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Significance The main stabilizer of the DNA double helix is not the base-pair hydrogen bonds but coin-pile stacking of base pairs, whose hydrophobic cohesion, requiring abundant water, indirectly makes the DNA interior dry so that hydrogen bonds can exert full recognition power. We report that certain semihydrophobic agents depress the stacking energy (measurable in single-molecule experiments), leading to transiently occurring holes in the base-pair stack (monitorable via binding of threading intercalators). Similar structures observed in DNA complexes with RecA and Rad51, and previous observations of spontaneous strand exchange catalyzed in semihydrophobic model systems, make us propose that some hydrophobic protein residues may have roles in catalyzing homologous recombination. We speculate that hydrophobic catalysis is a general phenomenon in DNA enzymes., Hydrophobic base stacking is a major contributor to DNA double-helix stability. We report the discovery of specific unstacking effects in certain semihydrophobic environments. Water-miscible ethylene glycol ethers are found to modify structure, dynamics, and reactivity of DNA by mechanisms possibly related to a biologically relevant hydrophobic catalysis. Spectroscopic data and optical tweezers experiments show that base-stacking energies are reduced while base-pair hydrogen bonds are strengthened. We propose that a modulated chemical potential of water can promote “longitudinal breathing” and the formation of unstacked holes while base unpairing is suppressed. Flow linear dichroism in 20% diglyme indicates a 20 to 30% decrease in persistence length of DNA, supported by an increased flexibility in single-molecule nanochannel experiments in poly(ethylene glycol). A limited (3 to 6%) hyperchromicity but unaffected circular dichroism is consistent with transient unstacking events while maintaining an overall average B-DNA conformation. Further information about unstacking dynamics is obtained from the binding kinetics of large thread-intercalating ruthenium complexes, indicating that the hydrophobic effect provides a 10 to 100 times increased DNA unstacking frequency and an “open hole” population on the order of 10−2 compared to 10−4 in normal aqueous solution. Spontaneous DNA strand exchange catalyzed by poly(ethylene glycol) makes us propose that hydrophobic residues in the L2 loop of recombination enzymes RecA and Rad51 may assist gene recombination via modulation of water activity near the DNA helix by hydrophobic interactions, in the manner described here. We speculate that such hydrophobic interactions may have catalytic roles also in other biological contexts, such as in polymerases.

The assembly of stacked dyes on DNA is of interest for electron transfer, light harvesting, sensing, and catalysis applications. A combination of UV/vis absorption, linear dichroism (LD), and circular dichroism (CD) was applied to characterize thoroughly the aggregation with DNA of the phenothiazine dyes methylene blue, azure B, and thionine. Aggregates of each dye with [poly(dG-dC)]2, [poly(dA-dT)]2, and calf thymus DNA were explored at high dye:DNA binding ratios, where excess dye groove-binds after all intercalation sites are filled. The organization of the aggregates (dimers, trimers, and multimers) with polydeoxynucleotides displays a structural diversity that depends on DNA sequence, extent of methylation of dye exocyclic amine groups, and ionic strength. The dyes typically form right-handed H-aggregates having negative LD, consistent with stepped stacking along the minor groove. However, aggregates in some dye:DNA aggregates show left-handed chirality or positive LD, indicating unusual modes of agg...

The binding mode of thionine (3,7-diamino-5-phenothiazinium) with alternating and non-alternating DNA polynucleotides at low binding ratios was conclusively determined using linear and circular dichroism spectroscopies. The binding to [poly(dG-dC)]

Binuclear polypyridine ruthenium compounds have been shown to slowly intercalate into DNA, following a fast initial binding on the DNA surface. For these compounds, intercalation requires threading of a bulky substituent, containing one Ru(II), through the DNA base-pair stack, and the accompanying DNA duplex distortions are much more severe than with intercalation of mononuclear compounds. Structural understanding of the process of intercalation may greatly gain from a characterisation of the initial interactions between binuclear Ru(II) compounds and DNA. We report a structural NMR study on the binuclear Ru(II) intercalator Λ,Λ-B (Λ,Λ-[μ-bidppz(bipy)4Ru2](4+); bidppz = 11,11'-bis(dipyrido[3,2-a:2',3'-c]phenazinyl, bipy = 2,2'-bipyridine) mixed with the palindromic DNA [d(CGCGAATTCGCG)]2. Threading of Λ,Λ-B depends on the presence and length of AT stretches in the DNA. Therefore, the latter was selected to promote initial binding, but due to the short stretch of AT base pairs, final intercalation is prevented. Structural calculations provide a model for the interaction: Λ,Λ-B is trapped in a well-defined surface-bound state consisting of an eccentric minor-groove binding. Most of the interaction enthalpy originates from electrostatic and van der Waals contacts, whereas intermolecular hydrogen bonds may help to define a unique position of Λ,Λ-B. Molecular dynamics simulations show that this minor-groove binding mode is stable on a nanosecond scale. To the best of our knowledge, this is the first structural study by NMR spectroscopy on a binuclear Ru compound bound to DNA. In the calculated structure, one of the positively charged Ru(2+) moieties is near the central AATT region; this is favourable in view of potential intercalation as observed by optical methods for DNA with longer AT stretches. Circular dichroism (CD) spectroscopy suggests that a similar binding geometry is formed in mixtures of Λ,Λ-B with natural calf thymus DNA. The present minor-groove binding mode is proposed to represent the initial surface interactions of binuclear Ru(II) compounds prior to intercalation into AT-rich DNA.

The influence of the highly fluorescent tricyclic cytosine base analogue (tC) on duplex DNA conformation is investigated. The duplex properties are characterized by absorbance and circular dichroism (CD) for all combinations of neighbouring bases to tC, and an NMR structure is determined for one tC-containing sequence. For the oligonucleotides with one tC incorporated instead of cytosine, the melting temperature is increased on average by 2.7 degrees C above that for the unmodified ones. CD spectra are practically identical for modified and unmodified sequences, indicating an unperturbed B-DNA conformation. The NMR structure determination of the self-complementary sequence 5'-CTC(tC)ACGTGGAG shows a DNA conformation consistent with B-form for the whole duplex. The root-mean-square distance for the nucleotides of the eight central base pairs between the 10 structures with lowest CYANA target functions and a mean structure is 0.45 +/- 0.17 A. The NMR data confirm correct base pairing for tC by the observation of both intrastrand and interstrand imino proton NOEs. Altogether, this suggests that tC works well as a cytosine analogue, i.e. it is situated in the base stack, forming hydrogen bonds with G in the complementary strand, without distorting the DNA backbone conformation. This first example of an artificial, highly fluorescent DNA base that does not perturb the DNA conformation could have valuable applications for the study of the structure and dynamics of nucleic acid systems.

We investigate how DNA interacts with drugs in humid polyvinyl alcohol (PVA) films by using a homologous set of cyanine dyes (YO(+), YO-PRO(2+), and YOYO(4+)) known to intercalate into DNA with increasing affinity with increasing charge. UV-vis spectroscopy shows that the PVA matrix destabilizes all three DNA-dye complexes compared to aqueous solution but to a lesser degree as the dye charge increases. The monovalent YO is fully dissociated from DNA within minutes, whereas the dissociation of the divalent YO-PRO takes about one hour and occurs by a two-step mechanism. The tetravalent homodimer YOYO is even less affected by the PVA environment and remains intercalated in the B-form DNA also in the PVA films. The reduced stability of the DNA-dye complexes is discussed in terms of steric and dielectric properties of the PVA matrix. After being kept in dry PVA films for 48 h the DNA-YOYO complexes can be reformed reversibly by rehumidifying the films for 30 min. The ability to store aligned and confined DNA intercalated with ligand complexes may be useful in studies on structural properties of nucleic acids.

We recently reported that ruthenium complexes, with general structure [mu-bidppz(bipy)4Ru2](4+) (B) or [mu-bidppz(phen)4Ru2](4+) (P) (bidppz=11,11'-bi(dipyrido[3,2- a:2',3'-c]phenazinyl)), show extreme kinetic selectivity for long AT tracts over mixed-sequence calf thymus DNA (ct-DNA), a selectivity that also varies markedly with the size (between B and P) and sense of chirality of the complex. Earlier studies, exploiting the great increase in luminescence intensity when the compound intercalates, have yielded complex kinetics indicating the presence of both first- and second-order processes. Even with a homogeneous DNA sequence, such as poly(dAdT)2, the luminescence kinetics generally requires more than a single exponential for a satisfactory fit. We here reveal that at least part of the complexity is a result of the extreme sensitivity of the effective quantum yield of the complexes, so that the luminescence trajectories also reflect subtle variations in the environment and binding geometry that the complex is sampling on its path to its final binding site. By monitoring the rearrangement process using circular dichroism (CD), we show that threading of both enantiomers of B and P into poly(dAdT)2 is effectively a monoexponential process, as expected if the compounds are not affecting each other during the intercalation process. Thus, the complex luminescence trajectories may be explained by slow relaxations in the binding geometry (DNA conformation) and associated changes in the environment of the entering complexes. To further disentangle the intriguing features of the threading intercalation kinetics, and how they may depend on the flexibility and size of the ruthenium complexes, we have also designed and studied two new ruthenium complexes, [mu-dtpf(phen)4Ru2](4+) (F) (dtpf=4,5,9,12,16,17,21,25-octaaza-23 H-ditriphenyleno[2,3-b:2,3-h]fluorene), in which the bridging ligand is made totally rigid, and [mu-bidppz([12]aneS4) 2Ru2](4+) (S), which has less bulky, nonaromatic ancillary ligands. The threading of F into poly(dAdT)2, also found to be a monoexponential process, is about 3 times slower than for P, indicating that the flexibility of the bridging ligand is an important factor for the intercalation rate. Surprisingly, in contrast to all other compounds, S requires two exponentials to fit its binding kinetics as monitored by CD. Also surprisingly, in view of the smaller steric bulk, even the fastest phase is roughly 2 times slower for S than for B and P. Thus, not only the size of the ancillary ligand but also other properties that can influence the energy landscape of the threading path are rate-determining factors. With mixed-sequence ct-DNA, threading of B and that of P are both multiphasic processes when monitored with CD as well as with luminescence. The rate constants for threading into ct-DNA show much larger variations between complexes than for poly(dAdT)2, confirming earlier results based on luminescence data.

We here study the interactions of a polyamide with large DNA, and compare to those of minor groove binder distamycin (DST), including high ligand/DNA binding ratios. Specific as well as nonspecific binding is probed using polarized-light spectroscopy combined with singular value decomposition analysis. Circular and linear dichroism data confirm binding geometries consistent with minor groove binding for both of the ligands. Interestingly, at high and intermediate ligand/DNA ratios the polyamide exhibits no significant sequence discrimination between mixed-sequence (calf thymus) and AT DNA as compared to DST. Each ligand is concluded to exhibit two different binding modes depending upon ligand/DNA ratio and nucleo-base sequence. At high binding ratios, distinct differences between the ligands are observed: circular dichroism spectra exciton effects provide evidence of bimolecular interactions of the polyamide when bound to AT-DNA, whereas no effects are seen with DST or mixed-sequence DNA. Also linear dichroism indicates that a change in binding geometry occurs at high polyamide/AT ratios, and that the effect occurs only with polyamide in contrast to DST. Since the effect is insignificant with DST, or with calf thymus DNA, it is concluded that it relates to the sizes of the ligands and the minor grooves, becoming critical in the limit of crowding.

Circular dichroism (CD) of enantiomers of [Ru(phen)(2)dppz](2+) oriented in a octanoate-decanol-water lamellar liquid crystal has been measured parallel to the orientation axis. where the sample does not exhibit linear dichroism (LD). At an inclined incidence, the emerging LD shows that the chromophores have an along-chain orientation in the liquid crystal. The changes in the CD spectrum compared to an isotropic sample, in conjunction with CD calculations, allow us to assess the absolute configuration of the enantiomers and assign the CD bands to specific electronic transitions.

[Fe(1,10-phenanthroline)(3)](2+) is known to racemise in solution and DNA is known to shift the equilibrium point of the Delta/Lambda[Fe(1,10-phenanthroline)(3)](2+) mixture from 50:50 to a position favouring a slight excess of the Delta enantiomer. In this paper it is shown that DNA catalyses the racemisation reaction, presumably by providing vibrational energy to species that bind in a less favoured mode for that enantiomer. The racemisation of [Co(1,10-phenanthroline)(3)](3+), however, is not enhanced by DNA unless [Co(1,10-phenanthroline)(3)](2+) is also added to the solution. In this case, the DNA acts as a template to facilitate the Co-II reversible arrow Co-III electron transfer. Racemisation occurs while the [Co(1,10-phenanthroline)(3)](n+) is in the labile Co-II form.

The interaction of the cellular delivery vector penetratin with a model system consisting of negatively charged phospholipid vesicles has been studied. Above a certain peptide to lipid molar ratio, the cationic oligopeptide induces vesicle aggregation. Interestingly, the aggregation is followed by spontaneous disaggregation, which may be related to membrane translocation of the peptide. Circular dichroism (CD) measurements indicate a conformational transition, from alpha -helix to antiparallel beta -pleated sheet, which is simultaneous with the aggregation process. The potential influence of spectroscopic artifacts on CD data due to the drastically increased turbidity during aggregation is discussed.

Four novel piperazinylcarbonyloxyethyl derivatives of anthracene and pyrene have been prepared and investigated with respect to sequence specificity and synergism between hydrophobic and electrostatic effects upon binding to DNA. Linear and circular dichroism spectroscopy was used to assess the orientation of the aromatic chromophores relative to the nucleobases. Anthracene and pyrene derivatives 2a and 3 are both concluded to bind to homo-polynucleotide poly(dA-dT)(2) by intercalation of their aromatic moieties between base pairs, with a binding constant K-AT of 4 x 10(5) M-1 and 2 x 10(6) M-1, respectively. Significantly reduced affinities (K-GC = 3 x 10(4) M-1 and 10(5) M-1, respectively) are observed with poly(dG-dC)(2), due to less favorable interactions of the piperazinium tail in the minor groove. Base pair specificity is reflected in the binding thermodynamics, with the binding to AT being more enthalpically driven than the binding to GC. Phenyl substitution at the quaternary piperazinium site of the anthracene derivative 2b, does not affect the ratio K-AT/K-GC, but reduces the affinity for both AT End GC slightly. Moreover, the phenyl group in the 10-position of 4 prevents intercalation, and apparently, this compound binds externally to both AT and GC duplex polynucleotides. The results are discussed in terms of general features of the interactions of the intercalating and minor-groove binding molecular moieties, and their interplay with each other, with potentials for tuning specificity.

The binding conformations of single anti- and syn-BPDE-N2-dG adducts in oligonucleotides of varying base composition have been studied by induced circular dichroism (ICD) and light absorption spectroscopy. The sign of the ICD in single-stranded oligonucleotide adducts correlates with the absolute configuration of the cyclohexyl moiety of the BPDE. Adducts in oligonucleotide duplexes with UV lambdamax350 nm exhibiting a significant duplex-induced positive ICD should have a minor groove location as the predominant conformation. Those with UV lambdamax350 nm exhibiting either positive or negative contributions to the ICD should have intercalated binding as the predominant conformation. The magnitude of the ICD is dependent on the sequence context of the adducted strand and the particular BPDE-adduct isomer under study. In some cases, the results suggest structural heterogeneity. For instance, the (+)- and the (-)-trans-anti-BPDE-N2-dG adducts in duplexes where a dT flanks the lesion site exhibit weak positive ICD or negative ICD. These results reflect a bimodal conformational adduct distribution with contributions from both externally and internally located adducts. A key observation for the (+)-cis-syn-BPDE-N2-dG complexes in 5'-d(TGC) and 5'-d(CGC) sequence contexts is that the near-UV absorption spectra showed distinct bands corresponding to minor groove binding (lambdamax congruent with 346 nm) as well as intercalative binding (lambdamax congruent with 354 nm). Evidence for an equilibrium between the different modes of localization is provided by the results from the temperature dependence of the near-UV absorption and ICD characteristics of (+)-cis-syn-BPDE-N2-dG complexes in 5'-d(TGC) and 5'-d(CGC) sequence contexts, respectively.

The electronically excited states of the phthalimide chromophore have been studied by means of linear dichroism (LD) of samples partially oriented in poly(vinyl alcohol) films, magnetic circular dichroism (MCD), and circular dichroism (CD) spectroscopy. On the basis of the LD measurements, the low-energy tail (340-320 nm) of the first absorption band is assigned to an out-of-plane polarized pi-->pi* transition (I). At higher energy, the electronic spectrum is resolved into contributions from five pi-->pi* transitions: II(300 nm, long-axis polarized), III (275 nm, short-axis polarized), IV (235 nm, short-axis polarized), V (220 nm, long-axis polarized), and VI (similar to 210 nm, short-axis polarized). The results from semiempirical (INDO/S-CI) and ab initio (CIS/6-31+G(d)) MO calculations compare well with the proposed assignments of the excited states. Degenerate exciton interaction between electric-dipole-allowed transitions of two phthalimide chromophores is observed in the electronic absorption spectra of the achiral bis-phthalimides 2a-c and in the CD spectrum of the chiral bis-phthalimide 3a. For the latter compound, the solid-state geometry has been determined by X-ray diffraction analysis. Good agreement between experimental and computed CD spectra confirms that the coupled-oscillator exciton model provides the basis for a reliable nonempirical method for the assignment of absolute configuration for this class of compounds. Nondegenerate exciton coupling between phthalimide and benzoate or phenyl chromophores is born out in the CD spectra of homochiral molecules 3c and 3d with the rigid cyclohexane skeleton. Finally, the exciton coupling method is used to make stereochemical assignments for the acyclic, conformationally flexible derivatives 4a-c and 5b.

The binding of 2,7-diazapyrene (DAP), N-methyl-2,7-diazapyrenium monocation (MDAP), and N,N‘-dimethyl-2,7-diazapyrenium dication (DMDAP) to calf thymus DNA has been studied with respect to molecular geometry and thermodynamics. It is concluded from flow linear dichroism (LD) and induced circular dichroism (CD) spectra that the three diazapyrenes bind by intercalation to alternating AT as well as GC polynucleotide duplexes, as indicated by strong interactions with the transitions of the nucleobases in conjunction with approximately perpendicular orientations of the in-plane symmetry axes relative to the DNA helix axis. The reduced LD (LDr = LD/Aiso) of the DNA complexes is characterized by marked fine structure, decreasing in the order DAP > MDAP > DMDAP. This finding is interpreted in terms of a microscopic heterogeneity associated with rotational mobility of the ligand in a tilted intercalation pocket, with the dication DMDAP having less rotational freedom than the neutral DAP has. Other distinct differe...

The electronic transitions giving rise to the UV-visible absorption spectra of two pyridinium-phenanthridinium viologens, 6,7-dihydropyridol[2',1':3,4]pyrazinol[1,2-f]phenanthridinediium dication (1) and 7,8-dihydro-6H-pyrido[2',1':3,4]diazepino[1,2-f]phenanthridinediium dication (2), have been investigated with respect to energies, intensities, and transition moment directions. A combination of methods has been applied: UV-visible absorption, circular dichroism, magnetic circular dichroism, fluorescence anisotropy, Linear dichroism In stretched poly(vinyl alcohol) films, and semiempirical molecular orbital calculations. For both drugs, the lowest energy absorption band, occurring around 400 nm, results from two separate transitions. The corresponding electric transition dipole moments lie in the phenanthridine plane and are polarized, respectively, in the direction of the pyridine moiety (the lower energy transition) and parallel to the phenanthridine long axis (the higher energy transition). Up to four additional different pi --> pi* transitions account for a second band that peaks at 250 nm; they show different polarizations within the phenanthridine plane. The lowest energy transition of the whole spectrum of both drugs corresponds to the promotion of an electron from the HOMO to the LUMO, which are molecular orbitals mainly localized in the phenanthridine and pyridine rings, respectively, thereby implying a charge transfer, upon excitation, from the phenanthridine toward the pyridine ring. The experimental and theoretical results are discussed in relation to the spectroscopic, redox, and photochemical properties of these drugs.

The electronic spectrum of the unnatural nucleic acid base 2-aminopurine is important in order to understand the spectroscopy and photophysics of the normal DNA bases. Knowledge of transition moment directions and effective absorption components is also a prerequisite for the interpretation of emission spectra of 2-aminopurine incorporated into DNA as a probe of nucleic acid base motion or excitation energy transfer processes. Using linear dichroism, fluorescence anisotropy, and ordinary and magnetic circular dichroism techniques, the near-UV spectrum of 2-aminopurine is resolved into contributions from five electronic transitions. Four moderately strong pi-->pi* transitions (I, III, IV, and V) are observed, polarized at +53 degrees (I), -72 degrees (III), -77 degrees (IV), and +57 degrees or -67 degrees (V) relative to the short molecular axis. In addition, one weak n --> pi* transition (II) polarized perpendicular to the molecular plane has been identified. Semiempirical INDO/S calculations support these assignments.

The binding of homochiral [Ru(II)(1,10-phenanthroline)(2)L](2+) complexes {where L = 1,10-phenanthroline (phen), dipyrido[3,2-a:2',3'-c]phenazine (DPPZ) or benzodipyrido[3,2-a:2',3'-c]phenazine (BDPPZ)} to poly(dT*dA-dT) triplex has been investigated by linear and circular dichroism and thermal denaturation. Analysis of the linear dichroism spectra indicates that the extended DPPZ and BDPPZ ligands lie approximately parallel to the base-pair and base-tripler planes consistent with intercalation which is also supported by strong hypochromism in the interligand absorption bands with either duplex or tripler. The spectral properties of any of the metal complex enantiomers were similar for binding to either duplex or tripler DNA, indicating that the third strand, which occupies the major groove of the template duplex, has little effect on the binding geometries and hence supports the hypothesis that the metal complexes all bind from the minor groove with the DPPZ and BDPPZ ligands intercalated but without intercalation in the case of [Ru(phen)(3)](2+). Third-strand stabilization depended on the nature of the third substituted phenanthroline chelate ligand but was not directly related to its size, with stabilizing power increasing in the order phen < BDPPZ < DPPZ. This observation further supports intercalation of the extended ligands from the minor groove of the tripler since the extended BDPPZ ligand that would protrude into the major groove of the template would have greater steric interference than DPPZ with the third DNA strand.

Hoechst 33258 binds with high affinity into the minor groove of AT-rich sequences of double-helical DNA. Despite extensive studies of this and analogous DNA binding molecules, there still remains uncertainty concerning the interactions when multiple ligand molecules are accommodated within close distance. Albeit not of direct concern for most biomedical applications, which are at low drug concentrations, interaction studies for higher drug binding are important as they can give fundamental insight into binding mechanisms and specificity, including drug self-stacking interactions that can provide base-sequence specificity. Using circular dichroism (CD), isothermal titration calorimetry (ITC), and proton nuclear magnetic resonance ((1)H NMR), we examine the binding of Hoechst 33258 to three oligonucleotide duplexes containing AT regions of different lengths: [d(CGCGAATTCGCG)]2 (A2T2), [d(CGCAAATTTGCG)]2 (A3T3), and [d(CGAAAATTTTCG)]2 (A4T4). We find similar binding geometries in the minor groove for all oligonucleotides when the ligand-to-duplex ratio is less than 1:1. At higher ratios, a second ligand can be accommodated in the minor groove of A4T4 but not A2T2 or A3T3. We conclude that the binding of the second Hoechst to A4T4 is not cooperative and that the molecules are sitting with a small separation apart, one after the other, and not in a sandwich structure as previously proposed.

Peptide nucleic acid (PNA) is a DNA analogue in which the negatively charged sugar phosphate backbone has been substituted by uncharged N-(2-aminoethyl)glycine units. The study of a PNA-DNA duplex and the corresponding DNA-DNA duplex gives a unique opportunity to compare two polyelectrolytes with virtually identical geometry but greatly different linear charge density. The results provide a basis for a study of the applicability of the Poisson-Boltzmann (PB) and counterion condensation (CC) theories. UV and circular dichroism spectroscopy as well as isothermal titration calorimetry (ITC) have been used to study the effect of different ions on the stability and conformation of PNA-DNA, PNA-PNA, and DNA-DNA duplexes having the same base sequences. Cations in general destabilize both antiparallel (N/3') and parallel (N/5') PNA-DNA duplexes whereas they stabilize the DNA-DNA duplex. Studies on the effect of monovalent salt such as NaCl on T-m were carried out over a wide range of salt concentrations (0.01 to 5 M). The decrease in the T-m of the N/3' PNA-DNA duplex with increasing ionic strength in the range of concentrations of 0.01 to 0.5 M, where electrostatic effects predominate, is explained in terms of counterion release upon duplex formation in contrast to the counterion association accompanying the formation of a DNA duplex. The uncharged PNA-PNA duplex shows no significant destabilization in this concentration range. The higher stability of the N/3' PNA-DNA compared to the DNA-DNA duplex (Delta Delta G similar to-7 kcal/mol) is ascribed to more favorable entropic contributions consistent with the counterion release that accompanies the PNA-DNA duplex formation. At high salt concentration (>1 M), where electrostatic contributions saturate, similar trends in the decrease in T-m, were observed for the three types of duplexes irrespective of their backbone charges. The destabilizing effects of a series of Na salts with various monovalent anions on N/3' PNA-DNA and PNA-PNA duplexes were found to follow the Hofmeister series, emphasizing the importance of the hydrophobic interaction between nucleobases for the stability of the PNA complexes in high salt concentration.

Homopyrimidine PNA can recognize a purine target of double-stranded DNA by local displacement of the DNA pyrimidine strand and formation of a PNA-DNA-PNA tripler. In order to elucidate the mechanism of this PNA/DNA recognition reaction we have studied the interaction of PNA-T oligomers with poly(da):poly(dT) as a model system. The PNA binding kinetics can be observed in situ by spectroscopy as a change in the circular dichroism spectrum. The overall reaction rate decreases with increasing ionic strength and proceeds in minutes at 50 mM NaCl. From the temperature dependence of the rate constants an activation energy of about 60 kJ/mol (at 50 mM NaCl) was estimated, consistent with the hypothesis that a rate limiting step could be the DNA opening frequency. As expected from the stability of a DNA double helix toward large-scale openings, also the activation energy of the strand displacement increases somewhat with increasing salt concentration. There is a nonlinear dependence of the overall rate constant of tripler formation on the PNA concentration with an exponent of 2 or somewhat higher. With PNA in excess, the CD signal shows an overshoot suggesting the presence of a third species. The CD spectrum of this intermediate indicates an ordered structure. The presence of intercalators ethidium bromide and 9-aminoacridine is found to increase the overall PNA binding rate, whereas minor groove binder DAPI and major groove binder methyl green both decrease the rate. The mechanism of strand invasion of duplex DNA by PNA is discussed in the light of these results.

To elucidate the binding mode of recombination protein A (RecA) to double-stranded (ds) DNA, the effects on the RecA-DNA interaction of several mono- and bisintercalators of the acridine, phenanthridine, and cyanine classes have been investigated by linear dichroism spectroscopy. Simple monointercalators lacking side chains efficiently promoted the binding of RecA to dsDNA in the absence of nucleotide cofactor, which is otherwise required. Bisintercalators varied in their ability to induce RecA binding, while monointercalators with aminoalkyl side chains proved inefficient. Modification of DNA structure by the intercalator appears to be necessary for induction of RecA binding, but if the intercalator has a bulky minor-groove-binding side chain, it does not induce RecA binding. In detailed studies with acridines, neither the binding geometry of intercalators nor the structure of DNA was significantly modified upon binding of RecA without cofactor. Judged by circular dichroism, similar RecA conformational changes accompanied bis-9-aminoacridine- and ATP gamma S-induced RecA association with DNA. In the presence of ATP gamma S, the intercalators inhibited the rate of RecA binding to dsDNA and were extruded from DNA upon binding of RecA. This competitive aspect may suggest that intercalation of some amino acid residue(s) plays a role in nucleotide-induced RecA binding. The stoichiometry of the RecA-DNA-intercalator filament was determined; in the fully formed filament the base pair:intercalator ratio is 2, and the base pair:RecA ratio also 2. This contrasts with a base pair:RecA ratio of 3 in the ATP gamma S-induced filament, although in both cases the DNA experiences 50% extension.

The binding of phenanthridine dyes to tripler poly(dT)*poly(dA). poly(dT) and its precursor duplex poly(dA). poly(dT) is characterized using linear dichroism and circular dichroism spectroscopy, and thermal denaturation. The two monomeric dyes ethidium bromide and propidium iodide are shown to behave similarly to each other in intercalating into and stabilizing both the duplex and the tripler structures. However, contrary to expectations, the extra cationic side-chain of propidium iodide provides no significant extra stabilization of tripler compared with ethidium bromide, although propidium does stabilize the duplex more than ethidium. The monomeric dyes appear to have somewhat different binding geometries with the duplex and tripler polymers. The dimeric dye ethidium homodimer is found to bis-intercalate in the tripler as well as the duplex but, in contrast to the monomers, no variation in geometry between duplex and tripler is observed. However, although dimer stabilizes the duplex, it has no effect on the thermal stability of the tripler. This lack of binding preferentiality of the dimer for tripler compared with the monomeric dyes indicates greater constraints on the accommodation of a bis-intercalator in the tripler structure than in the duplex.

The interactions of RecA with double-stranded DNA and with cofactor adenosine 5'-[3-thio]triphosphate (ATP[S] an analog of ATP) have been characterized by circular dichroism (CD) spectroscopy in a search for conformational changes associated with the formation of helical RecA ATP . DNA . fibers. Upon interaction with the RecA protein the cofactor is found to be structurally perturbed, possibly towards the syn ribose form of ATP[S], while the secondary structure of RecA remains unaffected. By contrast, when the ATP[S] . RecA . DNA complex is formed, a distinct change of the protein CD spectrum near 200 nm is observed as a result of interaction of RecA with DNA. The main change occurs upon the binding of the first DNA molecule [RecA can bind up to three DNA molecules simultaneously; Takahashi, M., Kubista, M. and Norden, B. (1991) Biochimie (Paris) 73, 219-226] and the effect appears to be independent of DNA sequence, suggesting a general change of protein conformation upon DNA binding. The CD of DNA is changed, indicating an alteration of the DNA structure, possibly related to stretching and unwinding. A small, reversible, decrease in the CD amplitude of RecA was observed when raising the temperature from 4 degrees C to 30 degrees C. The CD of RecA increases slightly with pH (up to 7.8) but is constant between pH 6.0 and 6.8. At pH below 6.0 or higher temperature (40 degrees C) slow irreversible denaturation of RecA occurs. The CD signal is effectively independent of salt, even in 2.2 M NaCl or 1 M sodium acetate, which is relevant regarding reported ATPase and coprotease activities promoted by salt. For high concentrations of magnesium (10 mM) at 30 degrees C the CD of RecA changes markedly and the appearance of light scattering indicates aggregation.

Cell-penetrating peptides and antimicrobial peptides are two classes of positively charged membrane active peptides with several properties in common. The challenge is to combine knowledge about the membrane interaction mechanisms and structural properties of the two classes to design peptides with membrane-specific actions, useful either as transporters of cargo or as antibacterial substances. Membrane active peptides are commonly rich in arginine and tryptophan. We have previously designed a series of arg/trp peptides and investigated how the position and number of tryptophans affect cellular uptake. Here we explore the antimicrobial properties and the interaction with lipid model membranes of these peptides, using minimal inhibitory concentrations assay (MIC), circular dichroism (CD) and linear dichroism (LD). The results show that the arg/trp peptides inhibit the growth of the two gram positive strains Staphylococcus aureus and Staphylococcus pyogenes, with some individual variations depending on the position of the tryptophans. No inhibition of the gram negative strains Proteus mirabilis or Pseudomonas aeruginosa was noticed. CD indicated that when bound to lipid vesicles one of the peptides forms an α-helical like structure, whereas the other five exhibited rather random coiled structures. LD indicated that all six peptides were somehow aligned parallel with the membrane surface. Our results do not reveal any obvious connection between membrane interaction and antimicrobial effect for the studied peptides. By contrast cell-penetrating properties can be coupled to both the secondary structure and the degree of order of the peptides.

The photophysical properties of the optical DNA probe YOYO (homodimeric derivative of oxazole yellow) have been characterized in terms of the monomeric part, the YO chromophore. In aqueous solutions YO is virtually nonfluorescent but upon binding to DNA its fluorescence quantum yield is strongly increased. A similar enhancement of the fluorescence is observed for YO in the viscous solvent glycerol. The high fluorescence quantum yield of YO, when bound to DNA or in a viscous solution, is proposed to be a result of decreased rotational mobility around the internuclear bridge between the two aromatic ring systems. This hypothesis is based on similar values of the activation energies for the temperature-dependent nonradiative decay processes (E(A) = 53 kJ/mol) and viscous flow (E(A) = 63 kJ/mol), suggesting related rate-limiting mechanisms. A single electronic transition is found to be responsible for the intense visible absorption band. This conclusion is based on the observation of an essentially wavelength-independent reduced linear dichroism and similarly wavelength independent fluorescence anisotropy, and the fact that the emission spectrum is very nearly a mirror image of the absorption spectrum. The conclusion is further supported by quantum mechanical calculations (CNDO/S). By combination of measurements of fluorescence anisotropy of YO in glycerol and linear dichroism of YO in a stretched poly(vinyl alcohol) film, the transition moment of the strong visible absorption band was found to be nearly long axis polarized, in agreement with the CNDO/S calculations. The low-energy electronic transition and its polarization direction in the YO chromophore remain essentially unperturbed in the YOYO dye, suggesting that the results obtained for the excited state of the YO chromophore are applicable also to YOYO. One difference, though, is that in aqueous solutions the two YO chromophores of YOYO interact with each other, forming an internal dimer, resulting in a distorted absorption spectrum.

The modes of binding of the phenothiazinium dye methylene blue (1) to alternating and nonalternating polynucleotides and to calf thymus (CT) DNA have been characterized using linear dichroism (LD) and circular dichroism (CD) spectroscopy. With the polynucleotide [poly(dG-dC)](2) the interaction at low binding ratios is shown to be purely intercalative and the binding mode is insensitive to changes in ionic strength. The observed CD spectrum is bisignate, which may be due to intercalation at the different base-pair steps (5'G-C3' and 5'C-G3'), giving rise to CD signals of different sign and shape, By contrast, a single intercalative binding mode with the alternating AT polynucleotide [poly(dA-dT)](2) is likely only at very low ionic strength; at high ionic strength (200 mM phosphate, pH 6.9), a second binding mode is also manifest which is attributed to groove binding of the dye. The absorption and linear dichroism spectroscopic features of the methylene blue/CT-DNA (42% GC) complex reflect those of complexes of the dye with both [poly(dA-dT)](2) and [poly(dG-dC)](2); the circular dichroism spectrum of the methylene blue/CT-DNA complex and its variation with ionic strength reflect the complexity of even this simple system where numerous possible binding sites exist. Comparative binding to the nonalternating polynucleotides poly(dA).poly(dT) and poly(da).poly(dC), which each possess only one base-pair step, was also examined. On the basis of the combined LD and CD evidence, it is proposed that the dye is loosely bound with poly(dA).poly(dT), probably in the major groove, and intercalated with poly(dG).poly(dC).

Utilizing linear dichroism (LD), circular dichroism (CD), and fluorescence energy transfer, the binding geometries of a series of Co(3+)-porphyrins and their free ligands were examined. The compounds studied were Co-meso-tetrakis(N-methylpyridinium-4-yl)porphyrin (CoTMPyP) and its free ligand (H2-TMPyP), Co-meso-tetrakis(N-n-butylpyridinium-4-yl)porphyrin (CoTBPyP) and its free ligand (H2TBPyP), and Co-meso-tetrakis(N-n-octylpyridinium-4-yl)porphyrin (CoTOPyP). The two non-metalloporphyrins exhibit negative LD, having angles of roughly 75 degrees relative to the DNA helix axis. They also display negative CD and a significant contact energy transfer from the DNA bases. On the other hand, the three metalloporphyrins display orientation angles of roughly 45 degrees between the porphyrin plane and the helix axis of DNA. Furthermore, they exhibit positive CD and no contact energy transfer from DNA bases. These observations show that the metalloporphyrins are not intercalated whereas non-metalloporphyrins having four freely rotating meso-aryl groups intercalate between the base pairs of DNA. In the presence of KHSO5, the cobalt porphyrins cleave closed circular PM2 DNA in a single strand manner, i.e., a single activation event on the porphyrin leads to a break in one of the DNA strands. A kinetic analysis of the cleavage data revealed that cleavage rates are in the order CoTMPyP > CoTBPyP > CoTOPyP with the difference being due to different DNA affinities rather than differences in cleavage rate-constants. Based on these and earlier observations, the metalloporphyrins appear bound to a partially melted region of DNA.

In the search for methods to study structure and function of membrane-associated proteins and peptides flow linear dichroism, LD, spectroscopy has emerged as a promising technique. Using shear-aligned lipid vesicles, conformations and binding geometries of membrane-bound bio-macromolecules can be assessed. Here we investigate anchoring properties and specific orientations of tryptophan relative to the peptide backbone and to the membrane normal for the model peptides gramicidin and melittin. We have monitored the conformational change associated with the refolding of non-channel gramicidin into its channel form, and quantitatively determined the average orientations of its tryptophan transition moments, suggesting that these residues adopt a well-defined orientation at the membrane interface. An important conclusion regards the structural variation of gramicidin between these two distinct transmembrane forms. Whilst circular dichroism (CD) spectra, as has been reported before, vary strongly between the two forms suggesting their structures might be quite different, the LD results clearly evidence both the peptide backbone orientation and tryptophan side-chain positioning to be very similar. The latter are oriented in accord with what is expected from their role to anchor peptide termini to the membrane surface. The variations in CD could be due to, the in LD observed, minor shifts in mutual orientation and distance between neighbouring tryptophans sensitively determining their exciton interactions. Our data dispute that the non-channel form of membrane-bound gramicidin would be any of the intertwined forms often observed in crystal as the positioning of tryptophans along the peptide axis would not be compatible with the strong interfacial positioning observed here. The general role of tryptophans as interfacial anchors is further assessed for melittin whose conformation shows considerable angular spread, consistent with a carpet model of its mechanism for induced membrane leakage, and a predominantly surface-aligned membrane orientation governed by amphipathic interactions.

Complexes of 4',6-diamidino-2-phenylindole (DAPI) with [poly(dG-dC)]2 and [poly(dI-dC)]2 were studied by optical spectroscopic techniques including linear dichroism (LD), circular dichroism (CD), and fluorescence measurements. The aim was to investigate the importance of the exocyclic amino group of guanine that protrudes into the minor groove of [poly(dG-dC)]2 but is absent in [poly(dI-dC)]2. When bound to [poly(dG-dC)]2, DAPI exhibits a negative, and strongly wavelength-dependent, reduced linear dichroism (LDr) in the DAPI absorption region, a weak positive CD, and a fluorescence behavior that is similar to that of free DAPI with accessibility to quenching by the aqueous solvent. These spectroscopic properties have been interpreted in terms of a major-groove binding geometry by Kim et al. (Kim, S. K.; Eriksson, S.; Kubista, M.; Norden, B. J. Am. Chem. Soc. 1993,115,3441-3447). By contrast, when bound to [poly(dI-dC)]2, DAPI exhibits a strong positive CD in the 300-420-nm region, a positive (wavelength-independent) LD(r), a strong increase of the fluorescence intensity, and shielding to added quencher. These spectroscopic properties closely resemble those of the DAPI-[poly(dA-dT)]2 complex, in which DAPI is situated deep in the minor groove of the polynucleotide. We conclude that the major groove binding geometry of DAPI when complexed with [poly(dG-dC)]2 is a result of a decreased affinity to the minor groove of [poly(dG-dC)]2 due to steric hindrance and decreased electronegative attraction caused by the amino group of guanine.

We have characterized the interaction of 4',6-diamidino-2-phenylindole (DAPI) with a series of DNA oligonucleotides containing a varying number of contiguous alternating AT base pairs in the center of a GC-stretch. The binding affinity of DAPI to the oligonucleotides increases with the number of contiguous AT base pairs. When entropy effects are taken into account, the microscopic affinity reaches a maximum value when the oligonucleotides contain three AT base pairs. Three is also the minimum number of base pairs that provides a binding site with all the characteristics of binding observed with DNA and [poly(dA-dT)]2 at low binding ratios. With none or only a single AT base pair in the center of a GC dodecamer, the spectral properties of bound DAPI are very similar to those of DAPI bound to [poly(dG-dC)]2. When DAPI is complexed with an oligonucleotide containing two AT base pairs, the absorption and fluorescence properties of DAPI closely resemble those of DAPI complexed with [poly(dG-dC)]2, while the circular dichroism spectrum resembles that of DAPI bound to [poly(dA-dT)]2.

The binding of an eightmer of peptide nucleic acid, H-T8-Lys-NH2 (=PNA-T8), to a polynucleotide, poly(dA), was studied by flow linear dichroism (LD) and circular dichroism (CD) spectroscopy. Whereas the single stranded DNA, due to its high flexibility, does not display any measurable LD signal when subjected to shear flow, the complex with PNA does. A titration shows that saturation occurs at a stoichiometry of two PNA thymine bases per DNA adenine base, indicating the formation of a triplex PNA2-DNA complex. The persistence length of the adduct remains small up to relatively high stoichiometries (above 1:1 T:A) indicating that no significant amounts of PNA:DNA duplex are formed. Instead triplex stretches seem to form surrounded by flexible parts of single stranded poly(dA). Upon approaching the stoichiometry 2:1 of T:A the LD increases dramatically demonstrating that the stiffness of the PNA-DNA triplex arises from base-base contacts preventing bending of the chain. It is also inferred that the main stiffness of duplex DNA very probably has a similar origin and is not primarily a result of the increased phosphate-phosphate repulsion. Circular dichroism spectra support the conclusion that a triplex is formed as the only PNA-DNA complex and that it is a right-handed helix. The wavelength dependence of the reduced linear dichroism shows that the inclination of the bases from perpendicularity relative to the helix axis is small. The base conformation of the poly(dA)[PNA-T8]2 triplex is very similar to that of the conventional poly(dA)[poly(dT)]2 triplex.

DNA strand exchange is catalyzed by molecular crowding and hydrophobic interactions in concentrated aqueous solutions of polyethylene glycol, a discovery of relevance for understanding the function of recombination enzymes and with potential applications to DNA nanotechnology.

A systematic theoretical study of the CD of [poly (dA-dT)]2 and its complexes with achiral small molecules is presented. The CD spectra of [poly (dA-dT)]2 and of poly (dA):poly(dT) are calculated for various DNA structures using the matrix method. The calculated and experimental spectra agree reasonably well for [poly(dA-dT)]2 but less well for poly(dA):poly(dT). The calculated CD spectrum of [poly(dA-dT)]2 fails to reproduce the wavelength region of 205-245 nm of the experimental spectrum. This discrepancy can be explained by a magnetic dipole allowed transition contributing significantly to the CD spectrum in this region. The induced CD of a transition moment of a molecule bound to [poly(dA-dT)]2 is also calculated. As was the case for [poly(dG-dC)]2, the induced CD of a groove bound molecule is one order of magnitude stronger than that of an intercalated molecule. The calculations also show considerable differences between pyrimidine-purine sites and purine-pyrimidine sites. Both signs and magnitudes of the CD induced into ligands bound in the minor groove agree with experimental observations.

In this work we examine the trapping and conversion of visible light energy into chemical energy using a supramolecular assembly. The assembly consists of a light-absorbing antenna and a porphyrin redox center, which are covalently attached to two complementary 14-mer DNA strands, hybridized to form a double helix and anchored to a lipid membrane. The excitation energy is finally trapped in the lipid phase of the membrane as a benzoquinone radical anion that could potentially be used in subsequent chemical reactions. In addition, in this model complex, the hydrophobic porphyrin moiety acts as an anchor into the liposome positioning the DNA construct on the lipid membrane surface. The results show the suitability of our system as a prototype for DNA-based light-harvesting devices, in which energy transfer from the aqueous phase to the interior of the lipid membrane is followed by charge separation.

The interaction of tubulin with thiocolchicine and two thiocolchicine analogues, one lacking the B ring and one with a six-membered B ring, has been studied by using near-UV and CD spectroscopies. Rapid, reversible binding of the latter analogue to tubulin demonstrates the ability of the colchicine binding site to accommodate the phenyltropone system with a more coplanar conformation than is present in free colchicine. There is no evidence, however, that bound thiocolchicine should have a much less twisted conformation than free thiocolchicine. Thiocolchicine and the bicyclic analogue appear to have approximately the same conformation of the phenyltropone system, in both the free and the bound states, suggesting that this conformation has an optimal arrangement of the phenyl and tropone rings for binding to tubulin. In contrast to colchicine and related derivatives, the three thiocolchicine analogues show pronounced near-UV CD bands upon association to tubulin. No simple relation could be found between the sign pattern of the CD components in the near-UV band of the thiocolchicinoid chromophore and its axial chirality.

Despite extensive study of DNA interaction with propeller-shaped metal complexes, such as the DELTA and LAMBDA enantiomers of [Ru(1,10-phenanthroline)3]2+, the basis for their enantioselectivity, and even their binding modes, are not yet fully understood. H-1 NMR studies of the interactions with the self-complementary oligonucleotide d(CGCGATCGCG)2 indicate that both enantiomers bind into the minor groove of the central AT-TA region, but with a rapid exchange between the bound and free states. Flow linear dichroism (FLD) and circular dichroism (CD) show different binding geometries for the two enantiomers. These two geometries are found in natural DNA as well as in a number of different B form polynucleotides, virtually independent of base composition and of methylation. The DNA interaction with the [Ru(1,10-phenanthroline)3]2+ complexes will be reconsidered in the light of NMR, FLD, CD and fluorescence results.

In this work we demonstrate how polarized light absorption spectroscopy (linear dichroism (LD)) analysis of the peptide ultraviolet-visible spectrum of a membrane-associated protein (cytochrome (cyt) c) allows orientation and structure to be assessed with quite high accuracy in a native membrane environment that can be systematically varied with respect to lipid composition. Cyt c binds strongly to negatively charged lipid bilayers with a distinct orientation in which its alpha-helical segments are on average parallel to the membrane surface. Further information is provided by the LD of the pi-pi( *) transitions of the heme porphyrin and transitions of aromatic residues, mainly a single tryptophan. A good correlation with NMR data was found, and combining NMR structural data with LD angular data allowed the whole protein to be docked to the lipid membrane. When the redox state of cyt c was changed, distinct variations in the LD spectrum of the heme Soret band were seen corresponding to changes in electronic transition energies; however, no significant change in the overall protein orientation or structure was observed. Cyt c is known to interact in a specific manner with the doubly negatively charged lipid cardiolipin, and incorporation of this lipid into the membrane at physiologically relevant levels was indeed found to affect the protein orientation and its alpha-helical content. The detail in which cyt c binding is described in this study shows the potential of LD spectroscopy using shear-deformed lipid vesicles as a new methodology for exploring membrane protein structure and orientation.

Electrostatic shielding and steric blocking by histones are two significant factors that participate in the control of the local rates of transcription in chromatin. As a simple model system to determine how the degree of DNA condensation affects enzyme accessibility and gene expression, we have used generation 5 polyamidoamine (G5 PAMAM) cationic dendrimer particles (size 5.4 nm) as a synthetic histone model together with an in vitro transcription assay. The degree of compaction, conformation, and binding availability of the dendrimer-DNA complexes is characterized by linear and circular dichroism, dynamic light scattering, and competitive binding of ethidium. Using ultracentrifugation we are able to show explicitly, for the first time, that dendrimer particles bind to DNA in a highly cooperative manner, and that the dendrimer-induced condensation of the DNA strongly attenuates transcription. Two fractions with different properties can be identified: a low-density fraction which behaves very similar to uncondensed DNA and a high-density fraction which is condensed to a high extent and where binding availability and transcription are strongly reduced. Circular dichroism gives clues to the structure of the condensed DNA indicating long-range order between the helices such as in polymer-salt-induced cholesteric liquid crystalline domains, one possible shape being a toroidal structure. On the basis of the experimental data, we propose a model for the self-assembly of the dendrimer-DNA system.

pH-sensitive HA2 fusion peptides from influenza virus hemagglutinin have potential as endosomal escape-inducing components in peptide-based drug delivery. Polarized light spectroscopy and tryptophan fluorescence were used to assess the conformation, orientation, effect on lipid order, and binding kinetics of wild-type peptide HA2(1-23) and a glutamic acid-enriched analogue (INF7) in large unilamellar POPC or POPC/POPG (4:1) lipid vesicles (LUVs). pH-sensitive membrane leakage was established for INF7 but not HA2(1-23) using an entrapped-dye assay. A correlation is indicated between leakage and a low degree of lipid chain order (assessed by linear dichroism, LD, of the membrane orientation probe retinoic acid). Both peptides display poor alignment in zwitterionic POPC LUVs compared to POPC/POPG (4:1) LUVs, and it was found that peptide-lipid interactions display slow kinetics (hours), resulting in reduced lipid order and increased tryptophan shielding. At pH 7.4, INF7 displays tryptophan emission and LD features indicative of a surface-orientated peptide, suggesting that its N-terminal glutamic acid residues prevent deep penetration into the hydrocarbon core. At pH 5.0, INF7 displays weaker LD signals, indicating poor orientation, possibly due to aggregation. By contrast, the orientation of the HA2(1-23) peptide backbone supports previously reported oblique insertion ( approximately 60-65 degrees relative to the membrane normal), and aromatic side-chain orientations are consistent with an interfacial (pH-independent) location of the C-terminus. We propose that a conformational change upon reduction of pH is limited to minor rearrangements of the peptide "hinge region" around Trp14 and repositioning of this residue.

Reports on serious artifacts associated with the use of cell fixation in studies of the cellular uptake of cell-penetrating peptides, also denoted protein transduction domains, have demonstrated the need for a reevaluation of the current understanding of peptide-mediated cellular delivery of large, hydrophilic molecules. In a recent study on the internalization in unfixed cells of penetratin and its analogues in which tryptophans are substituted for phenylalanines (Pen2W2F), lysines for arginines (PenArg), and arginines for lysines (PenLys), we revealed large dissimilarities in cell interactions among the peptides [Thoren et al. (2003) Biochem. Biophys. Res. Commun. 307, 100-107]. We here investigated possible correlations with their respective affinities for the lipid membranes of large unilamellar vesicles. The variations found in membrane affinity correlated qualitatively with differences in hydrophobicity among the peptides but were by far too small to account for the striking differences in cell membrane binding. Interestingly, we found that the inclusion of a small fraction of lipids conjugated to poly(ethylene glycol) (PEG) in the vesicles both stabilized the vesicle dispersion against peptide-induced aggregation and, furthermore, enhanced the binding of the peptides to the membrane. By use of PEG-conjugated lipids, it could be shown that vesicle aggregation drives an alpha-helix to beta-sheet conformational transition for these peptides. A similar transition was discovered at submicellar concentrations of sodium dodecyl sulfate in aqueous solution for all peptides except PenLys. Finally, significant changes of the contributions to CD spectra from aromatic residues due to their insertion into the membrane were observed.

For further characterization of the hybridization properties of peptide nucleic acids (PNAs), the thermodynamics of hybridization of mixed sequence PNA-DNA duplexes have been studied. We have characterized the binding of PNA to DNA in terms of binding affinity (perfectly matched duplexes) and sequence specificity of binding (singly mismatched duplexes) using mainly absorption hypochromicity melting curves and isothermal titration calorimetry. For perfectly sequence-matched duplexes of varying lengths (6-20 bp), the average free energy of binding (DeltaG degrees ) was determined to be -6.5+/-0.3 kJ mol(-1) bp(-1), corresponding to a microscopic binding constant of about 14 M(-1) bp(-1). A variety of single mismatches were introduced in 9- and 12-mer PNA-DNA duplexes. Melting temperatures (T(m)) of 9- and 12-mer PNA-DNA duplexes with a single mismatch dropped typically 15-20 degrees C relative to that of the perfectly matched sequence with a corresponding free energy penalty of about 15 kJ mol(-1) bp(-1). The average cost of a single mismatch is therefore estimated to be on the order of or larger than the gain of two matched base pairs, resulting in an apparent binding constant of only 0.02 M(-1) per mismatch. The impact of a mismatch was found to be dependent on the neighboring base pairs. To a first approximation, increasing the stability of the surrounding region, i.e., the distribution of A.T and G.C base pairs, decreases the effect of the introduced mismatch.

The RecA protein requires ATP or dATP for its coprotease and strand exchange activities. Other natural nucleotides, such as ADP, CTP, GTP, UTP and TTP, have little or no activation effect on RecA for these activities. We have investigated the activation mechanism, and the selectivity for ATP, by studying the effect of various nucleotides on the DNA binding and the helical structure of the RecA filament. The interaction with DNA was investigated via fluorescence measurements with a fluorescent DNA analog and fluorescein-labeled oligonucleotides, assisted by linear dichroism. Filament structure was investigated via small-angle neutron scattering. There is no simple correlation between filament elongation, DNA binding affinity of RecA, and DNA structure in the RecA complex. There may be multiple conformations of RecA, Both coprotease and strand exchange activities require formation of a rigid and well organized complex. The triphosphate nucleotides which do not activate RecA, destabilize the RecA-DNA complex, indicating that the chemical nature of the nucleotide nucleobase is very important for the stability of RecA-DNA complex. Higher stability of the RecA-DNA complex in the presence of adenosine 5'-O-3-thiotriphosphate or guanosine 5'-O-3-thiotriphosphate than ATP or GTP indicates that contact between the protein and the chemical group at the gamma position of the nucleotide also affects the stability of the RecA-DNA complex. This contact appears also important for the rigid organization of DNA because ADP strongly decreases the rigidity of the complex.

The thermodynamics of hybridization and the conformations of decameric mixed purine-pyrimidine sequence PNA/PNA, PNA/DNA, and DNA/DNA duplexes have been studied using fluorescence energy transfer (FET), absorption hypochromicity (ABS), isothermal titration calorimetry (ITC), and circular dichroism (CD) techniques. The interchromophoric distances determined in the FET experiments on fluorescein- and rhodamine-labeled duplexes indicate that the solution structures of the duplexes are extended helices in agreement with available NMR (PNA/DNA) and crystal X-ray data (PNA/PNA). The melting thermodynamics of the duplexes was studied with both FET and ABS. The thermodynamic parameters obtained with ABS are in good agreement with the parameters from calorimetric measurements while FET detection of duplex melting gives in most cases more favorable free energies of hybridization. This discrepancy between FET and ABS detection is ascribed to the conjugated dyes which affect the stability of the duplexes substantially. Especially, the dianionic fluorescein attached via a flexible linker either to PNA or to DNA seems to be involved in an attractive interaction with the opposite dicationic lysine when hybridized to a PNA strand. This interaction leads to an increased thermal stability as manifested as a 3-4 degrees C increase of the melting temperature. For the PNA/DNA duplex where fluorescein is attached to the PNA strand, a large destabilization (Delta T-m = -12 degrees C) occurs relative to the unlabeled duplex, probably originating from electrostatic repulsion between the fluorescein and the negatively charged DNA backbone. In the case of the PNA/PNA duplex, the sense of helicity of the duplex is reversed upon conjugation of fluorescein via a flexible linker arm, but not when the fluorescein is attached without a linker to the PNA.

The binding of an antiviral quinoxaline derivative, 2,3-dimethyl- 6 - (dimethylaminoethyl) - 9 - hydroxy - 6H - indolo - [2,3 - b]quinoxaline (9-OH-B220), to synthetic double and triple helical DNA (poly(dA).poly(dT) and poly(dA).2poly(dT)) and RNA (poly(rA). poly(rU) and poly (rA).2poly(rU)) has been characterized using flow linear dichroism (LD), circular dichroism (CD), fluorescence spectroscopy, and thermal denaturation. When either of the DNA structures or the RNA duplex serve as host polymers a strongly negative LD is displayed, consistent with intercalation of the chromophoric ring system between the base-pairs/triplets of the nucleic acid structures. Evidence for this geometry also includes weak induced CD signals and strong increments of the fluorescence emission intensities upon binding of the drug to each of these polymer structures. In agreement with intercalative binding, 9-OH-B220 is found to effectively enhance the thermal stability of both the double and triple helical states of DNA as well as the RNA duplex. In the case of poly(dA).2poly(dT), the drug provides an unusually large stabilization of its triple helical state; upon binding of 9-OH-B220 the triplex-to-duplex equilibrium is shifted towards higher temperature by 52.5 deg. C in a 10 mM sodium cacodylate buffer (pH 7.0) containing 100 mM NaCl and 1 mM EDTA. When triplex RNA serves as host structure, LD indicates that the average orientation angle between the drug chromophore plane and the helix axis of the triple helical RNA is only about 60 to 65 degrees. Moreover, the thermal stabilizing capability, as well as the fluorescence increment, CD inducing power and perturbations of the absorption envelope, of 9-OH-B220 in complex with the RNA triplex are all less pronounced than those observed for the complexes with DNA and duplex RNA. These features indicate binding of 9-OH-B220 in the wide and shallow minor groove of poly(rA).2poly(rU). Based on the present results, some implications for the applications of this low-toxic, antiviral and easily administered drug in an antigene strategy, as well as its potential use as an antiretroviral agent, are discussed.

Peptide nucleic acid (PNA) is an oligonucleotide mimic in which the backbone of DNA has been replaced by a pseudopeptide. Thymine-rich homopyrimidine PNA oligomers have been found to recognize double-stranded DNA targets by displacement of the pyrimidine DNA strand and forming an internal Watson-Crick-Hoogsteen base-paired PNA(pyr)-DNA(pu)-PNA(pyr) tripler. We here show that cytosine-rich homopyrimidine PNA sequences instead add to double-stranded polynucleotide targets as Hoogsteen strands forming PNA(pyr)-DNA(pu)-DNA(pyr) triplexes. Furthermore, PNA strands with homopurine or alternating thymine-guanine sequences are shown to invade their respective DNA targets by displacing the identical DNA strands of the polynucleotides and forming new PNA-DNA duplexes. These results indicate distinct mechanistic variations as to how PNA interacts with a DNA target depending on choice of nucleobases, which could be of importance for future design of gene-specific diagnostic or therapeutic agents.