Analysis of time-resolved fluorescence anisotropy decays.

We discuss the analysis of time-correlated single photon counting measurements of fluorescence anisotropy. Particular attention was paid to the statistical properties of the data. The methods used previously to analyze these experiments were examined and a new method was proposed in which parallel- and perpendicular-polarized fluorescence curves were fit simultaneously. The new method takes full advantage of the statistical properties of the measured curves; and, in some cases, it is shown to be more sensitive than other methods to systematic errors present in the data. Examples were presented using experimental and simulated data. The influence of fitting range on extracted parameters and statistical criteria for evaluating the quality of fits are also discussed.     

Theory of light quenching: effects of fluorescence polarization, intensity, and anisotropy decays.

Experimental studies have recently demonstrated that fluorescence emission can be quenched by laser light pulses from modern high repetition rate lasers, a phenomenon we call "light quenching." We now describe the theory of light quenching and some of its effects on the steady-state and time-resolved intensity and anisotropy decays of fluorophores. Light quenching can decrease or increase the steady-state or time-zero anisotropy. Remarkably, the light quenching can break the usual z axis symmetry of the excited-state population, and the emission polarization can range from -1 to +1 under selected conditions. The measured anisotropy (or polarization) depends upon whether the observation axis is parallel or perpendicular to the propagation direction of the light quenching beam. The effects of light quenching are different for a single pulse, which results in both excitation and quenching, as compared with a time-delayed quenching pulse. Time-delayed light quenching pulses can result in step-like changes in the time-dependent intensity or anisotropy and are predicted to cause oscillations in the frequency-domain intensity and anisotropy decays. The increasing availability of pulsed laser sources offers the opportunity for a new class of two-pulse or multiple-pulse experiments where the sample is prepared by an excitation pulse, the excited state population is modified by the quenching pulse(s), followed by time- or frequency-domain measurements of the resulting emission.     

Tryptophan fluorescence intensity and anisotropy decays of human serum albumin resulting from one-photon and two-photon excitation.

We measured the emission spectra, intensity decays and anisotropy decays of the single tryptophan residue of human serum albumin (HSA) resulting from one-photon (295-298 nm) and two-photon (590-596) excitation. The emission spectra and intensity decays were independent of the mode of excitation. The anisotropy decays were superficially similar for one- and two-photon excitation. However, upon consideration of the different orientation photoselection for one- and two-photon excitation, the anisotropy data reveal different angles between the absorption and emission oscillators for one-photon and two-photon excitation. This result suggests different relative one-photon and two-photon cross-sections for the 1La and 1Lb transitions of the indole residue. This first report of the time-resolved anisotropy decay of a protein resulting from two-photon excitation suggests that such measurement will yield insights into the complex photophysical properties of tryptophan residues in proteins.     

Effects of polyamines and analogs on staphylococcal nuclease.

The promoting activity of polyamine analogs (IV approximately XV) on staphylococcal nuclease with DNA as the substrate was compared with that of natural polyamines (I APPROXIMATELY III): I. NH2(CH2)3NH(CH2)4NH(CH2)3NH2(spermine); II. NH2(CH2)3NH(CH2)3NH(CH2)3NH2(thermine); III. NH2(CH2)4NH2 (putrescine); IV. CN(CH2)2NH(CH2)4NH(CH2)2CN; V. HOOC(CH2)2NH(CH2)4NH(CH2)2COOH; VI. C2H5OOC(CH2)2NH(CH2)4NH(CH2)2COOC2H5; VII. HO(CH2)3NH(CH2)4HH(CH2)3OH; VIII. CH3COHH(CH2)3NH(CH2)4NH(CH2)3NHCOCH3; IX. C2H5NH(CH2)3NH(CH2)4NH(CH2)3NHC2H5; X. NH2(CH2)3S(CH2)4S(CH2)3NH2; XI. NH2(CH2)3NH(CH2)2O(CH2)2NH(CH2)3NH2; XII. NH2(CH2)3NCH3(CH2)4HCH3(CH2)3NH2; XIII. CN(CH2)2NCH3(CH2)4NCH3(CH2)2CN; XIV. (CH3)2N(CH2)3NCH3(CH2)4NCH3(CH2)3N(CH3)2; XV. NH2(CH2)2O(CH2)2NH2 Replacement of the terminal groups by CN, COOH, COOEt, NHAc, NHEt, or N(CH3)2 remarkably decreased the activity. The compound VII with terminal hydroxyl groups had a lower promoting activity at low concentrations, but revealed higher activity at higher concentrations and, in contrast to spermine, no inhibition at all even at very high concentrations. Replacement of both internal amino groups by sulfur or NCH3 decreased the activity. The introduction of an ether bond into the internal methylene groups (compound XI) highly decreased the activity. Based upon these findings the possible relationship between structure and activity is discussed.     

Guanidine hydrochloride denaturation studies of mutant forms of staphylococcal nuclease

Several mutant forms of staphylococcal nuclease with one or two defined amino acid substitutions have been purified, and the effects of the altered amino acid sequence on the stability of the folded conformation have been analyzed by guanidine hydrochloride denaturation. Two nuc- mutations, which greatly reduced the level of enzyme activity accumulated in E coli colonies carrying a recombinant plasmid with the mutant nuc gene (ie, a NUC- phenotype), both result in protein unfolding at significantly lower guanidine hydrochloride concentrations than the wild-type protein, whereas three sup mutations isolated on the basis of their ability to suppress partially the NUC- phenotype of the above two mutations result in unfolding at significantly higher guanidine hydrochloride concentrations. Characterization of nuclease molecules with two different amino acid substitutions, either nuc- + sup pairs or sup + sup pairs, suggests that the effect of an amino acid substitution on the stability of the native conformation, as measured by the value of delta delta GD, may not be a constant, but rather a variable that is sensitive to the presence of other substitutions at distant sites in the same molecule. Surprisingly, the slopes of the log Kapp vs guanidine hydrochloride concentration plots vary by as much as 35% among the different proteins.     

Effects of proline mutations on the folding of staphylococcal nuclease

Effects of proline isomerizations on the equilibrium unfolding and kinetic refolding of staphylococcal nuclease were studied by circular dichroism in the peptide region (225 nm) and fluorescence spectra of a tryptophan residue. For this purpose, four single mutants (P11A, P31A, P42A, and P56A) and four multiple mutants (P11A/P47T/P117G, P11A/P31A/P47T/P117G, P11A/P31A/P42A/P47T/P117G, and P11A/P31A/P42A/P47T/P56A/P117G) were constructed. These mutants, together with the single and double mutants for Pro47 and Pro117 constructed in our previous study, cover all six proline sites of the nuclease. The P11A, P31A, and P42A mutations did not change the stability of the protein remarkably, while the P56A mutation increased protein stability to a small extent by 0.5 kcal/mol. The refolding kinetics of the protein were, however, affected remarkably by three of the mutations, namely, P11A, P31A, and P56A. Most notably, the amplitude of the slow phase of the triphasic refolding kinetics of the nuclease observed by stopped-flow circular dichroism decreased by increasing the number of the proline mutations; the slow phase disappeared completely in the proline-free mutant (P11A/P31A/P42A/P47T/P56A/P117G). The kinetic refolding reactions of the wild-type protein assessed in the presence of Escherichia coli cyclophilin A showed that the slow phase was accelerated by cyclophilin, indicating that the slow phase was rate-limited by cis-trans isomerization of the proline residues. Although the fast and middle phases of the refolding kinetics were not affected by cyclophilin, the amplitude of the middle phase decreased when the number of the proline mutations increased; the percent amplitudes for the wild-type protein and the proline-free mutants were 43 and 13%, respectively. In addition to these three phases detected with stopped-flow circular dichroism, a very fast phase of refolding was observed with stopped-flow fluorescence, which had a shorter dead time (3.6 ms) than the stopped-flow circular dichroism. The following conclusions were drawn. (1) The effects of the P11A, P31A, and P56A mutations on the refolding kinetics indicate that the isomerizations of the three proline residues are rate-limiting, suggesting that the structures around these residues (Pro11, Pro31, and Pro56) may be organized at an early stage of refolding. (2) The fast phase corresponds to the refolding of the native proline isomer, and the middle phase whose amplitude has decreased when the number of proline mutations was increased may correspond to the slow refolding of non-native proline isomers. The occurrence of the fast- and slow-refolding reactions together with the slow phase rate-limited by the proline isomerization suggests that there are parallel folding pathways for the native and non-native proline isomers. (3) The middle phase did not completely disappear in the proline-free mutant. This suggests that the slow-folding isomer is produced not only by the proline isomerizations but also by another conformational event that is not related to the prolines. (4) The very fast phase detected with the fluorescent measurements suggests that there is an intermediate at a very early stage of kinetic refolding.     

Crystallization and preliminary X-ray analysis of a quadruple mutant of staphylococcal nuclease

A quadruple mutant of staphylococcal nuclease, nuclease (V66L/G79S/G88V/L108V), has been crystallized in a form well suited to moderate-to-high resolution x-ray diffraction analysis. This mutant is highly unstable; only about 20% of the protein in solution at room temperature is in its folded form. Under the crystallization conditions, the protein exhibits circular dichroism properties similar to, but not identical with, those of native wild type protein. The crystals belong to the space group P6(1)22 or P6(5)22 with unit cell dimensions of a = b = 61.1 A, c = 170.1 A and diffract to at least 2.5 A resolution. A data set complete to 3.7 A resolution has been collected and processed; attempts to determine the structure using molecular replacement techniques are under way.     

Fluorescence lifetime studies with staphylococcal nuclease and its site-directed mutant. Test of the hypothesis that proline isomerism is the basis for nonexponential decays.

Using frequency domain methods, the fluorescence decay of Trp-140 in staphylococcal nuclease and its site-directed mutant (Pro-117----Gly) has been examined. Based on nuclear magnetic resonance (NMR) studies (Evans, P. A., C. M. Dobson, R. A. Kautz, G. Hatfull, and R. O. Fox. 1987. Nature [Lond.]. 329:266-268), it is believed that nuclease exists in two macroscopic, native conformations and that the slow interconversion of these conformations is controlled by the cis----trans isomerization of Pro-117. The above mutant shows only one native conformation in NMR experiments. To test the hypothesis that the biexponential fluorescence decay of Trp-140 of nuclease can also be related to the existence of these conformational states of the protein, we have compared the decay patterns of the wild type and mutant. Essentially no difference was observed, which indicates that there is some other basis for the nonexponential decay of Trp-140. We have used global nonlinear least squares analysis to link the fit of data at several temperatures.     

Analysis of fluorescence anisotropy decays by a least square method

A method of fluorescence anisotropy decay analysis is described in this work. The transient anisotropy r(ex)(t) measured in a photocounting pulsefluorimeter is fitted by a non linear least square procedure to the ratio of convolutions of the apparatus response function g(t) by sums of appropriate exponential functions. This method takes rigorously into account the apparatus response function and is applicable to any shape of the later as well as to any values of fluorescence decay times and correlation times. The performances of the method have been tested with data simulated from measured response functions corresponding to an air lamp and a high pressure nitrogen lamp. The statistical standard errors of the anisotropy deca parameters have been found to be smaller than the standard errors previously calculated for the moment method. A systematic error delta in the fluorescence decay time entailed an error deltatheta in the correlation time such as Deltatheta/theta < deltatau/tau. By this method, good fitting of experimental data have been achieved very conveniently and accurately.     

Studies of the unfolding of an unstable mutant of staphylococcal nuclease: Evidence for low temperature unfolding and compactness of the high temperature unfolded state

Fluorescence and circular dichroism data as a function of temperature were obtained to characterize the unfolding of nuclease A and two of its less stable mutants. These spectroscopic data were obtained with a modified instrument that enables the nearly simultaneous detection of both fluorescence and CD data on the same sample. A global analysis of these multiple datasets yielded an excellent fit of a model that includes a change in the heat capacity change, ΔC_p, between the unfolded and native states. This analysis gives a ΔC_p of 2.2 kcal/mol/·K for thermal unfolding of the WT protein and 1.3 and 1.8 kcal/mol/K for the two mutants. These ΔC_p values are consistent with significant population of the cold unfolded state at ∼0°C. Independent evidence for the existence of a cold unfolded state is the observation of a separately migrating peak in size exclusion chromatography. The new chromatographic peak is seen near 0°C, has a partition coefficient corresponding to a larger hydrodynamic radius, and shows a red-shifted fluorescence spectrum, as compared to the native protein. Data also indicate that the high-temperature unfolded form of mutant nuclease is relatively compact. Size exclusion chromatography shows the high temperature unfolded form to have a hydrodynamic radius that is larger than that for the native form, but smaller than that for the urea or pH-induced unfolded forms. Addition of chemical denaturants to the high-temperature unfolded form causes a further unfolding of the protein, as indicated by an increase in the apparent hydrodynamic radius and a decrease in the rotational correlation time for Trp140 (as determined by fluorescence anisotropy decay measurements). Proteins 28:227–240, 1997 © 1997 Wiley-Liss Inc.     

Kinetic and magnetic resonance studies of the glutamate-43 to serine mutant of staphylococcal nuclease

The Glu-43 residue of staphylococcal nuclease has been proposed to function as a general base that facilitates the attack of water on the phosphodiester substrate [Cotton, F. A., Hazen, E. E., & Legg, M. J. (1979) Proc. Natl. Acad. Sci. U.S.A. 76, 2551-2555]. With DNA as substrate, Vmax in the glutamate-43--serine (E43S) mutant enzyme is decreased by 2700-fold at pH 7.4 but only 376-fold at pH 9.9. With the wild-type enzyme, Vmax increases with pH to pH 9.2, above which it becomes less sensitive to further increase in pH, leveling off at pH 9.8. In contrast, Vmax of the E43S mutant continues to rise, first order in [OH-], to pH 9.8. Above pH 10 both activities fall irreversible. Hence the hydroxyl ion can partially replace the effect of Glu-43 on kcat, in accord with the proposed role of Glu-43 as a general base. The inflection point in the curve relating pH to log Vmax of the wild-type enzyme at pH 9.4 may reflect the ionization of a Ca2+-bound water, or of a Lys or Tyr residue at the active site. The activator Ca2+ and the competitive inhibitor Mn2+ bind to the E43S mutant an order of magnitude more weakly than to the wild-type enzyme as detected by kinetics and by direct metal binding studies, and approximately one additional water ligand on Mn2+ is found in the binary Mn2+ complex of the E43S mutant (1.4 +/- 0.2) as compared to that of the wild-type enzyme (0.8 +/- 0.2). These data suggest that Glu-43 coordinates the divalent cation in the binary enzyme-metal complex but dissociates from the metal to create a water binding site and to function as a general base in the ternary enzyme-metal-DNA complex. While a 2-fold weaker binding of DNA to the Ca2+ complex of the E43S mutant than to the wild-type enzyme is found by kinetic studies, an order of magnitude tighter binding of the competitive inhibitor 3',5'-pdTp to the Mn2+ and Ca2+ complexes of E43S is found by direct binding studies. Distances from Co2+ to phosphorus in the ternary enzyme-Co2+-pdTp complexes reveal coordination of only the 5'-phosphate by Co2+ on the wild-type enzyme but coordination of both the 3'- and 5'-phosphates of pdTp on the E43S mutant.(ABSTRACT TRUNCATED AT 400 WORDS)     

Nanosecond fluorescence anisotropy decays of 1,6-diphenyl-1,3,5-hexatriene in membranes

Nanosecond decays of the fluorescence anisotropy, $\text{r}$, were studied for the emission of 1,6-diphenyl-l,3,5-hexatriene (DPH) embedded in a series of mixed multilamellar liposomes containing egg yolk phosphatidylcholine, phosphatidylethanolamine and cholesterol in varying molar ratios, as well as in membranes of intact cells and in virus envelopes.The relative contributions of the fast and the infinitely slow decaying component to the steady-state value, $\text{r}$, of the fluorescence anisotropy were very similar for artifical and biological membranes.Angles, θ, of the cone, by which the motion of the fluorescent molecule is limited, were calculated from the intensity of the infinitely slow decaying anisotropy component and compared with steady-state fluorescence anisotropies and with ‘microviscosities’, 〈η〉. An increase in 〈η〉 from 1.5 to 5.2 P in our systems was accompanied by a decrease in θ from 49° to 30° while the decrease in the mean motional relaxation times, $\text{φ}{}_{\mathrm{<mtext>f</mtext>}}$, of the label molecule was not more than 1 ns and due mainly to changes in the potential, by which the diffusion of DPH in the membrane is restricted. From these observations we conclude that differences in the steady-state fluorescence anisotropy and in ‘microviscosities’ of cholesterol-containing membranes ($\text{r}\text{> 0.15}$) represent changes in the degree of static orientational constraint rather than changes in diffusion rates of the label.     

Structure and dynamics of staphylococcal nuclease mutants as studied by fluorescence quenching techniques

Fluorescence techniques have been used to investigate the effect of mutations on the structure and dynamics of staphylococcal nuclease. An estimate of the accessibility to acrylamide of the enzyme's single tryptophan residue (Trp140) was obtained from the Stern-Volmer constant for fluorescence quenching. This was indicative of a partially buried tryptophan in the wild-type nuclease. Five single-site mutant nucleases (H124L, V66L, G88V, G79S and F76V) and one double mutant (V66L + G88V), with widely differing stabilities to denaturants, gave Stern-Volmer constants which were very similar to that of their parent enzyme. Studies of the temperature- and viscosity-dependence of quenching suggest that access by acrylamide to Trp140 is limited by diffusion rather than by protein structural fluctuations. Lifetime-resolved fluorescence anisotropy studies using steady-state instrumentation suggest that there is very little segmental motion of the Trp140; most of the anisotropy therefore decays due to protein rotation in the solution. Rotational correlation times for several nuclease mutants have been determined and these are very similar to that of the native nuclease. Thus it appears that these substitutions in the primary amino acid sequence, which have significant effects on the stability of the folded proteins, do not cause a significant change in the protein structure or dynamics around Trp140.     

Characterization of the stable, acid-induced, molten globule-like state of staphylococcal nuclease.

Titration of a salt-free solution of native staphylococcal nuclease by HCl leads to an unfolding transition in the vicinity of pH 4, as determined by near- and far-UV circular dichroism. At pH 2-3, the protein is substantially unfolded. The addition of further HCl results in a second transition, this one to a more structured species (the A state) with the properties of an expanded molten globule, namely substantial secondary structure, little or no tertiary structure, relatively compact size as determined by hydrodynamic radius, and the ability to bind the hydrophobic dye 1-anilino-8-naphthalene sulfonic acid. The addition of anions, in the form of neutral salts, to the acid-unfolded state at pH 2 also causes a transition leading to the A state. Fourier transform infrared analysis of the amide I band was used to compare the amount and type of secondary structure in the native and A states. A significant decrease in alpha-helix structure, with a corresponding increase in beta or extended structure, was observed in the A state, compared to the native state. A model to account for such compact denatured states is proposed.     

Interactions of the acid and base catalysts on staphylococcal nuclease as studied in a double mutant.

The mechanism of the phosphodiesterase reaction catalyzed by staphylococcal nuclease is believed to involve concerted general acid-base catalysis by Arg-87 and Glu-43. The mutual interactions of Arg-87 and Glu-43 were investigated by comparing kinetic and thermodynamic properties of the single mutant enzymes E43S (Glu-43 to Ser) and R87G (Arg-87 to Gly) with those of the double mutant, E43S + R87G, in which both the basic and acidic functions have been inactivated. Denaturation studies with guanidinium chloride, CD, and 600-MHz 1D and 2D proton NMR spectra, indicate all enzyme forms to be predominantly folded in absence of the denaturant and reveal small antagonistic effects of the E43S and R87G mutations on the stability and structure of the wild-type enzyme. The free energies of binding of the divalent cation activator Ca2+, the inhibitor Mn2+, and the substrate analogue 3',5'-pdTp show simple additive effects of the two mutations in the double mutant, indicating that Arg-87 and Glu-43 act independently to facilitate the binding of divalent cations and of 3',5'-pdTP by the wild-type enzyme. The free energies of binding of the substrate, 5'-pdTdA, both in binary E-S and in active ternary E-Ca(2+)-S complexes, show synergistic effects of the two mutations, suggesting that Arg-87 and Glu-43 interact anticooperatively in binding the substrate, possibly straining the substrate by 1.6 kcal/mol in the wild-type enzyme. The large free energy barriers to Vmax introduced by the R87G mutation (delta G1 = 6.5 kcal/mol) and by the E43S mutation (delta G2 = 5.0 kcal/mol) are partially additive in the double mutant (delta G1+2 = 8.1 kcal/mol). These partially additive effects on Vmax are most simply explained by a cooperative component to transition state binding by Arg-87 and Glu-43 of -3.4 kcal/mol. The combination of anticooperative, cooperative, and noncooperative effects of Arg-87 and Glu-43 together lower the kinetic barrier to catalysis by 8.1 kcal/mol.     

One- and two-photon excited fluorescence lifetimes and anisotropy decays of green fluorescent proteins

We have used one- (OPE) and two-photon (TPE) excitation with time-correlated single-photon counting techniques to determine time-resolved fluorescence intensity and anisotropy decays of the wild-type Green Fluorescent Protein (GFP) and two red-shifted mutants, S65T-GFP and RSGFP. WT-GFP and S65T-GFP exhibited a predominant approximately 3 ns monoexponential fluorescence decay, whereas for RSGFP the main lifetimes were approximately 1.1 ns (main component) and approximately 3.3 ns. The anisotropy decay of WT-GFP and S65T-GFP was also monoexponential (global rotational correlation time of 16 +/- 1 ns). The approximately 1.1 ns lifetime of RSGFP was associated with a faster rotational depolarization, evaluated as an additional approximately 13 ns component. This feature we attribute tentatively to a greater rotational freedom of the anionic chromophore. With OPE, the initial anisotropy was close to the theoretical limit of 0.4; with TPE it was higher, approaching the TPE theoretical limit of 0.57 for the colinear case. The measured power dependence of the fluorescence signals provided direct evidence for TPE. The general independence of fluorescence decay times, rotation correlation times, and steady-state emission spectra on the excitation mode indicates that the fluorescence originated from the same distinct excited singlet states (A*, I*, B*). However, we observed a relative enhancement of blue fluorescence peaked at approximately 440 nm for TPE compared to OPE, indicating different relative excitation efficiencies. We infer that the two lifetimes of RSGFP represent the deactivation of two substates of the deprotonated intermediate (I*), distinguished by their origin (i.e., from A* or B*) and by nonradiative decay rates reflecting different internal environments of the excited-state chromophore.     

Picosecond resolution of tyrosine fluorescence and anisotropy decays by 2-GHz frequency-domain fluorometry

We extended the technique of frequency-domain fluorometry to an upper frequency limit of 2000 MHz. This was accomplished by using the harmonic content of a laser pulse train (3.76 MHz, 5 ps) from a synchronously pumped and cavity-dumped dye laser. We used a microchannel plate photomultiplier as the detector to obtain the 2-GHz bandwidth. This new instrument was used to examine tyrosine intensity and anisotropy decays from peptides and proteins. These initial data sets demonstrate that triply exponential tyrosine intensity decays are easily recoverable, even if the mean decay time is less than 1 ns. Importantly, the extended frequency range provides good resolution of rapid and/or multiexponential tyrosine anisotropy decays. Correlation times as short as 15 ps have been recovered for indole, with an uncertainty of +/- 3 ps. We recovered a doubly exponential anisotropy decay of oxytoxin (29 and 454 ps), which probably reflects torsional motions of the phenol ring and overall rotational diffusion, respectively. Also, a 40-ps component was found in the anisotropy decay of bovine pancreatic trypsin inhibitor, which may be due to rapid torsional motions of the tyrosine residues and/or energy transfer among these residues. The rapid component has an amplitude of 0.05, which is about 16% of the total anisotropy. The availability of 2-GHz frequency-domain data extends the measurable time scale for fluorescence to overlap with that of molecular dynamics calculations.     

Effects of denaturants at low concentrations on the reversible denaturation of staphylococcal nuclease

Three very unstable mutant forms of staphylococcal nuclease were used to quantitate the change in the apparent equilibrium constant for reversible denaturation (Kapp) as a function of denaturant concentration for a variety of different denaturing solutes. The value of this equilibrium constant in the absence of denaturant (Kapp,0) was determined by renaturation of the mutant proteins with a combination of glycerol and calcium ion, the latter of which binds at the active site in the native conformation. Because Kapp,0 fell in the easily measurable range between 0.1 and 1, the change in Kapp, and thus the change in free energy (delta Gapp), at very low concentrations of denaturants could be accurately measured. With guanidine hydrochloride (GuHCl), the rate of change of the apparent free energy of denaturation with respect to denaturant concentration (d(delta Gapp)/dCGuHCl or mGuHCl) was found to be remarkably constant down to zero denaturant concentration, even though this value was different for each of the three proteins. Unlike GuHCl, urea exhibited a slightly reduced value of d delta Gapp/dCurea at low concentrations. Results with a number of thiocyanate, perchlorate, and iodide salts confirmed that the Hofmeister series holds for concentrations below 0.1 M; that is, with regard to efficacy as a denaturant SCN- greater than ClO4- greater than I- and Li+,NH4+ greater than Na+,K+. However, all of the chaotropic salts analyzed exhibited markedly increased values of d(delta Gapp)/dCsalt at concentrations below 0.2 M. One possible explanation for these large deviations from a linear relationship between delta Gapp and salt concentration is that weak binding or adsorption of chaotropic anions is occurring at a saturable number of sites in hydrophobic regions of the denatured state.     

Nanosecond fluorescence anisotropy decays of 1,6-diphenyl-1,3,5-hexatriene in membranes.

Nanosecond decays of the fluorescence anisotropy, r, were studied for the emission of 1,6-diphenyl-1,3,5-hexatriene (DPH) embedded in a series of mixed multilamellar liposomes containing egg yolk phosphatidylcholine, phosphatidylethanolamine and cholesterol in varying molar ratios, as well as in membranes of intact cells and in virus envelopes. The relative contributions of the fast and the infinitely slow decaying component to the steady-state value r, of the fluorescence anisotropy were very similar for artifical and biological membranes. Angles, theta, of the cone, by which the motion of the fluorescent molecule is limited, were calculated from the intensity of the infinitely slow decaying anisotropy component and compared with steady-state fluorescence anisotropies and with 'microviscosities', (eta). An increase in (eta) from 1.5 to 5.2 P in our systems was accompanied by a decrease in theta from 49 degrees to 30 degrees while the decrease in the mean motional relaxation times, phi f, of the label molecule was not more than 1 ns and due mainly to changes in the potential, by which the diffusion of DPH in the membrane is restricted. From these observations we conclude that differences in the steady-state fluorescence anisotropy and in 'microviscosities' of cholesterol-containing membranes (r greater than 0.15) represent changes in the degree of static orientational constraint rather than changes in diffusion rates of the label.     

Thermal unfolding of staphylococcal nuclease and several mutant forms thereof studied by differential scanning calorimetry.

The effects of eight mutations on the thermodynamics of the reversible thermal unfolding of staphylococcal nuclease have been determined over a range of pH and protein concentration by means of differential scanning calorimetry. Variation of the protein concentration was included in our study because we found a significant dependence of the thermodynamics of protein unfolding on concentration. Values for the change in the standard free energy of unfolding, delta delta G0d, produced by the mutations in the pH range 5.0-7.0 varied from 1.9 kcal mol-1 (apparent stabilization) for H124L to -2.8 kcal mol-1 (apparent destabilization) for L25A. As has been observed in numerous other cases, there is no correlation in magnitude or sign between delta delta G0d and the corresponding values for delta delta Hd and T delta delta S0d, the latter quantities being in most cases much larger in magnitude than delta delta G0d. This fact emphasizes the difficulty in attempting to correlate the thermodynamic changes with structural changes observed by X-ray crystallography.