Protein dynamics. A time-resolved fluorescence, energetic and molecular dynamics study of ribonuclease T1

Studies using time-resolved fluorescence depolarization were performed on the internal motion of Trp 59 of ribonuclease T1 (EC 3.1.27.3) in the free enzyme, 2'-GMP-enzyme complex and 3'-GMP-enzyme complex. The Trp 59 motion was also studied in the free enzyme using molecular dynamics simulations. Energetic analysis of activation barriers to the Trp 59 motion was performed using both the transition state theory and Kramers' theory. The activation parameters showed a dependence on solvent viscosity indicating the transition state approach in aqueous solution to be inadequate. When taking solvent viscosity contributions into account agreement between the transition state and Kramers' theories was obtained. The results indicate the three enzyme forms to have different conformations with the free enzyme and 3'-GMP-enzyme complex being similar. Comparison of the experimental and theoretical results showed a good agreement on the Trp 59 motion in the free enzyme. Trp 59 appears to vibrate rapidly, with a relaxation time of the order of 1 ps, within free space in the protein matrix and to have a slower motion, with a relaxation time of the order of 100 ps, which is related to breathing of the surrounding protein matrix. Molecular dynamics results indicate high mobility in regions of the enzyme involved in the interaction with the guanine base of the inhibitor or substrate while much lower mobility occurred in residues involved in the catalytic mechanism of ribonuclease T1.     

Three-dimensional structure of ribonuclease T1 complexed with an isosteric phosphonate substrate analogue of GpU: alternate substrate binding modes and catalysis

The X-ray crystal structure of a complex between ribonuclease T1 and guanylyl(3'-6')-6'-deoxyhomouridine (GpcU) has been determined at 2. 0 A resolution. This ligand is an isosteric analogue of the minimal RNA substrate, guanylyl(3'-5')uridine (GpU), where a methylene is substituted for the uridine 5'-oxygen atom. Two protein molecules are part of the asymmetric unit and both have a GpcU bound at the active site in the same manner. The protein-protein interface reveals an extended aromatic stack involving both guanines and three enzyme phenolic groups. A third GpcU has its guanine moiety stacked on His92 at the active site on enzyme molecule A and interacts with GpcU on molecule B in a neighboring unit via hydrogen bonding between uridine ribose 2'- and 3'-OH groups. None of the uridine moieties of the three GpcU molecules in the asymmetric unit interacts directly with the protein. GpcU-active-site interactions involve extensive hydrogen bonding of the guanine moiety at the primary recognition site and of the guanosine 2'-hydroxyl group with His40 and Glu58. On the other hand, the phosphonate group is weakly bound only by a single hydrogen bond with Tyr38, unlike ligand phosphate groups of other substrate analogues and 3'-GMP, which hydrogen-bonded with three additional active-site residues. Hydrogen bonding of the guanylyl 2'-OH group and the phosphonate moiety is essentially the same as that recently observed for a novel structure of a RNase T1-3'-GMP complex obtained immediately after in situ hydrolysis of exo-(Sp)-guanosine 2',3'-cyclophosphorothioate [Zegers et al. (1998) Nature Struct. Biol. 5, 280-283]. It is likely that GpcU at the active site represents a nonproductive binding mode for GpU [Steyaert, J., and Engleborghs (1995) Eur. J. Biochem. 233, 140-144]. The results suggest that the active site of ribonuclease T1 is adapted for optimal tight binding of both the guanylyl 2'-OH and phosphate groups (of GpU) only in the transition state for catalytic transesterification, which is stabilized by adjacent binding of the leaving nucleoside (U) group.     

Modes of mononucleotide binding to ribonuclease T1.

The binding of the mononucleotide inhibitors 2'-GMP, 3'-GMP, and 5'-GMP to genetically engineered ribonuclease T1 has been investigated by conventional inhibition kinetics, fluorimetric titrations, molecular modeling, and fast relaxation techniques. The fluorimetric titrations in conjunction with molecular modeling revealed that apart from the already known primary binding site, three to four additional sites are present on the enzyme's surface. The association constants obtained from the fluorimetric titrations and the temperature jump experiments range between 3.1 x 10(6) M-1 and 4.3 x 10(6) M-1, indicating that the binding of the mononucleotides to the specific binding site of ribonuclease T1 is at least one order of magnitude tighter than has been anticipated so far. The kinetics of binding are nearly diffusion controlled with a kon determined for 2'-GMP and 3'-GMP, as (5.0 +/- 0.5 x 10(9) and 6.1 +/- 0.5 x 10(9) M-1, s-1 and koff as 1.2 +/- 0.2 x 10(3) and 2.0 +/- 0.3 x 10(3) s-1, respectively. Molecular modeling studies indicate that all three nucleotides are able to bind via their phosphate group to a positively charged array of surface amino acids including His27, His40, Lys41, and most probably Lys25 without obvious stereochemical hindrance. We propose that RNA wraps around RNase T1 in a similar fashion via phosphate binding when enzymatic hydrolysis occurs.     

Picosecond time-resolved fluorescence spectroscopy of K-590 in the bacteriorhodopsin photocycle.

The fluorescence spectrum of a distinct isometric and conformational intermediate formed on the 10(-11) s time scale during the bacteriorhodopsin (BR) photocycle is observed at room temperature using a two laser, pump-probe technique with picosecond time resolution. The BR photocycle is initiated by pulsed (8 ps) excitation at 565 nm, whereas the fluorescence is generated by 4-ps laser pulses at 590 nm. The unstructured fluorescence extends from 650 to 880 nm and appears in the same general spectral region as the fluorescence spectrum assigned to BR-570. The transient fluorescence spectrum can be distinguished from that assigned to BR-570 by a larger emission quantum yield (approximately twice that of BR-570) and by a maximum intensity near 731 nm (shifted 17 nm to higher energy from the maximum of the BR-570 fluorescence spectrum). The fluorescence spectrum of BR-570 only is measured with low energy, picosecond pulsed excitation at 590 nm and is in good agreement with recent data in the literature. The assignment of the transient fluorescence spectrum to the K-590 intermediate is based on its appearance at time delays longer than 40 ps. The K-590 fluorescence spectrum remains unchanged over the entire 40-100-ps interval. The relevance of these fluorescence data with respect to the molecular mechanism used to model the primary processes in the BR photocycle also is discussed.     

Picosecond time-resolved study of MgCl2-induced chlorophyll fluorescence yield changes from chloroplasts

The MgCl2-induced chlorophyll fluorescence yield changes in broken chloroplasts, suspended in a cation-free medium, treated with 3,-(3',4'-dichlorophenyl)-1,1-dimethylurea and pre-illuminated, has been investigated on a pico-second time scale. Chloroplasts in the low fluorescing state showed a fluorescence decay law of the form exp --At1/2, where A was found to be 0.052 ps-1/2, and may be attributed to the rate of spillover from Photosystem II to Photosystem I. Addition of 10 mM MgCl2 produced a 50% increase in the steady-state fluorescence quantum yield and caused a marked decrease in the decay rate. The fluorescence deday law was found to be predominantly exponential with a 1/e lifetime of 1.6 ns. These results support the hypothesis that cation-induced changes in the fluorescence yield of chlorophyll are related to the variations in the rate of energy transfer from Photosystem II to Photosystem I, rather than to changes in the partitioning of absorbed quanta between the two systems.     

Conformational heterogeneity of the copper binding site in azurin. A time-resolved fluorescence study.

Comparison of the fluorescence spectra and the effect of temperature on the quantum yields of fluorescence of Azurin (from Pseudomonas fluorescens ATCC-13525-2) and 3-methylindole (in methylcyclohexane solution) provides substantive evidence that the tryptophan residue in azurin is completely inaccessible to solvent molecules. The quantum yields of azurin (CuII), azurin (CuI), and apoazurin (lambda ex = 291 nm) were 0.052, 0.054, and 0.31, respectively. Other evidence indicates that there is no energy transfer from tyrosine to tryptophan in any of these proteins. The fluorescence decay behavior of each of the azurin samples was found to be invariant with emission wavelength. The fluorescences of azurin (CuII) and azurin (CuI) decay with dual exponential kinetics (tau 1 = 4.80 ns, tau 2 = 0.18 ns) while that of apoazurin obeys single exponential decay kinetics (tau = 4.90). The ratio of pre-exponentials of azurin (CuII), alpha 1/alpha 2, is found to be 0.25, and this ratio increases to 0.36 on reduction to azurin (CuI). The results are interpreted as originating from different interactions of the tryptophan with two conformers of the copper-ligand complex in azurin.     

pH dependence of the urea and guanidine hydrochloride denaturation of ribonuclease A and ribonuclease T1

To investigate the pH dependence of the conformational stability of ribonucleases A and T1, urea and guanidine hydrochloride denaturation curves have been determined over the pH range 2-10. The maximum conformational stability of both proteins is about 9 kcal/mol and occurs near pH 4.5 for ribonuclease T1 and between pH 7 and 9 for ribonuclease A. The pH dependence suggests that electrostatic interactions among the charged groups make a relatively small contribution to the conformational stability of these proteins. The dependence of delta G on urea concentration increases from about 1200 cal mol-1 M-1 at high pH to about 2400 cal mol-1 M-1 at low pH for ribonuclease A. This suggests that the unfolded conformations of RNase A become more accessible to urea as the net charge on the molecule increases. For RNase T1, the dependence of delta G on urea concentration is minimal near pH 6 and increases at both higher and lower pH. An analysis of information of this type for several proteins in terms of a model developed by Tanford [Tanford, C. (1964) J. Am. Chem. Soc. 86, 2050-2059] suggests that the unfolded states of proteins in urea and GdnHCl solutions may differ significantly in the extent of their interaction with denaturants. Thus, the conformations assumed by unfolded proteins may depend to at least some extent on the amino acid sequence of the protein.     

Picosecond time-resolved absorption and fluorescence dynamics in the artificial bacteriorhodopsin pigment BR6.11.

The picosecond molecular dynamics in an artificial bacteriorhodopsin (BR) pigment containing a structurally modified all-trans retinal chromphore with a six-membered ring bridging the C11=C12-C13 positions (BR6.11) are measured by picosecond transient absorption and picosecond time-resolved fluorescence spectroscopy. Time-dependent intensity and spectral changes in absorption in the 570-650-nm region are monitored for delays as long as 5 ns after the 7-ps, 573-nm excitation of BR6.11. Two intermediates, J6.11 and K6.11/1, both with enhanced absorption to the red (> 600 nm) of the BR6.11 spectrum are observed within approximately 50 ps. The J6.11 intermediate decays with a time constant of 12 +/- 3 ps to form K6.11/1. The K6.11/1 intermediate decays with an approximately 100-ps time constant to form a third intermediate, K6.11/2, which is observed through diminished 650-nm absorption (relative to that of K6.11/1). No other transient absorption changes are found during the remainder of the initial 5-ns period of the BR6.11 photoreaction. Fluorescence in the 650-900-nm region is observed from BR6.11, K6.11/1, and K6.11/2, but no emission assignable to J6.11 is found. The BR6.11 fluroescence spectrum has a approximately 725-nm maximum which is blue-shifted by approximately 15 nm relative to that of native BR-570 and is 4.2 +/- 1.5 times larger in intensity (same sample optical density). No differences in the profile of the fluorescence spectra of BR6.11 and the intermediates K6.11/1 and K6.11/2 are observed. Following ground-state depletion of the BR6.11 population, the time-resolved fluroescence intensity monitored at 725 nm increases with two time constants, 12 +/- 3 and approximately 100 ps, both of which correlate well with changes in the picosecond transient absorption data.(ABSTRACT TRUNCATED AT 250 WORDS)     

Frequency domain measurements of the fluorescence lifetime of ribonuclease T1.

Using multifrequency phase/modulation fluorometry, we have studied the fluorescence decay of the single tryptophan residue of ribonuclease T1 (RNase T1). At neutral pH (7.4) we find that the decay is a double exponential (tau 1 = 3.74 ns, tau 2 = 1.06 ns, f1 = 0.945), in agreement with results from pulsed fluorometry. At pH 5.5 the decay is well described by a single decay time (tau = 3.8 ns). Alternatively, we have fitted the frequency domain data by a distribution of lifetimes. Temperature dependence studies were performed. If analyzed via a double exponential model, the activation energy for the inverse of the short lifetime component (at pH 7.4) is found to be 3.6 kcal/mol, as compared with a value of 1.0 kcal/mol for the activation energy of the inverse of the long lifetime component. If analyzed via the distribution model, the width of the distribution is found to increase at higher temperature. We have also repeated, using lifetime measurements, the temperature dependence of the acrylamide quenching of the fluorescence of RNase T1 at pH 5.5. We find an activation energy of 8 kcal/mol for acrylamide quenching, in agreement with our earlier report.     

Picosecond time-resolved study of MgCl2-induced chlorophyll fluorescence yield changes from chloroplasts

The MgCl₂-induced chlorophyll fluorescence yield changes in broken chloroplasts, suspended in a cation-free medium, treated with 3,-(3′,4′-dichlorophenyl)-1,1-dimethylurea and pre-illuminated, has been investigated on a picosecond time scale. Chloroplasts in the low fluorescing state showed a fluorescence decay law of the form exp $\text{?At}{}^{\mathrm{<mtext>1</mtext><mtext>2</mtext>}}$, where A was found to be 0.052 $\text{ps}{}^{\mathrm{<mtext>?1</mtext><mtext>2</mtext>}}$, and may be attributed to the rate of spillover from Photosystem II to Photosystem I. Addition of 10 mM MgCl₂ produced a 50% increase in the steady-state fluorescence quantum yield and caused a marked decrease in the decay rate. The fluorescence decay law was found to be predominantly exponential with a 1/e lifetime of 1.6 ns. These results support the hypothesis that cation-induced changes in the fluorescence yield of chlorophyll are related to the variations in the rate of energy transfer from Photosystem II to Photosystem I, rather than to changes in the partitioning of absorbed quanta between the two systems.     

Picosecond time-resolved infrared study of 2-aminopurine ionisation in solution.

Two photon ionisation of 2-aminopurine (2AP) has been monitored following 267 nm irradiation in neutral and acidic aqueous solutions using picosecond time-resolved infrared spectroscopy (ps-TRIR). The transient infrared spectra obtained in neutral and acidic conditions show significant differences that are consistent with the formation of different species, namely the 2AP radical cation, 2AP+*, in acidic conditions and the uncharged radical, 2AP*(-H+), in neutral conditions. The ps-TRIR data indicate that deprotonation of 2AP+* in neutral solution takes place within <2 ps following photoionisation. DFT calculations (EDF1/6-31+G*) were used to support the assignment of the intermediates observed in these spectroscopic experiments.     

Relaxation kinetics of ribonuclease T1 binding with guanosine and 3'-GMP.

Temperature-jump relaxation kinetic studies were undertaken at 25 degrees C with ribonuclease T1 (RNase T1) alone and in the presence of guanosine (Guo) and 3'-guanylic acid (3'-GMP). No relaxations were observed in the absence of ligands and only one process was observed in their presence which reflected a simple on-off reaction in both cases. Apparent association rate constants, k(on), and dissociation rate constants, k(off), were evaluated at several pH values and their ratios, k(on)/k(off), were contrasted with independently determined values of the equilibrium association constant, Ka(eq). The value of k(on)/k(off) for Guo was significantly greater than Ka(eq), whereas Ka(eq) was significantly greater than k(on)/k(off) for 3'-GMP. The simplest interpretation of the result for Guo is that free RNase T1 undergoes a relatively slow undetected isomerization and Guo can bind only with one isomer. 3'-GMP can be considered to bind with the same preference, but in this case the initial enzyme complex undergoes a relatively slow undetected isomerization. These results are consistent with a recent NMR study which suggested that RNase T1 binding with Guo and 3'-GMP are coupled to slow exchange processes in a ligand dependent manner (Shimada, I. and Inagaki, F. (1990) Biochemistry 29, 757-764). It is tentatively concluded that binding of Guo and 3'-GMP at the active site of RNase T1 is limited to a sub-population of conformers involving the base-recognition site and that the phosphomonoester group of the nucleotide can engage in additional conformationally linked interactions at the adjacent catalytic site.     

Substrate and substrate analogue binding properties of Renilla luciferase.

Luciferase from the anthozoan coelenterate Renilla reniformis catalyzes the oxidative decarboxylation of luciferin consuming 1 mol of O2 per mol of luciferin oxidized and producing 1 mol of CO2, 1 mol of oxyluciferin, and light (lambdaB, 480 nm) with a 5.5% quantum yield. In this work we have examined the binding characteristics of luciferin, luciferin analogues, and competitive inhibitors of the luciferin-luciferase reaction. The results show that luciferin binding and orientation in the single luciferin binding site of luciferase are highly specific for and dependent upon the three group substituents of the luciferin molecule while the imidazolone-pyrazine nucleus of luciferin is not directly involved in binding. Anaerobic luciferin binding promotes a rapid concentration-dependent aggregation of luciferase which results in irreversible inactivation of the enzyme. This aggregation phenomenon is not observed upon binding of oxyluciferin, luciferyl sulfate, or luciferin analogues in which the substituent at the 2 position of the imidazolone-pyrazine ring has been substantially altered.     

A fluorescence study of substrate and inhibitor binding to bovine liver dihydrofolate reductase

• 1.1. Covalent coupling of fluorescein to methotrexate (MTX) by a 5-carbon spacer yields a dihydrofolate reductase (DHFR) inhibitor (FMTX) with K_i = 11 nM.
• 2.2. FMTX shows a fluorescence quenching with respect to fluorescein which is relieved by binding to the enzyme.
• 3.3. The dissociation constants (K_d) of MTX, FMTX, NADPH and 7,8-dihydrofolate (DHF) from bovine liver DHFR have been determined by fluorometric titrations.
• 4.4. The K_d values for NADPH, MTX and FMTX from the complementary binary complexes (MTX·DHFR, FMTX·DHFR and NADPH·DHFR) were also obtained; these show a 2- to 4-fold decrease with respect to those obtained by titration of the free enzyme.
• 5.5. A competitive assay for MTX has been developed by exploiting the fluorescence enhancement of DHFR-bound FMTX. This assay may be useful for the routine determination of MTX in the concentration range from 10⁻⁹ to 10⁻⁷ M.

     

Viscosity dependence of acrylamide quenching of ribonuclease T1 fluorescence. The gating mechanism.

The structural regulation of the access of acrylamide molecules, as quenchers, to the buried tryptophans of a protein can be modelled by a simple gate concept. Such a gate, when open, allows transient exposure of the fluorophore to the quencher molecule in solution. We have previously shown that the observed viscosity dependence of acrylamide quenching process in ribonuclease T1 (RNAse T1) is not reconcilable with the gating mechanism. However, on that occasion, we neglected the effect of changes in the activity of the quencher molecule and the possible presence of static quenching. The experimental observation of a considerable contribution by static quenching and the realization that static quenching might produce dramatic effects in steady state measurements led us to reexamine the question. It is shown that in a gating model the static component can also influence the apparent dynamic quenching. In this paper, we present derived equations for the gated quenching mechanism including possible contributions from the static component. We also carefully remeasured the acrylamide quenching of RNAase T1 as a function of increasing glycerol concentration. Computer simulations were carried out to compare the experimental data set to the generalized model. We reach the conclusion that even the new, quite complex equations fail to predict the qualitative and quantitative features of the observed quenching experiments. We arrived at the conclusion that the fluorophore is never the target of the quencher molecules in solution.     

A time-resolved fluorescence study of azurin and metalloazurin derivatives

Nickel and cobalt derivatives of Pseudomonas fluorescens (ATCC 13525) azurin were prepared and their steady-state fluorescence and time-resolved fluorescence monitored. Like the copper-containing native protein, the fluorescence decay of both metallo derivatives was best fit to a sum of three exponentials, whereas the apoazurin from which they were prepared obeyed single-exponential decay kinetics. However, comparison of the lifetimes and fractional of each of the components in these derivatives to those in the oxidized and reduced native proteins revealed significant differences. These results suggest that the presence of a metal center in azurin imparts a conformational heterogeneity which is strongly dependent on the nature of the metal center. Further, the results are used to comment on current ideas concerning the geometry of the active site in this redox protein.