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D G Gorenstein

Publications and source records attributed to D G Gorenstein.

At least 73 records · Page 4Linked to original sources

Time-dependent 31P saturation transfer in the phosphoglucomutase reaction. Characterization of the spin system for the Cd(II) enzyme and evaluation of rate constants for the transfer process.

Time-dependent 31P saturation-transfer studies were conducted with the Cd2+-activated form of muscle phosphoglucomutase to probe the origin of the 100-fold difference between its catalytic efficiency (in terms of kcat) and that of the more efficient Mg2+-activated enzyme. The present paper describes the equilibrium mixture of phosphoglucomutase and its substrate/product pair when the concentration of the Cd2+ enzyme approaches that of the substrate and how the nine-spin 31P NMR system provided by this mixture was treated. It shows that the presence of abortive complexes is not a significant factor in the reduced activity of the Cd2+ enzyme since the complex of the dephosphoenzyme and glucose 1,6-bisphosphate, which accounts for a large majority of the enzyme present at equilibrium, is catalytically competent. It also shows that rate constants for saturation transfer obtained at three different ratios of enzyme to free substrate are mutually compatible. These constants, which were measured at chemical equilibrium, can be used to provide a quantitative kinetic rationale for the reduced steady-state activity elicited by Cd2+ relative to Mg2+ [cf. Ray, W.J., Post, C.B., & Puvathingal, J.M. (1989) Biochemistry (following paper in this issue)]. They also provide minimal estimates of 350 and 150 s-1 for the rate constants describing (PO3-) transfer from the Cd2+ phosphoenzyme to the 6-position of bound glucose 1-phosphate and to the 1-position of bound glucose 6-phosphate, respectively. These minimal estimates are compared with analogous estimates for the Mg2+ and Li+ forms of the enzyme in the accompanying paper.

Binding Sites↗

Two-dimensional 1H and 31P NMR spectra of a decamer oligodeoxyribonucleotide duplex and a quinoxaline ((MeCys3, MeCys7)(TANDEM) drug duplex complex.

Assignment of the 1H and 31P NMR spectra of a decamer oligodeoxyribonucleotide duplex, d(CCCGATCGGG), and its quinoxaline ((MeCys3, MeCys7]TANDEM) drug duplex complex has been made by two-dimensional 1H-1H and heteronuclear 31P-1H correlated spectroscopy. The 31P chemical shifts of this 10 base pair oligonucleotide follow the general observation that the more internal the phosphate is located within the oligonucleotide sequence, the more upfield the 31P resonance occurs. While the 31P chemical shifts show sequence-specific variations, they also do not generally follow the Calladine "rules" previously demonstrated. 31P NMR also provides a convenient monitor of the phosphate ester backbone conformational changes upon binding of the drug to the duplex. Although the quinoxaline drug, [MeCys3, MeCys7]TANDEM, is generally expected to bind to duplex DNA by bis-intercalation, only small 31P chemical shift changes are observed upon binding the drug to duplex d(CCCGATCGGG). Additionally, only small perturbations in the 1H NMR and UV spectra are observed upon binding the drug to the decamer, although association of the drug stabilizes the duplex form relative to the other states. These results are consistent with a non-intercalative mode of association of the drug. Modeling and molecular mechanics energy minimization demonstrate that a novel structure in which the two quinoxaline rings of the drug binds in the minor groove of the duplex is possible.

Animals↗

Assignments of 31P NMR resonances in oligodeoxyribonucleotides: origin of sequence-specific variations in the deoxyribose phosphate backbone conformation and the 31P chemical shifts of double-helical nucleic acids.

It is now possible to unambiguously assign all 31P resonances in the 31P NMR spectra of oligonucleotides by either two-dimensional NMR techniques or site-specific 17O labeling of the phosphoryl groups. Assignment of 31P signals in tetradecamer duplexes, (dTGTGAGCGCTCACA)2, (dTAT-GAGCGCTCATA)2, (dTCTGAGCGCTCAGA)2, and (dTGTGTGCGCACACA)2, and the dodecamer duplex d(CGTGAATTCGCG)2 containing one base-pair mismatch, combined with additional assignments in the literature, has allowed an analysis of the origin of the sequence-specific variation in 31P chemical shifts of DNA. The 31P chemical shifts of duplex B-DNA phosphates correlate reasonably well with some aspects of the Dickerson/Calladine sum function for variation in the helical twist of the oligonucleotides. Correlations between experimentally measured P-O and C-O torsional angles and results from molecular mechanics energy minimization calculations show that these results are consistent with the hypothesis that sequence-specific variations in 31P chemical shifts are attributable to sequence-specific changes in the deoxyribose phosphate backbone. The major structural variation responsible for these 31P shift perturbations appears to be P-O and C-O backbone torsional angles which respond to changes in the local helical structure. Furthermore, 31P chemical shifts and JH3'-P coupling constants both indicate that these backbone torsional angle variations are more permissive at the ends of the double helix than in the middle. Thus 31P NMR spectroscopy and molecular mechanics energy minimization calculations appear to be able to support sequence-specific structural variations along the backbone of the DNA in solution.

Base Sequence↗

Assignment of phosphorus-31 and nonexchangeable proton resonances in a symmetrical 14 base pair lac pseudooperator DNA fragment.

The 31P chemical shifts of all 13 phosphates and the chemical shifts of nearly all of the non-exchangeable protons of a symmetrical 14 base pair lac pseudooperator DNA fragment have been assigned by regiospecific labeling with oxygen-17 and two-dimensional NMR techniques. At 22 degrees C, 8 of the 13 phosphorus resonances can distinctly be resolved while the remaining 5 resonances occur in two separate overlapping regions. The 31P chemical shifts of this particular 14 base pair oligonucleotide do not follow the general observation that the more internal the phosphate is located within the oligonucleotide sequence the more upfield the 31P resonance occurs, as shown from other 31P assignment studies. Failure of this general rule is believed to be a result of helical distortions that occur along the oligonucleotide double helix, on the basis of the analysis of Callidine [Callidine, C.R. (1982) J. Mol. Biol. 161, 343-352]. Notable exceptions to the phosphate position relationship are 5'-Py-Pu-3' dinucleotide sequences, which resonate at a lower field strength than expected in agreement with similar results as reported by Ott and Eckstein [Ott, J., & Eckstein, F. (1985) Biochemistry 24, 253]. A reasonable correlation exists between 31P chemical shifts values of the 14-mer and the helical twist sum function of Calladine. The most unusual 31P resonance occurs most upfield in the 31P spectrum, which has been assigned to the second phosphate position (5'-GpT-3') from the 5' end. This unusual chemical shift may be the result of the predicted large helical twist angle that occurs at this position in the 14-mer sequence. Further, it is believed that the large helical twist represents a unique structural feature responsible for optimum binding contact between lac repressor protein and this 14-mer lac pseudooperator segment. Assignments of proton resonances were made from two-dimensional 1H-1H nuclear Overhauser effect (NOESY) connectivities in a sequential manner applicable to right-handed B-DNA, in conjunction with two-dimensional homonuclear and heteronuclear J-correlated spectroscopies (1H-1H COSY and 31P-1H HETCOR). Most nonexchangeable base proton and deoxyribose proton (except for some unresolved H4', H5', and H5" protons) resonances were assigned.

Base Sequence↗

31P and two-dimensional 31P/1H correlated NMR spectra of Duplex d(Ap[17O]Gp[18O]Cp[16O]T) and assignment of 31P signals in d(ApGpCpT)2-actinomycin D complex.

A solid-phase phosphoramidite method was used for the synthesis of unlabeled and phosphoryl-labeled d(Ap-[17O]Gp[18O]Cp[16O]T). The ability to label the phosphoryl oxygens of d(ApGpCpT) and thus assign the 31P signals, combined with a two-dimensional 31P/1H chemical shift correlated NMR spectral technique, provided a novel means for the ready assignment of the H5' and H3' protons coupled to the phosphates. Phosphoryl labeling has also allowed us to assign the 31P NMR signals in the actinomycin D-d(Ap-[17O]Gp[18O]Cp[16O]T)2 duplex complex and confirm that the drug intercalates between the GpC stacked base pairs.

Binding Sites↗

Stereoelectronic control in peptide bond formation. Ab initio calculations and speculations on the mechanism of action of serine proteases.

Ab initio molecular orbital calculations have been performed on the reaction profile for the addition/elimination reaction between ammonia and formic acid, proceeding via a tetrahedral intermediate: NH3 + HCO2H----H2NCH(OH)2----NH2CHO + H2O. Calculated transition state energies for the first addition step of the reaction revealed that a lone pair on the oxygen of the OH group, which is antiperiplanar to the attacking nitrogen, stabilized the transition state by 3.9 kcal/mol, thus supporting the hypothesis of stereoelectronic control for this reaction. In addition, a secondary, counterbalancing stereoelectronic effect stabilizes the second step, water elimination, transition state by 3.1 kcal/mol if the lone pair on the leaving water oxygen is not antiperiplanar to the C-N bond. The best conformation for the transition states was thus one with a lone pair antiperiplanar to the adjacent scissile bond and also one without a lone-pair orbital on the scissile bond oxygen or nitrogen antiperiplanar to the adjacent polar bond. The significance of these stereoelectronic effects for the mechanism of action of serine proteases is discussed.

Calorimetry↗

Phosphorus-31 nuclear magnetic resonance of ethidium complexes with ribonucleic acid model systems and phenylalanine-accepting transfer ribonucleic acid.

The temperature dependence of the 31P NMR spectra of the ethidium complexes with poly(A) X oligo(U) and the 31P spectra of phenylalanine tRNA (yeast) in various molar ratios of ethidium ion (Et) are presented. In the poly(A) X oligo(U) X Et complex, a new peak about 2.0 ppm downfield from the double-helix peak appears. We have assigned this peak to phosphates perturbed by ethidium. The chemical shift of this peak is consistent with the intercalation mode of binding and provides additional support for our hypothesis that 31P shifts are sensitive probes of phosphate ester conformations. The main effect of ethidium on the 31P spectra of tRNAPhe is the broadening of several of the scattered signals. These scattered signals are associated with phosphates involved in tertiary interactions. We propose that these broadened signals arise from phosphates near the Et binding site.

Ethidium↗

High-resolution phosphorus nuclear magnetic resonance spectroscopy of transfer ribonucleic acids: multiple conformations in the anticodon loop.

The temperature dependence of the 31P NMR spectra of yeast phenylalanine tRNA, E. coli tyrosine, glutamate (2), and formylmethionine tRNA is presented. The major difference between the 31P NMR spectra of the different acceptor tRNAs is in the main cluster region between -0.5 and -1.3 ppm. This confirms an earlier assignment of the main cluster region to the undistorted phosphate diesters in the hairpin loops and helical stems. In addition the 31P NMR spectra for all tRNAs reveal approximately 16 nonhelical diester signals spread over approximately 7 ppm besides the downfield terminal 3'-phosphate monoester. In the presence of 10 mM Mg2+ most scattered and main cluster signals do not shift between 22 and 66 degrees C, thus supporting our earlier hypothesis that 31P chemical shifts are sensitive to phosphate ester torsional and bond angles. At greater than 70 degrees C, all of the signals merge into a single random-coil conformation signal. A number of the scattered peaks are shifted (0.2-1.7 ppm) and broadened between 22 and 66 degrees C in the presence of Mg2+ and spermine as a result of a conformational transition in the anticodon loop. The 31P NMR spectrum of the dimer formed between yeast tRNAPhe and E. coli tRNA 2Glu is reported. This dimer simulates codon-anticodon interaction since the anticodon triplets of the two tRNAs are complementary. Evidence is presented that the anticodon-anticodon interaction alters the anticodon conformation and partially disrupts the tertiary structure of the tRNA.

Anticodon↗

Proton and fluorine nuclear magnetic resonance spectroscopic observation of hemiacetal formation between N-acyl-p-fluorophenylalaninals and alpha-chymotrypsin.

Proton nuclear magnetic resonance (NMR) spectroscopy shows that the free aldehyde and not the hydrate of N-acetyl-DL-p-fluorophenylalaninal binds to alpha-chymotrypsin. A proton NMR cross-saturation experiment shows that the initial noncovalent complex is in equilibrium with a hemiacetal formed between the aldehyde and the active site serine residue. Fluorine NMR spectra of N-acetyl-DL- (and N-acetyl-L-) p-fluorophenylalaninal in the presence of alpha-chymotrypsin show separate signals for the hemiacetal complex, the bound aldehyde, the free aldehyde, and the free hydrate. N-Benzoyl-DL-p-fluorophenylalaninal fluorine NMR signals are also observed for all species except the bound aldehyde form in the presence of alpha-chymotrypsin. The D and L enantiomers of the hydrate of the N-acetyl aldehyde inhibitor give separate fluorine NMR signals, arising from chemical exchange between the L-aldehyde-alpha-chymotrypsin complex and the free L hydrate. The enzyme-bound inhibitor fluorine signals disappear upon proton decoupling due to a negative nuclear Overhauser effect. Upon gated decoupling of protons, the L hydrate and free aldehyde fluorine signals are reduced in intensity relative to that of the D hydrate signal in the racemate aldehyde complex. This is attributed to a saturation transfer of the heteronuclear nuclear Overhauser effect.

Animals↗

High resolution phosphorus NMR spectroscopy of transfer ribonucleic acids.

The temperature dependence of the 31P NMR spectra of yeast phenylalanine tRNA, E. coli tyrosine, glutamate (2), and formylmethione tRNA, and bovine liver aspartate (2b) tRNA is presented. The major difference between the 31P NMR spectra of the different acceptor tRNAs is in the main cluster region between -0.5 and -0.3 ppm. This confirms earlier assignment of the main cluster region to the undistorted phosphate diesters in the hair-pin loops and helical stems. In addition the 31P NMR spectra for all tRNAs reveal approximately 16 non-helical diester signals spread over approximately 7 ppm besides the downfield terminal 3'-phosphate monoester. In the presence of 10 mM Mg++, most scattered and main cluster signals do not shift between 22 and 66 degrees C, thus supporting our earlier hypothesis that 31P chemical shifts are sensitive to phosphate ester torsional and bond angles. At greater than 70 degrees, all of the signals merge into a single random coil conformation signal. Measured spin-lattice and spin-spin relaxation times for tRNAPhe reveal another lower temperature transition associated with a conformational change of the anticodon loop besides the thermal denaturation process. A number of the scattered peaks are shifted (0.2--1.7 ppm) and broadened between 22 and 66 degrees C in the presence of Mg++ as a result of this conformational transition. The effects Mg++ and Mn++ ions on the 31P NMR spectra of tRNAPhe have been used to identify some of the scattered signals upfield and downfield from the main cluster signals. The 31P NMR spectrum of the dimer formed between yeast tRNAPhe and E. coli tRNA2Glu is reported. This dimer stimulates codon-anticodon interaction since the anticodon triplets of the two tRNAs are complementary. Evidence is presented that the anticodon-anticodon interaction alters the anticodon conformation and partially disrupts the tertiary structure of the tRNA.

Animals↗

Phosphorus-31 nuclear magnetic resonance of double- and triple-helical nucleic acids. Phosphorus-31 chemical shifts as a probe of phosphorus-oxygen ester bond torsional angles.

The temperature dependence to the 31P NMR spectra of poly[d(GC)] . poly [d(GC)],d(GC)4, phenylalanine tRNA (yeast) and mixtures of poly(A) + oligo(U) is presented. The 31P NMR spectra of mixtures of complementary RNA and of the poly d(GC) self-complementary DNA provide torsional information on the phosphate ester conformation in the double, triple, and "Z" helix. The increasing downfield shift with temperature of the single-strand nucleic acids provides a measure of the change in the phosphate ester conformation in the single helix to coil conversion. A separate upfield peak (20-60% of the total phosphates) is observed at lower temperatures in the oligo(U) . poly(A) mixtures which is assigned to the double helix/triple helix. Proton NMR and UV spectra confirm the presence of the multistrand forms. The 31P chemical shift for the double helix/triple helix is 0.2-0.5 ppm upfield from the chemical shift for the single helix which in turn is 1.0 ppm upfield from the chemical shift for the random coil conformation.

Magnetic Resonance Spectroscopy↗

High-resolution phosphorus nuclear magnetic resonance spectra of yeast phenylalanine transfer ribonucleic acid. Metal ion effects and tentative partial assignment of signals.

The temperature and metal ion dependence of the 31P NMR spectra of yeast phenylalanine tRNA is presented, and a tentative assignment of some of the individual phosphate signals is offered. Signals A, C, F, P, and T have been assigned to the magnesium binding site of phosphates by monitoring the magnesium ion dependence in the 31P NMR spectra. In the presence of 10 mM Mg2+, specific paramagnetic line broadening effects are observed for signals A, D, E, and U upon addition of 0.001-0.1 Mn2+ ion per tRNA molecule. Through the combination of the above metal in experiments, X-ray studies, and earlier 1H and 31P NMR studies [particularly the tRNA modification 31P NMR experiments of Salemink et al. [Salemink, P..J.M., Swarthof T., & Hilbers, C.W. (1979) Biochemistry 18, 3477]], an initial assignment of some of these signals is attempted.

Base Sequence↗

High-resolution phosphorus nuclear magnetic resonance spectra of yeast phenylalanine transfer ribonucleic acid. Melting curves and relaxation effects.

In a continuation of our studies on structural effects on the 31P chemical shifts of nucleic acids, we present 31P NMR spectra of yeast phenylalanine tRNA in the presence and absence of Mg2+. Superconducting field (146 MHz) and 32-MHz 31P NMR spectra reveal approximately 15 nonhelical diester signals spread over approximately 7 ppm besides the downfield terminal 3'-phosphate monoester. In the presence of 10 mM Mg2+, most scattered and main cluster signals do not shift between 22--66 degrees C, thus supporting our earlier hypothesis that 31P chemical shifts are sensitive to phosphate ester torsional and bond angles. At 70 degrees C, all of the signals merge into a single random coil conformation signal. Similar effects are observed in the absence of Mg2+ except that the transition melting temperature is approximately 20 degrees C lower. Measured spin-lattice and spin-spin relaxation times reveal another lower temperature transition besides the thermal denaturation process. A number of the scattered peaks are shifted (0.2--1.7 ppm) and broadened between 22 and 66 degrees C in the presence of Mg2+ as a result of this conformational transition between two intact tertiary structures. The loss of the scattered peaks in the absence of Mg2+ occurs in the temperature range expected for melting of a tertiary structure. An attempt to simulate the 31P spectra of tRNA Phe based upon the X-ray crystallographically determined phosphate ester torsional agles supports the suggestion that the large shifts in the scattered peaks are due to bond angle distortions in the tertiary structure.

Kinetics↗

Evidence for hemiacetal formation between N-acyl-L-phenylalaninals and alpha-chymotrypsin by cross-saturation nuclear magnetic resonance spectroscopy.

N-Acetyl-L-phenylalaninal exists predominantly in its hydrated form in aqueous solution, but the aldehyde and not the hydrate is shown by nuclear magnetic resonance (NMR) spectroscopy to be the effective inhibitor of alpha-chymotrypsin. NMR spectroscopy also indicates that the initial alpha-chymotrypsin-N-acetyl-L-phenylalaninal complex is in equilibrium with a hemiacetal formed between the aldehyde and the active site serine residue. The rate of the latter equilibration is slow on the NMR time scale but the hemiacetal can be detected by cross-saturation NMR spectroscopy. N-Benzoyl-L-phenylalaninal is a more potent inhibitor of alpha-chymotrypsin than the N-acetyl derivative and both the formation of the enzyme-inhibitor complex and the hemiacetal are slow on the NMR time scale, but the hemiacetal in the enzyme can be detected by cross-saturation NMR spectroscopy. The N-acyl-L-phenylalaninals also bind to N-methylhistidinyl-57-alpha-chymotrypsin, but clear evidence for hemiacetal formation was not obtained by cross-saturation NMR spectroscopy either because the hemiacetal was not formed or more probably because the rate of dissociation was slow compared with the rate of relaxation of the hemiacetal proton. The dissociation constant of N-benzoyl-L-phenylalaninal to dehydroalaninyl-195-alpha-chymotrypsin was found to be high relative to the dissociation constant to native alpha-chymotrypsin, supporting the NMR evidence that a hemiacetal with the Ser-195 is formed on association of N-benzoyl-L-phenylalaninal with alpha-chymotrypsin.

Acetals↗