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M Guéron

Publications and source records attributed to M Guéron.

At least 37 records · Page 2Linked to original sources

Proton exchange and internal motions in two chromomycin dimer-DNA oligomer complexes.

Previous structural studies on the complexes of the chromomycin (CHR) dimer with duplexes of d(A1-A2-G3-G4-C5-C6-T7-T8) and of d(A1-G2-G3-A4-T5-C6-C7-T8) in solution [one Mg(II) and two drugs per duplex] are extended to hydrogen exchange measurements. Exchange of the OH8 proton of chromomycin, measured by real time proton-deuterium exchange, is very slow and requires dissociation of the complex, whose lifetime is thus determined. The lifetimes and apparent dissociation constants of base pairs are deduced from the catalysis of imino proton exchange by ammonia. The four central base pairs, which interact with the CHR chromophores in the minor groove (Gao & Patel, 1990), may open within the complex, but the opening rate is less than in the free duplex by one to two orders of magnitude. The activation energy for base-pair opening and the differences between the lifetimes of adjacent pairs suggest that single base-pair opening is the predominant imino proton exchange pathway in all cases. In the symmetrical complex of chromomycin with the first duplex, the lifetimes of the central base pairs (G3.C6 and G4.C5) are in the same range (52 and 29 ms, respectively, at 38 degrees C). In the asymmetrical complex formed with the second duplex, the base-pair lifetimes in the G2-G3-A4-T5 segment that interacts with the chromophore moiety are strongly increased. That of G3.C6 is particularly long. Above 50 degrees C, exchange of the G3 imino proton is opening limited.(ABSTRACT TRUNCATED AT 250 WORDS)

Ammonia↗

A coupled resonator model of the detection of nuclear magnetic resonance: radiation damping, frequency pushing, spin noise, and the signal-to-noise ratio.

Magnetic resonance involves two coupled resonating systems: the spins and the tuned receiver coil. We simulate the spin system by an equivalent electrical resonator. An analysis of coupled resonators leads to a straightforward derivation of properties such as radiation damping, frequency pushing, and spin noise. The theory is applied to recent experiments (M. Guéron and J. L. Leroy, J. Magn. Reson. 85, 209-215 (1989]. The sensitivity of the spin noise experiment is shown to be T2/tau 0, where 1/tau 0 is the rate of radiation damping. This result leads directly to a fundamental formulation of the usual signal-to-noise ratio, (SNR)2 = (m0 B/tau 0)/(4Fk theta delta v), where m0 is the equilibrium magnetic moment, theta is the temperature, and F is the noise figure of the receiver. An equivalent electrical resonator can also be used to describe the active medium of masers.

Computer Simulation↗

Insulin increases the rate of degradation of 2-deoxy-glucose-6-phosphate in the perfused rat heart: a 31P NMR study.

The effect of insulin on the production and degradation of 2-deoxyglucose-6-phosphate (2DG6P) from 2-deoxyglucose (2DG) in the Langendorff-perfused rat heart was studied by 31P NMR. The 2DG concentrations ranged from 0.25 to 20 mM in the 5 mM acetate perfusion medium, and from 2 to 4 mM in the 12 mM glucose medium. With acetate as the carbon source, the apparent Km for the production of 2DG6P was 7 mM and Vmax was 1.8 mumols/min/mg prot. Insulin enhanced Vmax 7-fold without change in Km of the transporter. With glucose perfusion, insulin had no effect on the initial rate of production of 2DG6P. The interpretation is that glucose phosphorylation is regulated by work when glucose is the energy substrate. In acetate-perfused hearts, in the conditions where the 2DG6P content reached a plateau, the rate of production of 2DG6P (equal to the measured degradation rate, see below) was eight times smaller than the initial rate, both with and without insulin. In glucose-perfused hearts, it was the same as the initial rate. The degradation of 2DG6P upon interruption of 2DG perfusion was exponential. The time constant was the same in acetate or glucose. It was strongly affected by insulin, being 225 +/- 60 min without, and 92 +/- 13 min with insulin. The observation that 2DG6P degradation is sensitive to insulin in the heart shows that its rate may vary. This possibility should be kept in mind in the analysis of PET studies of glucose metabolism.

Acetates↗

Processes of base-pair opening and proton exchange in Z-DNA.

Using proton magnetic resonance, we have investigated imino and amino proton exchange in the Z form of the four oligomers d(Cbr8GCGCbr8G), d(CGm5CGCG), d(CG)6, and d(CG)12. In the latter two oligomers, all five exchangeable protons have been assigned. We find that proton acceptors such as NH3 or the basic form of Tris enhance imino proton exchange. The base-pair lifetime can then be obtained by extrapolation of the exchange time to infinite concentration of proton acceptor. For d(CG)6 and d(CG)12, the values are ca. 3.5 ms at 80 degrees C and ca. 130 ms at 35 degrees C. The latter value is about 65 times longer than in the same oligomers in the B form. The activation energy of base-pair opening, 80 kJ/mol, is the same in the Z and the B forms of d(CG)12. At 5 degrees C, the base-pair lifetime is about 3 s, much smaller than the time constant of the Z to B transition, to which it is therefore unrelated. The base-pair dissociation constant at 35 degrees C, 0.5 X 10(-6), is 5 times smaller than for the same oligomers in the B form. In the absence of added catalyst, at pH 7, the exchange time of the imino proton is 30 min at 5 degrees C. That of both cytidine amino protons, assigned by NOE, is about 50 min. The longest proton exchange time, ca. 330 min, is assigned unambiguously to the guanosine amino protons. Thus assigned and interpreted in terms of exchange chemistry rather than structural kinetics, the exchange times do not support earlier models of Z-DNA internal motions.

Base Composition↗

Evidence from base-pair kinetics for two types of adenine tract structures in solution: their relation to DNA curvature.

We have measured the base-pair lifetimes in oligodeoxynucleotides containing tracts of A.T base pairs using imino proton magnetic resonance. When the tract contains more than four consecutive A.T base pairs, possibly including a 5'-AT step but not a 5'-TA step, anomalously long lifetimes are observed. For example, the lifetimes of the central A.T base pairs of the dodecamer 5'-d-CGCAAAAAAGCG are 122 and 91 ms at 15 degrees C whereas, in the same conditions, the lifetime of the central A.T pair of the decamer 5'-d-CGCGATCGCG is only 4 ms, a value similar to those measured in several other B-DNA oligoduplexes [Leroy et al. (1988) J. Mol. Biol. 200, 223-238]. This strongly suggests that, in tracts of four A.T pairs or more, a conformation distinct from standard B-DNA is formed cooperatively. All sequences known to generate curved DNA exhibit anomalously long base-pair lifetimes. This is the first local and physical property shown to correlate with DNA curvature. Our observations suggest that the structure responsible for the long lifetimes is involved in the curvature of DNA.

Adenine↗

Characterization of base-pair opening in deoxynucleotide duplexes using catalyzed exchange of the imino proton.

Using nuclear magnetic resonance line broadening, longitudinal relaxation and magnetization transfer from water, we have measured the imino proton exchange times in the duplex form of the 10-mer d-CGCGATCGCG and in seven other deoxy-duplexes, as a function of the concentration of exchange catalysts, principally ammonia. All exchange times are catalyst dependent. Base-pair lifetimes are obtained by extrapolation to infinite concentration of ammonia. Lifetimes of internal base-pairs are in the range of milliseconds at 35 degrees C and ten times more at 0 degrees C. Lifetimes of neighboring pairs are different, hence base-pairs open one at a time. Lifetimes of d(G.C) are about three times longer than those of d(A.T). The nature of neighbors usually has little effect, but lifetime anomalies that may be related to sequence and/or structure have been observed. In contrast, there is no anomaly in the A.T base-pair lifetimes of d-CGCGA[TA]5TCGCG, a model duplex of poly[d(A-T)].poly[d(A-T)]. The d(A.T) lifetimes are comparable to those of r(A.U) that we reported previously. End effects on base-pair lifetimes are limited to two base-pairs. The low efficiency of exchange catalysts is ascribed to the small dissociation constant of the deoxy base-pairs, and helps to explain why exchange catalysis had been overlooked in the past. This resulted in a hundredfold overestimation of base-pair lifetimes. Cytosine amino proteins have been studied in the duplex of d-CGm5CGCG. Exchange from the closed base-pair is indicated. Hence, the use of an amino exchange rate to evaluate the base-pair dissociation constant would result in erroneous, overestimated values. Catalyzed imino proton exchange is at this time the safest and most powerful, if not the only probe of base-pair kinetics. We propose that the single base-pair opening event characterized here may be the only mode of base-pair disruption, at temperatures well below the melting transition.

Base Composition↗

Sustained function of normoxic hearts depleted in ATP and phosphocreatine: a 31P-NMR study.

A model of high-energy phosphate depletion was developed in the normoxic isovolumic rat heart perfused with acetate, 2-deoxy-D-glucose (2DG), and insulin. Intracellular phosphorylation of 2DG abstracts phosphorus from its normal pathways. This results in a decrease of high-energy phosphates without any increase in Pi. During the first 15 min of 2DG phosphorylation, the changes in ATP, Pi, and intracellular pH (pHi) were slight, and work was unaltered, although phosphocreatine (PCr) concentration dropped by 50%. After 45 min, the heart reached a new steady state characterized by a drastic reduction in both PCr and ATP: PCr was 15% of control, and in most hearts ATP became invisible on the nuclear magnetic resonance (NMR) spectra. Nevertheless, the heart still developed 65% of its original systolic pressure, whereas diastolic pressure was unchanged. Oxygen consumption per unit work remained constant during 2DG perfusion. This is, to our knowledge, the first experimental model of sustained cardiac contractility at such low contents of both ATP and PCr. However, our results are compatible with present knowledge of the cytosolic energy transfer by PCr and of the control of force in myofilaments.

Adenine Nucleotides↗

Proton exchange and base-pair lifetimes in a deoxy-duplex containing a purine-pyrimidine step and in the duplex of inverse sequence.

Using proton relaxation and magnetization transfer from water we have measured the imino proton exchange kinetics in two dodecadeoxynucleotide duplexes. One is formed by the self-complementary sequence 5'-d(C-C-T-T-T-C-G-A-A-A-G-G), the other by the inverse sequence. The imino proton exchange rates are found to depend on the concentration of ammonia or imidazole, acting as basic catalysts of proton exchange. Extrapolation of exchange times to infinite catalyst concentration yields the base-pair lifetimes, for instance 40 milliseconds for the central G.C base-pair of the 5'-d(C-C-T-T-T-C-G-A-A-A-G-G) duplex and four milliseconds for its A.T neighbour, at 15 degrees C. These results differ markedly from those reported by other laboratories for similar deoxy compounds. An explanation of the discrepancy has been proposed recently. Differences between base-pair lifetimes indicate that opening is not co-operative. From the catalyst efficiency relative to exchange from isolated nucleosides, we estimate the dissociation constant of each base-pair, e.g. 0.3 x 10(-6) and 1.5 x 10(-5) at 15 degrees C, for the same G.C and A.T base-pairs. The lifetime and dissociation constant of corresponding base-pairs of the two duplexes are similar, except for the central G.C base-pair. This correlates with differences in the solution structures reported by others. We have completed the assignments of the imino protons and of the six cytosine amino protons of the 5'-d(G-G-A-A-A-G-C-T-T-T-C-C) 12-mer. A new base-pair numbering scheme is proposed.

Base Composition↗

Proton exchange and base-pair kinetics of poly(rA).poly(rU) and poly(rI).poly(rC).

Proton exchange of poly(rA).poly(rU) and poly(rI).poly(rC) has been studied by nuclear magnetic resonance line broadening and saturation transfer from H2O. Five exchangeable peaks are observed. They are assigned to the imino, amino and 2'-OH ribose protons. The aromatic spectrum is also assigned. Contrary to previous observations, we find that the exchange of the imino proton is strongly buffer sensitive. This property is used to derive the base-pair lifetime, which is in the range of milliseconds at 27 degrees C, 100 times smaller than published values. The enthalpy for the base-opening reaction (-86 kJ/mol) and the insensitivity of the reaction to magnesium suggest that the open state involves a small number of base-pairs. The similarities in the exchange from the two duplexes indicate that the same open state is responsible for exchange of purine and pyrimidine imino protons. For the lifetime of the open state and for the base-pair dissociation constant, we obtain only lower limits. At 27 degrees C they are three microseconds and 10(-3), respectively. The analysis that yields the much larger values published previously is based on the assumption that amino protons exchange only from open base-pairs. But theory and preliminary experiments indicate that it may occur from the closed duplex. The exchange of amino protons is slower than that of the imino protons. Exchange of the 2'-OH protons from the duplexes is much slower than from single-stranded poly(rU), and it is accelerated by magnesium. This could indicate hydrogen-bonding to backbone phosphate. Discrepancies between our results and those of previous studies are discussed.

Kinetics↗

Significance and mechanism of divalent-ion binding to transfer RNA.

Phosphorus NMR shows that divalent ions (manganese) bind to tRNA phosphates as to those of DNA or isolated phosphodiesters. The time for dissociation of a phosphate-divalent ion complex is in the microsecond range. For no single phosphate is the affinity to divalent ions greater than 10 times that of the average phosphate. It is often stated that a small number of strong binding sites exist and are structurally and functionally important. This concept originates from binding curves whose properties should, instead, be traced to the polyelectrolyte nature of nucleic acids. The 31P NMR data preclude the existence of strong sites to which divalent ions would bind very selectively. The Spectroscopic and crystallographic observations of sites for divalent ions do not in fact demonstrate selective binding to these sites.

Animals↗

Demonstration of different complexation modes between cobalt and 5' AMP, by direct NMR observation of the low-temperature complex.

We report the first direct NMR observation of transition metal-nucleotide complexes. The phosphorus and proton spectra of a cobalt-5' AMP complex were observed in water, pH 7, -- 10 degrees C. This complex is different from the high temperature species : for instance its 31P chemical shift is -- 50 ppm, whereas the published value obtained indirectly for the high temperature form corresponds to ca. -- 1200 ppm. The -- 50 ppm complex is present in significant proportion at 20 degrees C and possibly at higher temperatures. Multiple complexation modes are also observed for Co-ATP.

Adenosine Monophosphate↗

Comparative conformations of uridine and pseudouridine and their derivatives.

Stimulated by the suggestion that pseudouridine psi-39 in yeast tRNAPhe could be in a syn conformation [R. E. Hurd and B. R. Reid (1977) Nucleic Acid Research 4, 2747-2755], we have made a comparative study of the solution conformations of psi and U derivatives, using the proton-proton Overhauser effect. Rotation around the glycosidic bond is observed for pseudouridine and 3 psi MP as well as for uridine and 3'UMP. However pseudouridine an 3 psi MP are mostly syn, whereas uridine, 3'-UMP and 5'UMP are mostly anti. There is no evidence for a correlation between sugar conformation and orientation around the glycosidic bond. The results are confirmed by relaxation measurements. They are discussed in the light of earlier studies. They tend to support the suggestion of Hurd and Reid. They raise the question of the orientation of the pseudouridine found elsewhere in tRNA (e.g. in the T psi C loop).

Magnetic Resonance Spectroscopy↗

Molar absorbance of tRNA.

Examination of some published values suggests that the concentration of most tRNAs can be evaluated on the basis of epsilon 260 = 7200/base, in magnesium buffer.

Base Composition↗

Role of divalent ions in folding of tRNA.

The native structure of tRNA is not achieved in low salt (4.5 mM Na+, 25 degrees C), but can be restored by addition of divalent ions. We have explored the structure of the central region in Escherichia coli tRNAfMet by absorption and emission spectroscopy of 4-thiouracil, and the structure of the anticodon loop in yeast tRNAPhe by fluorescence of the 'Y' base, versus the number of manganese ions bound to tRNA, which was derived from electron spin resonance. The fluorescence of the reduced 8-13 photoproduct (in which 4-thiouracil at position 8 is crosslinked to cytosine at position 13) was also analysed. In low salt (e.g. 4.5 mM Na+), the region of 4-thiouracil is affected strongly as the first eight Mn2+ bind to tRNA, whereas the fluorescence of the 'Y' base is affected only after four Mn2+ are bound. Considering the structural similarities of the two tRNAs, this suggests that the reorganisation brought about by divalent ions starts in the central region, the anticodon loop being affected later. The binding of divalent ions to each region starts together with its restructuration. Monovalent ions can substitute for divalent ions in this process, a 15 mM sodium concentration being equivalent to the binding of the first five Mn2+. If divalent ions are then added, even the first ones distribute themselves between both the central and the anticodon region. Alternatively, the renaturation may be achieved by monovalent ions only, implying that no sites exist whose occupancy by divalent ions is crucial for the native structure. These observations suggest that the role and means of divalent ion binding to tRNA are largely explainable in terms of a simple maganese-phosphate binding supplemented by electrostatic interaction with distant phosphates.

Anticodon↗

Electron paramagnetic resonance of Hb St Louis beta28 (B10) Leu replaced by Gln.

Hemoglobin St Louis beta28 (B10) Leu replaced by Gln is a new mutant which occurs as a natural valency hybrid (alpha2beta+2), or hemoglobin M (Cohen-Solal, M., Seligmann, M., Thillet, J. and Rosa, J. (1973) FEBS Lett. 33, 37-41). The electron paramagnetic resonance (EPR) spectrum of native Hb St Louis at pH 6.2 shows a mixture of three species. Two are high spin, one with tetragonal symmetry, like Hb+ A, the other with rhombic distortion. The third is a low-spin form corresponding to a hemichrome with the distal (E7) histidine as the sixth ligand of the ferric iron. The hemichrome is also found in red blood cells. After oxidation to the alpha+2beta+2 form, three EPR species are seen. Surprisingly, there remains only one high-spin signal, with almost tetragonal symmetry. Besides the low-spin hemichrome, a hydroxy signal is observed even at pH 6.2. These observations imply interactions between the alpha and beta hemes.

Electron Spin Resonance Spectroscopy↗

31P magnetic resonance of tRNA.

We have observed well-resolved 31P resonances at 65 kG (109 MHz) in solutions of Escherichia coli tRNAGlu and yeast tRNAPhe. One resolved resonance, identified as the terminal phosphate, titrates with a pK = 6.35. Upon melting the yeast tRNAPhe in 0.1 M NaCl, without Mg++, the resolved peaks broaden and disappear in the vicinity of 35 degrees while the central cluster narrows drastically, shifts slightly, and loses its structure. Addition of Mg++ shifts one resolved peak and changes the shape of the cluster. The 31P lines are broader when observed at 65 kG than at 24 kG. The broadening is shown to come from chemical shift anisotropy which is estimated to be about 140 ppm.

Escherichia coli↗