A dual functional turn off florescence sensor using metal–organic framework for sensitive detection of aluminum(III) in aqueous solution

Aluminum, classified as one of the toxic heavy metals, has a recommended daily consumption limit of 3–10 mg, as specified by the World Health Organization (WHO). Herein, the selective and sensitive aluminum(III) fluorescence sensor based on TMU-16 metal–organic frameworks (MOFs) in aqueous medium, is reported. A sensing pathway was found via the cation exchange between aluminum(III) and zinc(II) ions, and caused selectivity and sensitivity detection of aluminum(III) with a 5–100 ppm linear range and 1.99 ppm limit of detection (LOD). This sensor offers the advantage of accurately determining the concentration range of aluminum(III) ions. At low concentrations, only fluorescence quenching was observed, while at higher concentrations, fluorescence emission not only undergoes quenching but also exhibits a blue shift in wavelength. Notably, the sensor demonstrates no interference from cation solutions of mercury(II), zinc(II), nickel(II), lead(II), cobalt(II), cadmium(II), silver(I), chromium(III), and iron(III). Another significant feature of this sensor is its selectivity toward copper(II) and aluminum(III) ions, due to quenching fluorescence in the presence of copper(II) ion. The results presented the sensor's selectivity toward copper(II) at low concentrations and aluminum(III) at high concentrations.     

Influence of copper(II) and magnesium(II) ions on the ciprofloxacin binding to DNA

The influence of magnesium(II) and copper(II) ions on the binding of ciprofloxacin to double stranded calf thymus DNA was studied by fluorescence emission spectroscopy, ultraviolet- and circular dichroism (CD) spectroscopy. The interaction of ciprofloxacin and copper(II) ions was followed by strong fluorescence quenching which was almost unaffected by the presence of DNA. On the other hand, only a slight decrease in fluorescence emission intensity, which was enhanced in the presence of DNA, was observed for ciprofloxacin interaction with magnesium(II) ions. Furthermore, magnesium(II) ions increase the thermal stability of the DNA, while, in the presence of ciprofloxacin, the degree of stabilisation is smaller. In contrast, copper(II) ions destabilise double helical DNA to heat, while ciprofloxacin slightly affects only the second transition of the biphasic melting curve of calf thymus DNA. Magnesium(II) ions at 25 degrees C induce conformational transitions of DNA at concentrations of 1.5 mM and 2.5 M, as monitored by CD. On the other hand copper(II) ions induce only one conformational transition, at a concentration of 12.7 microM. At higher concentrations of copper(II) ions (c>700 microM) DNA starts to precipitate. Significant changes in the CD spectra of DNA were observed after addition of ciprofloxacin to a solution containing DNA and copper(II) ions, but not to DNA and magnesium(II) ions. Based on our spectroscopic results, we propose that copper(II) ions are not directly involved into ciprofloxacin binding to DNA via phosphate groups as it has been suggested for magnesium(II) ions.     

Crystal structure of plant light‐harvesting complex shows the active,energy‐transmitting state

Plants dissipate excess excitation energy as heat by non‐photochemical quenching (NPQ). NPQ has been thought to resemble in vitro aggregation quenching of the major antenna complex, light harvesting complex of photosystem II (LHC‐II). Both processes are widely believed to involve a conformational change that creates a quenching centre of two neighbouring pigments within the complex. Using recombinant LHC‐II lacking the pigments implicated in quenching, we show that they have no particular role. Single crystals of LHC‐II emit strong, orientation‐dependent fluorescence with an emission maximum at 680 nm. The average lifetime of the main 680 nm crystal emission at 100 K is 1.31 ns, but only 0.39 ns for LHC‐II aggregates under identical conditions. The strong emission and comparatively long fluorescence lifetimes of single LHC‐II crystals indicate that the complex is unquenched, and that therefore the crystal structure shows the active, energy‐transmitting state of LHC‐II. We conclude that quenching of excitation energy in the light‐harvesting antenna is due to the molecular interaction with external pigments in vitro or other pigment–protein complexes such as PsbS in vivo, and does not require a conformational change within the complex.     

The conformer substates of nonoriented B-type DNA in double helical poly(dG-dC)

A nonoriented hydrated film of poly(dG-dC) with ?20 water molecules per nucleotide (called B* by Loprete and Hartman (Biochem. 32, 4077-4082 (1993)) was studied by Fourier transform infrared (FT-IR) spectroscopy either as equilibrated sample between 290 and 270 K or, after quenching into the glassy state, as nonequilibrated film isothermally at 200 and 220 K. IR spectral changes on isothermal relaxation at 200 and 220 K, caused by interconversion of two conformer substates, are revealed by difference spectra. Comparison with difference curves obtained in the same manner from two classical B-DNA forms, namely the d(CGCGAATTCGCG)(2) dodecamer and polymeric NaDNA from salmon testes, revealed that the spectral changes on B(I)-to-B(II) interconversion in the classical B-DNA forms are very similar to those in the B*-form, and that the spectroscopic differences between the B(I) and B(II) features from classical B-DNA and those from the modified B*-form are minor. Nonexponential kinetics of the B(I)-->B(II) transition in the B*-form of poly(dG-dC) at 200 K showed that the structural relaxation time is about three times of that in the classical B-DNA forms (approximately equal to 30 versus approximately equal to 10 min at 200 K). The unexpected reversal of conformer substates interconversion (that is B(II)-->B(I) transition on cooling from 290 K and B(I)-->B(II) transition on isothermal relaxation at 200 K) observed for classical B-DNA occurs also in the modified B*-form. We therefore conclude that restructuring of hydration shells rules the low-temperature dynamics of the B*-form via its two conformer substates in the same manner reported for classical B-DNA by Pichler et al. (J. Phys. Chem. B 106, 3263-3274 (2002)).     

The incorporation of divalent metal ions into recombinant human tyrosine hydroxylase apoenzymes studied by intrinsic fluorescence and 1H-NMR spectroscopy.

Three isoforms of human tyrosine hydroxylase were expressed in Escherichia coli and purified to homogeneity as the apoenzymes (metal-free). The apoenzymes exhibit typical tryptophan fluorescence emission spectra when excited at 250-300 nm. The emission maximum (342 nm) was not shifted by the addition of metal ions, but reconstitution of the apoenzymes with Fe(II) at pH 7-9 reduced the fluorescence intensity by about 35%, with an end point at 1.0 iron atom/enzyme subunit. The fluorescence intensity of purified bovine adrenal tyrosine hydroxylase, containing 0.78 mol tightly bound iron/mol subunit, was reduced by only 6% on addition of an excess amount of Fe(II). Other divalent metal ions [Zn(II), Co(II), Mn(II), Cu(II) and Ni(II)] also reduced the fluorescence intensity of the human enzyme by 12-30% when added in stoichiometric amounts. The binding of Co(II) at pH 7.2 was also found to affect its 1H-NMR spectrum and this effect was reversed by lowering the pH to 6.1. The quenching of the intrinsic fluorescence of the human isoenzymes by Fe(II) was reversed by the addition of metal chelators. However, the addition of stoichiometric amounts of catecholamines, which are potent feedback inhibitors of tyrosine hydroxylase, to the iron-reconstituted enzyme, prevented the release of iron by the metal chelators. Fluorescence quenching, nuclear magnetic relaxation measurements and EPR spectroscopy all indicate that the reconstitution of an active holoenzyme from the isolated apoenzyme, with stoichiometric amounts of Fe(II) at neutral pH, occurs without a measurable change in the redox state of the metal. However, on addition of dopamine or suprastoichiometric amounts of iron, the enzyme-bound iron is oxidized to a high-spin Fe(III) (S = 5/2) form in an environment of nearly axial symmetry, thus providing an explanation for the inhibitory action of the catecholamines.     

Interaction of cobalt(II) and copper(II) hydroxamates with polyriboadenylic acid: An insight into RNA based drug designing

The polyadenylic acid [poly(A)] tail of mRNA plays a noteworthy role in the initiation of the translation, maturation, and stability of mRNA. It also significantly contributes to the production of alternate proteins in eukaryotic cells. Hence, it has recently been recognized as a prospective drug target. Binding affinity of bis(N-p-tolylbenzohydroxamato)Cobalt(II), [N-p-TBHA-Co(II)] (1) and bis(N-p-naphthylbenzohydroxamato)Copper(II), [N-p-NBHA-Cu(II)] (2) complexes with poly(A) have been investigated by biophysical techniques namely, absorption spectroscopy, fluorescence spectroscopy, diffuse reflectance infrared Fourier transform spectroscopy, circular dichroism spectroscopy, viscometric measurements and through molecular docking studies. The intrinsic binding constants (K_b) of complexes were determined following the order of N-p-TBHA-Co(II)] > N-p-NBHA-Cu(II), along with hyperchromism and a bathochromic shift for both complexes. The fluorescence quenching method revealed an interaction between poly(A)-N-p-TBHA-Co(II)/poly(A)-N-p-NBHA-Cu(II). The mode of binding was also determined via the fluorescence ferrocyanide quenching method. The increase in the viscosity of poly(A) that occurred from increasing the concentration of the N-p-TBHA-Co(II)/N-p-NBHA-Cu(II) complex was scrutinized. The characteristics of the interaction site of poly(A) with N-p-TBHA-Co(II)/N-p-NBHA-Cu(II) were adenine and phosphate groups, as revealed by DRS-FTIR spectroscopy. Based on these observations, a partial intercalative mode of the binding of poly(A) has been proposed for both complexes. Circular dichroism confirmed the interaction of both the complexes with poly(A). The molecular docking results illustrated that complexes strongly interact with poly(A) via the relative binding energies of the docked structure as ?259.39eV and ?226.30eV for N-p-TBHA-Co(II) and N-p-NBHA-Cu(II) respectively. Moreover, the binding affinity of N-p-TBHA-Co(II) is higher in all aspects than N-p-NBHA-Cu(II) for poly(A).     

Analysis of the slow phases of the in vivo chlorophyll fluorescence induction curve. Changes in the redox state of Photosystem II electron acceptors and fluorescence emission from Photosystems I and II

An analysis of the photo-induced decline in the in vivo chlorophyll a fluorescence emission (Kautsky phenomenon) from the bean leaf is presented. The redox state of PS II electron acceptors and the fluorescence emission from PS I and PS II were monitored during quenching of fluorescence from the maximum level at P to the steady state level at T. Simultaneous measurement of the kinetics of fluorescence emission associated with PS I and PS II indicated that the ratio of PS I/PS II emission changed in an antiparallel fashion to PS II emission throughout the induction curve. Estimation of the redox state of PS II electron acceptors at given points during P to T quenching was made by exposing the leaf to additional excitation irradiation and determining the amount of variable PS II fluorescence generated. An inverse relationship was found between the proportion of PS II electron acceptors in the oxidised state and PS II fluorescence emission. The interrelationships between the redox state of PS II electron acceptors and fluorescence emission from PS I and PS II remained similar when the shape of the induction curve from P to T was modified by increasing the excitation photon flux density. The contributions of photochemical and non-photochemical quenching to the in vivo fluorescence decline from P to T are discussed.     

Light-induced quenching of chlorophyll fluorescence at 77 K in leaves,chloroplasts and Photosystem II particles

The light-induced chlorophyll (Chl) fluorescence decline at 77 K was investigated in segments of leaves, isolated thylakoids or Photosystem (PS) II particles. The intensity of chlorophyll fluorescence declines by about 40% upon 16 min of irradiation with 1000 μmol m⁻² s⁻¹ of white light. The decline follows biphasic kinetics, which can be fitted by two exponentials with amplitudes of approximately 20 and 22% and decay times of 0.42 and 4.6 min, respectively. The decline is stable at 77 K, however, it is reversed by warming of samples up to 270 K. This proves that the decline is caused by quenching of fluorescence and not by pigment photodegradation. The quantum yield for the induction of the fluorescence decline is by four to five orders lower than the quantum yield of Q_A reduction. Fluorescence quenching is only slightly affected by addition of ferricyanide or dithionite which are known to prevent or stimulate the light-induced accumulation of reduced pheophytin (Pheo). The normalised spectrum of the fluorescence quenching has two maxima at 685 and 695 nm for PS II emission and a plateau for PS I emission showing that the major quenching occurs within PS II. ‘Light-minus-dark’ difference absorbance spectra in the blue spectral region show an electrochromic shift for all samples. No absorbance change indicating Chl oxidation or Pheo reduction is observed in the blue (410–600 nm) and near infrared (730–900 nm) spectral regions. Absorbance change in the red spectral region shows a broad-band decrease at approximately 680 nm for thylakoids or two narrow bands at 677 and 670–672 nm for PS II particles, likely resulting also from electrochromism. These absorbance changes follow the slow component of the fluorescence decline. No absorbance changes corresponding to the fast component are found between 410 and 900 nm. This proves that the two components of the fluorescence decline reflect the formation of two different quenchers. The slow component of the light-induced fluorescence decline at 77 K is related to charge accumulation on a non-pigment molecule of the PS II complex. This revised version was published online in June 2006 with corrections to the Cover Date.     

Purification and some novel properties of Escherichia coli RNase II.

RNase II of Escherichia coli (EC 3.1.4.23) has been purified to apparent homogeneity. The K+-activated diesterase activity against poly(U), which defines RNase II, cochromatographs with activity against T4 mRNA or pulse-labeled E. coli RNA successively on DEAE-cellulose, hydroxyapatite or phosphocellulose, and Sephadex G-150 columns. Activities with both substrates are selectively reduced to less than 2% of the wild type level in a newly isolated mutant strain, S296, or after thermal inactivation in a mutant strain with temperature-sensitive RNase II. RNase II releases 5'-XMP without a lag as its only detectable alcohol-soluble produce from all substrates and has an apparent molecular weight of 80,000 to 90,000 in both nondissociating and sodium dodecyl sulfate-polyacrylamide gels. The pure enzyme shows the standard K+ activation against poly(A), poly(U), or poly(C), but only a slight preference for K+ over Na+ ions with T4 mRNA or pulse labeled E. coli RNA as substrate. Uniformly labeled E. coli rRNA or tRNA is degraded little if at all.     

Cobalt substitution studies on bovine erythrocyte superoxide dismutase: evidence for a novel cobalt-superoxide dismutase derivative

Three cobalt derivatives of bovine erythrocyte superoxide dismutase (superoxide:superoxide oxidoreductase, EC 1.15.1.1) have been prepared under different pH conditions using a cobalt-thiocyanate complex which has already proved to yield specific substitutions on other copper proteins. The cobalt-protein derivatives have been characterized by optical, circular dichroism and fluorescence spectroscopies. One derivative, referred to as Co2Co2-protein, contains Co(II) ions specifically bound at both Zn(II) and Cu(II) sites. On the basis of their spectroscopic properties, the other two derivatives can be referred as E2Co2- and Co2E2-superoxide dismutase, with cobalt substituting, respectively, at the zinc and the copper sites leaving the contiguous site empty (E). The Co2E2-protein complex represents a novel derivative, since it has never been described in literature. The optical spectrum in the visible region of Co2-Co2-protein well corresponds to the sum of the spectra of the other two derivatives. The circular dichroism spectrum of Co2Co2-derivative, however, is not the sum of individual E2Co2- and Co2E2-proteins, suggesting that the presence of Co(II) in one site strongly affects the geometry of the neighbouring site. Some discrepancies between our spectroscopic data and those reported in literature are discussed. The results obtained from fluorescence experiments indicate that Co(II) ions exert a different quenching effect on the tyrosine emission, depending on whether they are located in the Zn(II) or in the Cu(II) site. The fluorescence quenching can be attributed to a 'heavy atom' and 'paramagnetic ion' effect by Co(II) ions.     

Tyrosine quenching of tryptophan phosphorescence in glyceraldehyde-3-phosphate dehydrogenase from Bacillus stearothermophilus.

Tyrosine is known to quench the phosphorescence of free tryptophan derivatives in solution, but the interaction between tryptophan residues in proteins and neighboring tyrosine side chains has not yet been demonstrated. This report examines the potential role of Y283 in quenching the phosphorescence emission of W310 of glyceraldehyde-3-phosphate dehydrogenase from Bacillus stearothermophilus by comparing the phosphorescence characteristics of the wild-type enzyme to that of appositely designed mutants in which either the second tryptophan residue, W84, is replaced with phenylalanine or Y283 is replaced by valine. Phosphorescence spectra and lifetimes in polyol/buffer low-temperature glasses demonstrate that W310, in both wild-type and W84F (Trp84-->Phe) mutant proteins, is already quenched in viscous low-temperature solutions, before the onset of major structural fluctuations in the macromolecule, an anomalous quenching that is abolished with the mutation Y283V (Tyr283-->Val). In buffer at ambient temperature, the effect of replacing Y283 with valine on the phosphorescence of W310 is to lengthen its lifetime from 50 micros to 2.5 ms, a 50-fold enhancement that again emphasizes how W310 emission is dominated by the local interaction with Y283. Tyr quenching of W310 exhibits a strong temperature dependence, with a rate constant kq = 0.1 s(-1) at 140 K and 2 x 10(4) s(-1) at 293 K. Comparison between thermal quenching profiles of the W84F mutant in solution and in the dry state, where protein flexibility is drastically reduced, shows that the activation energy of the quenching reaction is rather small, Ea < or = 0.17 kcal mol(-1), and that, on the contrary, structural fluctuations play an important role on the effectiveness of Tyr quenching. Various putative quenching mechanisms are examined, and the conclusion, based on the present results as well as on the phosphorescence characteristics of other protein systems, is that Tyr quenching occurs through the formation of an excited-state triplet exciplex.     

Comparative studies on the interactions of dihydroartemisinin and artemisinin with bovine serum albumin using spectroscopic methods

The interactions of dihydroartemisinin (DHA) and artemisinin (ART) with bovine serum albumin (BSA) have been investigated using fluorescence, UV/vis absorption and Fourier transform infrared (FTIR) spectra under simulated physiological conditions. The binding characteristics of DHA/ART and BSA were determined by fluorescence emission and resonance light scattering (RLS) spectra. The quenching mechanism between BSA and DHA/ART is static. The binding constants and binding sites of DHA/ART–BSA systems were calculated at different temperatures (293, 298, 304 and 310 K). According to Förster non‐radiative energy transfer theory, the binding distance of BSA to DHA/ART was calculated to be 1.54/1.65 nm. The effect of DHA/ART on the secondary structure of BSA was analyzed using UV/vis absorption, FTIR, synchronous fluorescence and 3D fluorescence spectra. In addition, the effects of common ions on the binding constants of BSA–DHA and BSA–ART systems were also discussed. Copyright © 2014 John Wiley & Sons, Ltd.     

De novo design of a copper(II)-binding helix-turn-helix chimera: the prion octarepeat motif in a new context

A chimeric Cu-binding peptide has been designed on the basis of a turn substitution of the prion (PrP) octarepeat Cu-binding site into the engrailed homeodomain helix-turn-helix motif (HTH). This system is a model for the investigation of a single PrP Cu-binding site in a defined protein context. The 28-mer Cu-HTH peptide P7 spectroscopically mimics the PrP octarepeat (P7 = TERRRQQLSHGGGWGEAQIKIWFQNKRA). The Cu(II)-binding affinity of P7 was determined by ESI-MS and tryptophan fluorescence titrations to be K(d) = 2.5 +/- 0.7 microM at pH = 7.0. The quenching of fluorescence of the Trp within the binding loop (underlined above) is pH dependent and highly specific for Cu(II). No Trp quenching was observed in the presence of divalent Zn, Mn, Co, Ni, or Ca ions, and ESI-MS titrations confirmed that these divalent ions do not appreciably bind to P7. The EPR spectrum of Cu(II)-P7 shows that the Cu environment is axial and consistent with 6-coordinate N(3)O(H(2)O)(2) or N(4)(H(2)O)(2) coordination (A( parallel) = 172 x10(-)(4) cm(-)(1); g( parallel) = 2.27), very similar to that of the PrP octarepeat itself. Also like PrP, circular dichroism studies show that apo P7 is predominantly disordered in solution, and the structure is slightly enhanced by Cu binding. These data show the Cu-PrP HTH peptide reproduces the Cu-binding behavior of a single PrP octarepeat in a new context.     

Effect of metal ions on the interaction between bovine serum albumin and berberine chloride extracted from a traditional Chinese Herb coptis chinensis franch

The effect of four metal ions Cu(2+), Ni(2+), Zn(2+) and Co(2+) on the interaction between bovine serum albumin (BSA) and berberine chloride (BC) extracted from a traditional Chinese Herb coptis chinensis franch, was investigated mainly by means of UV and fluorescence spectroscopy in this paper. The four metal ions make the quenching efficacy of BC to BSA higher than that in the absence of these metal ions because of the possible transition of BSA molecular conformation caused by metal ions. It was found that the quenching mechanism is a combination of static quenching with nonradiative energy transfer. In the presence of metal ions, the apparent association constant K(A) and the number of binding sites of BC on BSA are both decreased in a range of 8-19% and 25-28%, respectively, which indicates that the metal ions decrease the binding efficacy of BC on BSA and increase the concentration of free BC simultaneously. The scheme of interaction between BC and BSA in the presence of metal ions is a strong quenching but a weak binding.     

A quantitative study of the slow decline of chlorophyll a fluorescence in isolated chloroplasts.

A detailed study of the photo-induced decline in chlorophyll a fluorescence intensity (Kautsky phenomenon) in coupled isolated chloroplasts from a high level (P) to a low stationary level (S) is presented. 1. A linear relationship between P leads to S quenching and intrathylakoid H+ concentration was found. When the light-induced proton gradient was abolished by uncoupling, the fluorescence emission at room temperature was lowered proportionally to increased H+ concentration in the medium. 2. Fluorescence spectra at -196 degrees C of samples frozen at the P and S states showed no significant differences in the Photosystem I/Photosystem II ratio of fluorescence emission. Furthermore, freezing to -196 degrees C reversed the P leads to S quenching. This indicates that the P leads to S quenching is not related to an increase of spillover of excitation energy from Photosystem II to Photosystem I. 3. When Mg2+ was added to thylakoids suspended in a medium free of divalent cations, the inhibition of spillover required lower Mg2+ concentrations (half saturation at 0.6 mM). Increased proton concentration in the medium also inhibited spillover. 4. The results are interpreted in terms of two sites of Mg2+ and H+ effects on excitation deactivation in Photosystem II. One site is located on the outer face of the thylakoid membrane; action of both Mg2+ and H+ at this side diminishes spillover. The second site is located on the inner face of the membrane; as Mg2+ is displaced there by protons, a non-photochemical quenching of Photosystem II fluorescence is induced, which is manifested by the P leads to S decline.     

Conformation of adenosine deaminase in complexes with inhibitors: application of selective quenching of fluorescence emission

The effect of inhibitors, 1-deazaadenosine (1-dAdo) and erythro-9-(2-hydroxy-3-nonyl)adenine (EHNA), on the conformation of adenosine deaminase was studied using the method of selective quenching of fluorescence emission by acrylamide, I- and Cs+. Both in free adenosine deaminase and in its complexes with the inhibitors, the wavelength maxima and half-width of the emission characterize the environment of fluorescing tryptophan residues in adenosine deaminase as weak polar with limited access to solvent. The formation of complexes with the ground state inhibitors used did not quench or change the main emission characteristics of tryptophan fluorescence in adenosine deaminase. Small blue shifts of emission maxima were observed upon quenching in all three samples. The Stern-Volmer parameters of tryptophan fluorescence quenching by acrylamide were not essentially influenced by complex formation of the enzyme with the inhibitors: in general, the folding of the enzyme molecule in the complexes is not perturbed. On the contrary, the emission quenching by charged heavy ions, I- and Cs+, in the complexes was hindered in comparison with free adenosine deaminase. In the complex with 1-deazaadenosine, the parameters for quenching by both ions evidence the essential worsening of their interaction with tryptophans. In the complex with erythro-9-(2-hydroxy-3-nonyl)adenine, along with the worse quenching by I-, complete prohibition of quenching by Cs+ was observed. These data indicate that the local environments of fluorescing tryptophan residues is substantially distorted compared with free adenosine deaminase, which leads to their screening from charged heavy ions.     

Spectral Studies of a Chlorophyll Pigment with Fluorescence Maximum at 698 mμ

A chlorophyll type pigment (F698) fluorescing maximally at 698 mμ at 77°K has been observed in preparations of chlorophyll. This fluorescence is quenched by small amounts of naturally occurring materials, including plastoquinone and the ubiquinones, and by nitrobenzene, probably by formation of a nonfluorescent complex. Fluorescence quenching does not occur in the presence of carotenes, xanthophylls, or reduced plastoquinone and ubiquinone. The fluorescence is sharply temperature dependent, with a steep rise in intensity occurring at 165°K. At 77°K the fluorescence yield is between 0.8 and 1.0. The red absorption maximum of the pigment is at 675 mμ at room temperature and at 688 mμ at 77°K. In vivo, a low temperature emission is also observed at 698 mμ, and this fluorescence is quenched by nitrobenzene. It is proposed that the pigment found in vitro is also the one responsible for emission at 698 mμ in vivo. A reaction of F698 with plastoquinone is suggested as the primary photochemical step in system II of photosynthesis.     

Interaction of metal ions with polynucleotides and related compounds. IX. Unwinding and rewinding of poly(A + U) and poly(I + C) by copper(II) ions

It is demonstrated that, poly(A + U) and poly(I + C) are both formed under low ionic strength conditions. Continuous variation studies indicate the formation of copper(II) complexes of poly A, poly C, and poly I, but not of poly U. Copper(II) in a 1:1 ratio to polynucleotide prevents the formation of poly(A + U) and brings about the dissociation of the poly (A + U) complex produced in the absence of the metal. Poly (I + C) is similarly dissociated by copper(II) ions. The addition of sufficient electrolyte reverses the copper(II) induced dissociation of poly(I + C). The effect of copper(II) on ordered synthetic polynucleotides is thus very similar to its effect on DNA.     

Protochlorophyllide forms and energy transfer in dark-grown wheat leaves. Studies by conventional and laser excited fluorescence spectroscopy between 10 K–100 K

The fluorescence properties and role in energy transfer of protochlorophyllide (Pchlide) forms were studied in dark-grown wheat leaves by conventional and laser excited high resolution methods in the 10 K–100 K temperature range. The three major spectral bands, with emission maxima at 633, 657 (of highest intensity) and 670 nm as Bands I, II, and III were analyzed and interpreted as the contributions of six different structural forms. Band I is the envelope of three (0,0) emission bands with maxima at 628, 632 and 642 nm. Laser excitation studies in the range of Band II at 10 K reveal the presence of a spectrally close donor band besides the acceptor, Band II. The intensity in Band III originates mostly from being the vibronic satellite of Band II, but contains also a small (0,0) band with absorption maximum at 674 nm. Excitation spectra show that besides the Pchlides with absorption around 650 nm within Band II, another significant population of Band I with absorption around 640 nm is also coupled by energy transfer to the acceptor of Band II. The spectral difference between the two donor forms indicate different dipolar environments. Upon increasing the temperature, the intensity of Band II and its satellite, Band III decrease, while Band I remains unaffected. Band II shows also a broadening towards the blue side at higher temperatures. Both the quenching of fluorescence and the spectral change was explained by a thermally activated formation of a non-fluorescent intermediate state in the excited state of Pchlide acceptors.     

Structural studies on the active site of Escherichia coli RNA polymerase. 1. Interaction of metals on the i and i + 1 sites

The two substrates between which an internucleotide bond is formed in RNA synthesis occupy two subsites, i and i + 1, on the active site of Escherichia coli RNA polymerase, and each subsite is associated with a metal ion. These ions are therefore useful as probes of substrate interaction during RNA synthesis. We have studied interactions between the metals by EPR spectroscopy. The Zn(II) in the i site and the Mg(II) in the i + 1 site were substituted separately or jointly by Mn(II). The proximity of the metals was established by EPR monitoring of the titration at 5.5 K of the enzyme containing Mn(II) in i with Mn(II) going into the i + 1 site, and the 1:1 ratio of the metals in the two sites was confirmed in this way. The distance between the two metals was determined by EPR titration at room temperature of both the enzyme containing Zn(II) in i and Mn(II) in i with Mn(II) going into the i + 1 site, making use of the fact that EPR spectra are affected by dipolar interactions between the metals. The distances calculated in the presence of enzyme alone, in the presence of enzyme and two ATP substrates, and when poly(dAdT).poly(dAdT) was added to the latter system ranged from 5.2 to 6.7 A.