“…Recently, Dr. David Kearns (private communication, and Ref. 19) informed us that a combination of absorption and fluorescence experiments on EtdBr binding to tRNAPhe in his laboratory suggested the existence of one strong binding site with a fluorescence lifetime of about 30 nsec and three weaker sites with a fluorescence lifetime on the order of 5-15 nsec. These results are totally consistent with our interpretation and analysis of the thermodynamics of the interaction of EtdBr to the putative unique binding site.…”
A self‐consistent thermodynamic characterization of the binding of ethidium to yeast phenylalanine‐specific tRNA at 25°C, pH 7.0, in 11 nM MgCl2, 375 nM NaCl, and 25 mM sodium phosphate has been obtained. Two ethidium molecules bind per tRNA under these conditions. The stronger site has a dissociation constant equal to 1.9 ± 0.5 μM and ΔHdis°′ = 12 ± 1 Kcal/mol, and the weaker sites has a dissociation constant equal to 24 ± 9 μM and ΔHdis°′ = 8.9 ± 1.5 Kcal/mol. The average calorimetric ΔHdis°′ for the to sites 10.6 ± 0.4 kcal/mol. The thermodynamics of binding to the stranger sites are most probably the thermodynamics of interaction between A·U (6) and A·U (7), the unique site identified by Jones and Kearns. The binding is enthalpically driven and classical hydrophobic interactions do not appear to be important in the binding reaction.
“…Recently, Dr. David Kearns (private communication, and Ref. 19) informed us that a combination of absorption and fluorescence experiments on EtdBr binding to tRNAPhe in his laboratory suggested the existence of one strong binding site with a fluorescence lifetime of about 30 nsec and three weaker sites with a fluorescence lifetime on the order of 5-15 nsec. These results are totally consistent with our interpretation and analysis of the thermodynamics of the interaction of EtdBr to the putative unique binding site.…”
A self‐consistent thermodynamic characterization of the binding of ethidium to yeast phenylalanine‐specific tRNA at 25°C, pH 7.0, in 11 nM MgCl2, 375 nM NaCl, and 25 mM sodium phosphate has been obtained. Two ethidium molecules bind per tRNA under these conditions. The stronger site has a dissociation constant equal to 1.9 ± 0.5 μM and ΔHdis°′ = 12 ± 1 Kcal/mol, and the weaker sites has a dissociation constant equal to 24 ± 9 μM and ΔHdis°′ = 8.9 ± 1.5 Kcal/mol. The average calorimetric ΔHdis°′ for the to sites 10.6 ± 0.4 kcal/mol. The thermodynamics of binding to the stranger sites are most probably the thermodynamics of interaction between A·U (6) and A·U (7), the unique site identified by Jones and Kearns. The binding is enthalpically driven and classical hydrophobic interactions do not appear to be important in the binding reaction.
“…Classical DNA intercalators such as ethidium have been known for some time to interact with RNA. 35 Simple DNA binders such as Hoechst dyes 33342 and 33258 are inactive in the FRET assay (data not shown). Though the term intercalation in DNA has specific associations, which are not appropriate for RNA, some element of base-stacking between base-pairs is common to the rbt418/550 series and to DNA intercalators.…”
Section: Interaction Of Rbt550/418 Series With Tar Rnamentioning
“…Spectrally resolved FLIM Q. S. Hanley S85 dequenching process similar to EB (Olmsted & Kearns 1977;Jones et al 1978;Leupin et al 1985). These data (figure 2) were originally published as plots of phase and modulation lifetime spectra.…”
Placing an imaging spectrograph or related components capable of generating a spectrum between a microscope and the image intensifier of a conventional fluorescence lifetime imaging (FLIM) system creates a spectrally resolved FLIM (SFLIM). This arrangement provides a number of opportunities not readily available to conventional systems using bandpass filters. The examples include: simultaneous viewing of multiple fluorophores; tracking of both the donor and acceptor; and observation of a range of spectroscopic changes invisible to the conventional FLIM systems. In the frequency-domain implementation of the method, variation in the fractional contributions from different fluorophores along the wavelength dimension can behave as a surrogate for a frequency sweep or spatial variations while analysing fluorophore mixtures. This paper reviews the development of the SFLIM method, provides a theoretical and practical overview of frequency-domain SFLIM including: presentation of the data; manifestations of energy transfer; observation of multiple fluorophores; and the limits of single frequency methods.
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