Non-use of cancer information services among people experiencing cancer in Ireland.

PURPOSE: The purpose of this study was to explore the reasons for non-use of a national cancer society's cancer information services among people experiencing cancer. METHOD: This study used a qualitative design. Semi-structured interviews were conducted with a total of 17 participants who had not previously utilised the Cancer Society's information services. Data were analysed using Thematic Analysis. RESULTS: The key themes to emerge from the date were 'living in the here and now' and 'awareness of the Cancer Society'. For most participants, not utilising cancer information services was a means of coping with the initial diagnosis and the impact of treatment. Those who progressed to being ready to seek information identified the multi-disciplinary team as the primary source of trusted information, with particular mention of cancer nurse specialists. For participants with children, their role as a parent was central in how they managed their diagnosis. The majority of participants lacked awareness of the range of services provided by the Cancer Society. CONCLUSIONS: Reasons for non-use of cancer information services were identified as: readiness to seek information and a lack of knowledge of the Cancer Societies' services. Cancer information services need to continue make a concerted effort to enhance visibility and awareness of its services to optimise patient engagement.

ESR determination of membrane order parameter in yeast sterol mutants.

ESR investigations designed to determine membrane order parameter in sterol mutants of Saccharomyces cerevisiae were conducted using the membrane probe, 5-doxyl stearic acid. These mutants are blocked in the ergosterol biosynthetic pathway and thus do not synthesize ergosterol, the end product sterol. They do not require exogenous ergosterol for growth and, therefore, incorporate ergosterol biosynthetic intermediates in their membrane. Increasing order parameter is reflective of an increase in membrane rigidity. Single mutants involving B-ring delta 8 leads to delta 7 isomerization (erg 2) and C-24 methylation (erg 6) showed greater membrane rigidity than wild-type during exponential growth. A double mutant containing both lesions (erg 6/2) showed an even greater degree of membrane rigidity. During stationary phase the order of decreasing membrane rigidity was erg 6 greater than erg 6/2 greater than erg 2 = wild-type. The increased membrane order parameter was attributed to the presence of substituted sterols rather than increased sterol content or altered fatty acid synthesis.

Structure-fluorescence correlations in a single tryptophan mutant of carp parvalbumin: solution structure, backbone and side-chain dynamics.

Heterogeneous fluorescence intensity decays of tryptophan in proteins are often rationalized using a model which proposes that different rotameric states of the indole alanyl side-chain are responsible for the observed fluorescence lifetime heterogeneity. We present here the study of a mutant of carp parvalbumin bearing a single tryptophan residue at position 102 (F102W) whose fluorescence intensity decay is heterogeneous and assess the applicability of a rotamer model to describe the fluorescence decay data. We have determined the solution structure of F102W in the calcium ligated state using multi-dimensional nuclear magnetic resonance (NMR) and have used the minimum perturbation mapping technique to explore the possible existence of multiple conformations of the indole moiety of Trp102 of F102W and, for comparison, Trp48 of holo-azurin. The maps for parvalbumin suggest two potential conformations of the indole side-chain. The high energy barrier for rotational isomerization between these conformers implies that interwell rotation would occur on time-scales of milliseconds or greater and suggests a rotamer basis for the heterogeneous fluorescence. However, the absence of alternate Trp102 conformers in the NMR data (to within 3 % of the dominant species) suggests that the heterogeneous fluorescence of Trp102 may arise from mechanisms independent of rotameric states of the Trp side-chain. The map for holo-azurin has only one conformation, and suggests a rotamer model may not be required to explain its heterogeneous fluorescence intensity decay. The backbone and Trp102 side-chain dynamics at 30 degrees C of F102W has been characterized based on an analysis of (15)N NMR relaxation data which we have interpreted using the Lipari-Szabo formalism. High order parameter (S(2)) values were obtained for both the helical and loop regions. Additionally, the S(2) values imply that the calcium binding CD and EF loops are not strictly equivalent. The S(2) value for the indole side-chain of Trp102 obtained from the fluorescence, NMR relaxation and minimum perturbation data are consistent with a Trp moiety whose motion is restricted.

Reactive oxygen species cause endothelial dysfunction in chronic flow overload.

Although elevation of shear stress increases production of vascular reactive oxygen species (ROS), the role of ROS in chronic flow overload (CFO) has not been well investigated. We hypothesize that CFO increases ROS production mediated in part by NADPH oxidase, which leads to endothelial dysfunction. In six swine, CFO in carotid arteries was induced by contralateral ligation for 1 wk. In an additional group, six swine received apocynin (NADPH oxidase blocker and anti-oxidant) treatment in conjunction with CFO for 1 wk. The blood flow in carotid arteries increased from 189.2 ± 25.3 ml/min (control) to 369.6 ± 61.9 ml/min (CFO), and the arterial diameter increased by 8.6%. The expressions of endothelial nitric oxide synthase (eNOS), p22/p47(phox), and NOX2/NOX4 were upregulated. ROS production increased threefold in response to CFO. The endothelium-dependent vasorelaxation was compromised in the CFO group. Treatment with apocynin significantly reduced ROS production in the vessel wall, preserved endothelial function, and inhibited expressions of p22/p47phox and NOX2/NOX4. Although the process of CFO remodeling to restore the wall shear stress has been thought of as a physiological response, the present data implicate NADPH oxidase-produced ROS and eNOS uncoupling in endothelial dysfunction at 1 wk of CFO.

Tryptophan sidechain dynamics in hydrophobic oligopeptides determined by use of 13C nuclear magnetic resonance spectroscopy.

Two oligopeptides, t-boc-LAWAL-OMe and t-boc-LALALW-OMe, were synthesized for the purpose of examining the sidechain dynamics of the tryptophan residue in hydrophobic environments by 13C nuclear magnetic resonance and fluorescence spectroscopy. In both peptides, the tryptophan sidechain was greater than 95% enriched with 13C at the C delta 1 position. Spin-lattice relaxation time (T1) and steady-state nuclear Overhauser effect (NOE) data were obtained at 50.3 and 75.4 MHz for both peptides in CD3OD, and at 75.4 MHz for t-boc-LALALW-OMe in lysolecithin-D2O micelles. We have adapted the model-free approach of G. Lipari and A. Szabo (1982, J. Am. Chem. Soc. 104:4546) to interpret the 13C-NMR data. Computer-generated curves based on experimental data obtained at a single frequency demonstrate relationships between an effective correlation time for tryptophan sidechain motion (tau e), a generalized order parameter (sigma) describing the extent of motional restriction, and an overall correlation time for the peptide (tau m). Assuming predominantly dipolar relaxation, least-squares fits of the dual frequency relaxation data provide values for these parameters for both peptides. The contribution of chemical shift anisotropy (CSA), however, is also explicitly assessed in the data analysis, and is shown to perturb the predicted sigma, tau e, and tau m values and to decrease chi(2) values observed in nonlinear least-squares analysis of the data. Because of uncertainty in the contribution of CSA to the relaxation of the indole ring 13C delta 1 atom, nonlinear least-squares analysis of the relaxation data were performed with and without inclusion of a CSA term in the appropriate relaxation equations. Neglecting CSA, an overall peptide correlation time of 0.69 ns is predicted for t-boc-LAWAL-OMe in CD3OD at 20 degrees C compared with 1.28 ns for t-boc-LALALW-OMe. Given these tau m values and taking into account the effect of measurement error in the T1 and NOE data, the internal dynamics of the tryptophan residue of t-boc-LAWAL-OMe in this isotropic environment are described by a range of tau e values from 70 to 112 ps and sigma values between 0.22 and 0.36. Similarly, for t-boc-LALALW-OMe, 68 less than or equal to tau e less than or equal to 93 ps and 0.09 less than or equal to sigma less than or equal to 0.17. The Ch-terminal position of the tryptophan residue in the hexapeptide may account for its lower order parameter. In lysolecithin micelles, the model-free approach applied tot-boc-LALALW-OMe predicts a Te between 0.87 and 1.08 ns, and an order parameter range of 0.72-0.80, assuming an average Tm of 14 ns (Saunders, L. 1966. Biochim. Biophys. Acta. 125:70) for a typical peptide-micelle complex. In this case, measurement of only two 13C relaxation parameters at a single frequency yields sufficient information, plotted in the form of a composite T1-NOE solution curve, to constrain the allowed values of the model-free motional parameters within a relatively narrow range. The predicted range of eV and Te values for the peptide-micelle complex demonstrate that both the rate and spatial mobility of the indole moiety are markedly restrained in the anisotropic micelle environment relative to free methanol solution. Steady-state fluorescence anisotropy measurements made on the peptides dissolved in methanol or with synthetic lysolecithins in water were used to calculate apparent order parameters for tryptophan motion; these values agree well with order parameters calculated from 13C NMR data. The reported results are relevant to the issue of protein dynamic events occurring on the picosecond time scale predicted by molecular dynamics simulations.

Characterization of selectively 13C-labeled synthetic melittin and melittin analogues in isotropic solvents by circular dichroism, fluorescence, and NMR spectroscopy.

The spectroscopic and functional characterization of 13C-labeled synthetic melittin and three analogues is described. Selectively 13C-enriched tryptophan ( [13C delta 1]-L-Trp) and glycine ( [13C alpha]Gly) were incorporated into melittin and three analogues by de novo peptide synthesis. 13C-Labeled tryptophan was incorporated into melittin at position 19 and into single-tryptophan analogues of melittin at positions 17, 11, and 9, respectively. Each of the synthetic peptides contained 13C-labeled glycine at position 12 only. The peptides were characterized functionally in a cytolytic assay, and spectroscopically by CD, fluorescence, and NMR. The behavior of 13C-labeled synthetic melittin was, in all respects, indistinguishable from that of the naturally occurring peptide. All of the analogues were found to be efficient lytic agents and thus were functionally similar to the native peptide, yet no evidence was found for formation of a melittin-like tetramer by any of the analogues in aqueous media, although there was a propensity for apparently nonspecific peptide aggregation, especially for MLT-W9. Since the analogues did exhibit fractional helicities by CD comparable to or even greater than melittin itself in the presence of methanol, we infer that tetramer assembly requires not only the ability to form alpha-helix but also a very precise packing of amino acid side chains of the constituent monomers. The 13C chemical shift of the Gly-12 C alpha was found to be a sensitive marker for helix formation in all of the peptides. For melittin itself, 13C NMR spectra revealed a downfield shift of approximately 1.8 ppm for the Gly-12 13C alpha resonance of the tetramer relative to that observed for the free monomer in D2O. In mixed samples containing melittin monomer and tetramer, two discrete Gly-12 13C alpha peaks were observed simultaneously, suggestive of slow exchange between the two species. We conclude that melittin's ability to form a soluble tetramer is not a prerequisite for cytolytic activity, nor is cytolytic potential precisely correlated with the ability to form an amphiphilic helix.

Fluorescence and 13C NMR determination of side-chain and backbone dynamics of synthetic melittin and melittin analogues in isotropic solvents.

The dynamics in isotopic solvents of selectively 13C labeled synthetic melittin and three analogues have been investigated by using NMR and fluorescence techniques both separately and in combination. In conjunction with the "model-free" approach to interpretation of NMR relaxation data [Lipari, G., & Szabo, A. (1982) J. Am. Chem. Soc. 104, 4546-4570], the availability of steady-state fluorescence anisotropy and lifetime data augment T1, T2, and NOE data to provide quantitative information about fluorophore dynamics in these peptides. A method is presented for using combined fluorescence and NMR data to obtain technique- and model-independent values for parameters describing local motion of 13C-labeled fluorophores in peptides and proteins. The dynamics of melittin and melittin analogues are found to be consistent with structural characteristics inferred from CD, fluorescence, and NMR spectral information presented in the preceding paper (Weaver et al., 1989). In particular, the mobility of the random coil peptide monomers is shown to be quite similar, while side-chain as well as peptide backbone motion in the aggregated or oligomeric species differs markedly among the analogues. For melittin itself, experimentally determined overall rotational correlation times for the monomer and tetramer agree very well with values predicted on the basis of solvent-accessible protein surface area. The local dynamics of selectively 13C-labeled Trp-19 and Gly-12 residues of melittin are also found to be consistent with peptide structure. In random coil melittin monomer, a specific model for the motion indicates that the Trp side chain moves through an approximate angle of +/- 71 degrees about the beta-gamma bond with a correlation time of 159 +/- 24 ps. In melittin tetramer, the indole moiety is spatially more confined with a flip angle of +/- 37 degrees, yet demonstrates an increased rate of motion with a correlation time of 56 +/- 8 ps. The constrained mobility of the Trp-19 side chain is consistent with motional constraints inferred from the X-ray structure of melittin tetramer. These results show that protein side-chain motion, even of moieties as large as indole, can occur on the picosecond time scale and that these motions are reasonably similar to those inferred from molecular dynamics simulations.

Comparison of 15N- and 13C-determined parameters of mobility in melittin.

Backbone and tryptophan side-chain mobilities in the 26-residue, cytolytic peptide melittin (MLT) were investigated by 15N and 13C NMR. Specifically, inverse-detected 15N T1 and steady-state NOE measurements were made at 30 and 51 MHz on MLT at 22 degrees C enriched with 15N at six amide positions and in the Trp19 side chain. Both the disordered MLT monomer (1.2 mM peptide at pH 3.6 in neat water) and alpha-helical MLT tetramer (4.0 mM peptide at pH 5.2 in 150 mM phosphate buffer) were examined. The relaxation data were analyzed in terms of the Lipari and Szabo model-free formalism with three parameters: tau m, the correlation time for the overall rotation; S2, a site-specific order parameter which is a measure of the amplitude of the internal motion; and tau e, a local, effective correlation time of the internal motion. A comparison was made of motional parameters from the 15N measurements and from 13C measurements on MLT, the latter having been made here and previously [Kemple et al. (1997) Biochemistry, 36, 1678-1688]. tau m and tau e values were consistent from data on the two nuclei. In the MLT monomer, S2 values for the backbone N-H and C alpha-H vectors in the same residue were similar in value but in the tetramer the N-H order parameters were about 0.2 units larger than the C alpha-H order parameters. The Trp side-chain N-H and C-H order parameters, and tau e values were generally similar in both the monomer and tetramer. Implications of these results regarding the dynamics of MLT are examined.

Main chain and side chain dynamics of peptides in liquid solution from 13C NMR: melittin as a model peptide.

Peptide backbone and lysine and tryptophan side chain mobilities in the synthetic, 26-residue peptide melittin (MLT) enriched with 13C were investigated in liquid solution by 13C T1 and steady state nuclear Overhauser effect measurements at two magnetic fields and by Trp fluorescence anisotropy measurements and were analyzed using the Lipari and Szabo model-free approach. The overall rotational correlation times at 20 degrees C were 1.28, 1.4, 2.8, and 4.2 ns for monomeric random coil MLT, for monomeric helical MLT (in CD3OD), for tetrameric MLT in neat D2O, and for the tetramer in 50 mM phosphate buffer, respectively. Motion of the backbone in the interior of the sequence was most restricted in the monomeric helix and least restricted in the tetramer. In the monomeric disordered peptide, relatively less restricted backbone motion extending from the N terminus to the fourth residue was observed. Such "end effects" continued only to the third residue in the monomeric helix and were observed just in the amino terminus glycine in the tetramer. The three Lys side chains showed the least restricted motion in the monomers and a differential restriction in the tetramers consistent with the tetramer structure. The motion of the Trp side chain was more restricted than that of Lys side chains and generally as restricted as that of the interior backbone atoms. The effective correlation times for the local motion of the backbone atoms were in the motional narrowing limit and showed distinct patterns. Agreement between NMR relaxation and Trp fluorescence anisotropy data was good for the monomer but not for the tetramer. Implications of these results for peptide dynamics in general are examined.

Fluorescence, CD, attenuated total reflectance (ATR) FTIR, and 13C NMR characterization of the structure and dynamics of synthetic melittin and melittin analogues in lipid environments.

The structure and dynamics of synthetic melittin (MLT) and MLT analogues bound to monomyristoylphosphatidylcholine micelles, dimyristoylphosphatidylcholine vesicles, and diacylphosphatidylcholine films have been investigated by fluorescence, CD, attenuated total reflectance (ATR) FTIR, and 13C NMR spectroscopy. All of these methods provide information about peptide secondary structure and/or about the environment of the single tryptophan side chain in these lipid environments. ATR-FTIR data provide additional information about the orientation of helical peptide segments with respect to the bilayer plane. Steady-state fluorescence anisotropy, fluorescence lifetime, and 13C NMR relaxation data are used in concert to provide quantitative information about the dynamics of a single 13C-labeled tryptophan side chain at position 19 in lipid-bound MLT, and at positions 17, 11, and 9, respectively, in lipid-bound MLT analogues. Peptide chain dynamics are probed by NMR relaxation studies of 13C alpha-labeled glycine incorporated into each of the MLT peptides at position 12. The cumulative structural and dynamic data are consistent with a model wherein the N-terminal alpha-helical segment of these peptides is oriented perpendicular to the bilayer plane. Correlation times for the lysolipid-peptide complexes provide evidence for binding of a single peptide monomer per micelle. A model for the membranolytic action of MLT and MLT-like peptides is proposed.

Structure and dynamics of melittin in lysomyristoyl phosphatidylcholine micelles determined by nuclear magnetic resonance.

Mixed micelles of the 26-residue, lytic peptide melittin (MLT) and 1-myristoyl-2-hydroxyl-sn-glycero-3-phosphocholine (MMPC) in aqueous solution at 25 degrees C were investigated by (13)C- and (31)P-NMR spectroscopy. (13)C alpha chemical shifts of isotopically labeled synthetic MLT revealed that MLT in the micelle is predominantly alpha-helical and that the peptide secondary structure is stable from pH 4 to pH 11. Although the helical transformation of MLT as determined from NMR is evident at lipid:peptide molar ratios as low as 1:2, tryptophan fluorescence measurements demonstrate that well-defined micellar complexes do not predominate until lipid:peptide ratios exceed 30:1. (31)P linewidth measurements indicate that the interaction between phosphate ions in solution and cationic groups on MLT is pH dependent, and that the phosphoryl group of MMPC senses a constant charge, most likely +2, on MLT from pH 4 to pH 10. (13)C-NMR relaxation data, analyzed using the model-free formalism, show that the peptide backbone of MLT is partially, but not completely, immobilized in the mixed micelles. Specifically, order parameters (S(2)) of C alpha-H vectors averaged 0.7 and were somewhat larger for residues in the N-terminal half of the molecule. The amino terminal glycine had essentially the same range of motion as the backbone carbons. Likewise, order parameters for the trp side chain were similar to those found for the peptide C alpha moieties, as was verified by trp fluorescence anisotropy decay data. In contrast, the motion of the lysine side chains was less restricted, the average S(2) values for the C epsilon-H vectors being 0.19, 0.30, and 0.44 for lys-7, 21, and 23, respectively, for MLT in the mixed micelles. Values of the effective correlation time of the local motion tau e were in the motional narrowing limit and usually longer for side-chain atoms than for those in the backbone. The dynamics were independent of pH from pH 4 to pH 9, but at pH 11 the correlation time for the rotational motion of the mixed micelles as a whole increased from 10 ns to 16 ns, and S(2) for the lys side chains increased. Overall it appears that the MLT helix lies near the surface of the micelle at low to neutral pH, but at higher pH its orientation changes, accompanied by deeper penetration of the lysine side chains into the micelle interior. It is apparent, however, that the MLT-lipid interaction is not dependent on deprotonation of any of the titratable cationic groups in the peptide in the pH 4-10 range, and that there is substantial backbone and side-chain mobility in micelle-bound MLT.

Dynamics of palmitic acid complexed with rat intestinal fatty acid binding protein.

Dynamics of palmitic acid (PA), isotopically enriched with 13C at the second, seventh, or terminal methyl position, were investigated by 13C NMR. Relaxation measurements were made on PA bound to recombinant rat intestinal fatty acid binding protein (I-FABP) at pH 5.5 and 23 degreesC, and, for comparison, on PA incorporated into 1-palmitoyl-2-hydroxy-sn-glycero-3-phosphocholine (MPPC) micelles, and dissolved in methanol. The 13C relaxation data, T1, and steady-state nuclear Overhauser effect (NOE) obtained at two different magnetic fields were interpreted using the model-free approach [Lipari, G., and Szabo, A. (1982) J. Am. Chem. Soc. 104, 4546-4559]. The overall rotational correlation time of the fatty acid.protein complex was 2.5 +/- 0.4 ns, which is substantially less than the value expected for the protein itself (>6 ns). Order parameters (S2), which are a measure of the amplitude of the internal motion of individual C-H vectors with respect to the PA molecule, while largest for C-2 and smallest for the methyl carbon, were relatively small (<0.4) in the protein complex. S2 values for given C-H vectors also were smaller for PA in the MPPC micelles and in methanol than in the protein complex. Correlation times reflective of the time scale of the internal motion of the C-H vectors were in all cases <60 ps. These results support the view that the fatty acid is not rigidly anchored within the I-FABP binding pocket, but rather has considerable freedom to move within the pocket.

N-terminus and lysine side chain pKa values of melittin in aqueous solutions and micellar dispersions measured by 15N NMR.

Melittin (MLT) is a 26-amino acid cytolytic peptide from the Apis mellifera honey bee. It is known to exist as an alpha-helical tetramer, as an alpha-helical monomer, or as a monomeric random coil depending on solvent conditions. The charge state of MLT is believed to be a major factor in determining its aggregation properties and its interaction with lipids. Several, contradictory, indirect measurements of the pKa values of the three lysine groups in MLT have been reported. In the present study, high-resolution 15N NMR at 50.6 MHz was used to directly measure the pKa values of the amino groups of the Gly-1, Lys-7, Lys-21, and Lys-23 residues of MLT. Specifically, the pH dependence of MLT 15N chemical shifts was measured separately for the isotopically enriched backbone nitrogen of Gly-1 and the side chain nitrogen atoms of Lys-7, Lys-21, and Lys-23 at a MLT concentration of 1.2 mM and a temperature of 23 degrees C. Measurements were made for MLT in potassium phosphate buffer, in neat water, and in 1-myristoyl-2-hydroxyl-sn-glycero-3-phosphocholine (MMPC) lipid micelles. The experiments showed for MLT tetramer in aqueous phosphate buffer that the amino nitrogen of Gly-1 has a pKa of 8.15, and that the Lys-7, Lys-21, and Lys-23 side chain nitrogen atoms have pKa values of 10.21, 10.03, and 10.24 respectively.(ABSTRACT TRUNCATED AT 250 WORDS)

13C alpha-NMR assignments of melittin in methanol and chemical shift correlations with secondary structure.

Melittin is a naturally occurring hexacosa peptide which forms an amphiphilic helix in methanol, a random coil in water, and a tetramer of helices at basic pH or in the presence of a high salt concentration. The monomeric structure in methanol has been well characterized by proton NMR (Pastore et al. (1989) Eur. Biophys. J., 16, 363-367). In the present paper, chemical shifts of the backbone alpha-carbons of melittin in methanol were determined by mapping previously published alpha-proton shifts (Bazzo et al. (1988) Eur. J. Biochem., 173, 139-146), to natural abundance (1H)13C cross peaks appearing in the 2D heteronuclear multiple-quantum NMR spectrum. Changes in chemical shifts consequent to stepwise increases in the percentage of water in a mixed methanol/water solvent system were observed in similar spectra. The alpha-carbon shifts varied more smoothly than the corresponding alpha-proton shifts and were found to correlate with the transition from the helix to the random coil conformer in parallel with changes in the circular dichroism spectrum. Chemical shifts of this peptide are interpreted with regard to the current database of assignments in proteins of known 3D structure (Wishart et al. (1991) J. Mol. Biol., 222, 311-333). The N-terminal region of the peptide shows increased flexibility at lower methanol concentrations, as evidenced by the merger of the alpha-proton resonances of G1 (at 40% and 15% methanol) and G3 (at 15% methanol). Conformational exchange rates for G1 and G3 were estimated by comparison of the experimental spectra with simulated spectra and found to be as large as 4000 s-1 for G1 in 40% and 15% methanol and 600 s-1 for G3 in 15% methanol. Overall, these 1H and 13C chemical shift data support the description of monomeric melittin in methanol currently evolving in the literature and suggest a structure composed of a linked pair of helices with different structural stabilities, each of which experiences dynamical fraying at its free terminus.

Electron paramagnetic resonance spectroscopy of Cu2+ in hen egg-white lysozyme.

We have obtained the electron paramagnetic resonance spectrum of Cu2+ bound in a tetragonal single crystal of hen egg-white lysozyme. A part of this spectrum has been shown to originate from Cu2+ ions bound at the site designated as B by Teichberg et al. [Teichberg, V.I., Sharon, N., Moult, J., Smilansky, A. & Yonath, A. (1974) J. Mol. Biol. 87, 357-368]. The values of the spin hamiltonian parameters that describe this part of the spectrum are reported. The implications of these values with respect to the chemical nature and configuration of ligands are discussed. The other features of the spectrum are also described.

Electron paramagnetic resonance of spin-labeled aequorin.

Aequorin is a Ca-activated bioluminescent protein from jellyfish. This protein contains two sulfhydryl groups, one of which is essential for its bioluminescence. Little information concerning the structure of and relationship between the metal binding sites of aequorin and the sulfhydryl group(s) is known. Aequorin was modified by attachment of either a maleimide spin-label [studied by electron paramagnetic resonance (EPR)] or the fluorescent label Acrylodan at the essential sulfhydryl in order to gain such information. These modifications caused destabilization of the chromophore of aequorin. Both of the attached labels showed considerable freedom of motion. The spin-label was quite accessible to the solvent, and the fluorescent label was less so. In addition the metal binding properties of the spin-labeled aequorin were studied by Mn(II) EPR. One tight Mn(II) binding site per spin-labeled aequorin was found. The distance between the Mn(II) binding site and the spin-label is at least 20 A. Furthermore, the relative affinity of spin-labeled aequorin for various metal ions was found to be in the order Pr(III) greater than Mn(II) greater than Ca(II) greater than Mg(II).

Mn(II)-EPR measurements of cation binding by aequorin.

Cation binding at 5 degrees C by aequorin, a bioluminescent protein from the jellyfish Aequorea victoria, was examined by means of Mn(II) EPR. The bioluminescence of aequorin is triggered by Ca(II), as well as by trivalent lanthanides, and is inhibited by Mg(II) and Mn(II). Three EF-hand Ca(II)-binding domains have been identified in the aequorin amino acid sequence. In the work reported here, active native aequorin was found to have a single tight binding site for Mn(II) with an association constant of 0.566 microM-1. Ca(II) and La(III) competed for the Mn(II) site with association constants of 1.92 microM-1 and 1.38 microM-1, respectively. The affinity of Ca(II) and La(III) for their two other (presumed) sites on aequorin was an order of magnitude less than their affinity for the Mn(II) site. Mg(II) competed for the Mn(II) site as well but with a much smaller association constant of 0.0109 microM-1. Ca(II)-independent discharged aequorin did not bind Mn(II) to a significant degree. Conjectures on the location of the Mn(II) site in the aequorin amino acid sequence and on the relationship between the binding parameters of the cations and their influence on aequorin activity are given.

Proton NMR of aequorin. Structural changes concomitant with calcium-independent light emission.

Aequorin, a Ca(II)-sensitive bioluminescent protein from jellyfish, emits light at 469 nm from an excited state of a substituted pyrazine (oxyluciferin) which results from the oxidation of a chromophore molecule that is noncovalently bound to the protein. The chromophore is oxidized when Ca(II) or other activating metal ions are bound by aequorin. In the absence of Ca(II), spontaneous emission of light, referred to as Ca(II)-independent light emission, occurs at a rate less than 10(-6) of that for Ca(II)-induced emission. Proton nuclear magnetic resonance (NMR), circular dichroism (CD), and fluorescence were used to study structural changes of aequorin accompanying Ca(II)-independent light emission. Time course studies by 1H NMR and CD demonstrate that as a result of Ca(II)-independent light emission, aequorin progressively changes from a rigid, fully active form showing little segmental mobility to a practically unfolded, discharged (i.e., inactive) form in which a number of amino acid residues are significantly mobile. This slow discharged protein (SDP) is distinct in nature and conformation from aequorin which has been discharged by Ca(II), i.e., the blue fluorescent protein. The rate of Ca(II)-independent discharge of aequorin is substantially reduced in the presence of excess Mg(II); the time constant for inactivation at 5 degrees C is 30 days with no Mg(II) present and 70 days with Mg(II) present. The NMR spectra are nearly identical at a given stage of inactivation whether or not Mg(II) is present. Oxyluciferin remains bound to SDP. If it is removed, however, by column chromatography, the resulting apo-SDP partially refolds, and the segmental mobility acquired in the formation of SDP is significantly attenuated particularly for some of the aromatic amino acid residues.

13C NMR and fluorescence analysis of tryptophan dynamics in wild-type and two single-Trp variants of Escherichia coli thioredoxin.

The rotational motion of tryptophan side chains in oxidized and reduced wild-type (WT) Escherichia coli thioredoxin and in two single-tryptophan variants of E. coli thioredoxin was studied in solution in the temperature range 20-50 degrees C from 13C-NMR relaxation rate measurements at 75.4 and 125.7 MHz and at 20 degrees C from steady-state and time-resolved trp fluorescence anisotropy measurements. Tryptophan enriched with 13C at the delta 1 and epsilon 3 sites of the indole ring was incorporated into WT thioredoxin and into two single-trp mutants, W31F and W28F, in which trp-28 or trp-31 of WT thioredoxin was replaced, respectively, with phenylalanine. The NMR relaxation data were interpreted using the Lipari and Szabo "model-free" approach (G. Lipari and A. Szabo. 1982. J. Amer. Chem. Soc. 104:4546-4559) with trp steady-state anisotropy data included for the variants at 20 degrees C. Values for the correlation time for the overall rotational motion (tau m) from NMR of oxidized and reduced WT thioredoxin at 35 degrees C agree well with those given by Stone et al. (Stone, M. J., K. Chandrasekhar, A. Holmgren, P. E. Wright, and H. J. Dyson. 1993. Biochemistry. 32:426-435) from 15N NMR relaxation rates, and the dependence of tau m on viscosity and temperature was in accord with the Stokes-Einstein relationship. Order parameters (S2) near 1 were obtained for the trp side chains in the WT proteins even at 50 degrees C. A slight increase in the amplitude of motion (decrease in S2) of trp-31, which is near the protein surface, but not of trp-28, which is partially buried in the protein matrix, was observed in reduced relative to oxidized WT thioredoxin. For trp-28 in W31F, order parameters near 1 (S2 > or = 0.8) at 20 degrees C were found, whereas trp-31 in W28F yielded the smallest order parameters (S2 approximately 0.6) of any of the cases. Analysis of time-resolved anisotropy decays in W28F and W31F yielded S2 values in good agreement with NMR, but gave tau m values about 60% smaller. Generally, values of tau e, the effective correlation time for the internal motion, were < or = 60 ps from NMR, whereas somewhat longer times were obtained from fluorescence. The ability of NMR and fluorescence techniques to detect subnanosecond motions in proteins reliably is examined.

Photochemically-induced dynamic nuclear polarization proton-NMR of aequorin discharged by calcium-independent light emission.

Photochemically-induced dynamic nuclear polarization was used to identify exposed amino-acid residues and to assign resonances in the 1H-NMR spectrum of Ca(II)-independent discharged (inactivated) aequorin. A previous nuclear magnetic resonance, circular dichroism and fluorescence study [Ray, B.D., Ho, S., Kemple, M. D., Prendergast, F. G. and Nageswara Rao, B.D. (1985) Biochemistry 24, 4280-4287] indicated that as the Ca(II)-activated bioluminescent protein aequorin from jellyfish spontaneously emits light in the absence of Ca(II), it changes from a rigid, fully active form to a discharged form in which a number of amino-acid residues are more mobile than in the native protein. Laser-photochemically-induced dynamic nuclear polarization experiments identified tryptophan and tyrosine residues, but not histidine residues, in Ca(II)-independent discharged aequorin to be accessible to the flavin dye used. These exposed residues are also among the mobile residues of the Ca(II)-independent discharged protein. Resonances of all the protons (including the alpha protons) of the accessible tryptophan and tyrosine residues were assigned with the aid of two-dimensional photochemically-induced dynamic nuclear polarization J-correlated spectroscopy. The oxidized chromophore, from which light is emitted in aequorin, was not accessible to the dye in the Ca(II)-independent discharged protein. No exposed residue was detected in the photochemically-induced dynamic nuclear polarization spectrum of Ca(II)-independent discharged aequorin from which the oxidized chromophore was removed, corroborating the previous finding that in this apo-discharged form the protein partially refolds and thereby loses some of the mobility acquired in the formation of the Ca(II)-independent discharged protein.