Biomedical subjects
D G Gorenstein
Publications and source records attributed to D G Gorenstein.
Effect of Elicitation and Changes in Extracellular pH on the Cytoplasmic and Vacuolar pH of Suspension-Cultured Soybean Cells.
We have employed both (31)P nuclear magnetic resonance spectroscopy and two intracellular fluorescent pH indicator dyes to monitor the pH of the vacuole and cytoplasm of suspension-cultured soybean cells (Glycine max Merr cv Kent). For the (31)P nuclear magnetic resonance studies, a flow cell was constructed that allowed perfusion of the cells in oxygenated growth medium throughout the experiment. When the perfusion medium was transiently adjusted to a pH higher than that of the ambient growth medium, a rapid elevation of vacuolar pH was observed followed by a slow (approximately 30 minute) return to near resting pH. In contrast, the concurrent pH changes in the cytoplasm were usually fourfold smaller. These data indicate that extracellular pH changes are rapidly communicated to the vacuole in soybean cells without significantly perturbing cytoplasmic pH. When elicitors were dissolved in a medium of altered pH and introduced into the cell suspension, the pH of the vacuole, as above, quickly reflected the pH of the added elicitor solution. In contrast, when the pH of either a polygalacturonic acid or Verticillium dahliae elicitor preparation was adjusted to the same pH as the ambient medium, no significant change in either vacuolar or cytoplasmic pH was observed during the 35 minute experiment. These results were confirmed in experiments with pH-sensitive fluorescent dyes. We conclude that suspension-cultured soybean cells do not respond to elicitation by significantly changing the pH of their vacuolar or cytoplasmic compartments.
How accurately can oligonucleotide structures be determined from the hybrid relaxation rate matrix/NOESY distance restrained molecular dynamics approach?
The accuracy and precision of structures derived from a combined hybrid relaxation rate matrix/NOESY distance restrained molecular dynamics methodology were examined with simulations that included typical experimental errors. NOESY data were simulated for a DNA dodecamer duplex, d-(CGCGAATTCGCG)2, with added volume error of approximately 20% and low-level thermal noise. Distances derived from a hybrid relaxation matrix analysis of the NOE data were used as constraints in molecular dynamics driven structural refinements of several initial model geometries. The final structures were compared against results obtained from the traditional isolated two-spin approximation treatment of these NOESY volumes and also against refined structures that employed error-free data. Results show that the structures derived from the relaxation rate matrix analysis of the NOESY data are more accurate than those derived from a simple two-spin approximation analysis and it is possible to achieve refinement to the level of simulated experimental error. Results may be significantly improved with the use of either more accurately measured NOESY volumes or additional matrix-derived constraints. Many of the helical parameters and backbone torsional angles may be accurately reproduced by the hybrid matrix methodology.
Two-dimensional NMR and structure determination of salmon calcitonin in methanol.
The structure of the 32-residue peptide salmon calcitonin (sCT) in 90% MeOH-10% H2O has been investigated by two-dimensional NMR techniques and molecular modeling. Sequential assignments for nearly all of the 32 spin systems have been obtained, and results indicate that the heptaresidue loop formed by the disulfide bond between Cys-1 and Cys-7 is followed by an alpha-helical segment from Val-8 through Tyr-22. A region of conformational heterogeneity is observed for residues 20-25, resulting from the slow isomerism of the cis and trans forms of Pro-23. The C-terminal segment is found to exist in an extended conformation.
NMR structural refinement of a tandem G.A mismatched decamer d(CCAAGATTGG)2 via the hybrid matrix procedure.
A complete relaxation matrix approach employing a matrix eigenvalue/eigenvector solution to the Bloch equations is used to evaluate the NMR solution structure of a tandemly positioned G.A double mismatch decamer oligodeoxyribonucleotide duplex, d(CCAAGATTGG)2. An iterative refinement method using a hybrid relaxation matrix combined with restrained molecular dynamics calculations is shown to provide structures having good agreement with the experimentally derived structures. Distances incorporated into the MD simulations have been calculated from the relaxation rate matrix evaluated from a hybrid NOESY volume matrix whose elements are obtained from the merging of experimental and calculated NOESY intensities. Starting from both A- and B-DNA and mismatch syn and anti models, it is possible to calculate structures that are in good atomic RMS agreement with each other (less than 1.6 A RMS) but differ from the reported crystal structure (greater than 3.6 A). Importantly, the hybrid matrix derived structures are in excellent agreement with the experimental solution conformation as determined by comparison of the 200-ms simulated and experimental NOESY spectra, while the crystallographic data provide spectra that are grossly different.
2D NMR and structural model for a mitochondrial signal peptide bound to a micelle.
The 19 amino acid signal peptide of rat liver aldehyde dehydrogenase, possessing a lysine substitution for an arginine and containing 3 extra amino acid residues at the C terminus, was studied by two-dimensional NMR in a dodecylphosphocholine micelle. In this membrane-like environment, the peptide contains two alpha-helical regions, both of which are amphiphilic, separated by a hinge region. The helix located closer to the C terminus is more stable than is the helix located near the N terminus. This suggests that the hydrophobic face of the C-terminal helix is buried within the hydrophobic region of the micelle. On the basis of these results a general model for protein translocation is presented in which the C-terminal amphiphilic helix of the signal region in the preprotein first binds to the mitochondrial membrane and then diffuses to the translocation receptor. The receptor then recognizes the N-terminal helix of the signal region, which is not anchored to the membrane. To explain how this signal peptide was imported into isolated mitochondria in the absence of energy or receptor protein [Pak, Y. K., & Weiner, H. (1990) J. Biol. Chem. 265, 14298-14307], a model for signal peptide translocation across a membrane barrier without the need for auxiliary membrane proteins is proposed. In this model the faces of the two helices fold upon each other, resulting in the mutual shielding of positively charged residues by the complementary hydrophilic face of the other amphiphilic helix.
Two-dimensional 1H and 31P NMR spectra and restrained molecular dynamics structure of a covalent CPI-CDPI2-oligodeoxyribonucleotide decamer complex.
CPI-CDPI2 is a synthetic analogue of CC-1065, which is a naturally occurring antitumor antibiotic. Assignment of the 1H NMR spectra of a CPI-CDPI2-oligodeoxyribonucleotide decamer, d-(CGCTTAAGCG)2, complex has been made by two-dimensional 1H/1H spectroscopy. The solution structure of the complex was calculated by an iterative hybrid relaxation matrix method combined with NOESY distance restrained molecular dynamics. Refinement proceeded in two steps in which the decamer was initially refined alone and then CPI-CDPI2 was added to the structure to allow initial estimates of drug-DNA contacts. A hybrid matrix/MD refinement was used to better take into account problems associated with spin diffusion. Thus the distances from the 2D NOESY spectra were calculated from the relaxation rate matrix which were evaluated from a hybrid NOESY volume matrix comprising elements from the experimental spectrum and those calculated from an initial structure. The hybrid matrix derived distances were then used in a restrained molecular dynamics procedure to obtain a new structure that better approximates the NOESY spectra. The resulting partially refined structure was then used to calculate an improved theoretical NOESY volume matrix which is once again merged with the experimental matrix until refinement is complete. The efficacy of CC-1065 has been attributed to its minor groove binding and alkylation to the N3 position of adenosine. CPI-CDPI2 appears to bind to the decamer in a similar manner. The effect of CPI-CDPI2 on the decamer's 1H and 31P spectrum was consistent with a minor groove binding motif with the drug alkylating at A17 with the CDPI rings oriented toward the 5'-end of the alkylated strand. In addition, the NMR data support one major adduct but also indicate the presence of a minor adduct. The latter could represent a drug alkylation of the DNA at a secondary site (or alternative orientation of the rings).
Two-dimensional 1H and 31P NMR spectra and restrained molecular dynamics structure of a mismatched GA decamer oligodeoxyribonucleotide duplex.
Assignment of the 1H and 31P NMR spectra of a tandem G.A mismatched base pair decamer oligodeoxyribonucleotide duplex, d(CCAAGATTGG)2, has been made by two-dimensional 1H-1H and heteronuclear 31P-1H correlated spectroscopy. Unusual downfield 31P resonances have been assigned by a pure absorption phase constant-time heteronuclear 31P-1H correlated spectrum to be associated with the phosphates on the 5'- and 3'-sides of the mismatched guanosine residue. JH3'-P coupling constants for each of the phosphates of the decamer were obtained from the 1H-31P J-resolved selective proton-flip 2D spectrum. The two most downfield-shifted 31P resonances each appear to consist of two overlapping signals that can be resolved into two distinct doublets with different coupling constants in the J-resolved spectrum. This as well as the temperature dependence of the 31P spectra demonstrates that two distinct conformations exist at lower temperatures. By use of a modified Karplus relationship, the C4'-C3'-O3'-P torsional angles (epsilon) were obtained. A linear correlation between 31P chemical shifts and the measured coupling constants is quite good (only when the larger set of coupling constants of the two most downfield 31P signals is included). The 31P chemical shifts as well as the measured coupling constants tend to follow the positional variation seen in other duplexes of interior phosphates resonating more upfield than terminal residues and of interior phosphates exhibiting smaller coupling constants; however, this pattern is disrupted at the site of the mismatch. Modeling and initial NOESY distance restrained molecular mechanics energy minimization and restrained molecular dynamics support previous observations that the mismatched guanine and adenine bases are both in anti conformations. Most significantly, the epsilon backbone torsional angle variaions calculated from the NOESY distance restrained structures are in agreement with both the crystal structure values and the measured JH3'-P coupling constants.
31P NMR spectra of an oligodeoxyribonucleotide duplex lac operator-repressor headpiece complex.
The interaction of a symmetric lac operator duplex, d(TGTGAGCGCTCACA)2, with the N-terminal 56-residue headpiece fragment of the lac repressor protein was monitored by 31P NMR spectroscopy. The changes in the 31P chemical shifts upon addition of the headpiece demonstrated an end point of two headpiece fragments per symmetric 14-mer duplex with each headpiece binding to the T1pG2pT3pG4pA5 ends of the duplex. The specific phosphate 31P perturbations observed are consistent with those residues implicated in protein binding by previous NMR, molecular biological, and biochemical techniques. Upon complexation, the 31P signals of phosphates G2-A5 showed upfield or downfield shifts (less than 0.2 ppm) while most other residues were unperturbed. The interactions were dependent on ionic strength. The 31P NMR data provide direct evidence for predominant recognition of the 5' strand of the 5'-TGTGA/3'-ACACT binding site.
Effect of distortions in the deoxyribose phosphate backbone conformation of duplex oligodeoxyribonucleotide dodecamers containing GT, GG, GA, AC, and GU base-pair mismatches on 31P NMR spectra.
We have previously suggested that variations in the 31P chemical shifts of individual phosphates in duplex oligonucleotides are attributable to torsional angle changes in the deoxyribose phosphate backbone. This hypothesis is not directly supported by analysis of the 1H/31P two-dimensional J-resolved spectra of a number of mismatch dodecamer oligonucleotide duplexes including the following sequences: d-(CGTGAATTCGCG), d(CGUGAATTCGCG), d(CGGGAATTCGCG), d(CGAGAATTCGCG), and d(CGCGAATTCACG). The 31P NMR signals of the dodecamer mismatch duplexes were assigned by 2D 1H/31P pure absorption phase constant time (PAC) heteronuclear correlation spectra. From the assigned H3' and H4' signals, the 31P signals of the base-pair mismatch dodecamers were identified. JH3'-P coupling constants for each of the phosphates of the dodecamers were obtained from 1H/31P J-resolved selective proton flip 2D spectra. By use of a modified Karplus relationship, the C4'-C3'-O3'-P torsional angles (epsilon) were obtained. JH3'-P coupling constants were measured for many of the oligonucleotides as a function of temperature. There exists a good linear correlation between 31P chemical shifts and the epsilon torsional angle. This correlation can be further extended to the C3'-O3'-P-O5' torsional angle (zeta) by using a linear relationship between epsilon and zeta obtained from crystal structure studies. The 31P chemical shifts follow the general observation that the more internally the phosphate is located within the oligonucleotide sequence, the more upfield the 31P resonance occurs. In addition, 31P chemical shifts show sequence- and site-specific variations. Analysis of the backbone torsional angle variations from the coupling constant analysis has provided additional information regarding the origin of these variations in 31P chemical shifts.
NMR structural refinement of an extrahelical adenosine tridecamer d(CGCAGAATTCGCG)2 via a hybrid relaxation matrix procedure.
Until very recently interproton distances from NOESY experiments have been derived solely from the two-spin approximation method. Unfortunately, even at short mixing times, there is a significant error in many of these distances. A complete relaxation matrix approach employing a matrix eigenvalue/eigenvector solution to the Bloch equations avoids the approximation of the two-spin method. We have calculated the structure of an extrahelical adenosine tridecamer oligodeoxyribonucleotide duplex, d(CGCAGAATTCGCG)2, by an iterative refinement approach using a hybrid relaxation matrix method combined with restrained molecular dynamics calculations. Distances from the 2D NOESY spectra have been calculated from the relaxation rate matrix which has been evaluated from a hybrid NOESY volume matrix comprising elements from the experiment and those calculated from an initial structure. The hybrid matrix derived distances have then been used in a restrained molecular dynamics procedure to obtain a new structure that better approximates the NOESY spectra. The resulting partially refined structure is then used to calculate an improved theoretical NOESY volume matrix which is once again merged with the experimental matrix until refinement is complete. Although the crystal structure of the tridecamer clearly shows the extrahelical adenosine looped out way from the duplex, the NOESY distance restrained hybrid matrix/molecular dynamics structural refinement establishes that the extrahelical adenosine stacks into the duplex.
Two-dimensional 1H and 31P NMR spectra and restrained molecular dynamics structure of an oligodeoxyribonucleotide duplex refined via a hybrid relaxation matrix procedure.
Assignment of the 1H and 31P resonances of a decamer DNA duplex, d(CGCTTAAGCG)2 was determined by two-dimensional COSY, NOESY and 1H-31P Pure Absorption phase Constant time (PAC) heteronuclear correlation spectroscopy. The solution structure of the decamer was calculated by an iterative hybrid relaxation matrix method combined with NOESY-distance restrained molecular dynamics. The distances from the 2D NOESY spectra were calculated from the relaxation rate matrix which were evaluated from a hybrid NOESY volume matrix comprising elements from the experiment and those calculated from an initial structure. The hybrid matrix-derived distances were then used in a restrained molecular dynamics procedure to obtain a new structure that better approximates the NOESY spectra. The resulting partially refined structure was then used to calculate an improved theoretical NOESY volume matrix which is once again merged with the experimental matrix until refinement is complete. JH3'-P coupling constants for each of the phosphates of the decamer were obtained from 1H-31P J-resolved selective proton flip 2D spectra. By using a modified Karplus relationship the C4'-C3'-O3'-P torsional angles (epsilon) were obtained. Comparison of the 31P chemical shifts and JH3'-P coupling constants of this sequence has allowed a greater insight into the various factors responsible for 31P chemical shift variations in oligonucleotides. It also provides an important probe of the sequence-dependent structural variation of the deoxyribose phosphate backbone of DNA in solution. These correlations are consistent with the hypothesis that changes in local helical structure perturb the deoxyribose phosphate backbone. The variation of the 31P chemical shift, and the degree of this variation from one base step to the next is proposed as a potential probe of local helical conformation within the DNA double helix. The pattern of calculated epsilon and zeta torsional angles from the restrained molecular dynamics refinement agrees quite well with the measured JH3'-P coupling constants. Thus, the local helical parameters determine the length of the phosphodiester backbone which in turn constrains the phosphate in various allowed conformations.
Two-dimensional 1H and 31P NMR spectra and restrained molecular dynamics structure of an extrahelical adenosine tridecamer oligodeoxyribonucleotide duplex.
Assignment of the 1H and 31P NMR spectra of an extrahelical adenosine tridecamer oligodeoxyribonucleotide duplex, d(CGCAGAATTCGCG)2, has been made by two-dimensional 1H-1H and heteronuclear 31P-1H correlated spectroscopy. The downfield 31P resonance previously noted by Patel et al. (1982) has been assigned by both 17O labeling of the phosphate as well as a pure absorption phase constant-time heteronuclear 31P-1H correlated spectrum and has been associated with the phosphate on the 3' side of the extrahelical adenosine. JH3'-P coupling constants for each of the phosphates of the tridecamer were obtained from the 1H-31P J-resolved selective proton-flip 2D spectrum. By use of a modified Karplus relationship the C4-C3'-O3-P torsional angles (epsilon) were obtained. There exists a good linear correlation between 31P chemical shifts and the epsilon torsional angle. The 31P chemical shifts and epsilon torsional angles follow the general observation that the more internal the phosphate is located within the oligonucleotide sequence, the more upfield the 31P resonance occurs. Because the extrahelical adenosine significantly distorts the deoxyribose phosphate backbone conformation even several bases distant from the extrahelical adenosine, 31P chemical shifts show complex site- and sequence-specific variations. Modeling and NOESY distance-restrained energy minimization and restrained molecular dynamics suggest that the extrahelical adenosine stacks into the duplex. However, a minor conformation is also observed in the 1H NMR, which could be associated with a structure in which the extrahelical adenosine loops out into solution.
Sequence-dependent variations in the 31P NMR spectra and backbone torsional angles of wild-type and mutant Lac operator fragments.
Assignment of the 31P resonances of a series of six sequenced-related tetradecamer DNA duplexes, d(TGTGAGCGCTCACA)2, d(TATGAGCGCTCATA)2, d(TCTGAGCGCTCAGA)2, d(TGTGTGCGCACACA)2, d(TGTGACGCGTCACA)2 and d(CACAGTATACTGTG)2, related to the lac operator DNA sequence was determined either by site-specific 17O labeling of the phosphoryl groups or by two-dimensional 1H-31P pure absorption phase constant time (PAC) heteronuclear correlation spectroscopy. J(H3'-P) coupling constants for each of the phosphates of the tetradecamers were obtained from 1H-31P J-resolved selective proton flip 2D spectra. By use of a modified Karplus relationship the C4'-C3'-O3'-P torsional angles (epsilon) were obtained. Comparison of the 31P chemical shifts and J(H3'-P) coupling constants of these sequences has allowed greater insight into those various factors responsible for 31P chemical shift variations in oligonucleotides and provided an important probe of the sequence-dependent structural variation of the deoxyribose phosphate backbone of DNA in solution. These sequence-specific variations in the conformation of the DNA sugar phosphate backbone of various lac operator DNA sequences can possibly explain the sequence-specific recognition of DNA by DNA binding proteins, as mediated through direct contacts between the phosphates and the protein.
31P NMR spectra of ethidium, quinacrine, and daunomycin complexes with poly(adenylic acid).poly(uridylic acid) RNA duplex and calf thymus DNA.
31P NMR provides a convenient monitor of the phosphate ester backbone conformational changes upon binding of the intercalating drugs ethidium, quinacrine, and daunomycin to sonicated poly(A).poly(U) and calf thymus DNA. 31P chemical shifts can also be used to assess differences in the duplex unwinding angles in the presence of the drug. Thus a new 31P signal, 1.8-2.2 ppm downfield from the double-stranded helix signals, is observed in the ethidium ion-poly(A).poly(U) complex. This signal arises from phosphates which are in perturbed environments due to intercalation of the drug. This is in keeping with the hypothesis that the P-O ester torsional angle in phosphates linking the intercalated base pairs is more trans-like. Similar though smaller deshielding of the 31P signals is observed in sonicated poly(A).poly(U)-quinacrine complexes as well as in the daunomycin complexes. The effect of added ethidium ion, quinacrine, and daunomycin on the 31P spectra of sonicated calf thymus DNA is consistent with Wilson and Jones' (1982) earlier study. In these drug-DNA complexes the drug produces a gradual downfield shift in the DNA 31P signal without the appearance of a separate downfield peak. These differences are attributed to differences in the rate of chemical exchange of the drug between free and bound duplex states. The previous correlation of 31P chemical shift with drug duplex unwinding angle (Wilson & Jones, 1982) is confirmed for both the RNA and DNA duplexes.
UDP-galactose 4-epimerase. Phosphorus-31 nuclear magnetic resonance analysis of NAD+ and NADH bound at the active site.
The phosphorus atoms of NAD+ bound within the active site of UDP-galactose 4-epimerase from Escherichia coli exhibit two NMR signals, one at delta = -9.60 +/- 0.05 ppm and one at delta = -12.15 +/- 0.01 ppm (mean +/- standard deviation of four experiments) relative to 85% H3PO4 as an external standard. Titration of epimerase.NAD+ with UMP causes a UMP-dependent alteration in the chemical shifts of the resulting exchange-averaged spectra, which extrapolate to delta = -10.51 ppm and delta = -11.06 ppm, respectively, for the fully liganded enzyme, with an interconversion rate between epimerase.NAD+ and epimerase.NAD+.UMP of at least 490 s-1. Conversely, the binding of 8-anilinonaphthalene-1-sulfonate, which is competitive with UMP, causes a significant sharpening of the epimerase.NAD+ resonances but very little alteration in their chemical shifts, to delta = -9.38 ppm and delta = -12.16 ppm, respectively. UMP-dependent reductive inactivation by glucose results in the convergence of the two resonances into a single signal of delta = -10.57 ppm, with an off-rate constant for UMP dissociation from the epimerase.NADH.UMP complex estimated at 8 s-1. Reductive inactivation by borohydride under anaerobic conditions yields a single, broad resonance centered at about delta = -10.2 ppm. The data are consistent with, and may reflect, the activation of NAD+ via a protein conformational change, which is known from chemical studies to be driven by uridine nucleotide binding. Incubation of epimerase.NAD+ with UMP in the absence of additional reducing agents causes a very slow reductive inactivation of the enzyme with an apparent pseudo-first-order rate constant of 0.013 +/- 0.001 h-1, which appears to be associated with liberation of inorganic phosphate from UMP.
31P NMR of covalent phosphorylated derivatives of alpha-chymotrypsin.
The structures of various covalent phosphorylated derivatives of alpha-chymotrypsin (alpha-CT) have been studied by 31P NMR spectroscopy. Diisopropylphosphoryl-alpha-chymotrypsin (alpha-DIPCT) shows a single 31P signal at ca. 0.0 ppm (pH 4). At low pH, the 31P NMR spectrum of alpha-DIPCT gradually changed with the appearance of one or two additional peaks. The ratio of the peaks varied with pH, time, and concentration. One of these two new downfield peaks (both at ca. 2.0 ppm) has been previously identified by Markley and co-workers (Markley, 1979; Porubcan et al., 1979) and van der Drift et al. (1985) as an aged monoisopropylphosphoryl-alpha-chymotrypsin (alpha-MIPCT) and is confirmed by our studies. A new additional downfield signal, separate from the alpha-MIPCT signal, is attributed to a dimer of the phosphorylated alpha-DIPCT. Phosphorylation of the enzyme with diphenyl chlorophosphate yields a monophenylphosphoryl-alpha-chymotrypsin (alpha-MPPCT) that also showed a single 31P signal at -2.1 ppm (pH 7). However, the spectrum did not change as a function of pH, incubation time, or concentration. Comparison of the 31P chemical shifts of the native and denatured phosphorylated derivatives of alpha-chymotrypsin suggests changes in the conformation about the P-O ester bonds are at least partially responsible for the various 31P chemical shift differences.
Solution conformation of a synthetic fragment of human pituitary growth hormone. Two-dimensional NMR of an alpha-helical dimer.
Circular dichroism and two-dimensional NMR spectra indicate that a peptide fragment consisting of the first 28 residues from the N-terminus of human growth hormone (hGH 1-28) has considerable alpha-helical structure. The peptide, (1) H-Phe-Pro-Thr-Ile-Pro-Leu-Ser-Arg-Leu-Phe-Asp-Asn-Ala-Met-Leu-Arg-Ala-Hi s-Arg- Leu-His-Gln-Leu-Ala-Phe-Asp-Thr-Tyr-OH (28), was synthesized on an automated peptide synthesizer using the Merrifield solid-phase method. The peptide can be modeled as an amphiphilic helix, and the unusual stability of the alpha-helix in aqueous solution is suggested to be attributable to formation of a dimer of alpha-helices. Most of the 1H NMR signals were assigned through pure absorption phase COSY/NOESY and single- and double-relay COSY 2D NMR spectra by using the sequential assignment methodology. The NOEs were large and negative, suggesting that the peptide was not a random coil and that it existed in solution primarily as a large, fairly rigid macromolecule, consistent with the dimer structure. A network of N alpha Hi-N alpha Hi+1 NOESY crosspeaks is observed from residues 13 to 18 as are several other crosspeaks which indicate that the peptide has considerable alpha-helical structure between residues 8 and 24. In addition, gel filtration of the peptide is consistent with a dimer structure, presumably involving packing of the two hydrophobic faces of the amphiphilic alpha-helices.