Fluorescence anisotropy decay of ethidium bound to chromatin

The fluorescence anisotropy decays of the chromatin ethidium complexes have been measured in solutions in which the dye was bound to the high affinity sites of the nucleosome DNA. Energy transfers between chromatin-bound ethidium molecules cause an increase of the anisotropy decay rate for much smaller values of the concentration ratio of dye to nucleotide than in the case of nacked DNA-ethidium complexes. This result implies that the high affinity sites are clustered on a short nucleosomal DNA segment. Quantitative analysis of the experimental data by computer simulations of the energy transfer process, shows that these sites are gathered on a single nucleosomal DNA segment, 28 base pairs long. Such a segment probably belongs to the nucleosome “linker”, contributing about half of it.     

Fluorescence anisotropy decay of ethidium bound to nucleosome core particles. 1. Rotational diffusion indicates an extended structure at low ionic strength

The fluorescence decay of ethidium intercalated into the DNA of nucleosome core particles increases in average lifetime from about 22 ns in H2O to about 39 ns in D2O. This increase, combined with the acquisition of large amounts of data (on the order of 10(8) counts per decay), allows measurement of anisotropy decays out to more than 350 ns. The overall slow rotational motions of the core particle may thereby be more clearly distinguished from the faster torsional motions of the DNA. In 10 mM NaCl at 20 degrees C, we recover a long correlation time of 198 ns in D2O (159 ns when corrected to a viscosity of 1.002 cP), in agreement with the value of 164 ns obtained in H2O. These values are consistent with hydrodynamic calculations based on the expected size and shape of the hydrated particle. To support our conclusion that this long correlation time derives from Brownian rotational diffusion, we show that the value is directly proportional to the viscosity and inversely proportional to the temperature. No significant changes in the rotational correlation time are observed between 1 and 500 mM ionic strength. Below 1 mM, the particle undergoes the "low-salt transition" as measured by steady-state tyrosine fluorescence anisotropy. However, we observe little change in shape until the ionic strength is decreased below approximately 0.2 mM, where the correlation time increases nearly 2-fold, indicating that the particle has opened up into an extended form. We have previously shown that the transition becomes nonreversible below 0.2 mM salt.     

The use of fluorescence anisotropy decay of poly d(A-T) ethidium bromide complex to estimate the unwinding angle of the double helix.

We measured the fluorescence decay under polarized light, of ethidium bromide bound to the poly d(A-T) isolated from Cancer Pagurus. The decay of the whole fluorescence is a single exponential function revealing a good homogeneity of the binding sites. The anisotropy decay due to energy transfers between the ethidium bromide molecules bound to a same poly d(A-T) molecule has been analysed, with a Monte Carlo calculation. We found the dye unwinds the poly d(A-T) duplex by an angle of 17 degrees plus or minus 2 degrees. This result is in agreement with the value previously found in the case of calf thymus DNA-ethidium bromide complex, although the base compositions of the two nucleic acids are different.     

Fluorescence anisotropy decay of ethidium bound to nucleosome core particles. 2. The torsional motion of the DNA is highly constrained and sensitive to pH

The effects of pH on the torsional flexibility of DNA bound to nucleosome core particles were investigated by using time-resolved fluorescence anisotropy decays of intercalated ethidium. The decays were collected by using time-resolved single-photon counting and were fit to a model developed by J. M. Schurr [(1984) Chem. Phys. 84, 71-96] with a nonlinear least-squares-fitting algorithm developed for this purpose. As the torsional flexibility of DNA is affected by the presence of an intercalating dye, the decays were studied at different ethidium bromide to core particle binding ratios. Because we see large increases in DNA flexibility and in the rotational diffusion coefficient at binding ratios of 0.6 ethidium/core particle and above, we conclude that, under these conditions, the DNA begins to detach from the protein. At lower binding ratios, we observe only small changes in the anisotropy decay. The torsional parameters obtained are a function of N, the number of base pairs of DNA between points of attachment to the histone core. Only if N is greater than 30 base pairs is the torsional rigidity of DNA on a nucleosome core particle higher than that for DNA free in solution. Also, for reasonable values of N (less than 30), the friction felt by the DNA on a core particle is much higher than that felt by free DNA. This indicates that the region of the DNA to which the ethidium binds is highly constrained in its motions. pH changes nearly neutrality at moderate ionic strengths (100 mM) have a substantial effect on the fluorescence anisotropy decays, particularly at early times. These analyses indicated that the observed change on increasing pH can be attributed either to a loosening of the contacts between the DNA and the histone core (increasing N) or to a substantial relaxing of the torsional rigidity of the DNA.     

Fluorescence lifetime analysis of DNA intercalated ethidium bromide and quenching by free dye

The fluorescence characteristics of ethidium bromide (Eb) complexed to calf thymus DNA have been examined using fluorescence lifetime analysis for a range of DNA (effective nucleotide concentration) to Eb molar ratios. Control of both temperature and ion concentration is necessary for reproducible analyses. Eb complexed to double stranded DNA has a maximum fluorescence lifetime of 23 ns and is easily distinguishable from a fluorescence lifetime value of 1.67 ns corresponding to unbound Eb. In a solution of calf thymus DNA containing excess Eb a binding equilibrium is reached, and this corresponds to one Eb molecule for every five nucleotides. With increasing amounts of unbound Eb, the fluorescence lifetime of the DNA-Eb complex decreases with a concomitant drop in the steady state fluorescence intensity, without a change in the amount of Eb bound to DNA. It is concluded that unbound Eb, acting via a quenching mechanism, shortens the fluorescence lifetime of bound Eb and consequently decreases the overall fluorescence intensity. This means that a different approach is necessary: time-resolved fluorescence spectroscopy directly distinguishes between a decrease in fluorescence intensity due to quenching by an excess of unbound Eb from that due to a decrease in Eb binding to double-stranded DNA. These studies suggest that techniques which measure total steady state fluorescence intensity of bound Eb in order to infer relative amounts of double-stranded DNA must be interpreted with caution. For such assays to be valid it is essential that no unbound Eb be present; otherwise a variable correction factor is required to account for unbound Eb.     

Fluorescence quenching of parallel-stranded DNA bound ethidium bromide: the effect of 7-deaza-2'-deoxyisoguanosine and 7-halogenated derivatives

Parallel stranded (ps) duplexes were constructed by incorporating 7-deaza-2′-deoxyisoguanosine (1a) or its 7-halogenated analogs 1b,c in place of 2′-deoxyisoguanosine. UV and T_m analyses prove the high affinity of ethidium bromide (EB) to these modified duplexes. Steady-state fluorescence measurement shows that the fluorescence is quenched when EB is bound to ps duplexes containing compounds 1a–c. The quenching effect depends on the 7-substituent of the nucleobase.     

Effect of quinone on the fluorescence decay dynamics of endogenous flavin bound to bacterial luciferase

The interaction of quinone with luciferase from Photobacterium leiognathi was studied based on the fluorescence decay measurements of the endogenous flavin bound to the enzyme. Homologous 1,4-quinones, 1,4-benzoquinone, methyl-1,4-benzoquinone, 2-methyl-5-isopropyl-1,4-benzoquine and 1,4-naphthoquinone, were investigated. In the absence of quinone, the fluorescence intensity and anisotropy decays of the endogenous flavin exhibited two intensity decay lifetimes (~ 1 and 5 ns) and two anisotropy decay lifetimes (~ 0.2 and 20 ns), suggesting a heterogeneous quenching and a rotational mobility microenvironment of the active site of the luciferase, respectively. In the presence of quinone, the intensity decay heterogeneity was largely maintained, whereas the fraction of the short anisotropy decay component and the averaged rotational rate of FMN increased with the increasing hydrophobicity of the quinone. We hypothesize that the hydrophobicity of the quinone plays a role in the non-specific inhibition mechanism of xenobiotic molecules in the bacterial bioluminescence system via altering the rotational mobility of the endogenous flavin in the luciferase.