Homogeneous model immunoassay of thyroxine by phase-modulation fluorescence spectroscopy

We describe a homogeneous competitive model immunoassay for determination of thyroxine by multifrequency phase-modulation fluorescence. Using a nonradiative energy transfer transduction mechanism, B-phycoerythrin conjugated to thyroxine is the energy donor and a carboxymethylindocyanine dye conjugated to anti-thyroxine antibody is the energy acceptor. Energy transfer from B-phycoerythrin to the acceptor results in a decreased lifetime and/or phase angle. The fluorescence lifetime change reflects the extent of energy transfer. In the competitive immunoassay format, the donor-thyroxine conjugate and an analytical sample of thyroxine compete for acceptor-antibody binding sites, resulting in a phase angle change which is dependent on the amount of thyroxine in the sample. Dose-response curves of phase angle versus thyroxine concentration are comparable to steady-state intensity curves. Since phase-modulation lifetime measurements are largely independent of total signal intensity, sources of optical interference are minimized. The potential for whole blood measurements exists since the energy transfer lifetime method can be extended to longer wavelengths.

Styryl-based wavelength-ratiometric probes: a new class of fluorescent calcium probes with long wavelength emission and a large Stokes' shift

We describe the chemical synthesis and fluorescence spectral characterization of a styryl-benzothiazole probe which contains the Ca2+ chelating group BAPTA as an integral part of the chromophoric system. The visible absorption spectrum of this probe displays a dramatic shift in the long wavelength maxima from 508 to 407 nm upon complexation with Ca2+, with a Ca2+ dissociation constant of 1.5 microM. The emission maximum centered at 615 nm is well shifted from the absorption. The emission spectrum displays a small blue shift upon binding Ca2+, allowing this probe to possibly be used as an emission wavelength-ratiometric probe using a single-excitation wavelength. This probe is likely to be the first of a series of long-wavelength ratiometric Ca2+ probes whose structure can be modified for improved quantum yield or altered Ca2+ affinity.

Time-resolved energy transfer measurements of donor-acceptor distance distributions and intramolecular flexibility of a CCHH zinc finger peptide

Time-resolved frequency-domain fluorescence energy transfer measurements have been used to investigate the solution structure of a single-domain CCHH-type zinc finger peptide. These measurements reveal not only the range of accessible distances for a given donor-acceptor pair within the molecule but also the degree of conformational flexibility that occurs in solution. Two donor-acceptor (D-A)-pair zinc finger peptides have been synthesized. A single tryptophan residue located at the midpoint of the sequence was the energy donor for two different acceptors. One acceptor, attached at the amino terminus was a 5-(dimethylamino)-1-naphthalenesulfonyl (DNS) group; the second acceptor was a 7-amino-4-methyl-coumarin-3-acetyl (AMCA) group, attached to the epsilon-amino function of a carboxy-terminal lysine residue. Distance distributions and the mutual site-to-site diffusion coefficients were determined for these two D-A-labeled peptides under zinc-bound, metal-free, and denatured conditions. The D-A distance distributions determined for these two peptides under metal-free and zinc-bound conditions indicated a shorter distance and a unique conformation (narrow distribution) when metal was bound and a longer distance with greater conformational flexibility when metal ion was absent. No site-to-site diffusion was detected for the zinc-bound peptide, whereas an appreciable amount of diffusion was measured for both metal-free and denatured peptide. Anisotropy measurements on the peptides indicated increased flexibility of all regions of the peptide chain in the absence of zinc and a more compact, less flexible structure when zinc was bound. It was concluded from these results that the metal-bound conformation represents a unique, well-defined structure. Comparison of distance distributions measured for metal-free and denatured peptide indicated that there is some residual structure present in the metal-free peptide.

Intensity and anisotropy decays of [Leu5] enkephalin tyrosyl fluorescence by 10 GHz frequency-domain fluorometry

The technique of 10 GHz frequency-domain fluorometry was used to resolve the complex picosecond intensity and anisotropy decays of the tyrosyl emission of [Leu5] enkephalin. Enhanced resolution of anisotropy decay was obtained by using acrylamide quenching of the tyrosyl fluorescence and global analysis of the frequency-domain anisotropy data obtained with different amounts of acrylamide. The data indicates a 44 ps correlation time for local tyrosine motions, and a 219 ps correlation time for overall rotational diffusion of the pentapeptide. Our data are consistent with an initial loss of fluorescence anisotropy from r0 = 0.4 to a value of r0 = 0.326 occurring during the first two picoseconds after excitation.

Optical measurements of pH using fluorescence lifetimes and phase-modulation fluorometry

We measured the pH-dependent fluorescence decay times of the seminaphthofluoresceins (SNA-FL), seminaphthorhodafluors (SNARF), and BCE-CF using phase-modulation fluorometry. The phase and modulation values were found to be strongly pH-dependent in the physiological pH range, over the easily accessible range of light modulation frequencies from 10 to 300 MHz, making these probes useful as lifetime-based pH sensors. The phase and modulation values are dependent on excitation and emission wavelength as well as pH. This dependence allows the range of pH sensitivity to be chosen by selection of the wavelength(s) and enables increased precision of the pH measurements by use of phase and/or modulation measurements at several wavelengths. These probes can be excited using a a green He-Ne laser at 543 nm, which allows their use in low cost instrumentation. Phase and modulation measurements are especially suitable for sensing applications because they are insensitive to the changes in signal intensity that result from photobleaching, probe washout, and/or light losses.

Characterization of p-bis(O-methylstyryl)benzene as a lifetime and anisotropy decay standard for two-photon induced fluorescence

We describe the fluorescence spectral properties of p-bis(O-methylstyryl)benzene (bis-MSB) as a standard for time-resolved measurements of two-photon induced fluorescence. Bis-MSB displays the same single exponential intensity decay in several solvents for one- and two-photon excitation. The anisotropy decay displays the same single correlation time of one- and two-photon excitation. The amplitudes of the anisotropy decay are distinct for one- and two-photon excitation. At some excitation wavelengths the anisotropy amplitude appears to be solely the result of one- and two-photon photoselection, but at shorter wavelengths the anisotropy amplitudes are not related by single constant factor. The absorption range of bis-MSB makes it a suitable standard for one- and two-photon excitation of intrinsic protein fluorescence and extrinsic fluorophores.

End-to-end diffusion coefficients and distance distributions from fluorescence energy transfer measurements: enhanced resolution by using multiple acceptors with different Förster distances

We measured distance distributions and end-to-end diffusion coefficients of donor-acceptor pairs linked by a flexible methylene chain using frequency-domain fluorescence energy transfer measurements. The donor was an indole group, and two acceptors with different Förster distances were used. The uncertainties in the recovered parameters describing the end-to-end distance distribution and diffusion coefficient were rather large when each donor-acceptor pair was analyzed separately. It was not possible to resolve distance distributions in the presence of intra-molecular diffusion when the Förster distance was comparable to the mean and half-width of the distribution. Global analysis using two acceptors dramatically improved the resolution. Surprisingly, the Förster distances need not be very different, and a 20% difference between the two R0 values resulted in substantial improvements in resolution. Both the simulations and the experiments suggest the benefit of using global analysis with different Förster distances to obtain reliable distance distribution parameters in the presence of diffusion.

Phase-resolved fluorescence lifetime measurements for flow cytometry

A flow cytometer capable of measuring fluorescence lifetimes by the phase shift method has been built and evaluated. Under optimal conditions, the resolution of the fluorescence lifetime measurement is shown to be under 200 picoseconds. Pulse intensity variations are normalized using limiting amplifiers and electronic filtering. Normalization of signal intensities provides a lifetime measurement that is independent of fluorescence intensity over at least a 50-fold (17 dB) range in fluorescence intensity. The fluorescence lifetimes of unbound dye, fluorescent beads, cells stained with ethidium bromide, propidium iodide, and phycoerythrin-conjugated monoclonal antibodies have been measured. The fluorescence lifetimes measured for these particles are well correlated with lifetime measurements made using a standard fluorimeter. Cells stained with ethidium bromide and propidium iodide at various nucleotide-to-dye ratios are shown to exhibit similar behavior to static cuvette measurements. The fluorescence lifetime parameter is also shown to resolve phycoerthyrin fluorescence from propidium iodide fluorescence.

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.

Frequency domain imaging of absorbers obscured by scattering

Multiple pixel, frequency domain measurements of phase shift, theta, and modulation, m, in a phantom containing an absorber obscured by a relatively non-absorbing scattering solution are presented in combination with a theory of photon migration imaging. Results employing a single point source show that two dimensional theta measurements made in the presence (theta presence) and in the absence (theta absence) of an absorber can be used to create delta theta images. delta theta (theta absence-theta presence) images can be used to detect as well as locate the three dimensional position of the absorber. Images of mpresence measured in the presence of the absorber normalized by mabsence also provided detection and two dimensional location of its position. Images of % mpresence/mabsence at higher modulation frequencies provided greater resolution as predicted by photon migration theory. Neither theta nor m images alone could be used to detect or locate the presence of the absorber.

Fluorescence lifetime imaging

We describe a new fluorescence imaging methodology in which the image contrast is derived from the fluorescence lifetime at each point in a two-dimensional image and not the local concentration and/or intensity of the fluorophore. In the present apparatus, lifetime images are created from a series of images obtained with a gain-modulated image intensifier. The frequency of gain modulation is at the light-modulation frequency (or a harmonic thereof), resulting in homodyne phase-sensitive images. These stationary phase-sensitive images are collected using a slow-scan CCD camera. A series of such images, obtained with various phase shifts of the gain-modulation signal, is used to determine the phase angle and/or modulation of the emission at each pixel, which is in essence the phase or modulation lifetime image. An advantage of this method is that pixel-to-pixel scanning is not required to obtain the images, as the information from all pixels is obtained at the same time. The method has been experimentally verified by creating lifetime images of standard fluorophores with known lifetimes, ranging from 1 to 10 ns. As an example of biochemical imaging we created life-time images of Yt-base when quenched by acrylamide, as a model for a fluorophore in distinct environments that affect its decay time. Additionally, we describe a faster imaging procedure that allows images in which a specific decay time is suppressed to be calculated, allowing rapid visualization of unique features and/or regions with distinct decay times. The concepts and methodologies of fluorescence lifetime imaging (FLIM) have numerous potential applications in the biosciences. Fluorescence lifetimes are known to be sensitive to numerous chemical and physical factors such as pH, oxygen, temperature, cations, polarity, and binding to macromolecules. Hence the FLIM method allows chemical or physical imaging of macroscopic and microscopic samples.

Time-Resolved Fluorescence Intensity and Anisotropy Decays of 2,5-Diphenyloxazole by Two-Photon Excitation and Frequency-Domain Fluorometry

We report the first time-resolved fluorescence measurements of the intensity and anisotropy decays resulting from two-photon excitation. A 10-GHz frequency-domain fluorometer (Rev. Sci. Instrum 1990, 61, 2331), equipped with two focal lenses and an emission monochromator, was used for steady-state and time-resolved measurements of PPO fluorescence. The emission spectra and the intensity decays observed with single- and two-photon excitation were essentially identical. The steady-state limiting anisotropy r 0 of PPO in glycerol at -5 °C measured for two-photon excitation is significantly higher than that observed for one-photon excitation. The r 0 value of 0.54 for two-photon excitation is well in excess of the theoretical maximum of 0.4 for single-photon excitation. A similar value of r 0 ≃ 0.50 was obtained from the frequency-domain anisotropy data with two-photon excitation of PPO in methanol, butanol, and propylene glycol at 20 °C. These higher values of r 0 indicate that two-photon excitation results in a more highly oriented photoselected population, which can increase the resolution of rotational correlation times and/or complex anisotropy decays. The anisotropy resolution can still be increased by using global analysis of anisotropy decays measured with single- and two-photon excitation.

Electroluminescent lamp-based phase fluorometer and oxygen sensor

We have tested 454-nm violet-emitting solid state electroluminescent lamps (ELLs) as inexpensive intensity-modulated excitation light sources for phase fluorometric oxygen sensors. Compared with blue-emitting silicon carbide LEDs, planar surface ELLs can be produced in various shapes and in large sizes. Accordingly, the overall optical output power emitted by ELLs is much higher than that of blue LEDs. By arranging a large-size ELL close to a large-size fluorescent chemical sensor, we obtained a large number of fluorescence photons allowing for the use of a pin photodiode instead of a photomultiplier tube as the detector. For a sinusoidal driving voltage at a frequency f, the ELL output light is modulated at 2f and at harmonics of 2f. Because of this nonlinear modulation characteristic, we used a square wave driving signal, resulting in a pulsed light output at a repetition rate twice the square wave frequency. The shortest light pulses obtained had a FWHM close to about 1 microsecond. This means that the violet ELLs used in our tests provide modulation frequencies at twice the square wave driving frequency and at all harmonics thereof up to about 1 MHz. This would allow the use of fluorescent chemical sensors with decay times as short as 30 ns, assuming that a phase shift of 10 degrees is adequate for the application. Due to the high ELL driving voltage, effective shielding is required to avoid electromagnetic interference between the modulated light source and the photodetector. Depending on the driving frequency and voltage applied, the ELLs showed a decrease in the optical output power to 50 or even 10% during the first 100 h of operation.

Fluorescence lifetime imaging of calcium using Quin-2

We describe the use of a new imaging technology, fluorescence lifetime imaging (FLIM), for the imaging of the calcium concentrations based on the fluorescence lifetime of a calcium indicator. The fluorescence lifetime of Quin-2 is shown to be highly sensitive to [Ca2+]. We create two-dimensional lifetime images using the phase shift and modulation of the Quin-2 in response to intensity-modulated light. The two-dimensional phase and modulation values are obtained using a gain-modulated image intensifier and a slow-scan CCD camera. The lifetime values in the 2D image were verified using standard frequency-domain measurements. Importantly, the FLIM method does not require the probe to display shifts in the excitation or emission spectra, which may allow Ca2+ imaging using other Ca2+ probes not in current widespread use due to the lack of spectral shifts. Fluorescence lifetime imaging can be superior to stationary (steady-state) imaging because lifetimes are independent of the local probe concentration and/or intensity, and should thus be widely applicable to chemical imaging using fluorescence microscopy.

Fluorescence lifetime imaging of free and protein-bound NADH

We introduce a methodology, fluorescence lifetime imaging (FLIM), in which the contrast depends on the fluorescence lifetime at each point in a two-dimensional image and not on the local concentration and/or intensity of the fluorophore. We used FLIM to create lifetime images of NADH when free in solution and when bound to malate dehydrogenase. This represents a challenging case for lifetime imaging because the NADH decay times are just 0.4 and 1.0 ns in the free and bound states, respectively. In the present apparatus, lifetime images are created from a series of phase-sensitive images obtained with a gain-modulated image intensifier and recorded with a charge-coupled device (CCD) camera. The intensifier gain is modulated at the light-modulation frequency or a harmonic thereof. A series of stationary phase-sensitive images each obtained with various phase shifts of the gain-modulation signal, is used to determine the phase angle or modulation of the emission at each pixel, which is in essence the lifetime image. We also describe am imaging procedure that allows specific decay times to be suppressed, allowing in this case suppression of the emission from either free or bound NADH. Since the fluorescence lifetimes of probes are known to be sensitive to numerous chemical and physical factors such as pH, oxygen, temperature, cations, polarity, and binding to macromolecules, this method allows imaging of the chemical or property of interest in macroscopic and microscopic samples. The concept of FLIM appears to have numerous potential applications in the biosciences.

Frequency-domain reflectance for the determination of the scattering and absorption properties of tissue

Measurements of the phase and modulation of amplitudemodulated light diffusely reflected by turbid media can be used to deduce absorption and scattering coefficients.

Resolution of end-to-end diffusion coefficients and distance distributions of flexible molecules using fluorescent donor-acceptor and donor-quencher pairs

We used time-dependent fluorescence energy transfer, time-dependent collisional quenching, and global analysis of the data resulting from these through-space and contact interactions to recover the end-to-end distance distributions and diffusion coefficients of flexible fluorescent molecules. The fluorescence decays of covalently linked tryptamine-acceptor and tryptamine-quencher pairs were measured by the frequency-domain method. These data were fit using numerical solutions of the differential equation, which predicts the time- and distance-dependent population of the excited state donors in the presence of energy transfer or collisional quenching, followed by transformation to the frequency domain for nonlinear least-squares comparison with the experimental data. We found that the energy transfer data for the donor-acceptor pair alone were adequate to recover the starting distribution and the end-to-end diffusion coefficient; however, the resolution is dramatically improved by the use of both the through-space and contact interactions.

Effects of temperature on the fluorescence intensity and anisotropy decays of staphylococcal nuclease and the less stable nuclease-conA-SG28 mutant

Frequency-domain fluorescence spectroscopy was used to investigate the effects of temperature on the intensity and anisotropy decays of the single tryptophan residues of Staphylococcal nuclease A and its nuclease-conA-SG28 mutant. This mutant has the beta-turn forming hexapeptide, Ser-Gly-Asn-Gly-Ser-Pro, substituted for the pentapeptide Tyr-Lys-Gly-Gln-Pro at positions 27-31. The intensity decays were analyzed in terms of a sum of exponentials and with Lorentzian distributions of decay times. The anisotropy decays were analyzed in terms of a sum of exponentials. Both the intensity and anisotropy decay parameters strongly depend on temperature near the thermal transitions of the proteins. Significant differences in the temperature stability of Staphylococcal nuclease and the mutant exist; these proteins show characteristic thermal transition temperatures (Tm) of 51 and 30 degrees C, respectively, at pH 7. The temperature dependence of the intensity decay data are shown to be consistent with a two-state unfolding model. For both proteins, the longer rotational correlation time, due to overall rotational diffusion, decreases dramatically at the transition temperature, and the amplitude of the shorter correlation time increases, indicating increased segmental motions of the single tryptophan residue. The mutant protein appears to have a slightly larger overall rotational correlation time and to show slightly more segmental motion of its Trp than is the case for the wild-type protein.

Structural perturbation of the transmembrane region interferes with calcium binding by the Ca2+ transport ATPase

The Ca(2+)-ATPase of sarcoplasmic reticulum reacts with N-cyclohexyl-N'-(4-dimethylamino-1-naphthyl) carbodiimide (NCD4) yielding a fluorescence labeling that interferes with calcium binding to activating and transport sites of the enzyme and, thereby, with Ca(2+)-dependent ATPase activity. On the other hand, the catalytic site does not appear altered, as revealed by the normal occurrence of Ca(2+)-independent reactions, such as enzyme phosphorylation with Pi in the reverse direction of the catalytic cycle. This reaction is not inhibited by Ca2+ in the labeled enzyme, while it is inhibited in the native enzyme. The NCD4 reaction which is involved in functional inactivation occurs in the membrane-bound portion of the ATPase. Sodium dodecyl sulfate solubilization of hydrophobic peptides, electrophoresis, and microsequencing of transblotted electrophoretic bands revealed that the fluorescent NCD4 label resides in a segment of tryptic fragment A1, intervening between Glu231 and Glu309. This segment includes two transmembrane helices, and does not include the domain involved in the phosphoryl transfer reaction during catalytic activity. This specific labeling does not occur when the NCD4 derivatization procedure is carried out in the presence of Ca2+ concentrations that also prevent functional inactivation. Fluorescence characterization by steady state and intensity decay measurements shows only negligible energy transfer between the NCD4 label and fluorescein isothiocyanate label of Lys515, indicating that the NCD4 label is unlikely to reside within the extramembranous region of the ATPase. On the other hand, the fluorescence emission of intrinsic tryptophan residues clustered within or near the transmembrane region of the ATPase, is distinctly affected by NCD4 label specifically bound to the ATPase, and NCD4 label nonspecifically bound to the sarcoplasmic reticulum membrane. The combined sequencing and spectroscopic observations indicate that derivatization with NCD4 induces a perturbation within or near the transmembrane region of the ATPase (at a relatively large distance from the catalytic site) that interferes with specific calcium binding. This is in agreement with experiments (Clarke et al., 1989) demonstrating that mutations of any of six amino acids within the transmembrane region of the ATPase interfere with enzyme activation by Ca2+.

Correction for incomplete labeling in the measurement of distance distributions by frequency-domain fluorometry

Measurements of time-resolved fluorescence are now being used to recover conformational distributions of biological macromolecules. The fluorescence data of the donor are easily corrupted by incomplete labeling of the macromolecules by the acceptor. In the present paper we describe a general procedure to correct for incomplete acceptor labeling in the determination of distance distributions from frequency-domain measurements of the donor fluorescence decay kinetics. The method can also be used to determine the extent of acceptor labeling. Simulated data were used to determine the effect of incomplete labeling on resolution of the distance distribution and the effect on the recovered distributions if one fails to account for incomplete labeling by the acceptor. The expressions and implemented algorithm were verified using known mixtures of donor-control and donor-acceptor pair molecules, which simulated the presence of a donor population lacking the acceptor. Finally, we present data on the distance distributions between two labeled sites in myosin S1 (Cys-697 to Cys-707) where it was not possible to obtain complete labeling of the acceptor site.

Distance distributions and anisotropy decays of troponin C and its complex with troponin I

We used frequency domain measurements of fluorescence resonance energy transfer to recover the distribution of distances between Met 25 and Cys 98 in rabbit skeletal troponin C. These residues were labeled with dansylaziridine as energy donor and 5-(iodoacetamido)eosin as acceptor and are located on the N- and C-terminal lobes of the two-domain protein, respectively. We developed a procedure to correct for the fraction of the sample that was incompletely labeled with the acceptor independent of chemical data. At pH 7.5 and in the presence of Mg2+, the mean distance was near 15 A with a half-width of the distribution of 15 A; when Mg2+ was replaced by Ca2+, the mean distance increased to 22 A with a decrease in the half-width by 4 A. Similar but less pronounced differences in the mean distance and half-width between samples containing Mg2+ and Ca2+ were also observed with troponin C complexed to troponin I. The results suggest that the conformation of troponin C is altered by Ca2+ binding to the Ca(2+)-specific sites and displacing bound Mg2+ at the Ca2+/Mg2+ sites. This alteration may play an important role in Ca2+ signaling in muscle. At pH 7.5, the anisotropy decays of the donor-labeled troponin C showed two components, with the long rotational correlation time (12 ns) reflecting the overall motion of the protein. When the pH was lowered from 7.5 to 5.2, the mean distribution distance of apotroponin C increased from 22 to 32 A and the half-width decreased by a factor of 2 from 13 to 7 A. The long correlation time of apotroponin C increased to 19 ns at the acidic pH. These results are discussed in terms of a model in which skeletal troponin C is a dimer at low pH and enable comparison of the solution conformation of the protein at neutral pH with a crystal structure obtained at pH 5.2. While the conformation of the monomeric unit of troponin C dimer at pH 5.2 is extended and consistent with the crystal structure, the conformation at neutral pH is likely more compact than the crystal structure predicts.

Conformational flexibility of the Cys 697-Cys 707 segment of myosin subfragment-1. Distance distributions by frequency-domain fluorometry

The separation between Cys 697 (SH1) and Cys 707 (SH2) of the heavy chain of myosin subfragment-1 was previously measured by fluorescence resonance energy transfer with a donor linked to SH1 and an acceptor to SH2. In the present study the distribution of the distances between the two thiols was recovered from frequency-domain fluorometry. In the native state and in the presence of ligands such as MgADP, pyrophosphate, orthovanadate (Vi) and actin, we found wide distributions of the separations between SH1 and SH2 (11-16 A) comparable to that found in the random-coil state (20 A). These results suggest that the SH1-SH2 segment has a high degree of conformational flexibility even in native S1. The flexibility is not much affected by the physiological state of S1. However, the ligands MgADP, Vi and MgADP + Vi decrease significantly the mean SH1-SH2 distance from 27 to 17 A with the effect of MgADP+ Vi being the most pronounced. The anisotropy decay of donor-labeled S1 is biphasic with two rotational correlation times. The long component is decreased by these ligands from 289 to 93 ns, suggesting a more compact symmetric structure of S1 in the presence of the ligands. The complex S1(MgADP)Vi has been shown to be a stable analogue of S1(MgADP)Pi, an unstable intermediate that is generated in the actomyosin ATPase cycle during muscle contraction. Since the power stroke of muscle is accompanied by release of Pi from S1(MgADP)Pi, the present results are consistent with a model in which force generation can be accompanied by transition of S1 from a highly symmetric or compact structure to a more extended structure.

Resolution of phospholipid conformational heterogeneity in model membranes by spin-label EPR and frequency-domain fluorescence spectroscopy

We have utilized both fluorescent and nitroxide derivatives of stearic acid as probes of membrane structural heterogeneity in phospholipid vesicles under physiological conditions, as well as conditions of varying ionic strengths and temperatures where spectral heterogeneity has been previously observed and attributed to multiple ionization states of the probes. To identify the source of this spectral heterogeneity, we have utilized complimentary measurements of the relaxation properties (lifetimes) and motion of both (a) spin labeled and anthroyloxy derivatives of stearic acid (i.e., SASL and AS) and (b) a diphenylhexatriene derivative of phosphatidylcholine (DPH-PC) in single component membranes containing dimyristoylphosphatidylcholine (DMPC). We use an 15N stearic-acid spin label for optimal sensitivity to membrane heterogeneity. The lifetime and dynamics of the fluorescent phospholipid analogue DPH-PC (with no ionizable groups over this pH range) were compared with those of AS, allowing us to discriminate between changes in membrane structure and the ionization of the label. The quantum yield and rotational dynamics of DPH-PC are independent of pH, indicating that changes in pH do not affect the conformation of the host phospholipids. However, both EPR spectra of SASL and the lifetime or dynamics of AS are affected profoundly by changes in solution pH. The apparent pKa's of these two probes in DMPC membranes were determined to be near pH 6.3, implying that at physiological pH and ionic strength these stearic-acid labels exist predominantly as a single ionized population in membranes. Therefore, the observed temperature- and ionic-strength-dependent alterations in the spectra of SASL as well as the lifetime or dynamics of AS in DMPC membranes at neutral pH are due to changes in membrane structure rather than the ionization of the probes. The possibility that ionic gradients across biological membranes induce alterations in phospholipid structures, thereby modulating lipid-protein interactions is discussed.

Resolution of the conformational distribution and dynamics of a flexible molecule using frequency-domain fluorometry

We report the first resolution of both the conformational distribution and end-to-end diffusion coefficient of a flexible molecule. This molecular information was recovered using only the donor intensity decay in a single solvent at a single viscosity, as observed by the technique of frequency-domain fluorometry. This technique can be extended to measurements of structural fluctuations of biological macromolecules.

A 4-GHz frequency-domain fluorometer with internal microchannel plate photomultiplier cross-correlation

We have developed and tested a multifrequency phase/modulation fluorometer based on the Hamamatsu Model R2024U gatable microchannel plate photomultiplier (MCP-PMT), using internal MCP-PMT cross-correlation. This internal mixing is accomplished by biasing and modulating the gating mesh which is located 0.2 mm behind the photocathode. Near the photocathode center, no high-frequency photocurrent modulation was achieved. Within a circular area near the photocathode edge, however, the R2024U allows accurate phase shift and demodulation measurements up to at least 4.5 GHz, the frequency limit of our PMT-modulation amplifier. By mixing immediately after the photocathode, there is no decrease in the time resolution due to transit time spread, and the MCP has to process only low-frequency signals. This means no low-level high-frequency signal voltages have to be handled in this fluorometer, and the problems of RF shielding become much less critical. Also, the effective output impedance of the PMT has been increased, resulting in a 43-dB increase in the PMT output signal power. In principle, more MCPs could be built into the PMT, allowing an improved fluorescence detection limit. We have used the method of reference fluorophores in order to compensate for pronounced PMT color effects, a wavelength-dependent modulation, and a wavelength-dependent time shift. No color correction is required in the case of time-dependent depolarization. The performance of the instrument was verified by measurements of the intensity decay of perylene, which showed a single-exponential decay, and by measurements of the decay of tryptophan in water, which showed a double-exponential decay, as expected.(ABSTRACT TRUNCATED AT 250 WORDS)