Fluorescence of delta 5,7,9(11),22-ergostatetraen-3 beta-ol in micelles, sterol carrier protein complexes, and plasma membranes

The fluorescent sterol analogue delta 5,7,9(11),22-ergostatetraen-3 beta-ol (dehydroergosterol) was synthesized and purified by reverse-phase high-performance liquid chromatography. Dehydroergosterol in aqueous solution had a critical micelle concentration of 25 nM and a maximum solubility of 1.3 microM as ascertained from fluorescence polarization and light scattering properties, respectively. Several lines of evidence indicated a close molecular interaction of dehydroergosterol with purified rat liver squalene and sterol carrier protein (SCP). SCP increased the maximal solubility of dehydroergosterol in aqueous buffer. The fluorescence emission spectrum of dehydroergosterol was blue shifted upon addition of SCP. The fluorescence lifetime of dehydroergosterol in aqueous buffer was 2.3 ns; addition of SCP resulted in the appearance of a second lifetime component near 12.4 ns. The SCP increased the fluorescence polarization of monomeric dehydroergosterol in aqueous buffer from 0.033 to 0.086. Scatchard analysis of the binding data indicated that dehydroergosterol interacted with purified rat liver SCP with an apparent KD = 0.88 microM and Bmax = 4.8 microM. At maximal binding, 1.0 mol of dehydroergosterol was specifically bound per mole of SCP. The close molecular interaction of dehydroergosterol with SCP was also demonstrated by energy-transfer experiments. The intermolecular distance between SCP and bound dehydroergosterol was evaluated by fluorescence energy transfer from tyrosine residues of SCP to the conjugated triene series of double bonds in dehydroergosterol. The transfer efficiency was 36%, and R, the apparent distance between the tyrosine energy donor and the dehydroergosterol energy acceptor, was 19 A. The significance of these data obtained in vitro for dehydroergosterol interaction with SCP was also tested in vivo.(ABSTRACT TRUNCATED AT 250 WORDS)     

Nanosecond pulse fluorometry of conformational change in phenylalanine hydroxylase associated with activation

Conformational change in rat liver phenylalanine hydroxylase associated with activation by phenylalanine or N-(1-anilinonaphth-4-yl)maleimide was investigated by measuring fluorescence spectra and fluorescence lifetimes of tryptophanyl residues as well as the probe fluorophore conjugated with SH groups of the hydroxylase. The fluorescence spectrum of tryptophan exhibited its maximum at 342 nm. It shifted by 8 nm toward longer wavelength accompanied by an increase in its intensity, by preincubation with 1 mM phenylalanine. The fluorescence intensity of tryptophan increased by 36% upon the activation. On the other hand, the binding of (6R)-L-erythro-tetrahydrobiopterin, a natural cofactor of the enzyme, induced a decrease in the fluorescence intensity by 79% without a shift of the maximum wavelength. The fluorescence lifetime of tryptophan of phenylalanine hydroxylase exhibited two components with lifetimes of 1.7 and 4.1 ns. The values of the lifetimes changed to 1.4 and 5.6 ns, respectively, upon the activation. It is considered that the change in the longer lifetime is correlated with the shift of the emission peak upon the activation. The values of both the lifetimes decreased to 0.64 and 3.6 ns upon the binding of (6R)-L-erythro-tetrahydrobiopterin, which is coincident with the decrease in the fluorescence intensity. Conjugation of N-(1-anilinonaphth-4-yl)maleimide with SH of phenylalanine hydroxylase brought about a decrease in both the fluorescence intensity and the value of the shorter lifetime of the tryptophanyl residues, while the longer lifetime remained unchanged.(ABSTRACT TRUNCATED AT 250 WORDS)     

Investigation of the structural determinants of the intrinsic fluorescence emission of the trp repressor using single tryptophan mutants.

The fluorescence decay properties of wild-type trp repressor (TR) have been characterized by carrying out a multi-emission wavelength study of the frequency response profiles. The decay is best analyzed in terms of a single exponential decay near 0.5 ns and a distribution of lifetimes centered near 3-4 ns. By comparing the recovered decay associated spectra and lifetime values with the structure of the repressor, tentative assignments of the two decay components recovered from the analysis to the two tryptophan residues, W19 and W99, of the protein have been made. These assignments consist of linking the short, red emitting component to emission from W99 and most of the longer bluer emitting lifetime distribution to emission from W19. Next, single tryptophan mutants of the repressor in which one of each of the tryptophan residues was substituted by phenylalanine were used to confirm the preliminary assignments, inasmuch as the 0.5-ns component is clearly due to emission from tryptophan 99, and much of the decay responsible for the recovered distribution emanates from tryptophan 19. The data demonstrate, however, that the decay of the wild-type protein is not completely resolvable due both to the large number of components in the wild-type emission (at least five) as well as to the fact that three of the five lifetime components are very close in value. The fluorescence decay of the wild-type decay is well described as a combination of the components found in each of the mutants. However, whereas the linear combination analysis of the 15 data sets (5 from the wild-type and each mutant) yields a good fit for the components recovered previously for the two mutants, the amplitudes of these components in the wild-type are not recovered in the expected ratios. Because of the dominance of the blue shifted emission in the wild-type protein, it is most likely that subtle structural differences in the wild-type as compared with the mutants, rather than energy transfer from tryptophan 19 to 99, are responsible for this failure of the linear combination hypothesis.     

A pulse fluorometry study of lipoamide dehydrogenase. Evidence for non-equivalent FAD centers.

The time dependence of the fluorescence of tryptophanyl and flavin residues in lipoamide dehydrogenase has been investigated with single-photon decay spectroscopy. When the two FAD molecules in the enzyme were directly excited the decay could only be analyzed in a sum of two exponentials with equal amplitudes. This phenomenon was observed at 4 degrees C (tau-1 = 0.8 ns, tau-2 = 4.7 ns) and at 20 degrees C (tau-1 = 0.8 ns, tau-2 = 3.4 ns) irrespective of the emission and excitation wavelengths. This result reveals a difference in the nature of the two FAD centers. By excitation at 290 nm the fluorescence decay curves of tryptophan and FAD were obtained. The decays are analyzed in terms of energy transfer from tryptophanyl to flavin residues. The results, which are in good agreement with those obtained previously with static fluorescence methods, show that one of the two tryptophanyl residues within the subunit transfers its excitation energy to the flavin located at a distance of 1.5 nm.     

Tyrosine and tyrosinate fluorescence of S-100b. A time-resolved nanosecond fluorescence study. The effect of pH, Ca(II), and Zn(II)

The properties of the tyrosine and tyrosinate emissions from brain S-100b have been studied by nanosecond time-resolved fluorescence at emission wavelengths in the range 305 to 365 nm. The effect of pH on the fluorescence has been studied at pH 6.5, 7.5, and 8.5 for the Ca(II) apo and holo forms of the protein, and for the apo and holo forms in the presence and absence of Zn(II) at pH 7.5. The fluorescence decay is biexponential at pH 8.5 and triexponential at pH 6.5 and 7.5. The three components of the decay have wavelength and metal ion dependent lifetimes in the ranges 0.06 to 1.05 ns, 0.49 to 3.76 ns, and 3.60 to 14.5 ns. The observation of a long lifetime component at wavelengths characteristic of emission from tyrosinate suggests that in class A proteins this may be a useful diagnostic of the environment of tyrosine in their native structures. The time-resolved emission spectra provide evidence for efficient, subnanosecond protolysis of the excited state of the single tyrosine (Tyr17) under all conditions studied except in 6 M guanidium chloride in which the protein shows only emission from tyrosine (lambda em 305 nm), suggesting that the tyrosinate emission is a property of the tertiary structure of the native protein. The Zn(II)-dependence of the fluorescence is fully consistent with the earlier suggestion that Tyr17 is near the Zn(II) binding site and remote from the high affinity Ca(II) binding site.     

Anomalous fluorescence of yeast 3-phosphoglucerate kinase.

The 3-phosphoglycerate kinase (EC 2.7.2.3) of yeast which contains two tryptophyl and eight tyrosyl residues per molecule, displayed an unusualy fluorescence emission spectrum with a maximum at 308 nm when excited at 280 nm. The emission peak shifted to 329 nm when excited at 295 nm. We could confirm that it was due to the efficient quenching of tryptophyl fluorescence as well as to the incomplete energy transfer from tyrosyl to tryptophyl residues. The average fluorescence quantum yield of this protein was 0.076 (excitation at 280 nm) and that of tryptophyl residues was 0.046 (excitation at 295 nm). As the pH of the solution was lowered, the fluorescence intensity of phosphoglycerate kinase at 329 nm dramatically increased between pH 5 and 4, while the position of the peak remained unchanged. When denatured in 4 M guanidine hydrochloride, the protein showed two emission peaks, one at 343 nm and the other at 303 nm.     

Exposure and electronic interaction of tyrosine and tryptophan residues in human apolipoprotein A-IV

We have investigated the exposure and electronic interaction of tyrosine and tryptophan residues in human apolipoprotein A-IV (apo A-IV). Differential absorption spectroscopy and chemical titration demonstrated that human apo A-IV contains six tyrosine residues, four of which are buried in the hydrophobic interior of the protein and two of which are exposed on the protein surface. Denaturation of the protein by guanidinium chloride caused progressive exposure of the buried tyrosines. The fluorescence emission spectra of apo A-IV were characterized by a blue-shifted tryptophan emission with a low relative quantum yield of 0.37 and a tyrosine emission with a relative quantum yield of 0.62. Fluorescence quenching studies demonstrated a low fractional exposure of tryptophan in the native state. Denaturation of apo A-IV was accompanied by an increase in the relative quantum yield which peaked at the denaturation midpoint. Fluorescence excitation techniques demonstrated energy transfer from tyrosine residues with a transfer efficiency of 0.40 in the native state; the efficiency was conformation dependent and decreased with protein unfolding. Fluorescence studies of tetranitromethane-modified apo A-IV suggested that a significant fraction of energy transfer proceeds from the exposed tyrosine residues. These data demonstrate the existence of intramolecular fluorescence energy transfer and tryptophan quenching in human apolipoprotein A-IV and suggest that the amino terminus of this protein is situated in a hydrophobic domain within energy-transfer range of nonvicinal tyrosine residues.     

The intrinsic tyrosine fluorescence of histone H1. Steady state and fluorescence decay studies reveal heterogeneous emission

In wavelength-resolved steady state spectra we observe three different kinds of emission from histone H1, a class A protein with only a single tyrosine residue. Unfolded H1 emissions that peak at approximately 300 and 340 nm can both be excited maximally at approximately 280 nm. Another, peaking much further to the red at approximately 400 nm, can be excited maximally at approximately 320 nm. The 300-nm fluorescence can be resolved by lifetime measurements into three components with decay times of approximately 1, 2, and 4 ns. On sodium-chloride-induced refolding of H1, simplification of the emission properties occurs. The 340 and 400-nm components disappear while the two shorter lifetime components of the 300-nm band diminish in amplitude and are replaced by the 4-ns decay. We believe that the 340-nm emission is tyrosinate fluorescence resulting from excited-state proton transfer. The origin of the 400-nm emission remains uncertain. We assign the 1 and 2-ns components of the 300-nm emission to two states of tyrosine in denatured H1 and the 4-ns decay to fluorescence of the single tyrosine residue in the globular region of refolded H1. Our results support the contention that salt induced folding of H1 is a cooperative two state process, and permit us to better understand the previously reported increases in fluorescence intensity and anisotropy on salt-induced folding.     

Association of the internal membrane protein with the lipid bilayer in influenza virus. A study with the fluorescent probe 12-(9-anthroyl)-stearic acid

The lipid fluorescent probe 12-(9-anthroyl)-stearic acid was introduced into the lipid bilayer of influenza virus particles. Fluorescent energy transfer was observed from the viral protein to the probe. This transfer persisted after removal of the glycoprotein spikes which cover the outside of the viral particle, demonstrating that the energy donor was an internal protein. It was concluded that the energy donor was the non-glycosylated membrane protein (M protein), the major protein component of the spikeless particle. Analysis of the emission spectrum of the spikeless particle excited at 275 nm shows that a substantial portion of the fluorescence arises from tyrosine residues, in contrast to most other proteins which contain both tryptophan and tyrosine.It is suggested that the donor residue(s) are located no more than 11 Å exterior to the bilayer surface, and that a portion of the M protein may penetrate into the bilayer.     

Sterol and squalene carrier protein interactions with fluorescent delta 5,7,9(11)-cholestatrien-3 beta-ol

The fluorescent sterol delta 5,7,9(11)-cholestatrien-3 beta-ol (cholestatrienol) was used as an analogue of cholesterol to determine the properties of the sterol in aqueous buffer and the interaction of cholesterol with sterol and squalene carrier protein (SCP). Cholestatrienol was synthesized and purified to a stable product by reverse phase high performance liquid chromatography. The critical micelle concentration of cholestatrienol in aqueous buffer was 1 nM while its maximum solubility was 1.15 microM as ascertained from fluorescence polarization and light scattering properties, respectively. Several lines of evidence indicated a close molecular interaction of cholestatrienol with purified rat liver SCP. The fluorescence emission spectrum of monomeric cholestatrienol in aqueous buffer was blue shifted upon addition of SCP. The fluorescence lifetime of monomeric cholestatrienol in aqueous buffer was increased by SCP from 5 to 12 ns. The SCP increased the fluorescence polarization of monomeric cholestatrienol from 0.002 to 0.38 in aqueous buffer. The close molecular interaction of cholestatrienol with SCP was also demonstrated by energy transfer experiments. Fluorescence energy transfer from tyrosine residues of SCP to the conjugated triene fluorophore in cholestatrienol had a transfer efficiency of 59%. R, the apparent distance between the tyrosine energy donor and the cholestatrienol energy acceptor, was 16.3 A. Binding analysis indicated that cholestatrienol interacted with SCP with an apparent KD = 0.5 microM and a Bmax = 3.54 microM. One mol of cholestatrienol was bound per mol of SCP. These results demonstrate the utility of cholestatrienol not only as a membrane sterol probe molecule but also as a probe for sterol-protein interactions.     

Tryptophan fluorescence lifetimes in lysozyme.

Tryptophan fluorescence lifetimes at pH 2 and pH 8 have been obtained for lysozyme and for lysozyme derivatives in which tryptophan-62 or tryptophan-108 or both are nonfluorescent. The lifetimes range from about 0.5 ns to 2.8 ns for the various emitting tryptophans. The tryptophan lifetimes appear to increase with exposure of tryptophan to solvent, but intramolecular contacts, probably with cystine residues, can considerably shorten the lifetime. Intertryptophanyl interactions can also affect fluorescence lifetimes. The trytophan-108 lifetime in lysozyme is shorter than in the derivative in which tryptophan-62 is oxidized; this is ascribed to energy transfer from tryptophan-108 to tryptophan-62. From the lifetime results the relative intensities emitted by specific tryptophans can be estimated, and these values also support the existence of intertryptophanyl energy transfer. The emission intensity from tryptophan-62 is greater in the presence of tryptophan-108, and the emission intensity of tryptophan-108 appears to be greater in the absence of tryptophan-62. Conformational effects accompanying chemical modification of tryptophan cannot be completely ruled out, however. The tryptophan-62 lifetime at pH 8 in lysozyme is shorter than in the derivatives, which might indicate a subtle conformational effect. Studies with tri-(N-acetyl-glucosamine)-protein complexes indicate that both the tryptophan lifetimes and the number of emitting tryptophans may be changing upon complexation. The results illustrate the usefulness and the limitations of lifetime measurements in understanding protein fluorescence.     

Determination of the excited-state lifetimes of the tryptophan residues in barnase, via multifrequency phase fluorometry of tryptophan mutants.

A multifrequency phase fluorometric study is described for wild-type barnase and engineered mutant proteins in which tryptophan residues have been replaced by less fluorescent residues which do not interfere with the determination of the tryptophan emission spectra and lifetimes. The lifetimes of the three tryptophans in the wild-type protein have been resolved. Trp-35 has a single fluorescence lifetime, which varies in the different proteins between 4.3 and 4.8 ns and is pH-independent between pH 5.8 and 8.9. Trp-71 and Trp-94 behave as an energy-transfer couple with both forward and reverse energy transfer. The couple shows two fluorescence lifetimes: 2.42 (+/-0.2) and 0.74 (+/-0.1) ns at pH 8.9, and 0.89 (+/-0.05) and 0.65 (+/-0.05) ns at pH 5.8. In the mutant Trp-94----Phe the lifetime of Trp-71 is 4.73 (+/-0.008) ns at high pH and 4.70 (+/-0.004) ns at low pH. In the mutant Trp-71----Tyr, the lifetime of Trp-94 is 1.57 (+/-0.01) ns at high pH and 0.82 (+/-0.025) ns at low pH. From these lifetimes, one-way energy-transfer efficiencies can be calculated according to Porter [Porter, G.B. (1972) Theor. Chim. Acta 24, 265-270]. At pH 8.9, a 71% efficiency was found for forward transfer (from Trp-71 to Trp-94) and 36% for reverse transfer. At pH 5.8 the transfer efficiency was 86% for forward and 4% for reverse transfer (all +/-2%). These transfer efficiencies correspond fairly well with the ones calculated according to the theory of F?rster [F?rster, T. (1948) Ann. Phys. (Leipzig) 2, 55-75].(ABSTRACT TRUNCATED AT 250 WORDS)     

Correlation between internal motion and emission kinetics of tryptophan residues in proteins

Time-resolved fluorescence anisotropy measurements of tryptophan residues were carried out for 44 proteins. Internal rotational motion with a sub-nanosecond correlation time (0.9 +/- 0.6 ns at 10 degrees C) was seen in a large number of proteins, though its amplitude varied from protein to protein. It was found that tryptophan residues which were almost fixed within a protein had either a long (greater than 4 ns) or short (less than 2 ns) fluorescence lifetime, whereas a residue undergoing a large internal motion had an intermediate lifetime (1.5-3 ns). It is suggested that the emission kinetics of a tryptophan residue is coupled with its internal motion. In particular, an immobile tryptophan residue emitting at long wavelength was characterized by a long lifetime (greater than 4 ns). It appears that a tryptophan residue fixed in a polar region has little chance of being quenched by neighboring groups.     

Concatenation of cyan and yellow fluorescent proteins for efficient resonance energy transfer

Highly efficient fluorescence resonance energy transfer between cyan(CFP) and yellow fluorescent proteins (YFP), the cyan- and yellow-emitting variants of the Aequorea green fluorescent protein, respectively, was achieved by tightly concatenating the two proteins. After the C-terminus of CFP and the N-terminus of YFP were truncated by 11 and 5 amino acids, respectively, the proteins were fused through a leucine-glutamate dipeptide. The resulting chimeric protein, which we called Cy11.5, exhibited a simple emission spectrum that peaked at 527 nm when the protein was excited at 436 nm. The time-resolved emission of Cy11.5 was measured using a streak camera. After excitation of Cy11.5 with a 400 nm ultrashort pulse, a fast decay of the CFP emission and a concomitant rise of the YFP emission were observed with a lifetime of 66 ps. By contrast, the emission from CFP alone showed a decay component with a lifetime of 2.9 ns. We concluded that in fully folded Cy11.5 molecules, intramolecular FRET occurred with an efficiency of 98%. Importantly, most Cy11.5 molecules were properly folded, and the protein was highly resistant to all of the tested proteases. In living cells, therefore, Cy11.5 behaved as a single fluorescent protein with a broad excitation spectrum. Moreover, Cy11.5 was used as an optical highlighter after photobleaching of YFP. When HeLa cells expressing Cy11.5 were irradiated at 514.5 nm, a 10-fold increase in the 475 nm fluorescence intensity was observed. These features make Cy11.5 useful as an optical highlighter and a new-colored fluorescent protein for multicolor imaging.     

Motion of aromatic side chains, picosecond fluorescence, and internal energy transfer in Escherichia coli thioredoxin studied by site-directed mutagenesis, time-resolved fluorescence spectroscopy, and molecular dynamics simulations

We have determined the picosecond fluorescence of the four aromatic amino acid residues (W28, W31, Y49, and Y70) in wild-type Escherichia coli thioredoxin (wt Trx) and a mutant Trx with W31 replaced by phenylalanine, Trx-W28-W31F. The internal motions of the four aromatic side chains were also analyzed. We examined the possibility of using internal energy transfer from tyrosine to tryptophan as a measure of long-range distances. The major features of the lifetime distribution of tryptophan fluorescence were unchanged in the W31F mutation, indicating that the environment of W28 is similar in both wt Trx and Trx-W28-W31F. However, the mutation of W31F changed the mobility of W28, situated close to the active-site disulfide/dithiol, but not the mobility of two tyrosines, Y49 and Y70, situated on the other side of the molecule. The mobility of the two tyrosine residues increased upon reduction of the active-site disulfide, indicating a looser structure with reduction. This increased motion could also be seen from molecular dynamics simulations. The change in energy transfer rates, as judged by tyrosine fluorescence lifetimes, was in agreement with energy transfer rates calculated from the molecular dynamics simulations. The anisotropy of tryptophan and tyrosine fluorescence could be separated in three parts: (I) overall rotation of the protein (10(-9)s), (II) internal mobility of side chains (10(-10)s), and (III) a very fast relaxation (10(-12)s). We can only experimentally detect this very fast relaxation when the internal motion is not present.     

A rare protein fluorescence behavior where the emission is dominated by tyrosine: case of the 33-kDa protein from spinach photosystem II

An abnormal fluorescence emission of protein was observed in the 33-kDa protein which is one component of the three extrinsic proteins in spinach photosystem II particle (PS II). This protein contains one tryptophan and eight tyrosine residues, belonging to a "B type protein". It was found that the 33-kDa protein fluorescence is very different from most B type proteins containing both tryptophan and tyrosine residues. For most B type proteins studied so far, the fluorescence emission is dominated by the tryptophan emission, with the tyrosine emission hardly being detected when excited at 280 nm. However, for the present 33-kDa protein, both tyrosine and tryptophan fluorescence emissions were observed, the fluorescence emission being dominated by the tyrosine residue emission upon a 280 nm excitation. The maximum emission wavelength of the 33-kDa protein tryptophan fluorescence was at 317 nm, indicating that the single tryptophan residue is buried in a very strong hydrophobic region. Such a strong hydrophobic environment is rarely observed in proteins when using tryptophan fluorescence experiments. All parameters of the protein tryptophan fluorescence such as quantum yield, fluorescence decay, and absorption spectrum including the fourth derivative spectrum were explored both in the native and pressure-denatured forms.     

Fluorescence and excitation Escherichia coli RecA protein spectra analyzed separately for tyrosine and tryptophan residues

The method for separation of emission (EM) and excitation (EX) spectra of a protein into EM and EX spectra of its tyrosine (Tyr) and tryptophan (Trp) residues was described. The method was applied to analysis of Escherichia coli RecA protein and its complexes with Mg(2+), ATPgammaS or ADP, and single-stranded DNA (ssDNA). RecA consists of a C-terminal domain containing two Trp and two Tyr residues, a major domain with five Tyr residues, and an N-terminal domain without these residues (R. M. Story, I. T. Weber, and T. A. Steitz (1992) Nature (London) 355, 374-376). Because the fluorescence of Tyr residues in the C-terminal domain was shown to be quenched by energy transfer to Trp residues, Trp and Tyr fluorescence of RecA was provided by the C-terminal and the major domains, respectively. Spectral analysis of Trp and Tyr constituents revealed that a relative spatial location of the C-terminal and the major domains in RecA monomers was different for their complexes with either ATPgammaS or ADP, whereas this location did not change upon additional interaction of these complexes with ssDNA. Homogeneous (that is, independent of EX wavelength) and nonhomogeneous (dependent on EX wavelength) types of Tyr and Trp fluorescence quenching were analyzed for RecA and its complexes with nucleotide cofactors and ssDNA. The former was expected to result from singlet-singlet energy transfer from these residues to adenine of ATPgammaS or ADP. By analogy, the latter was suggested to proceed through energy transfer from high vibrational levels of the excited state of Trp and Tyr residues to the adenine. In this case, for correct calculation of the overlap integral, Trp and Tyr donor emission spectra were substituted by the spectral function of convolution of emission and excitation spectra that resulted in a significant increase of the overlap integral and gave an explanation of the nonhomogeneous quenching of Trp residues in the C-terminal domain.     

An unusual fluorescence spectrum of a protein proteinase inhibitor, Streptomyces subtilisin inhibitor.

Streptomyces subtilisin inhibitor, a dimeric protein proteinase inhibitor isolated in crystalline form by Murae et al. in 1972, contains three tyrosine and one tryptophan residues per monomer unit and has unusual fluorescence properties. When excited at 280 nm, it shows a characteristic fluorescence spectrum having a peak at 307 nm and a shoulder near 340 nm, a feature which has been recognized only for a very few cases in proteins containing both tryosine and tryptophan residues. When excited at 295 nm, at which tryrosine scarcely absorbs, the inhibitor shows an emission spectrum with a peak at 340 nm characteristic of a tryptophan residue. The emission with a peak at 307 nm is considered to arise from the tryrosine residues. The tryptophan quantum yield of Streptomyces subtilisin inhibitor excited at 295 nm is very small, indicating that the tryptophan florescence is strongly quenched in the native state of the inhibitor. Below pH 4 the peak of the fluorescence spectrum of the inhibitor excited at 280 nm shifts toward 340-350 nm with a concomitant increase in the quantum yield. The structural change induced by low pH seems to release the tryptophan fluorescence from the quenching.     

Fluorescence and circular-dichroism properties of pig intestinal calcium-binding protein (Mr=9000), a protein with a single tyrosine residue.

Spectral properties of pig intestinal Ca2+-binding protein (CaBP) and its apoprotein have been examined by fluorescence, absorption and c.d. Direct fluorescence from some of the five phenylalanine residues is observed and excitation spectra show that there is also energy transfer from some phenylalanine residues to the tyrosine. Absorption and c.d. spectra show that the tyrosine hydroxy group does not ionize significantly below pH 12. Tyrosine fluorescence is reversibly quenched by a lysine residue with a pK of 10.05 in the Ca2+ form. At low pH the tyrosine fluorescence is enhanced with transitions with pK values of approx. 4.2. The c.d. spectrum of the Ca2+ form shows a decrease of the ellipticity band at 276nm with a transition similar to that of the fluorescence titration. The apoprotein, however, shows an additional transition with a pK of about 6. The results are interpreted in terms of the recently published structure of the cow intestinal CaBP [Szebenyi, Obendorf & Moffat (1981) Nature (London) 294, 327-332]. The single tyrosine has a very high pK, although it apparently lies on the surface of the protein molecule.     

Pressure and low temperature effects on the fluorescence emission spectra and lifetimes of the photosynthetic components of cyanobacteria.

The effects of hydrostatic pressure on the excited state reactions of the photosynthetic system of cyanobacteria were studied with the use of stationary and dynamic fluorescence spectroscopy. When the cells were excited with blue light (442 nm), hydrostatic pressure promoted a large increase in the fluorescence emission of the phycobilisomes (PBS). When PBS were excited at 565 nm, the shoulder originating from photosystem II (PSII) emission (F685) disappeared under 2.4 kbar compression, suggesting suppression of the energy transfer from PBS to PSII. At atmospheric pressure, the excited state decay was complex due to energy transfer processes, and the best fit to the data consisted of a broad Lorentzian distribution of short lifetimes. At 2.4 kbar, the decay data changed to a narrower distribution of longer lifetimes, confirming the pressure-induced suppression of the energy transfer between the PBS and PSII. When the cells were excited with blue light, the decay at atmospheric pressure was even more complex and the best fit to the data consisted of a two-component Lorentzian distribution of short lifetimes. Under compression, the broad distribution of lifetimes spanning the region 100-1,000 ps disappeared and gave rise to the appearance of a narrow distribution characteristic of the PBS centered at 1.2 ns. The emission of photosystem I underwent 2.2-fold increase at 2.4 kbar and room temperature. A decrease in temperature from 20 to -10 degrees C at 2.4 kbar promoted a further increase in the fluorescence emission from photosystem I to a level comparable with that obtained at temperatures below 120 degrees K and atmospheric pressure. On the other hand, when the temperature was decreased under pressure, the PBS emission diminished to very low value at blue or green excitation, suggesting the disassembly into the phycobiliprotein subunits.