Dimerization and inter-chromophore distance of Cph1 phytochrome from Synechocystis,as monitored by fluorescence homo and hetero energy transfer

We investigated the dimerization of phytochrome Cph1 from the cyanobacterium Synechocystis by fluorescence resonance energy transfer (FRET). As donor we used the chromophore analogue phycoerythrobilin (PEB) and as acceptor either the natural chromophore phycocyanobilin (PCB; hetero transfer) or PEB (homo transfer). Both chromophores bind in a 1:1 stoichiometry to apo-monomers expressed in Escherichia coli. Energy transfer was characterized by time-resolved fluorescence intensity and anisotropy decay after excitation of PEB by picosecond pulses from a tunable Ti-sapphire laser system. ApoCph1 was first assembled with PEB at a low stoichiometry of 0.1. The remaining sites were then sequentially titrated with PCB. In the course of this titration, the mean lifetime of PEB decreased from 3.33 to 1.25 ns in the P(r) form of Cph1, whereas the anisotropy decay was unaffected. In the P(fr)/P(r) photoequilibrium (about 65% P(fr)), the mean lifetime decreased significantly less, to 1.67 ns. These observations provide strong support for inter-chromophore hetero energy transfer in mixed PEB/PCB dimers. The reduced energy transfer in P(fr) may be due to a structural difference but is at least in part due to the difference in spectral overlap, which was 4.1 x 10(-13) and 1.6 x 10(-13) cm(3) M(-1) in P(r) and P(fr), respectively. From the changes in the mean lifetime, rates of hetero energy transfer of 0.68 and 0.37 ns(-1) were calculated for the P(r) form and the P(fr)/P(r) photoequilibrium, respectively. Sequential titration of apo Cph1 with PEB alone to full occupancy did not affect the intensity decay but led to a substantial increase in depolarization. This is the experimental signature of homo energy transfer. Values for the rate of energy transfer k(HT) (0.47 ns(-1)) and the angle 2theta between the transition dipole moment directions (2theta = 45 +/- 5 degrees) were determined from an analysis of the concentration dependence of the anisotropy at five different PEB/Cph1 stoichiometries. The independently determined rates of hetero and homo energy transfer are thus of comparable magnitude and consistent with the energy transfer interpretation. Using these results and exploiting the 2-fold symmetry of the dimer, the chromophore-chromophore distance R(DA) was calculated and found to be in the range 49 A < R(DA) < 63 A. Further evidence for energy transfer in Cph1 dimers was obtained from dilution experiments with PEB/PEB dimers: the lifetime was unchanged, but the anisotropy increased as the dimers dissociated with increasing dilution. These experiments allowed a rough estimate of 5 +/- 3 microM for the dimer dissociation constant. With the deletion mutant Cph1Delta2 that lacks the carboxy terminal histidine kinase domain less energy transfer was observed suggesting that in this mutant dimerization is much weaker. The carboxy terminal domain of Cph1 that is involved in intersubunit trans-phosphorylation and signal transduction thus plays a dominant role in the dimerization. The FRET method provides a sensitive assay to monitor the association of Cph1 monomers.     

Polarized absorption picosecond kinetics as a probe of energy transfer in phycobilisomes of Synechococcus 6301

The energy transfer between C-phycocyanin chromophores in intact phycobilisomes of Synechococcus 6301 is shown to lead to an anisotropy relaxation with a lifetime of 10 ± 2 ps. However, due to the molecular order within the hexameric units of C-phycocyanin the anisotropy does not decay to zero. The Förster dipole-dipole mechanism of energy transfer can qualitatively explain these data provided that there is no back transfer of excitation energy and that the chromophore distribution is non-random. The rate of energy transfer in phycobilisomes between C-phycocyanin and allophycocyanin can best be described by a double exponential with lifetimes of 12 ± 3 and 84 ± 8 ps.     

Time-dependent absorption anisotropy and rotational diffusion of proteins in membranes.

The decay of flash-induced absorption anisotropy, r(t), of a chromophore in a membrane protein is closely correlated with rotational diffusion of the protein in the membrane. We develop a theory of time-dependent absorption anisotropy which is applicable to both linear chromophores and planar chromophores which have two different absorption moments at right angles to one another. The theory treats two types of rotational diffusion of membrane proteins: one is rotation of the whole protein about the normal to the plane of the membrane, and the other is restricted wobbling of the whole or part of the protein molecule. In the former case, r(t) is determined by a rotational diffusion coefficient and an angle between the absorption moment(s) and the normal to the plane of the membrane. Rotation of rigid transmembrane proteins can be described by this treatment. In the latter case, r(t) is characterized by a wobbling diffusion coefficient and the degree of orientational constraint. This treatment may be applicable to independent wobbling of the hydrophilic part of membrane proteins. We further show that, for linear and circularly degenerate chromophores, the effect of the excitation flash intensity on r(t) can be accounted for by a constant scaling factor.     

Refined three-dimensional structures of two cyanobacterial C-phycocyanins at 2.1 and 2.5 A resolution. A common principle of phycobilin-protein interaction

The crystal structure of the light-harvesting protein-pigment complex C-phycocyanin (C-PC) from Mastigocladus laminosus (at 2.1 A resolution (1 A = 0.1 nm] has been refined by energy-restrained least-squares methods to a conventional R-factor of 21.7%. In the same way, the crystal structure of C-PC from Agmenellum quadruplicatum has been refined further (2.5 A, R = 18.4%); pyrrole rings C and D of the chromophore at position A84 have been corrected with respect to the previously reported structure. The two C-PC structures are very similar, 213 C alpha positions have a root-mean-square deviation of 0.49 A. Polar and ionic side-chain interactions are discussed in detail and the two subunits of C-PC from M. laminosus are compared to each other. All three chromophores are completely defined and their tetrapyrroles exhibit very similar geometry. The structure of a C-PC chromophore resembles a cleaved porphyrin which has been twisted roughly 180 degrees around the C-5-C-6 and C-14-C-15 bonds. Accordingly, the configuration/conformation of the chromophores is Z-anti, Z-syn, Z-anti (with the exception of the "configuration" of C-15 of chromophore B155, which is almost midway between Z and E). The three chromophores interact similarly with the protein. They arch around aspartate residues (A87, B87 and B39), and the nitrogens of pyrroles B and C are within hydrogen-bonding distance of one of the carboxylate oxygens. Most of the propionic side-chains of the chromophores form salt bridges with arginine and lysine residues. The updated relative chromophore distances and orientations confirm our conclusion that hexameric aggregates are probably the basic functional units, and that inter-hexameric energy transfer takes place preferentially via the central B84 chromophores.     

Molecular mechanism for the initial process of visual excitation. IV. Energy surfaces of visual pigments and photoisomerization mechanism.

Using the twisted conformations of the chromophores for visual pigments and intermediates which were theoretically determined in the previous paper, energy surfaces of the pigment at - 190 degrees C were obtained as functions of the torsional angles theta 9-10 and theta 11-12 or of the torsional angles theta 9-10 and theta 13-14. In these calculations, the existence of specific reaction paths between rhodopsin (R) and bathorhodopsin (B), between isorhodopsin I (I) and bathorhodopsin, and between isorhodopsin II (I') and bathorhodopsin were assumed. It was shown that the total energy surfaces of the excited states had minima C1 at theta 9-10 approximately -10 degrees and theta 11-12 approximately -80 degrees, C2 at theta 9-10 approximately -85 degrees and theta 11-12 approximately -5 degrees, and C3 at theta 9-10 approximately -0 degree and theta 13-14 approximately -90 degrees. These minima are considered to correspond to the thermally barrierless common states as denoted by Rosenfeld et al. Using the total energy surfaces in the ground and excited states, the molecular mechanism of the photoisomerization reaction was suggested. Quantum yields for the photoconversions among R, I, I' and B were related to the rates of vibrational relaxations, radiationless transitions and thermal excitations. Some discussion was made of the temperature effect on the quantum yield. Similar calculations of the energy surfaces were also made at other temperatures where lumirhodopsin or metarhodopsin I is stable. Relative energy levels of the pigments and the intermediates were discussed.     

Efficiency enhancement of long-range energy transfer by sequential multistep FRET using fluorescence labeled DNA.

The efficiency of long-range (ca. 80 A) fluorescence energy transfer was enhanced about 1.5 times by a third chromophore located midway between two chromophores. A third chromophore should act like a relay station in sequential multistep energy transfer.     

Origin and consequences of steric strain in the rhodopsin binding pocket

To study the origin and the effects of steric strain on the chromophore conformation in rhodopsin, we have performed quantum-mechanical calculations on the wild-type retinal chromophore and four retinal derivatives, 13-demethyl-, 10-methyl-13-demethyl-, 10-methyl-, and 9-demethylretinal. For the dynamics of the whole protein, a combined quantum mechanics/molecular mechanics method (DFTB/CHARMM) was used and for the calculation of excited-state properties the nonempirical CASSCF/CASPT2 method. After relaxation inside the protein, all chromophores show significant nonplanar distortions from C10 to C13, most strongly for 10-methylretinal and least pronounced for 9-demethylretinal. In all five cases, the dihedral angle of the C10-C11=C12-C13 bond is negative which attests to the strong chiral discrimination exerted by the protein pocket. The calculations show that the nonplanar distortion of the chromophore, including the sense of rotation, is caused by a combination of two effects: the fitting of both ends to the protein matrix which imposes a distance constraint and the bonding arrangement at the Schiff base terminus. With both the counterion Glu113 and Lys296 displaced off the plane of the chromophore, their binding to N16 exerts a torque on the chromophore. As a result, the polyene chain, from N16 to C13, is twisted in a clockwise manner against the remaining part of the chromophore, leading to a C11=C12 bond with the observed negative dihedral angle. Shifts of the absorption maxima are reproduced correctly, in particular, the red shift of the 10-methyl and the strong blue shift of the 9-demethyl analogue relative to the wild type. Calculated positive rotatory strengths of the alpha-CD bands are in agreement with the calculated absolute conformation of the mutant chromophores.     

Studies on chromophore coupling in isolated phycobiliproteins: III. Picosecond excited state kinetics and time-resolved fluorescence spectra of different allophycocyanins from Mastigocladus laminosus

The excited state kinetics of three different allophycocyanin (AP) complexes has been studied by picosecond fluorescence spectroscopy. Both the fluorescence kinetics and the decay-associated fluorescence spectra of the different complexes can be understood on the basis of a structural model for AP which uses (a) an analogy to the known x-ray determined structure of C-phycocyanin, (b) the biochemical analogies of AP and C-phycocyanin, and (c) the biochemical composition of AP-B (AP-681). A model is developed that describes the excited state kinetics as a mixture of internal conversion processes within a coupled exciton pair and energy transfer processes between exciton pairs. We found excited state relaxation times in the range of 13 ps (AP with linker peptide) up to 66 ps (AP-B). The trimeric aggregates AP 660 and AP 665 show one fast relaxation component each, as was expected on the basis of their symmetry properties. The lower symmetry of AP-B (AP-681) gives rise to two fast lifetime components (τ₁ = 23 ps and τ₂ = 66 ps) which are attributed to internal conversion and/or energy transfer between excitonic states formed by the coupling of symmetrically and spectrally nonequivalent chromophores. It is proposed that the internal conversion between exciton states of strongly coupled chromophores fulfills the requirements of the small energy gap limit. Thus, internal conversion rates in the order of tens of picoseconds are feasible. The influence of the interaction of the linker peptide on the properties of the AP trimer are manifested in the fluorescence kinetics. Lack of the linker peptide in AP 660 gives rise to a heterogeneity in the chromophore conformations and chromophore-chromophore interactions.     

Developing a structure-function model for the cryptophyte phycoerythrin 545 using ultrahigh resolution crystallography and ultrafast laser spectroscopy

Cryptophyte algae differ from cyanobacteria and red algae in the architecture of their photosynthetic light harvesting systems, even though all three are evolutionarily related. Central to cryptophyte light harvesting is the soluble antenna protein phycoerythrin 545 (PE545). The ultrahigh resolution crystal structure of PE545, isolated from a unicellular cryptophyte Rhodomonas CS24, is reported at both 1.1A and 0.97A resolution, revealing details of the conformation and environments of the chromophores. Absorption, emission and polarized steady state spectroscopy (298K, 77K), as well as ultrafast (20fs time resolution) measurements of population dynamics are reported. Coupled with complementary quantum chemical calculations of electronic transitions of the bilins, these enable assignment of spectral absorption characteristics to each chromophore in the structure. Spectral differences between the tetrapyrrole pigments due to chemical differences between bilins, as well as their binding and interaction with the local protein environment are described. Based on these assignments, and considering customized optical properties such as strong coupling, a model for light harvesting by PE545 is developed which explains the fast, directional harvesting of excitation energy. The excitation energy is funnelled from four peripheral pigments (beta158,beta82) into a central chromophore dimer (beta50/beta61) in approximately 1ps. Those chromophores, in turn, transfer the excitation energy to the red absorbing molecules located at the periphery of the complex in approximately 4ps. A final resonance energy transfer step sensitizes just one of the alpha19 bilins on a time scale of 22ps. Furthermore, it is concluded that binding of PE545 to the thylakoid membrane is not essential for efficient energy transfer to the integral membrane chlorophyll a-containing complexes associated with PS-II.     

Single-molecule spectroscopy selectively probes donor and acceptor chromophores in the phycobiliprotein allophycocyanin

We report on single-molecule fluorescence measurements performed on the phycobiliprotein allophycocyanin (APC). Our data support the presence of a unidirectional F?rster-type energy transfer process involving spectrally different chromophores, alpha84 (donor) and beta84 (acceptor), as well as of energy hopping amongst beta84 chromophores. Single-molecule fluorescence spectra recorded from individual immobilized APC proteins indicate the presence of a red-emitting chromophore with emission peaking at 660 nm, which we connect with beta84, and a species with the emission peak blue shifted at 630 nm, which we attribute to alpha84. Polarization data from single APC trimers point to the presence of three consecutive red emitters, suggesting energy hopping amongst beta84 chromophores. Based on the single-molecule fluorescence spectra and assuming that emission at the ensemble level in solution comes mainly from the acceptor chromophore, we were able to resolve the individual absorption and emission spectra of the alpha84 and beta84 chromophores in APC.     

Versatile design of biohybrid light-harvesting architectures to tune location,density, and spectral coverage of attached synthetic chromophores for enhanced energy capture

Biohybrid antennas built upon chromophore–polypeptide conjugates show promise for the design of efficient light-capturing modules for specific purposes. Three new designs, each of which employs analogs of the β-polypeptide from Rhodobacter sphaeroides, have been investigated. In the first design, amino acids at seven different positions on the polypeptide were individually substituted with cysteine, to which a synthetic chromophore (bacteriochlorin or Oregon Green) was covalently attached. The polypeptide positions are at –2, –6, –10, –14, –17, –21, and –34 relative to the 0-position of the histidine that coordinates bacteriochlorophyll a (BChl a). All chromophore–polypeptides readily formed LH1-type complexes upon combination with the α-polypeptide and BChl a. Efficient energy transfer occurs from the attached chromophore to the circular array of 875 nm absorbing BChl a molecules (denoted B875). In the second design, use of two attachment sites (positions –10 and –21) on the polypeptide affords (1) double the density of chromophores per polypeptide and (2) a highly efficient energy-transfer relay from the chromophore at –21 to that at –10 and on to B875. In the third design, three spectrally distinct bacteriochlorin–polypeptides were prepared (each attached to cysteine at the –14 position) and combined in an ~1:1:1 mixture to form a heterogeneous mixture of LH1-type complexes with increased solar coverage and nearly quantitative energy transfer from each bacteriochlorin to B875. Collectively, the results illustrate the great latitude of the biohybrid approach for the design of diverse light-harvesting systems.     

Anomalous negative fluorescence anisotropy in yellow fluorescent protein (YFP 10C): quantitative analysis of FRET in YFP dimers

Yellow fluorescent protein (YFP) is widely used as a genetically encoded fluorescent marker in biology. In the course of a comprehensive study of this protein, we observed an unusual, negative fluorescence anisotropy at pH 6.0 (McAnaney, T. B., Zeng, W., Doe, C. F. E., Bhanji, N., Wakelin, S., Pearson, D. S., Abbyad, P., Shi, X., Boxer, S. G., and Bagshaw, C. R. (2005) Biochemistry 44, 5510-5524). Here we report that the fluorescence anisotropy of YFP 10C depends on protein concentration in the low micromolar range that was not expected. We propose that the negative anisotropy is a result of unidirectional F?rster resonance energy transfer (FRET) in a dimer of YFP, with the donor chromophore in the neutral form and the acceptor chromophore in the anionic form. This unusual mechanism is supported by studies of a monomeric YFP (A206K YFP) and transient-absorption spectroscopy of YFP 10C. A detailed analysis of the chromophore transition dipole moment direction is presented. The anisotropy and rate constant of this energy transfer are consistent with values produced by an analysis of the dimer structure observed in crystals.     

Allophycocyanin complexes of the phycobilisome from Mastigocladus laminosus. Influence of the linker polypeptide L8.9C on the spectral properties of the phycobiliprotein subunits

The following phycobiliproteins and complexes of the allophycocyanin core were isolated from phycobilisomes of the thermophilic cyanobacterium Mastigocladus laminosus: alpha AP, beta AP, (alpha AP beta AP), (alpha AP beta AP)3, (alpha AP beta AP)3L8.9C, (alpha APB alpha AP2 beta AP3)L8.9C. The six proteins and complexes were characterised spectroscopically with respect to absorption, oscillator strength, extinction coefficient, fluorescence emission, relative quantum yield, fluorescence emission polarisation and fluorescence excitation polarisation. The interpretation of the spectral data was based on the three-dimensional structure model of (alpha PC beta PC)3 (Schirmer et al. (1985) J. Mol. Biol. 184, 257-277), which is related to the allophycocyanin trimer. The absorption and CD spectra of the complexes (alpha AP beta AP)3, (alpha AP beta AP)3L8.9C and (alpha APB alpha AP2 beta AP3)L8.9C could be deconvoluted into the spectra of the phycobiliprotein subunits. The assumptions made for the deconvolution could be checked by the synthesis of the spectra of (alpha APB beta AP)3. The synthesised spectra are in good agreement with the corresponding measured spectra published by other authors. Considering the deconvoluted spectra the following influences on the chromophores could be ascribed to L8.9C: L8.9C neither influences the alpha AP nor the alpha APB chromophores. L8.9C shifts the absorption maximum of the beta AP chromophore to longer wavelength than the absorption maximum of the alpha AP chromophore in trimeric complexes. L8.9C increases the oszillator strength of the beta AP chromophores to about the value of the alpha AP chromophores in trimeric complexes. L8.9C turns the beta AP chromophores from sensitizing into weak fluorescing chromophores. By means of the hydropathy plot and the predicted secondary structure, a postulated three-fold symmetry in the tertiary structure of L8.9C could be confirmed.     

The gene encoding human transmembrane secretory component (locus PIGR) is linked to D1S58 on chromosome 1

The human transmembrane secretory component (SC or poly-Ig receptor, PIGR) is expressed basolaterally on glandular epithelial cells and is responsible for the external translocation of polymeric IgA and IgM. SC is hence a key molecule in antibody protection of mucosal surfaces. The human SC gene (locus PIGR) is located on chromosome 1 (1q31–q41). Here we present the first genetic linkage study of PIGR versus syntenic markers, including D1S58 and F13B, which have been previously regionalized to 1q31–q32 and 1q31–q32.1, respectively. We found that PIGR is closely linked to D1S58 (lods + 5.06 at _max = 0.06, without sex difference). PIGR versus F13B showed + 1.46 at _max = 0.25 for both sexes combined. A recombination of 0.06 between F13B and D1S58 (lods + 2.24) was in contrast to a previously published study giving _max = 0.22 (lods + 3.9), the combined lods being 5.6 at _max = 0.20. The progeny of a triply heterozygotic female indicated that PIGR is the flanking locus, therefore suggesting a cen-F13B-D1S58-PIGR-qter gene sequence on human chromosome 1. Only negative lod scores to RH, C8@, and PGM1 on 1p, and FY on proximal 1q, were found. Current combined Norwegian allele frequencies were estimated for PIGR to be A1 = 0.63, A2 = 0.37 (370 chromosomes), and for D1S58 to be A1 = 0.44, A2 = 0.56 (218 chromosomes).     

Transfer of singlet energy within trypsin.

Transfers of singlet energy within trypsin were investigated by measuring the fluorescence absorption anisotropy of its tryptophan residues. A ratio of the anisotropy of trypsin to that for N-acetyl-L-tryptophanamide was determined between 306 and 250 nm. The ratio had an average value of 0.7, whether the trypsin anisotropy was measured at 228 of 296 K. However, trypsin dissolved in 5 M guanidine hydrochloride showed little fluorescence depolarization at 228 K (the anisotropy ratio was approximately equal to 0.9). Thus, there is an extensive conformation-dependent energy transfer between tryptophans in trypsin. The ratio of anisotropies of tyrpsin at 304--270 nm was used to estimate energy transfer from tyrosine to tryptophan. Ratios of 1.8 and 1.7 were obtained at 296 K for the native and guanidinium-unfolded enzyme, respectively. The comparable value for N-acetyl-L-tryptophanamide was 1.7. This indicates that there is little transfer from tyrosine to tryptophan in trypsin at 296 K. As confirmation, the excitation wavelength dependencies of the indole fluorescence quantum yield were the same for native and unfolded trypsin. When experiments were performed at 228 K, the 304--270-nm anisotropy ratios were 2.6 for native and 2.1 for unfolded trypsin at pH2. This indicates that the efficiency of energy transfer from tyrosine to tryptophan increases at low temperatures. A photochemical source of error in the quantitation of the efficiency of energy transfer from tyrosine to tryptophan is also described.     

Functional assignment of chromophores and energy transfer in C phycocyanin isolated from the thermophilic cyanobacterium Mastigocladus laminosus

The optical characteristics and pathway of energy transfer in the C phycocyanin trimer isolated from the thermophilic cyanobacterium Mastigocladus laminosus were investigated at steady state by absorption, circular dichroism, fluorescence and fluorescence polarization spectroscopy. Based on the comparison of optical data with the 3-dimensional structure of the C-phycocyanin trimer determined by X-ray analysis (Schirmer, T., Bode, W., Huber, R., Sidler, W. and Zuber, H. (1984) in Proceedings of the Symposium on Optical Properties and Structure of Tetrapyrroles, (Blauer, G. and Sund, M., eds.), pp. 445–449, Walter de Gruyter, Berlin, and (1985) J. Mol. Biol. 184, 257–277), the functional assignment of three types of chromophore was established. An α subunit has an s chromophore and the chromophores at the positions 84 and 155 in the amino acid sequence of the β subunit are assigned as f and s chromophores, respectively. In the C phycocyanin trimer energy transfer occurs from the α chromophore in one monomer to the β_f chromophore in an adjacent monomer, and from the β_s chromophore to the β_f chromophore in the same monomer. The direction of energy flow is from the outside to the inside of the trimer, where the locus for the binding of a colourless polypeptide is postulated. In the phycobilisomes the energy concentrated at the β_f chromophores might be transferred toward the allophycocyanin core mainly by the β_f chromophores in the phycocyanin rods.     

Proximity of lectin receptors on the cell surface measured by fluorescence energy transfer in a flow system.

Molecules of the lectin concanavalin A have been labeled separately with the fluorescein and rhodamine chromophores and jointly bound to the surface of transformed Friend erythroleukemia cells. The two dyes constitute an ideal donor-acceptor pair for fluorescence resonance energy transfer thereby permitting the determination of the proximity relationships between bound ligand molecules and the corresponding surface receptors. The transfer efficiency at saturation (about 57%) was measured in a multiparameter flow system using laser excitation at 488 nm and detection of fluorescein and rhodamine emission intensities as well as the emission anisotropy of the rhodamine fluorescence for each cell. The degree of energy transfer was estimated from the quenching of donor emission, the sensitization of acceptor emission, and the depolarization of acceptor fluorescence. The system has been modeled according to a formalism developed by Gennis and Cantor (Biochemistry 11: 2509, 1972). We estimate the separation between the surfaces of bound lectin molecules at saturation to be 0-40 A, a range possibly characteristic for micropatches induced by ligand binding.     

Diffusion-enhanced lanthanide energy-transfer study of DNA-bound cobalt(III) bleomycins: comparisons of accessibility and electrostatic potential with DNA complexes of ethidium and acridine orange

Energy transfer in the "rapid-diffusion" limit reflects the equilibrium properties of a donor-acceptor system. Rates of energy transfer from freely diffusing terbium chelates to DNA-binding chromophores change dramatically when DNA is added; energy transfer from an electrically neutral chelate is reduced because the energy acceptor becomes partially buried in DNA, while energy transfer from a positive chelate is increased because of electrostatic attraction. The rate constants for energy transfer to DNA-bound chromophores from a positively charged terbium chelate, relative to those from a neutral chelate, were used to estimate the following values for the electrostatic potential near the surface of each DNA-bound acceptor at 298 K in the presence of 1.0 mM added salt (in units of -e/kT): acridine orange, 4.54 +/- 0.11; ethidium, 4.66 +/- 0.07; green Co(III) bleomycin A2, 4.06 +/- 0.11; orange Co(III) bleomycin A2, 3.11 +/- 0.10. Smaller numbers indicate less negative potentials; these can be due to a combination of (1) positive charge on the chromophore, (2) location of the chromophore [particularly Co(III) bleomycin] away from the DNA phosphates, and/or (3) separation of DNA phosphate negative charges by an intercalator. The magnitudes of the individual rate constants indicate that all the DNA-bound chromophores can be directly encountered by the terbium probes. Energy-transfer rate constants from a neutral terbium chelate to DNA-bound and free acceptors can provide a measure of the accessibility of the terbium probe to each bound chromophore. The ratios of these rate constants were as follows: acridine orange, 0.17 +/- 0.01; ethidium, 0.27 +/- 0.02; green form of Co(III) bleomycin A2, 0.48 +/- 0.06; orange form of Co(III) bleomycin A2, 0.71 +/- 0.06. These results are consistent with the probable differences in binding mechanisms for the intercalating chromophores (ethidium and acridine orange) as compared to the Co(III) bleomycins (in which the relevant chromophores are nonintercalating metal centers). In addition, all the results imply that the green Co(III) bleomycin chromophore binds closer to DNA than the orange; this provides a first step toward understanding the structural basis for the different biological properties of these metallobleomycins. Control experiments and theoretical considerations necessary to establish the validity of the results are also presented.     

Lanthanide probes in biological systems: characterization of luminescence excitation spectra of terbium complexes with proteins

Upon irradiation in the ultraviolet region aromatic chromophores may transfer energy to a nearby Tb³⁺, which in turn emits a green phosphorescence. This paper reports the characterization of the ultraviolet excitation spectra of aromatic chromophores capable of transferring energy to Tb³⁺ by monitoring of the green Tb³⁺ emission in the 540-550 nm region. Results are included for complexes containing phenyl, hydroxyphenyl, indole. and catechol chromophores. Characteristic excitation spectra are presented for the aromatic chromophores occurring as side chains in proteins. Though it is preferable to compare entire excitation spectra, the ratio of intensities at 292 to 276 nm, R, is suggested as a useful diagnostic criterion. Numerical R values are indicative of the following aromatic side chains as the energy donor to Tb³⁺: R <0.2, unionized tyrosine; R = 0.5 to 1.0, tryptophan; and R > 1.8. ionized tyrosine. Tlie phenylalanyl chromophore displays a definitive excitation spectrum at shorter wavelengths. For ovotransferrin R = 0.9 and comparison of the full excitation spectra suggests that it contains comparable contributions from both ionized tyrosine and tryptophan side chains. Some difficulties in obtaining reliable excitation spectra are described. An analysis of inner-filtering of incident light reveals that for an absorbance less than 0.8 the excitation spectrum is broadened and flattened compared to the absorption spectrum. At maximum absorbances greater than 0.8 false maxima may appear to both sides of a real maximum. Two spurious maxima in an excitation spectrum were generated in a Tb³⁺ complex and compared to the correct excitation spectrum of the same complex obtained at lower absorbance.