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Recombination rates have been examined in two-point crosses of various defined cyc1 mutants using five mapping methods. Nucleotide sequences of mutant codons were identified in previous studies from alterations in functional iso-1-cytochromes c produced by intragenic revertants. Heteroallelic diploids were analyzed for rates of mitotic recombination that occurred spontaneously and that were induced with x-rays, ultraviolet light and the near-ultraviolet light emitted by sunlamps, as well as rates of meiotic recombination that occur after sporulation. Frequencies of both mitotic and meiotic recombination do not necessarily correspond with physical distances separating altered nucleotides. The most extreme discrepancy involved two adjacent intervals of thirteen basepairs which differed approximately thirty-fold in their spontaneous and X-ray-induced recombination rates. Marked disproportions between genetic and physical distances appear to be due to the interaction of the two nucleotide sequences in the heteroallelic combination and not to the sequences of the mutant codons alone. Recombination values that were obtained by all five methods could not be used to establish to correct order of mutant sitesmrelationships of the recombination rates for the various pairwise crosses are different after mitosis from those after meiosis, suggesting that these two recombinational processes are to some extent different in their dependence on particular nucleotide configurations. On the other hand, the relationships of the rates induced by UV-, sunlamp- and X-irradiation were identical or very similar. In addition to the intrinsic properties of the alleles affecting frequencies of mitotic and meiotic recombination rates, two- to threefold variations in recombination rates could be attributed to genetic backgrounds.
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Energy refinement of the structure of a linear peptide, hirudin56-65, bound to thrombin was carried out using a conformational search method in combination with restrained minimization. Five conformations originated from nmr data and distance geometry calculations having a similar global folding pattern but quite different backbone conformations were used as the starting structures. As a result of this approach, a series of low-energy conformations compatible with a set of upper and lower bounds of interproton distances determined from transferred nuclear Overhauser effects were found. A comparison among the lowest energy conformations of each run showed that the combination of energy refinement plus distance constraints led to a very well-defined structure for both the backbone and the side chains of the last 7 residues of the polypeptide. Furthermore, the low-energy conformations generated with this technique contain a segment of 3(10)-helix involving the last 5 residues at the COOH terminal end.
Histochemical, electron microscopic, and morphometrical techniques were employed in the determination of the effects attributed to K+-induced cerebrocortical swelling on cat cerebrocortical capillary diameter, length, surface area, volume, and minimal intercapillary distance. Bilaterally exposed and intact temporoparietal cerebral cortices of 4 conditioned adult cats were simultaneously superfused with isotonic, artificial CSF containing 3.5 mM K+ (control) and 54 mM K+ experimental), for 1h at 37 degrees C with monitoring of systemic vital function, hematocrit, arterial blood gases, and determination of cerebrocortical tissue water content. The mean values for cerebrocapillary diameter were 5% (P less than 0.05) greater in swollen tissues when compared with comparable mean values determined for controls. The values for minimal intercapillary distance determined from control and experimental animals plotted as relative frequency histograms represented two distinct populations (P less than 0.005). The significance of altered capillary morphometric parameters are discussed in relation to K+-induced cerebrocortical swelling.
By means of neutron solution scattering we determined the position and orientation of core enzyme and sigma-factor within the Escherichia coli RNA polymerase holoenzyme with the aim of improving existing models. The individual components, core enzyme (E) and sigma-factor (sigma), were highlighted by deuterium labeling and their center-to-center distances determined in the monomeric and the dimeric holoenzyme. The following distance parameters were obtained: dE1-sigma 1 = 8.6(+/- 1) nm, dE1-E2 = 11.5(+/- 1) nm, d sigma 1-sigma 2 = 12.0(+/- 0.7) nm, dE1-sigma 2 = 9(+/- 3) nm. Using a triangulation procedure the position of the sigma-factors, sigma 1 and sigma 2, were determined with respect to the mass center of the core enzyme molecules, E1 and E2, assuming a symmetrical arrangement of the holoenzyme molecules in the dimer (C2 symmetry). In addition, the orientation of the sigma-factor with respect to core enzyme was estimated by means of model calculations. The obtained model of holoenzyme depicts the sigma-factor as buried in a groove of core enzyme, probably between the large subunits beta' and beta.
The ion-channel-forming C-terminal fragment of colicin A binds to negatively charged lipid vesicles and provides an example of insertion of a soluble protein into a lipid bilayer. The soluble structure is known from X-ray crystallography and consists of a ten-helix bundle containing a hydrophobic helical hairpin. In this work fluorescence spectroscopy was used to study the membrane-bound structure. An extrinsic probe, N'-(iodoacetyl)-N'-(5-sulfol-naphthyl)ethylenediamine (IAEDANS) was attached to mutant proteins each of which bears a unique cysteine residue. Three mutants K39C (helix 2), T127C (between helices 6 and 7) and S16Crpt (helix 1, which bears a decapeptide repeat before the mutation) gave useful derivatives. In the soluble protein they showed emission wavelengths decreasing in the order K39C greater than T127C greater than S16Crpt and although all showed blue shifts on addition of dimyristoylphosphatidylglycerol (DMPG) this order was maintained in the membrane-bound state. These shifts were not indicative of deep membrane insertion. Polarization of IAEDANS revealed differences in mobility between mutants. The three tryptophan residues were used as a compound donor to IAEDANS in resonance energy transfer distance determinations. The values obtained for the soluble form were 1.2 A to 3.2 A longer than in the crystal structure. On addition of lipids the indicated distances increased: S16Crpt-I(AEDANS) 6.45 A (22%), K39C-I 5.45 A (18%) and T127C-I 2.4 A (14%). N-bromosuccinimide (NBS) completely abolishes the tryptophan emission from the thermolytic fragment. When lipids were added to a mixture containing ten NBS-treated channel-forming fragments to one IAEDANS labelled fragment the indicated distances increased rather more: S16Crpt-I 9.7 A (38%), K39C-I 8.1 A (36%) and T127C-I 2.5 A (16%). This showed that intermolecular transfer reduces the distance estimated in samples containing only labelled protein. The ensemble of results shows that the amphipathic helices of the C-terminal fragment open out on the surface of the lipid bilayer during the initial phase of membrane insertion.
The DNA octamer [d(GTATAATG].[(CATATTAC)], containing the prokaryotic upstream consensus recognition sequence, has been examined via proton homonuclear two-dimensional nuclear Overhauser effect (2D NOE) and double-quantum-filtered correlation (2QF-COSY) spectra. All proton resonances, except those of H5' and H5" protons, were assigned. A temperature dependence study of one-dimensional nuclear magnetic resonance (NMR) spectra, rotating frame 2D NOE spectroscopy (ROESY), and T1 rho measurements revealed an exchange process that apparently is global in scope. Work at lower temperatures enabled a determination of structural constraints that could be employed in determination of a time-averaged structure. Simulations of the 2QF-COSY cross-peaks were compared with experimental data, establishing scalar coupling constant ranges of the individual sugar ring protons and hence pucker parameters for individual deoxyribose rings. The rings exhibit a dynamic equilibrium of N and S-type conformers with 80 to 100% populations of the latter. A program for iterative complete relaxation matrix analysis of 2D NOE spectral intensities, MARDIGRAS, was employed to give interproton distances for each mixing time. According to the accuracy of the distance determination, upper and lower distance bounds were chosen. The distance bounds define the size of a flat-well potential function term, incorporated into the AMBER force-field, which was employed for restrained molecular dynamics calculations. Torsion angle constraints in the form of a flat-well potential were also constructed from the analysis of the sugar pucker data. Several restrained molecular dynamics runs of 25 picoseconds were performed, utilizing 184 experimental distance constraints and 80 torsion angle constraints; three different starting structures were used: energy minimized A-DNA, B-DNA, and wrinkled D-DNA, another member of the B-DNA family. Convergence to similar structures obtained with root-mean-square deviations between resulting structures of 0.37 to 0.92 A for the central hexamer of the octamer. The average structure from the nine different molecular dynamics runs was subjected to final restrained energy minimization. The resulting final structure was in good agreement with the structures derived from different molecular dynamics runs and exhibited a substantial improvement in the 2D NOE sixth-root residual index in comparison with the starting structures. An approximation of the structure in the terminal base-pairs, which displayed experimental evidence of fraying, was made by maintaining the structure of the inner four base-pairs and performing molecular dynamics simulations with the experimental structural constraints observed for the termini.(ABSTRACT TRUNCATED AT 400 WORDS)
To determine which spatial frequencies are most effective for letter identification, and whether this is because letters are objectively more discriminable in these frequency bands or because can utilize the information more efficiently, we studied the 26 upper-case letters of English. Six two-octave wide filters were used to produce spatially filtered letters with 2D-mean frequencies ranging from 0.4 to 20 cycles per letter height. Subjects attempted to identify filtered letters in the presence of identically filtered, added Gaussian noise. The percent of correct letter identifications vs s/n (the root-mean-square ratio of signal to noise power) was determined for each band at four viewing distances ranging over 32:1. Object spatial frequency band and s/n determine presence of information in the stimulus; viewing distance determines retinal spatial frequency, and affects only ability to utilize. Viewing distance had no effect upon letter discriminability: object spatial frequency, not retinal spatial frequency, determined discriminability. To determine discrimination efficiency, we compared human discrimination to an ideal discriminator. For our two-octave wide bands, s/n performance of humans and of the ideal detector improved with frequency mainly because linear bandwidth increased as a function of frequency. Relative to the ideal detector, human efficiency was 0 in the lowest frequency bands, reached a maximum of 0.42 at 1.5 cycles per object and dropped to about 0.104 in the highest band. Thus, our subjects best extract upper-case letter information from spatial frequencies of 1.5 cycles per object height, and they can extract it with equal efficiency over a 32:1 range of retinal frequencies, from 0.074 to more than 2.3 cycles per degree of visual angle.
Cosmid clones containing human or hamster inserts have been hybridized in situ and localized with fluorescent reporter molecules in interphase nuclei (pronuclei) obtained after fusion of hamster eggs with either human or hamster sperm. Hamster egg cytoplasm processes the tightly packaged sperm DNA into large diffuse networks of chromatin fiber bundles, providing hybridization targets more extended than those available in somatic interphase cell nuclei. Pronuclear physical distances between hybridization signals were measured in micrometers and correlated to genomic distances determined by restriction fragment analyses, using cosmids from the Chinese hamster DHFR region and from the human Factor VIII/color vision pigment gene region (Xq28). The mean pronuclear distances between hybridization sites were about three times as large as those measured in somatic interphase cells for equivalent genomic distances. The relationship between physical and genomic distances was linear from less than 50 kb to at least 800 kb. The results show that physical distance in the sperm-egg system promises to extend the mapping range obtainable in somatic interphase nuclei below 50 kb and up to at least 800 kb.
A quantitative theory for excitation of fluorescent molecules by beta decay electrons is reported in the accompanying manuscript; experimental detection methods and biological applications are reported here. The single photon signals produced by an excited fluorophore (single photon radioluminescence, SPR) provide quantitative information about the distance between radioisotope and fluorophore. Instrumentation was constructed for SPR signal detection. Photons produced in a 0.5-ml sample volume were detected by a cooled photomultiplier and photon counting electronics. To minimize electronic noise and drift for detection of very small SPR signals, a mechanical light chopper was used for gated-signal detection, and a pulse height analyzer for noise rejection. SPR signals of approximately 1 cps were reproducibly measurable. The influence of inner filter effect, sample turbidity, and fluorophore environment (lipid, protein, and carbohydrate) on SPR signals were evaluated experimentally. SPR was then applied to measure lipid exchange kinetics, ligand binding, and membrane transport, and to determine an intermolecular distance in an intact membrane. (a. Lipid exchange kinetics.) Transfer of 12-anthroyloxystearic acid (12-AS) from sonicated lipid vesicles and micelles to vesicles containing 3H-cholesterol was measured from the time course of increasing SPR signal. At 22 degrees C, the half-times for 12-AS transfer from vesicles and micelles were 3.3 and 1.1 min, respectively. (b. Ligand binding.) Binding of 3H-oleic acid to albumin in solution, and 3H-2,2'-dihydro-4,4'-diisothiocyanodisulfonic stilbene (3H-H2DIDS) to band 3 on the erythrocyte membranes were detected by the radioluminescence of the intrinsic tryptophans. The SPR signal from 5 microCi 3H-oleic acid bound to 0.3 mM albumin decreased from 13 +/- 2 cps to 3 +/- 2 cps upon addition of nonradioactive oleic acid, giving 2.7 high affinity oleic acid binding sites per albumin. The SPR signal from 1 microCi 3H-H2DIDS bound selectively to erythrocyte band 3 in erythrocyte ghosts (1.5 mg protein/ml) was 2.2 +/- 0.8 cps. (c. Membrane transport). Dilution of J774 macrophages loaded with 3H-3-O-methylglucose and BCECF gave a decreasing SPR signal with a half-time of 81 s due to methylglucose efflux; the SPR measurement of the efflux rate was in agreement with a conventional tracer efflux rate determination by filtration. 20 microM cytochalasin B inhibited efflux by 97%. (d. Distance determination.) The SPR signal from erythrocyte membranes labeled with 27 microCi 3H-oleic acid and 10 microM of fluorescein-labeled wheat germ agglutinin was 5.7 +/- 0.5 cps, giving an average glycocalyx-to-bilayer distance of 5 nm. The results establish methods for experimental detection of SPR signals and demonstrate the applications of radioluminescence to the measurement of lipid exchange kinetics, ligand binding, membrane transport, and submicroscopic distances in intact membranes in real time.
Dipole-dipole energy transfer between suitable donor and acceptor chromophores is an important luminescence quenching mechanism and has been shown to be useful for distance determination at the molecular level. In the rapid diffusion limit, where the excited-state lifetime of the donor is long enough to allow the donor and acceptor to diffuse many times their average separation before deexcitation, it is usually assumed that the relative dipolar orientation is completely averaged due to rotational Brownian motion. Under this simplifying assumption, analytical expressions have been derived earlier for the energy transfer rate between donor and acceptor characterized by different geometries. Most such expressions, however, are only approximate because complete angular averaging is permitted only in a geometry that possesses spherical symmetry surrounding each chromophore. In this paper analytical expressions that correctly account for incomplete angle averaging due to steric hindrance are presented for several geometries. Each of the equations reveals a dependence of the energy transfer rate on chromophore orientation. It is shown that correctly accounting for this effect can lead to improvements in estimates of the distance of closest approach from measured quenching rates based on energy transfer experiments.
Thirteen genetic loci spanning murine chromosome 15 from 15A2 (Mlvi-2) to 15F2-3 (Gdc-1) have been mapped. The genetic distance extends to 55.4 cM. Among 151 animals, only 1 animal with a double cross-over was found. The linear order is unambiguous, with the exception of the distal end on 15F1-3. Our analysis favors the order cen-Ela-1/Hox-3-Wnt-1-Gdc-1-ter. This ordering makes necessary the introduction of three tightly spaced double recombination events around and within the Hox-3 locus. Alternatively, Hox-3 may be most distal, and several double recombinations at the telomere lead to map expansion. Despite the unequal distribution along chromosome 15 of G-versus R-bands, a comparison of distances determined by physical and genetic mapping does not indicate an overt difference in distance between both mapping techniques.
Rotational resonance, a new solid-state NMR technique for determining internuclear distances, is used to measure a distance in the active site of bacteriorhodopsin (bR) that changes in different states of the protein. The experiments are targeted to the active site of bR through 13C labeling of both the retinal chromophore and the Lys side chains of the protein. The time course of the rotor-driven magnetization exchange between a pair of 13C nuclei is then observed to determine the dipolar coupling and therefore the internuclear distance. Using this approach, we have measured the distance from [14-13C]retinal to [epsilon-13C]Lys216 in dark-adapted bR in order to examine the structure of the retinal-protein linkage and its role in coupling the isomerizations of retinal to unidirectional proton transfer. This distance depends on the configuration of the intervening C=N bond. The 3.0 +/- 0.2 A distance observed in bR555 demonstrates that the C=N bond is syn, and the 4.1 +/- 0.3 A distance observed in bR568 demonstrates that the C=N bond is anti. These direct distance determinations independently confirm the configurations previously deduced from solid-state NMR chemical shift and resonance Raman vibrational spectra. The spectral selectivity of rotational resonance allows these two distances to be measured independently in a sample containing both bR555 and bR568; the presence of both states and of 25% lipid in the sample demonstrates the use of rotational resonance to measure an active site distance in a membrane protein with an effective molecular mass of about 85 kDa.(ABSTRACT TRUNCATED AT 250 WORDS)
Quenching of the room-temperature phosphorescence of Escherichia coli alkaline phosphatase by several freely diffusing molecules was studied, each of whose absorption spectrum overlaps the long-lived emission of this protein and which therefore can quench the excited triplet state by diffusion-enhanced Förster energy transfer. The presence of additional nonresonance transfer mechanisms was also detected, from a lack of linear dependence of quenching rate on spectral overlap. The quenching agents used were the dye molecules methyl red, methyl orange, and 2-[(4-hydroxyphenyl)azo]benzoic acid, as well as the embedded heme groups of myoglobin, metmyoglobin, and the reduced and oxidized forms of cytochrome c. Quenching was found to be greatly diminished upon reduction of each acceptor, indicating that electron transfer occurs efficiently from the excited tryptophan to the oxidized form of the acceptors. The elimination of this electron transfer in the reduced form affords the opportunity to separately measure the Förster transfer rates for the heme proteins. When the transfer rate constant thus measured for myoglobin is applied to a model where both donor and acceptor proteins are taken to be spherical with both tryptophan and the heme group placed off center (a model whose quenching rate equation is newly presented here), the depth of the phosphorescent tryptophan beneath the surface of alkaline phosphatase is found to be 16 A. This value is close to the depth of tryptophan 109 (which is known to be the phosphorescent residue in alkaline phosphatase), showing that with properly chosen probes this technique is indeed valuable for distance determinations in protein structure studies.(ABSTRACT TRUNCATED AT 250 WORDS)
The three-dimensional structure of the duplex formed by the association of the unnatural oligonucleotide alpha-d(TCTAAACTC) covalently linked to an acridine derivative (m5Acr) with its natural and parallel complementary sequence beta-d(AGATTTGAG) was investigated by nuclear magnetic resonance spectroscopy and constrained molecular mechanics calculations. All the nonexchangeable and exchangeable resonances were assigned in this duplex. The structure was refined by using interproton distances determined by NOE measurements. The NOE values were converted into distances by using the complete 190 x 190 relaxation matrix. The unnatural duplex Acrm5-alpha-d(TCTAAACTC)-beta-d(AGATTTGAG) forms a parallel right-handed helix with Watson-Crick base pairing; the alpha and beta deoxyriboses adopt a 3'-exo conformation. The acridine moiety was found stacked up the C9-G9 base pair. The structure of the first seven base pairs of this duplex was found similar to that of the duplex alpha-d(TCTAAAC)-beta-d(AGATTTG), which we had already investigated [Lancelot, G., et al. (1989) Biochemistry 28, 7871-7878]. Since these structures were generated by using experimental NOE values obtained independently on macromolecules whose global correlation time was different (3.8 and 2.2 ns), we conclude that this comparison is a good test of the viability of our method to generate three-dimensional structures of oligonucleotides in solution. Starting from different initial conformations, we show that the NOE constraints allow one to reach the same final restrained conformation, taking into account implicitly the solvent effect.
The binding of formate ion, a substrate for the peroxidatic reaction of catalase, has been investigated by magnetic resonance techniques. Comparative studies of formate binding to ferric myoglobin have also been performed. The nuclear magnetic relaxation (NMR) rate of formate and water protons is enhanced by the presence of ferric horse liver catalase. The enhancement is not changed significantly by the addition of cyanide, indicating that water and formate are still bound in the presence of cyanide. Formate proton to heme iron distances determined by magnetic resonance techniques indicate that formate does not directly bind to the heme iron of catalase or myoglobin but to the globin, and NMR relaxation occurs as a result of outersphere mechanisms. Evidence that water forms an innersphere complex with the iron atom of the catalase heme is presented. In similar experiments with ferric myoglobin, the addition of cyanide caused a large decrease in the enhancement of the proton relaxation rate of both formate and water, indicating the displacement of water and formate from the heme and the vicinity of the heme, respectively. Broad, high-spin, ferric ion electron paramagnetic resonance absorptions of catalase and myoglobin at room temperature obtained in the presence and absence of formate show that formate does not alter appreciably the heme environment of catalase or myoglobin or the spin state of the heme iron. Studies on the binding of formate to catalase as monitored by changes in the heme absorption spectrum in the visible region show one-to-one stoichiometry with heme concentration. However, the small changes observed in the visible region of the optical spectrum on addition of formate ion are attributed to a secondary effect of formate on the heme environment, rather than direct binding of formate to the heme moiety.
Solution structures for many proteins have been determined to date utilizing interproton distance constraints estimated from two-dimensional nuclear Overhauser effect (2D NOE) spectra. Although the simple isolated spin pair approximation (ISPA) generally used can result in systematic errors in distances, the large number of constraints enables protein structure to be defined with reasonably high resolution. Effects of these systematic errors on the resulting protein structure are examined. Iterative relaxation matrix calculations, which account for dipolar interactions between all protons in a molecule, can accurately determine internuclear distances with little or no a priori knowledge of the molecular structure. The value of this additional complexity is also addressed. To assess these distance determination methods, hypothetical "experimental" data, including random noise and peak overlap, are calculated for an arbitrary "true" protein structure. Three methods of obtaining distance constraints from 2D NOE peak intensities are examined: one entails a conservative use of ISPA, one assumes the ISPA to be fairly accurate, and one utilizes an iterative relaxation matrix method called MARDIGRAS (matrix analysis of relaxation for discerning the geometry of an aqueous structure), developed in this laboratory. A distance geometry algorithm was used to generate a family of structures for each distance set. The quality of the average structure from each family was good. The root-mean-square deviation of that average structure from the true structure was improved about 2-5% using the more restrictive rather than the more conservative ISPA approach. Use of MARDIGRAS in a conservative fashion--i.e., with a poor initial model--resulted in improvement in the root-mean-square deviation by 8-15%. With a better initial model, MARDIGRAS obtained even more accurate distances. MARDIGRAS also permits analysis of 2D NOE data at longer mixing times, yielding additional distances. Use of more restrictive ISPA distances did, however, result in a few systematically incorrect structural features in local regions of the protein, producing distortions of 2-3 A. Comparison between experimental data and spectra calculated for the structures correlates with root-mean-square deviation, offering a method of structure evaluation. An R factor for evaluating fit between experimental and calculated 2D NOE intensities is proposed.