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P Kollman

Publications and source records attributed to P Kollman.

17 recordsLinked to original sources
PubMed1999

The free energies for mutating S27 and W79 to alanine in streptavidin and its biotin complex: the relative size of polar and nonpolar free energies on biotin binding.

We have carried out calculations on the relative free energy of binding of biotin and its S27A and W79A mutants to streptavidin. Consistent with earlier suggestions by Miyamoto and Kollman from free energy component analysis and recent experiments by Stayton and coworkers, the reduction in binding strength by the W79A mutant is significantly larger than that of the S27A mutant. Proteins 1999;36:471-473.

Alanine↗
PubMed1997

Graphical visualization of mean hydration from molecular dynamics simulations.

How does one characterize water solvating a complex solute? Specific hydration of proteins and nucleic acids plays a key role in many biological processes. However, traditional pairwise descriptions of solvent structure (radial distribution functions, etc.) are incapable of adequately describing the hydration of these complex solutes. We have developed methods to visualize the average three-dimensional water structure surrounding a solute, as seen in a molecular dynamics (MD) simulation. Applications to simple solutes [sodium ion, N-methyl acetamide, 18-crown-6, (hydroxymethyl)phenols] are presented, and the extension of the method to larger molecules of biochemical interest is discussed.

Acetamides↗
PubMed1992

Comparison of solution structures of mutant bovine pancreatic trypsin inhibitor proteins using two-dimensional nuclear magnetic resonance.

Structural perturbations due to a series of mutations at the 30-51 disulfide bond of bovine pancreatic trypsin inhibitor have been explored using NMR. The mutants replaced cysteines at positions 30 and 51 by alanine at position 51 and alanine, threonine, or valine at position 30. Chemical shift changes occur in residues proximate to the site of mutation. NOE assignments were made using an automated procedure, NASIGN, which used information from the wild-type crystal structure. Intensity information was utilized by a distance geometry algorithm, VEMBED, to generate a series of structures for each protein. Statistical analyses of these structures indicated larger averaged structural perturbations than would be expected from crystallographic and other information. Constrained molecular dynamics refinement using AMBER at 900 K was useful in eliminating structural movements that were not a necessary consequence of the NMR data. In most cases, statistically significant movements are shown to be those greater than approximately 1 A. Such movements do not appear to occur between wild type and A30A51, a result confirmed by crystallography (Eigenbrot, C., Randal, M., & Kossiakoff, A.A., 1990, Protein Eng. 3, 591-598). Structural alterations in the T30A51 or V30A51 mutant proteins near the limits of detection occur in the beta-loop (residues 25-28) or C-terminal alpha-helix, respectively.

Amino Acid Sequence↗
PubMed1991

Free energy perturbation calculations on binding and catalysis after mutating threonine 220 in subtilisin.

We present the results of free energy perturbation calculations on binding and catalysis of a tetrapeptide substrate, acetyl-Phe-Ala-Ala-Phe-NMe, by native subtilisin BPN' and a subtilisin BPN' mutant (Thr220----Ala220). The calculated difference in the free energy of binding was 0.70 +/- 0.72 kcal/mol. The calculated difference in the free energy of catalysis was 1.48 +/- 0.89 kcal/mol. These calculated values compare well with the experimental values in which another substrate, succinyl-Ala-Ala-Pro-Phe-p-nitroanilide, was used. These findings suggest that Thr220 is more important for catalysis than substrate binding.

Amino Acid Sequence↗
PubMed1990

Simulations of the B-DNA molecular dynamics of d(CGCGAATTCGCG)2 and d(GCGCGCGCGC)2: an analysis of the role of initial geometry and a comparison of united and all-atom models.

Molecular dynamics simulations on the sequence d(CGCGAATTCGCG)2 have been carried out using both united atom and all-atom representations, and starting the simulations both from a regular repeating B-DNA structure and from the x-ray single crystal B-DNA structure. An all-atom B-DNA simulation on the sequence d(GCGCGCGCGC)2 has also been carried out, in order to compare it with a previous united atom simulation. The helix repeats, H-bonding, sugar pucker profiles, and average torsional angles are all in the range observed in crystallographic and nmr studies for B-DNA helices. In some of the sequences, there is a significant bend in the DNA helices. The individual helix repeats, with focus on 3'CpG5' and 3'GpC5' units, show the opposite helix repeat to that suggested by Calladine's rules.

Base Sequence↗
PubMed1989

A combined 2D-NMR and molecular dynamics analysis of the structure of the actinomycin D: d(ATGCAT)2 complex.

We present a comparative analysis of an NMR experiment and molecular and harmonic dynamics simulations of an actinomycin D: d(ATGCAT)2 complex. A comparison of NOE measurements and 1/R6 weighted proton-proton distances confirm the general correctness of the Actinomycin D-DNA model proposed by Sobell. There are, however, some substantial differences between the proton-proton distances inferred from the NOE results and the molecular and harmonic dynamics simulations. The remaining discrepancies could either come from contributions of other conformations to the average properties of the complex or from uncertainties in the NMR distance analysis. An analysis of the molecular dynamics helix properties, sugar puckers, hydrogen bonding, rms fluctuations and torsional properties are qualitatively consistent with those from previous simulations, but the presence of an intercalated drug leads to some new structural and dynamical features.

Chemical Phenomena↗
PubMed1987

Molecular mechanics and dynamics calculations on (dA)10.(dT)10 incorporating distance constraints derived from NMR relaxation measurements.

Structural constraints derived from proton NMR relaxation measurements on poly(dA).poly(dT) in the form of interproton separations and orientation have been combined with molecular mechanics and annealed molecular dynamics calculations to derive a model for the solution-state structure of this molecule. Three different possible starting configurations, including the standard A and B forms of Arnott and Hukins [Arnott, S., & Hukins, D. W. L. (1972) Biochem. Biophys. Res. Commun. 47, 1506-1509] and the heteronomous (H) structure [Arnott, S., Chandrasekaran, R., Hall, I. H., & Puigjaner, L. C. (1983) Nucleic Acids Res. 11, 4141-4155], were examined. Both the B- and H-DNA structures converged to the same B-like structure (approximately C2'-endo conformation on both the A and T sugars, glycosidic bond torsional angle of 63-73 degrees) with the same energies and average helical parameters that gave good fits of the NMR relaxation rates. This model also accounts for the experimental observation [Behling, R. W., & Kearns, D. R. (1986) Biochemistry 25, 3335-3346] that the AH2 proton interacts more strongly with the H1' sugar proton on the T strand than on the A strand. Although the helix repeat angle (39 degrees) is larger than that for standard B-DNA (36 degrees), this does not result in a significantly smaller minor groove, as monitored by the interstrand P-P separation. Calculations starting with the A-DNA structure lead to a very high energy structure that gave a poorer fit of the NMR data.

Calorimetry↗
PubMed1985

Molecular dynamics simulations of d(C-G-C-G-A) X d(T-C-G-C-G) with and without "hydrated" counterions.

We present the results of molecular dynamics simulations on d(C-G-C-G-A) X d(T-C-G-C-G) with fully charged phosphates with and without inclusion of counterions. The average structures found in the two simulations are similar, but the simulation with counterions does give an average helix repeat, tilt, and twist in better agreement with those found in the x-ray structure of d(C-G-C-G-A-A-T-T-C-G-C-G)2. The average sugar pucker phases and amplitudes are in qualitative agreement with those found in NMR studies of double-helical DNA, and a number of examples of sugar repuckering from C2' endo to C3' endo carbon conformations in the sugar ring are found. The hydrogen bond correlations as well as torsion correlations are analyzed, and some interesting long-range correlations between dihedral angles are found.

Magnetic Resonance Spectroscopy↗
PubMed1984

The structure of d(CGCGAAT[]TCGCG) . d(CGCGAATTCGCG); the incorporation of a thymine photodimer into a B-DNA helix.

In the light of the biological significance of thymine photodimers , studies of the energetics of the dodecanucleotide fragment d( CGCGAATTCGCG )2 have been carried out using the methods of molecular mechanics, with and without incorporation of a thymine dimer in the cis-syn configuration. The results of the calculations suggest that the thymine dimerized structures show no gross distortion in the double helix with the conformational changes relative to the normal B-DNA double helix restricted largely to the dimer region. The energetics of dTp[]dT reveal a number of conformers which are energetically almost equally favorable and are, as a group, qualitatively consistent with NMR studies on this molecule. The biological implications of the results of the conformational studies, reported here, have been examined vis-a-vis the currently available models for the recognition of DNA "damage" by repair enzymes.

DNA↗
PubMed1981

A molecular mechanical study of complexes formed between 4-nitroquinoline-N-oxide and dinucleoside phosphates.

Molecular mechanical calculations were done on complexes of 4-nitroquinoline-N-oxide (NQO) with various dinucleoside phosphates [(ApT)2, (CpG)2, (GpC)2, and (TpA)2]. Models built using proflavine (uniform C3' endo sugar puckers) and acridine orange (mixed C3' endo (3'-5') C2' endo sugar puckers) dinucleoside phosphate X-ray structures were used in the calculations. Relative binding energies, complex geometries, and various intercalator orientations in the complexes were studied. The results suggest qualitatively different geometries for pyr-(3'-5')-pur and pur-(3'-5')-pyr sequences. Specifically, we find marked distortion in some of the complexes (i.e. there is not a parallel coplanar relationship between the base pairs and intercalator), distortion of the NQO nitro group from planarity in the complexes and mobility of NQO in the intercalation site. We suggest that experimental studies of NQO-dinucleoside phosphate complexes may reveal intercalation complexes which deviate substantially more from a nearly parallel coplanar arrangement of bases and intercalator than has been previously observed.

4-Nitroquinoline-1-oxide↗