HU binding to bent DNA: a fluorescence resonance energy transfer and anisotropy study

HU, an architectural DNA-binding protein, either stabilizes DNA in a bent conformation or induces a bend upon binding to give other proteins access to the DNA. In this study, HU binding affinity for a bent DNA sequence relative to a linear sequence was investigated using fluorescence anisotropy measurements. A static bend was achieved by the introduction of two phased A4T4 tracts in a 20 bp duplex. Binding affinity for 20 bp duplexes containing two phased A-tracts in either a 5'-3' or 3'-5' orientation was found to be almost 10-fold higher than HU binding to a random sequence 20 bp duplex (6.1 vs 0.68 microM(-1)). The fluorescence technique of resonance energy transfer was used to quantitatively determine the static bend of the DNA duplexes and the HU-induced bend. DNA molecules were 5'-end labeled with fluorescein as the donor or rhodamine as the acceptor. From the efficiency of energy transfer, the end-to-end distance of the DNA duplexes was calculated. The end-to-end distance relative to DNA contour length (R/R(C)) yields a bend angle for the A-tract duplex of 45 +/- 7 degrees in the absence of HU and 70 +/- 3 degrees in the presence of HU. The bend angle calculated for the T4A4 tract duplex was 62 +/- 4 degrees after binding two HU dimers. Fluorescence anisotropy measurements reveal that HU binds in a 1:1 stoichiometry to the A4T4 tract duplex but a 2:1 stoichiometry to the T4A4 tract and random sequence duplex. These findings suggest that HU binding and recognition of DNA may be governed by a structural mechanism.     

Fluid-fluid membrane microheterogeneity: a fluorescence resonance energy transfer study

Large unilamellar vesicles of dimyristoylphosphatidylcholine/cholesterol mixtures were studied using fluorescence techniques (steady-state fluorescence intensity and anisotropy, fluorescence lifetime, and fluorescence resonance energy transfer (FRET)). Three compositions (cholesterol mole fraction 0.15, 0.20, and 0.25) and two temperatures (30 and 40 degrees C) inside the coexistence range of liquid-ordered (l(o)) and liquid-disordered (l(d)) phases were investigated. Two common membrane probes, N-(7-nitrobenz-2-oxa-1,3-diazol-4-yl)-dimyristoylphosphatidylethanolamine (NBD-DMPE) and N-(lissamine(TM)-rhodamine B)-dimyristoylphosphatidylethanolamine (Rh-DMPE), which form a FRET pair, were used. The l(o)/l(d) partition coefficients of the probes were determined by individual photophysical measurements and global analysis of time-resolved FRET decays. Although the acceptor, Rh-DMPE, prefers the l(d) phase, the opposite is observed for the donor, NBD-DMPE. Accordingly, FRET efficiency decreases as a consequence of phase separation. Comparing the independent measurements of partition coefficient, it was possible to detect very small domains (<20 nm) of l(o) in the cholesterol-poor end of the phase coexistence range. In contrast, domains of l(d) in the cholesterol-rich end of the coexistence range have comparatively large size. These observations are probably related to different processes of phase separation, nucleation being preferred in formation of l(o) phase from initially pure l(d), and domain growth being faster in formation of l(d) phase from initially pure l(o).     

Single-molecule fluorescence resonance energy transfer

Fluorescent resonance energy transfer (FRET) is a powerful technique for studying conformational distribution and dynamics of biological molecules. Some conformational changes are difficult to synchronize or too rare to detect using ensemble FRET. FRET, detected at the single-molecule level, opens up new opportunities to probe the detailed kinetics of structural changes without the need for synchronization. Here, we discuss practical considerations for its implementation including experimental apparatus, fluorescent probe selection, surface immobilization, single-molecule FRET analysis schemes, and interpretation.     

DNA tetraplex formation studied with fluorescence resonance energy transfer.

It is emerging that DNA tetraplexes are pivotal for many major cellular processes, and techniques that assess their structure and nature to the point are under development. Here we show how the structural conversion of largely unstructured single-stranded DNA molecules into compact intrastrand DNA tetraplexes can be monitored by fluorescence resonance energy transfer. We recently reported that intrastrand tetraplex formation takes place in a nuclease hypersensitive element upstream of the human c-myc proto-oncogene. Despite the highly repetitive guanine-rich sequence of the hypersensitive element, fluorescence resonance energy transfer measurements indicate that only one well defined tetraplex structure forms therein. The proposed structure, which is specifically stabilized by potassium ions in vitro, has a core of three stacked guanine tetrads that is capped by two intrastrand A-T base pairs.     

RecQ helicase-catalyzed DNA unwinding detected by fluorescence resonance energy transfer

A fluorometric assay was used to study the DNA unwinding kinetics induced by Escherichiacoli RecQ helicase.This assay was based on fluorescence resonance energy transfer and carried out onstopped-flow,in which DNA unwinding was monitored by fluorescence emission enhancement of fluoresceinresulting from helicase-catalyzed DNA unwinding.By this method,we determined the DNA unwinding rateof RecQ at different enzyme concentrations.We also studied the dependences of DNA unwinding magnitudeand rate on magnesium ion concentration.We showed that this method could be used to determine thepolarity of DNA unwinding.This assay should greatly facilitate further study of the mechanism for RecQ-catalyzed DNA unwinding.     

Characterization of DNA/lipid complexes by fluorescence resonance energy transfer

Fluorescence resonance energy transfer (FRET) is a potential method for the characterization of DNA-cationic lipid complexes (lipoplexes). In this work, we used FRET models assuming a multilamellar lipoplex arrangement. The application of these models allows the determination of the distance between the fluorescent intercalator on the DNA and a membrane dye on the lipid, and/or the evaluation of encapsulation efficiencies of this liposomal vehicle. The experiments were carried out in 1,2-dioleoyl-3-trimethylammonium-propane/pUC19 complexes with different charge ratios. We used 2-(3-(diphenylhexatrienyl)propanoyl)-1-hexadecanoyl-sn-glycero-3-phosphocholine (DPH-PC) and 2-(4,4-difluoro-5-octyl-4-bora-3a,4a-diaza-s-indacene-3-pentanoyl)-1-hexadecanoyl-sn-glycero-3-phosphocholine (BODIPY-PC) as membrane dyes, and ethidium bromide (EtBr) and BOBO-1 as DNA intercalators. In cationic complexes (charge ratios (+/-) >or= 2), we verified that BOBO-1 remains bound to DNA, and FRET occurs to the membrane dye. This was also confirmed by anisotropy and lifetime measurements. In complexes with all DNA bound to the lipid (charge ratio (+/-) = 4), we determined 27 A as the distance between the donor and acceptor planes (half the repeat distance for a multilamellar arrangement). In complexes with DNA unbound to the lipids (charge ratio (+/-) = 0.5 and 2), we calculated the encapsulation efficiencies. The presented FRET methodology is, to our knowledge, the first procedure allowing quantification of lipid-DNA contact.     

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.     

Polarized fluorescence resonance energy transfer microscopy

Current methods for fluorescence resonance energy transfer (FRET) microscopy of living cells involve taking a series of images with alternating excitation colors in separate camera exposures. Here we present a new FRET method based on polarization that requires only one camera exposure and thereby offers the possibility for better time resolution of dynamic associations among subcellular components. Polarized FRET (p-FRET) uses a simultaneous combination of excitation wavelengths from two orthogonally polarized sources, along with an emission channel tri-image splitter outfitted with appropriate polarizers, to concurrently excite and collect fluorescence from free donors, free acceptors, and FRET pairs. Based upon the throughput in each emission channel as premeasured on pure samples of each of the three species, decoupling of an unknown sample's three polarized fluorescence images can be performed to calculate the pixel-by-pixel concentrations of donor, acceptor, and FRET pairs. The theory of this approach is presented here, and its feasibility is experimentally confirmed by measurements on mixtures of cyan fluorescent protein (CFP), citrine ((Cit) a yellow fluorescent protein variant), and linked fusion proteins (CFP-L16-Cit, CFP-L7-Cit, CFP-L54-Cit) in living cells. The effects of shot noise, acceptor polarization, and FRET efficiency on the statistical accuracy of p-FRET experimental results are investigated by a noise-simulation program.     

Trajectory of nucleosomal linker DNA studied by fluorescence resonance energy transfer

While the structure of the nucleosome core is known in atomic detail, the precise geometry of the DNA beyond the core particle is still unknown. We have used fluorescence resonance energy transfer (FRET) for determining the end-to-end distance of DNA fragments assembled with histones into nucleosomes. The DNA of a length of 150-220 bp was labeled with rhodamine-X on one end and fluorescein or Alexa 488 on the other. Assembling nucleosomes on these DNA fragments leads to a measurable energy transfer. The end-to-end distance computed from the FRET increases from 60 +/- 5 A at 150 bp to 75 +/- 5 A at 170 bp without measurable change above it. These distances are compatible with different geometries of the linker DNA, all having in common that no crossing can be observed up to 220 bp. Addition of H1 histone leads to an increase in energy transfer, indicating a compaction of the linker DNA toward the nucleosome.     

Ion-induced folding of the hammerhead ribozyme: a fluorescence resonance energy transfer study.

The ion-induced folding transitions of the hammerhead ribozyme have been analysed by fluorescence resonance energy transfer. The hammerhead ribozyme may be regarded as a special example of a three-way RNA junction, the global structure of which has been studied by comparing the distances (as energy transfer efficiencies) between the ends of pairs of labelled arms for the three possible end-to-end vectors as a function of magnesium ion concentration. The data support two sequential ion-dependent transitions, which can be interpreted in the light of the crystal structures of the hammerhead ribozyme. The first transition corresponds to the formation of a coaxial stacking between helices II and III; the data can be fully explained by a model in which the transition is induced by a single magnesium ion which binds with an apparent association constant of 8000-10 000 M-1. The second structural transition corresponds to the formation of the catalytic domain of the ribozyme, induced by a single magnesium ion with an apparent association constant of approximately 1100 M-1. The hammerhead ribozyme provides a well-defined example of ion-dependent folding in RNA.     

Use of fluorescence resonance energy transfer to study serpin-proteinase interactions

One of the important questions in the serpin mechanism of inhibition of serine and cysteine proteinases of different specificities and structural classes is whether a common "crushing" mechanism of proteinase inactivation is used in all cases. This mechanism was seen in an X-ray structure of the complex between alpha(1)-proteinase inhibitor and trypsin and required the full insertion of the reactive center loop into beta-sheet A and translocation of the proteinase from one pole of the serpin to the other. However, it has yet to be shown to be general for serine proteinases of structural classes other than the trypsin-fold or for cysteine proteinases with the papain-fold or for the caspases. Fluorescence resonance energy transfer offers a potential means of obtaining an answer to this question for each of these classes, without the concern for the effect that increasing size has on the observed signal that applies to NMR spectroscopy. However, care must be taken to ensure that measurements made represent sufficient overdetermination that the answer obtained is unambiguous.     

Acridone-tagged DNA as a new probe for DNA detection by fluorescence resonance energy transfer and for mismatch DNA recognition

Acridone is highly fluorescent and stable against photodegradation, oxidation, and heat. It is also a small molecule with no charge, making it a promising fluorescent agent for use in a DNA probe. Thus, we have prepared 5'-terminal acridone-labeled DNAs by post-modification, and have examined their photophysical properties and their use as donors for a fluorescence resonance energy transfer (FRET) system in combination with a 3'-terminal dabcyl-tagged DNA as an acceptor, which can detect the target DNA by emission-quenching caused by FRET. The FRET with an acridone and dabcyl pair has been found to complement that with fluorescence and dabcyl and other fluorescence-quencher pairs. Significant amounts of quenching of the acridone emissions by guanine in the DNA were observed when guanine was close to acridone, which can be applied as a quencher-free probe for the detection of special sequence of DNA. The DNA bearing acridone at the C5 position of inner thymidine could discriminate the opposite T-T base mismatch, although enhancement of discrimination ability is needed for the practical use of SNP typing.     

DNA probes using fluorescence resonance energy transfer (FRET): designs and applications.

Fluorescence resonance energy transfer (FRET) is widely used in biomedical research as a reporter method. Oligonucleotides with a DNA backbone and one or several chromophore tags have found multiple applications as FRET probes. They are especially advantageous for the real-time monitoring of biochemical reactions and in vivo studies. This paper reviews the design and applications of various DNA-based probes that use FRET The approaches used in the design of new DNA FRET probes are discussed.     

用荧光共振能量转移研究synaptotagmin 胞质部分的寡聚化

目前人们公认synaptotagmin在神经递质释放过程中作为钙离子感受器而发挥作用。以前的研究发现,synaptotagmin存在两种形式的寡聚化,一种是通过跨膜区以及随后的中间链部分介导的寡聚化;另一种是通过胞质部分（C2AB）介导的寡聚化。对于后者有很多争议。在这篇文章中,作者用荧光共振能量转移的方法,在尽可能接近生理的条件下,证明了C2AB在有细胞膜和游离的钙离子的条件下能够寡聚化。而且,抽提细胞膜上的胆固醇或者封闭膜上的磷酸肌醇二磷酸能抑制C2AB在膜上的寡聚。     

Real-time measurements of DNA hybridization on microparticles with fluorescence resonance energy transfer

When capture oligonucleotides are tethered on planar surfaces, mass transport limitations influence the kinetics of solid-phase nucleic acid hybridizations. By diffusion theory, however, hybridization of oligonucleotides on microparticles should be reaction-rate limited. In an initial effort to understand the kinetics of microparticle hybridization reactions, we developed a fluorescence resonance energy transfer method for monitoring oligonucleotide hybridization on microparticles. Microparticles were coated with a fluoresceinated oligomer at surface densities of 20, 40, and 80% saturation, hybridized to a complementary oligonucleotide labeled with tetramethylrhodamine, and monitored over time for quenching of the fluorescein signal as hybridization occurred on the particle surface. Association rate constants were compared for microparticle-based hybridization and solution-phase hybridization. Rate constants for hybridizations on the particle surface were about an order of magnitude less than those for hybridization in solution, but decreasing the surface density of the capture oligonucleotide to 20% saturation improved particle hybridization rates. Although a bimolecular reaction model adequately described solution-phase hybridization kinetics, oligonucleotide hybridization on microparticles did not fit this model but exhibited biphasic reaction kinetics. Based on two different lines of reasoning, we argue that microparticle-based oligonucleotide hybridization was indeed reaction-rate limited in our system and not diffusion-rate limited.     

Scanning near-field fluorescence resonance energy transfer microscopy

A new microscopic technique is demonstrated that combines attributes from both near-field scanning optical microscopy (NSOM) and fluorescence resonance energy transfer (FRET). The method relies on attaching the acceptor dye of a FRET pair to the end of a near-field fiber optic probe. Light exiting the NSOM probe, which is nonresonant with the acceptor dye, excites the donor dye introduced into a sample. As the tip approaches the sample containing the donor dye, energy transfer from the excited donor to the tip-bound acceptor produces a red-shifted fluorescence. By monitoring this red-shifted acceptor emission, a dramatic reduction in the sample volume probed by the uncoated NSOM tip is observed. This technique is demonstrated by imaging the fluorescence from a multilayer film created using the Langmuir-Blodgett (LB) technique. The film consists of L-alpha-dipalmitoylphosphatidylcholine (DPPC) monolayers containing the donor dye, fluorescein, separated by a spacer group of three arachidic acid layers. A DPPC monolayer containing the acceptor dye, rhodamine, was also transferred onto an NSOM tip using the LB technique. Using this modified probe, fluorescence images of the multilayer film reveal distinct differences between images collected monitoring either the donor or acceptor emission. The latter results from energy transfer from the sample to the NSOM probe. This method is shown to provide enhanced depth sensitivity in fluorescence measurements, which may be particularly informative in studies on thick specimens such as cells. The technique also provides a mechanism for obtaining high spatial resolution without the need for a metal coating around the NSOM probe and should work equally well with nonwaveguide probes such as atomic force microscopy tips. This may lead to dramatically improved spatial resolution in fluorescence imaging.     

The renaissance of fluorescence resonance energy transfer

Recent advances in fluorescence resonance energy transfer have led to qualitative and quantitative improvements in the technique, including increased spatial resolution, distance range, and sensitivity. These advances, due largely to new fluorescent dyes, but also to new optical methods and instrumentation, have opened up new biological applications.