is 0.20 ± 0.01 for all three oligomers as well as for the two complexes with the label in position 9 or 11, while the position 6 labeled complex yields S=0.25. To further evaluate the origin of the slightly larger EPR effect observed with position 6 labeled material, molecular dynamics (MD) simulations were used to explore the space accessible to the probes in positions 6, 9, and 11. MD results gave similar nitroxide trajectories for all three labeled 26mers in the absence or presence of EcoRI. Thus, the small position 6 effect is attributed to a structural distortion in the major groove of the DNA at this location possibly corresponding to a bend induced by protein binding. The observation that the spectral changes are small indicates the absence of any significant structural disruption being propagated along the helix as a result of protein binding. Also, the fact that the line shape of the 26mers did not change as expected from hydrodynamic theory in view of the significant increase in molecular volume upon protein binding suggests that there are additional relaxation processes involving the protein and nucleic acid.