Conformational distributions of melittin in water/methanol mixtures from frequency-domain measurements of nonradiative energy transfer

We used fluorescence energy transfer to examine the effects of solvent composition on the distribution of distances between the single tryptophan residue of melittin (residue 19) to the N-terminal alpha-amino group, which was labeled with a dansyl residue. The tryptophan intensity decays, with and without the dansyl acceptor, were measured by the frequency-domain method. The data were analyzed by a least-squares algorithm which accounts for correlation between the parameters. A wide distribution of tryptophan to dansyl distances was found for the random-coil state, with a Gaussian half-width of 25 A. Increasing concentrations of methanol, which were shown to induce and alpha-helical conformation, resulted in a progressive decrease in the width of the distribution, reaching a limiting half-width of 3 A at 80% (v/v) methanol. The distance from the indole moiety of Trp-19 to the dansyl group in 80% (v/v) methanol/water was found to be 25 A, as assessed from the center of the distance distribution. A distance of 24-25 A was recovered from the X-ray crystal structure of the tetramer, which is largely alpha-helical. At low ionic strength (less than 0.01) the CD spectra revealed a small fraction or amount of alpha-helix for melittin in water, which implies a small fraction of residual structure. This residual structure is apparently lost in guanidine hydrochloride as demonstrated by a further broadening in the distribution of distances. These results demonstrate the usefulness of frequency-domain measurements of resonance transfer for resolution of conformational distributions of proteins.     

Time-resolved emission spectra of hemoglobin on the picosecond time scale

We used front-face illumination to examine the steady-state and time-resolved emission from the intrinsic tryptophan emission of human hemoglobin (Hb). Experimental conditions were identified which eliminated all contributions of scattered light. The sensitivity obtained using front-face optics was adequate to allow measurement of the wavelength-dependent frequency response of the emission to 2 GHz. The intensity decays displayed pico- and nanosecond components in the emission at all wavelengths from 315 to 380 nm. The contribution of the picosecond component decreased from 72 to 37% over this range of wavelengths. Frequency-domain measurements were used to calculate the time-resolved emission spectra and decay-associated emission spectra. These spectra indicate that the picosecond components of the emission display maxima near 320 nm, whereas the nanosecond components are centered at longer wavelengths near 335 nm. The nanosecond components appear to be due to residual impurities which remain even in highly purified samples of Hb. However, we cannot eliminate the possibility that some of these components are due to Hb itself.     

Measurement of subnanosecond anisotropy decays of protein fluorescence using frequency-domain fluorometry

We report the first anisotropy decays of protein fluorescence obtained using a frequency-domain fluorometer. The ultraviolet light source (300 nm) was a ring dye laser equipped with an intracavity frequency doubler, pumped by an argon ion laser. The data, measured at modulation frequencies from 2 to 200 MHz, reveal the presence of subnanosecond motions (0.1-0.2 ns) of the single tryptophan residues in melittin and monellin. For melittin the data also indicate the presence of slower motions near 1 ns, which may be the result of concerted motions of several peptide units. Smaller amplitude motions, on a similar timescale, were observed for the single tryptophan residue in staphylococcal nuclease. We demonstrate using N-acetyl-L-tryptophanamide in water that the method of frequency-domain fluorometry is capable of measuring correlation times as short as 50 ps. This method can provide data for the direct comparison of measured anisotropy decays with those predicted from molecular dynamics calculations.     

Analysis of fluorescence decay kinetics from variable-frequency phase shift and modulation data.

Recently it has become possible to measure fluorescence phase-shift and modulation data over a wide range of modulation frequencies. In this paper we describe the analysis of these data by the method of nonlinear least squares to determine the values of the lifetimes and fractional intensities for a mixture of exponentially decaying fluorophores. Analyzing simulated data allowed us to determine those experimental factors that are most critical for successfully resolving the emissions from mixtures of fluorophores. The most critical factors are the accuracy of the experimental data, the relative difference of the individual decay times, and the inclusion of data measured at multiple emission wavelengths. After measuring at eight widely spaced modulation frequencies, additional measurements yielded only a modest increase in resolution. In particular, the uncertainty in the parameters decreased approximately as the reciprocal of the square root of the number of modulation frequencies. Our simulations showed that with presently available precision and data for one emission bandpass, two decay times could be accurately determined if their ratio were greater than or equal to 1.4. Three exponential decays could also be resolved, but only if the range of the lifetimes were fivefold or greater. To reliably determine closely-spaced decay times, the data were measured at multiple emission wavelengths so that the fractional intensities of the components could be varied. Also, independent knowledge of any of the parameters substantially increased the accuracy with which the remaining parameters could be determined. In the subsequent paper we present experimental results that broadly confirm the predicted resolving potential of variable-frequency phase-modulation fluorometry.     

Resolution of mixtures of fluorophores using variable-frequency phase and modulation data

We measured fluorescence phase shift and modulation data for one-, two- and, three-component mixtures of fluorophores at modulation frequencies ranging from 1 to 140 MHz. These data were analyzed using the least-squares procedure described in the preceding paper (Lakowicz, J. R., G. Laczko, M. Cherek, E. Gratton, and M. Limkeman, 1984, Biophys. J., 46:463-477). Using data obtained at a single emission bandpass, the lifetimes and preexponential factors of two-component mixtures could be easily resolved if the lifetimes differed by a factor of 2. With currently available instrumental stability, three-component mixtures could be resolved when the overall range of decay times was 10-fold, (e.g., 1.3, 4.4, and 12 ns). Measurement of phase and modulation data at several emission wavelengths, where the ratio of the preexponential factors varied, enhanced our ability to resolve closely spaced two and three-component decays. Two-component mixtures could then be resolved if the lifetimes differed by 30% (4.4 and 6.2 ns). Also, the multiple-wavelength data allowed the lifetimes and emission spectra of the three-components of a mixture to be resolved. These results demonstrated that resolution of multiexponential decay laws was possible using frequency-domain phase-modulation fluorometry.     

Fractionation and characterization of rapidly phosphorylated nuclear proteins in salivary gland cells of Chironomus tentans

Rapidly phosphorylated nuclear proteins were investigated in explanted salivary gland cells of Chironomus tentans after labeling with ³²P_i. After sonication nuclei were fractionated by centrifugation at 18,000 g into sedimentable (80% of ³²P) and not sedimentable (supernatant) material. About 90% of ³²P in the supernatant fraction was sedimentable at 100,000 g (disperse chromatin). The disperse chromatin contained 20%–40% of the total nuclear DNA but only 5%–20% of ³²P. The ³²P-labeled phosphoproteins in the material pelleted at 20,000 g were further fractionated by differential solubility in lysis buffer. Electrophoretic analyses on SDS polyacrylamide gels resolved the ³²P-labeled nuclear proteins into 12 major bands in the M_r range of 12,000–120,000. The incorporation of ³²P into most bands reached a steady-state within 5–10 min of incubation with ³²P_i and was not measurably influenced by cycloheximide, an inhibitor of protein synthesis. The phosphate groups are linked to polypeptide chains by bonds vulnerable to pronase and alkaline phosphatase. All major bands in the pelleted chromatin were also present in the disperse chromatin except for an M_r 95,000 phosphoprotein. Two of the fastest moving ³²P-bands comigrated with the core histones H2A and H4. Both possessed a high pI value and were insoluble in 0.35 M NaCl. The H2A-like protein was partially soluble in lysis buffer while the H4-like one was not. The two fast moving ³²P-labeled bands with rapidly turned over phosphates may be fractions or variants of the core histones H2A and H4.     

87Rb, 23Na and 31P nuclear magnetic resonance spectroscopy of the perfused rat kidney

87Rb, 23Na and 31P nuclear magnetic resonance (NMR) were used to monitor changes in renal cations and energetics during the induction of hypoxia in the isolated perfused rat kidney. The NMR-determined unidirectional Rb+ flux in normoxic kidneys was shown to be a good measure of net intracellular K+ influx in the perfused rat kidney model. The changes in 87Rb, 23Na and 31P spectra following the induction of hypoxia are consistent with hypoxic depletion of intracellular adenosine triphosphate (ATP) and a subsequent decrease in Na-K-ATPase transport activity. The exponential rate constant for 87Rb+ efflux measured during Rb+ uptake in normoxic kidneys (0.12 +/- 0.01 min-1) was not significantly different to the rate constant for 87Rb+ efflux during the induction of hypoxia (0.16 +/- 0.07 min-1). We conclude that there is no direct effect of hypoxia on renal cellular membrane integrity and that renal cell sensitivity to hypoxia is due to an inability to sustain cellular ion gradients following depletion of intracellular ATP.     

Sedimentation velocity of sodium hyaluronate-lysozyme mixtures

A study of the sedimentation behaviour of lysozyme in sodium hyaluronate (Na-HA) solution and of the Na-HA medium itself, has been carried out to determine whether the strongly basic enzyme lysozyme forms complexes with Na-HA at physiological ionic strength. At typical physiological salt concentration, 0.146 m NaCl, and also in 0.100 M NaCl, lysozyme sedimentation in an Na-HA solution can be adequately described as independent sedimentation of a slightly associated protein through a three-dimensional network acting partially as a macromolecular sieve. The s_20,w of lysozyme when determined in 0.146 M NaCl, indicated partial aggregation of the enzyme at this salt concentration. Decreases in sedimentation coefficients of lysozyme with increase in Na-HA concentration show a pronounced sieving effect by the equality of observed sedimentation coefficient of lysozyme and Na-HA at higher Na-HA concentrations, but typically individual sedimentation coefficients when the macromolecular mixture was diluted approximately ten-fold.