Single-strand DNA binding of actinomycin D with a chromophore 2-amino to 2-hydroxyl substitution

A modified actinomycin D was prepared with a hydroxyl group that replaced the amino group at the chromophore 2-position, a substitution known to strongly reduce affinity for double-stranded DNA. Interactions of the modified drug on single-stranded DNAs of the defined sequence were investigated. Competition assays showed that 2-hydroxyactinomycin D has low affinity for two oligonucleotides that have high affinities (K(a) = 5-10 x 10(6) M(-1) oligomer) for 7-aminoactinomycin D and actinomycin D. Primer extension inhibition assays performed on several single-stranded DNA templates totaling around 1000 nt in length detected a single high affinity site for 2-hydroxyactinomycin D, while many high affinity binding sites of unmodified actinomycin D were found on the same templates. The sequence selectivity of 2-hydroxyactinomycin D binding is unusually high and approximates the selectivity of restriction endonucleases. Binding appears to require a complex structure, including residues well removed from the polymerase pause site.     

A study of interaction of 7-aminoactinomycin D with DNA by fluorescence correlation spectroscopy

The investigation of interaction of 7-aminoactinomycin D with DNA is hampered at nanomolar concentrations by low quantum yield of the dye fluorescence and high adsorbability of the dye. It was found that, instead of the increase in the fluorescence of 7-aminoactinomycin D after binding with DNA, a decrease in the fluorescence takes place, because 7-aminoactinomycin D complexed with DNA exists in two states: photochemically active and inactive. The presence of the photochemically active state of 7-aminoactinomycin D causes an apparent increase in the diffusion coefficient upon embedding of 7-aminoactinomycin D into DNA. The data obtained allow one to state that 7-aminoactinomycin D: (1) forms dimers at micromolar concentration, (2) has two specific photodestruction times, and (3) binds with DNA more effectively than actinomycin D. Polarization measurements made it possible to estimate numerically the adsorption of 7-aminoactinomycin D on the walls of the measuring cell.     

The intrinsic tyrosine fluorescence of histone H1. Steady state and fluorescence decay studies reveal heterogeneous emission

In wavelength-resolved steady state spectra we observe three different kinds of emission from histone H1, a class A protein with only a single tyrosine residue. Unfolded H1 emissions that peak at approximately 300 and 340 nm can both be excited maximally at approximately 280 nm. Another, peaking much further to the red at approximately 400 nm, can be excited maximally at approximately 320 nm. The 300-nm fluorescence can be resolved by lifetime measurements into three components with decay times of approximately 1, 2, and 4 ns. On sodium-chloride-induced refolding of H1, simplification of the emission properties occurs. The 340 and 400-nm components disappear while the two shorter lifetime components of the 300-nm band diminish in amplitude and are replaced by the 4-ns decay. We believe that the 340-nm emission is tyrosinate fluorescence resulting from excited-state proton transfer. The origin of the 400-nm emission remains uncertain. We assign the 1 and 2-ns components of the 300-nm emission to two states of tyrosine in denatured H1 and the 4-ns decay to fluorescence of the single tyrosine residue in the globular region of refolded H1. Our results support the contention that salt induced folding of H1 is a cooperative two state process, and permit us to better understand the previously reported increases in fluorescence intensity and anisotropy on salt-induced folding.     

Hydrophobic surfaces of tubulin probed by time-resolved and steady-state fluorescence of nile red

Binding of Nile Red to tubulin enhances and blue-shifts fluorescence emission to about 623 nm with a "shoulder" around 665 nm. Binding is reversible and saturable with an apparent Kd of approximately 0.6 microM. Nile Red does not alter tubulin polymerization, and polymerization in 2-(N-morpholino)ethanesulfonic acid (Mes) buffer does not alter the spectrum of the Nile Red-tubulin complex. In contrast, polymerization in glutamate buffer results in a red shift, reduction of intensity, and a decrease in lifetime, suggesting an increase in "polarity" of the binding environment. Lifetimes of 4.5 and 0.6 ns fluorescence in Mes buffer are associated with the 623-nm peak and the 665-nm shoulder, respectively. Indirect excitation spectra for these components are distinct and the 4.5-ns component exhibits tryptophan to Nile Red energy transfer. Acrylamide quenching yields linear Stern-Volmer plots with unchanged lifetimes, indicating static quenching. Apparent quenching constants are wavelength-dependent; global analysis reveals a quenchable component corresponding to the 4.5 ns component and an "unquenchable" component superposing the 0.6-ns spectrum. Analysis of anisotropy decay required an "associative" model which yielded rotational correlation times of greater than 50 ns for the 4.5-ns lifetime and 0.3 ns for the 0.6-ns lifetime. Dilution of tubulin in Mes results in an apparent red shift of emission without lifetime changes, due only to loss of the 623-nm component. These data are reconciled in terms of a model with two binding sites on the tubulin dimer. The more "nonpolar" site is located in a region of subunit-subunit contact which accounts for the fluorescence changes upon dilution; this permits estimation of a subunit dissociation constant of 1 microM.     

Purification and characterization of the bacteriophage T7 gene 2.5 protein. A single-stranded DNA-binding protein.

Bacteriophage T7 gene 2.5 protein has been purified to homogeneity from cells overexpressing its gene. Native gene 2.5 protein consists of a dimer of two identical subunits of molecular weight 25,562. Gene 2.5 protein binds specifically to single-stranded DNA with a stoichiometry of approximately 7 nucleotides bound per monomer of gene 2.5 protein; binding appears to be noncooperative. Electron microscopic analysis shows that gene 2.5 protein is able to disrupt the secondary structure of single-stranded DNA. The single-stranded DNA is extended into a chain of gene 2.5 protein dimers bound along the DNA. In fluorescence quenching and nitrocellulose filter binding assays, the binding constants of gene 2.5 protein to single-stranded DNA are 1.2 x 10(6) M-1 and 3.8 x 10(6) M-1, respectively. Escherichia coli single-stranded DNA-binding protein and phage T4 gene 32 protein bind to single-stranded DNA more tightly by a factor of 25. Fluorescence spectroscopy suggests that tyrosine residue(s), but not tryptophan residues, on gene 2.5 protein interacts with single-stranded DNA.     

A comparative study on the interaction of the putative anticancer alkaloids,sanguinarine and chelerythrine,with single- and double-stranded,and heat-denatured DNAs

A detailed investigation on the interaction of two benzophenanthridine alkaloids, sanguinarine (SGR) and chelerythrine (CHL), with the double-stranded (ds), heat-denatured (hd), and single-stranded (ss) DNA was performed by spectroscopy and calorimetry techniques. Binding to the three DNA conformations leads to quenching of fluorescence of SGR and enhancement in the fluorescence of CHL. The binding was cooperative for both of the alkaloids with all the three DNA conformations. The binding constant values of both alkaloids with the ds DNA were in the order of 10⁶ M^?1; binding was weak with hd and much weaker to the ss DNA. The fluorescence emission of the alkaloid molecules bound to the ds and hd DNAs was quenched much less compared to those bound to the ss DNA based on competition with the anionic quencher KI. For both double stranded and heat denatured structures the emission of the bound alkaloid molecules was polarized significantly and strong energy transfer from the DNA bases to the alkaloid molecules occurred. Intercalation of SGR and CHL to ds, hd, and ss DNA was proved from these fluorescence results. Calorimetric studies suggested that the binding to all DNA conformations was both enthalpy and entropy favored. Both the alkaloids preferred double-helical regions for binding, but SGR was a stronger binder than CHL to all the three DNA structures.     

Non stacking binding of 7-amino-actinomycin D and actinomycin D to DNA and model nucleotide systems in solutions

Mechanism of actinomycin D (AMD) and 7-aminoactinomycin D (7AAMD) interaction with DNA and model nucleotide compounds was studied by absorption and fluorescence spectroscopy (steady-state, phase-modulation, and polarization). It was shown that complex formation does not result in energy transfer from photoexcited nucleotides to phenoxazone chromophore of 7AAMD that indicates the absence of stacking-like intercalation. This fact is fundamentally important to explain the biological effect of actinomycin on cells. It was revealed a fundamental difference in the complex-forming properties of AMD and 7AAMD. Thus AMD is capable of binding to guanine micelles to destroy them. 7AAMD forms complexes neither guanine micelles nor polyguanilic acid. 7AAMD binding sites on DNA can differ substantially from AMD binding sites. However, a strong competition is observed between AMD and 7AAMD for binding site in oligonucleotide HP1 used as DNA hairpin model. The efficient diameters of 7AAMD-HP1 complex and free 7AAMD were determined using the Levshin-Perren equation.     

Nonstacking Binding of 7-Aminoactinomycin D and Actinomycin D to DNA and Model Nucleotide Systems in Solutions

The mechanism of actinomycin D (AMD) and 7-aminoactinomycin D (7AAMD) interaction with DNA and model nucleotide compounds was studied by absorption and fluorescence spectroscopy (steady-state, phase-modulation, and polarization). It was shown that complex formation does not result in energy transfer from photoexcited nucleotides to the phenoxazone chromophore of 7AAMD, which indicates the absence of stacking-like intercalation. This fact is fundamentally important to explain the biological effect of actinomycin on cells. A basic difference was revealed in the complex-forming properties of AMD and 7AAMD. Thus AMD is capable of binding to guanine micelles to destroy them; 7AAMD forms no complexes with either guanine micelles or polyguanylic acid. 7AAMD binding sites on DNA can differ substantially from AMD binding sites. However, strong competition is observed between AMD and 7AAMD for the binding site in oligonucleotide HP1 used as a DNA hairpin model. The effective diameters of 7AAMD–HP1 complex and free 7AAMD were determined using the Levshin–Perren equation.     

Texture analysis of fluorescence lifetime images of AT- and GC-rich regions in nuclei.

We used intensity and fluorescence lifetime microscopy (FLIM) of 3T3 nuclei to investigate the existence of AT-rich and GC-rich regions of the nuclear DNA. Hoechst 33258 (Ho) and 7-aminoactinomycin D (7-AAD) were used as fluorescence probes specific for AT and GC base pairs, respectively. YOYO-1 (Yo) was used as a dye that displays distinct fluorescence lifetimes when bound to AT or GC base pairs. We combined fluorescence imaging of Ho and 7-AAD with time-resolved measurements of Yo and took advantage of an additional information content of the time-resolved fluorescence. Because a single nucleus could not be stained and measured with all three dyes, we used texture analysis to compare the spatial distribution of AT-rich and GC-rich DNA in 100 nuclei in different phases of the cell cycle. The fluorescence intensity-based analysis of Ho- or 7-AAD-stained images indicates increased number and larger size of the DNA condensation centers in the G2/M-phases compared to G0/1-phases. The lifetime-based study of Yo-stained images suggests spatial separation of the AT- or GC-rich DNA regions in the G2/M-phase. Texture analysis of fluorescence intensity and lifetime images was used to quantitatively study the spatial change of condensation and separation of AT- and GC-rich DNA during the cell cycle.     

Fluorescence lifetime imaging of nuclear DNA: effect of fluorescence resonance energy transfer

BACKGROUND: DNA fluorescence dyes have been used to study DNA dynamics, chromatin structure, and cell cycle analysis. However, most microscopic fluorescence studies of DNA use only steady-state measurements and do not take advantage of the additional information content of the time-resolved fluorescence. In this paper, we combine fluorescence imaging of DNA with time-resolved measurements to examine the proximity of donors and acceptors bound to chromatin. METHODS: We used frequency-domain fluorescence lifetime imaging microscopy to study the spatial distribution of DNA-bound donors and acceptors in fixed 3T3 nuclei. Over 50 cell nuclei were imaged in the presence of an AT-specific donor, Hoechst 33258 (Ho), and a GC-specific acceptor, 7-aminoactinomycin D (7-AAD). RESULTS: The intensity images of Ho alone showed a spatially irregular distribution due to the various concentrations of DNA or AT-rich DNA throughout the nuclei. The lifetime imaging of the Ho-stained nuclei was typically flat. Addition of 7-AAD decreased the fluorescence intensity and lifetime of the Ho-stained DNA. The spatially dependent phase and modulation values of Ho in the presence of 7-AAD showed that the Ho decay becomes nonexponential, as is expected for a resonance energy transfer (RET) with multiple acceptors located over a range of distances. In approximately 40 nuclei, the intensity and lifetime decrease was spatially homogeneous. In approximately 10 nuclei, addition of 7-AAD resulted in a spatially nonhomogeneous decrease in intensity and lifetime. The RET efficiency was higher in G(2)/M than in G(0/1) phase cells. CONCLUSIONS: Because RET efficiency depends on the average distance between Ho and 7-AAD, data suggest that the heterogeneity of lifetimes and spatial variation of the RET efficiency are caused by the presence of highly condensed regions of DNA in nuclei.     

Fluorescence decay studies of the DNA-3,6-diaminoacridine complexes

The interaction of several 3,6-diaminoacridines with DNAs of various base composition has been studied by steady-state and transient fluorescence measurements. The acridine dyes employed are of the following two classes: class I - proflavine, acriflavine and 10-benzyl proflavine; class II - acridine yellow, 10-methyl acridine yellow and benzoflavine. It is found that the fluorescence decay kinetics follows a single-exponential decay law for free dye and the poly[d(A-T)]-dye complex, while that of the dye bound to DNA obeys a two-exponential decay law. The long lifetime (tau 1) for each complex is almost the same as the lifetime for the poly[d(A-T)]-dye complex, and the amplitude alpha 1 decreases with increasing GC content of DNA. The fluorescence quantum yields (phi F) of dye upon binding to DNA decrease with increasing GC content; the phi F values for class I are nearly zero when bound to poly(dG) X poly(dC), but those for class II are not zero. This is in harmony with the finding that GMP almost completely quenches the fluorescence for class I, whereas a weak fluorescence arises from the GMP-dye complex for class II. The fluorescence spectra of the DNA-dye complexes gradually shift toward longer wavelengths with increasing GC content. In this connection, the fluorescence decay parameters show a dependence on the emission wavelength; alpha 1 decreases with an increase in the emission wavelength. In view of these results, it is proposed that the decay behavior of the DNA-dye complexes has its origin in the heterogeneity of the emitting sites; the long lifetime tau 1 results from the dye bound to AT-AT sites, while the short lifetime tau 2 is attributable to the dye bound in the vicinity of GC pairs. Since GC pairs almost completely quench the fluorescence for class I, partly intercalated or externally bound dye molecules may play an important role in the component tau 2.     

Recognition and Binding of a Helix-Loop-Helix Peptide to Carbonic Anhydrase Occurs via Partly Folded Intermediate Structures

We have studied the association of a helix-loop-helix peptide scaffold carrying a benzenesulfonamide ligand to carbonic anhydrase using steady-state and time-resolved fluorescence spectroscopy. The helix-loop-helix peptide, developed for biosensing applications, is labeled with the fluorescent probe dansyl, which serves as a polarity-sensitive reporter of the binding event. Using maximum entropy analysis of the fluorescence lifetime of dansyl at 1:1 stoichiometry reveals three characteristic fluorescence lifetime groups, interpreted as differently interacting peptide/protein structures. We characterize these peptide/protein complexes as mostly bound but unfolded, bound and partly folded, and strongly bound and folded. Furthermore, analysis of the fluorescence anisotropy decay resulted in three different dansyl rotational correlation times, namely 0.18, 1.2, and 23 ns. Using the amplitudes of these times, we can correlate the lifetime groups with the corresponding fluorescence anisotropy component. The 23-ns rotational correlation time, which appears with the same amplitude as a 17-ns fluorescence lifetime, shows that the dansyl fluorophore follows the rotational diffusion of carbonic anhydrase when it is a part of the folded peptide/protein complex. A partly folded and partly hydrated interfacial structure is manifested in an 8-ns dansyl fluorescence lifetime and a 1.2-ns rotational correlation time. This structure, we believe, is similar to a molten-globule-like interfacial structure, which allows segmental movement and has a higher degree of solvent exposure of dansyl. Indirect excitation of dansyl on the helix-loop-helix peptide through Förster energy transfer from one or several tryptophans in the carbonic anhydrase shows that the helix-loop-helix scaffold binds to a tryptophan-rich domain of the carbonic anhydrase. We conclude that binding of the peptide to carbonic anhydrase involves a transition from a disordered to an ordered structure of the helix-loop-helix scaffold.     

Evidence for nonintercalative complexes formed from the reversible binding of benzo[a]pyrene metabolites to closed-circular, single-stranded M13mp19 DNA

The fluorescence excitation spectrum of complexes formed from the reversible binding of the proximate carcinogen, trans-7,8-dihydroxy-7,8-dihydro-benzo[a]pyrene (BP78D) to closed-circular, single-stranded, viral M13mp19 DNA (SS M13 DNA) exhibits a red-shift of 5 nm compared to the spectrum of BP78D measured without DNA or with native, calf thymus DNA. In SS M13 DNA which is 0.10 mM in PO4-, the fluorescence intensity of BP78D is 2.3 times smaller than the intensity measured without DNA; however, the fluorescence lifetime (42.7 nsec) of BP78D with SS M13 DNA is 1.7-1.8 times larger than the lifetimes of BP78D measured without DNA or with calf thymus DNA. These results are consistent with the conclusion that, in addition to binding sites which cause fluorescence quenching, SS M13 DNA contains sites which permit formation of BP78D inclusion complexes that have weaker interactions with nucleotide bases than those occurring in intercalated complexes. The association constant (1.45 +/- 0.01 x 10(5) M-1) for the binding of BP78D to SS M13 DNA is more than 9.0 times larger than that for binding to calf thymus DNA. It is 7.1 times larger than that for the binding of the less genotoxic metabolite, trans-4,5-dihydroxy-4,5-dihydrobenzo[a]pyrene (BP45D) to SS M13 DNA. UV Photoelectron data and results from ab initio molecular orbital calculations suggest that a difference in polarizability contributes to the greater SS M13 DNA binding of BP78D compared to that of BP45D.     

Texture analysis of fluorescence lifetime images of nuclear DNA with effect of fluorescence resonance energy transfer

BACKGROUND: Fluorescence lifetime imaging microscopy (FLIM) is becoming an important tool in cellular imaging. In FLIM, the image contrast is concentration insensitive, whereas it is sensitive to the local environment and interactions of fluorophores such as fluorescence resonance energy transfer (RET). METHODS: Fluorescence microscopy, lifetime imaging, and texture analysis were used to study the spatial distribution of fluorophores bound to nuclear DNA. 3T3-Swiss albino mice fibroblast nuclei were labeled with Hoechst 33258 (Ho), an AT-specific dye, and 7-aminoactinomycin D (7-AAD), a GC-specific dye. Ho is a RET donor to the 7-AAD acceptor. RESULTS: Texture analysis of 50 alcohol-fixed nuclei quantitatively showed changes of spatial distribution of apparent donor lifetimes. RET increased the spatial heterogeneity in the phase and modulation lifetime images. In most of the doubly stained cells (about 80%), the phase and modulation lifetime distributions were spatially homogeneous. In about 20% of the cells, we noticed that lower phase and modulation lifetimes caused by RET were correlated with regions of high Ho intensity in the nuclei. CONCLUSIONS: The spatial lifetime heterogeneity of Ho in presence of 7-AAD seems to be caused by RET between closely spaced strands in the three dimensionally condensed regions of DNA.     

Complex formation between p53 and replication protein A inhibits the sequence-specific DNA binding of p53 and is regulated by single-stranded DNA.

Human replication protein A (RP-A) (also known as human single-stranded DNA binding protein, or HSSB) is a multisubunit complex involved in both DNA replication and repair. Potentially important to both these functions, it is also capable of complex formation with the tumor suppressor protein p53. Here we show that although p53 is unable to prevent RP-A from associating with a range of single-stranded DNAs in solution, RP-A is able to strongly inhibit p53 from functioning as a sequence-specific DNA binding protein when the two proteins are complexed. This inhibition, in turn, can be regulated by the presence of various lengths of single-stranded DNAs, as RP-A, when bound to these single-stranded DNAs, is unable to interact with p53. Interestingly, the lengths of single-stranded DNA capable of relieving complex formation between the two proteins represent forms that might be introduced through repair and replicative events. Increasing p53 concentrations can also overcome the inhibition by steady-state levels of RP-A, potentially mimicking cellular points of balance. Finally, it has been shown previously that p53 can itself be stimulated for site-specific DNA binding when complexed through the C terminus with short single strands of DNA, and here we show that p53 stays bound to these short strands even after binding a physiologically relevant site. These results identify a potential dual role for single-stranded DNA in the regulation of DNA binding by p53 and give insights into the p53 response to DNA damage.