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  • 1
    Online Resource
    Online Resource
    AIP Publishing ; 2017
    In:  The Journal of Chemical Physics Vol. 147, No. 16 ( 2017-10-28)
    In: The Journal of Chemical Physics, AIP Publishing, Vol. 147, No. 16 ( 2017-10-28)
    Abstract: The ff15ipq protein force field is a fixed charge model built by automated tools based on the two charge sets of the implicitly polarized charge method: one set (appropriate for vacuum) for deriving bonded parameters and the other (appropriate for aqueous solution) for running simulations. The duality is intended to treat water-induced electronic polarization with an understanding that fitting data for bonded parameters will come from quantum mechanical calculations in the gas phase. In this study, we compare ff15ipq to two alternatives produced with the same fitting software and a further expanded data set but following more conventional methods for tailoring bonded parameters (harmonic angle terms and torsion potentials) to the charge model. First, ff15ipq-Qsolv derives bonded parameters in the context of the ff15ipq solution phase charge set. Second, ff15ipq-Vac takes ff15ipq’s bonded parameters and runs simulations with the vacuum phase charge set used to derive those parameters. The IPolQ charge model and associated protocol for deriving bonded parameters are shown to be an incremental improvement over protocols that do not account for the material phases of each source of their fitting data. Both force fields incorporating the polarized charge set depict stable globular proteins and have varying degrees of success modeling the metastability of short (5–19 residues) peptides. In this particular case, ff15ipq-Qsolv increases stability in a number of α-helices, correctly obtaining 70% helical character in the K19 system at 275 K and showing appropriately diminishing content up to 325 K, but overestimating the helical fraction of AAQAA3 by 50% or more, forming long-lived α-helices in simulations of a β-hairpin, and increasing the likelihood that the disordered p53 N-terminal peptide will also form a helix. This may indicate a systematic bias imparted by the ff15ipq-Qsolv parameter development strategy, which has the hallmarks of strategies used to develop other popular force fields, and may explain some of the need for manual corrections in this force fields’ evolution. In contrast, ff15ipq-Vac incorrectly depicts globular protein unfolding in numerous systems tested, including Trp cage, villin, lysozyme, and GB3, and does not perform any better than ff15ipq or ff15ipq-Qsolv in tests on short peptides. We analyze the free energy surfaces of individual amino acid dipeptides and the electrostatic potential energy surfaces of each charge model to explain the differences.
    Type of Medium: Online Resource
    ISSN: 0021-9606 , 1089-7690
    Language: English
    Publisher: AIP Publishing
    Publication Date: 2017
    detail.hit.zdb_id: 3113-6
    detail.hit.zdb_id: 1473050-9
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  • 2
    In: The Journal of Chemical Physics, AIP Publishing, Vol. 153, No. 6 ( 2020-08-14)
    Abstract: We present a new force field, AMBER ff15ipq-m, for simulations of protein mimetics in applications from therapeutics to biomaterials. This force field is an expansion of the AMBER ff15ipq force field that was developed for canonical proteins and enables the modeling of four classes of artificial backbone units that are commonly used alongside natural α residues in blended or “heterogeneous” backbones: chirality-reversed D-α-residues, the Cα-methylated α-residue Aib, homologated β-residues (β3) bearing proteinogenic side chains, and two cyclic β residues (βcyc; APC and ACPC). The ff15ipq-m force field includes 472 unique atomic charges and 148 unique torsion terms. Consistent with the AMBER IPolQ lineage of force fields, the charges were derived using the Implicitly Polarized Charge (IPolQ) scheme in the presence of explicit solvent. To our knowledge, no general force field reported to date models the combination of artificial building blocks examined here. In addition, we have derived Karplus coefficients for the calculation of backbone amide J-coupling constants for β3Ala and ACPC β residues. The AMBER ff15ipq-m force field reproduces experimentally observed J-coupling constants in simple tetrapeptides and maintains the expected conformational propensities in reported structures of proteins/peptides containing the artificial building blocks of interest—all on the μs timescale. These encouraging results demonstrate the power and robustness of the IPolQ lineage of force fields in modeling the structure and dynamics of natural proteins as well as mimetics with protein-inspired artificial backbones in atomic detail.
    Type of Medium: Online Resource
    ISSN: 0021-9606 , 1089-7690
    Language: English
    Publisher: AIP Publishing
    Publication Date: 2020
    detail.hit.zdb_id: 3113-6
    detail.hit.zdb_id: 1473050-9
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  • 3
    Online Resource
    Online Resource
    AIP Publishing ; 2007
    In:  The Journal of Chemical Physics Vol. 127, No. 21 ( 2007-12-07)
    In: The Journal of Chemical Physics, AIP Publishing, Vol. 127, No. 21 ( 2007-12-07)
    Abstract: Alchemical free energy calculations provide a means for the accurate determination of free energies from atomistic simulations and are increasingly used as a tool for computational studies of protein-ligand interactions. Much attention has been placed on efficient ways to deal with the “endpoint singularity” effect that can cause simulation instabilities when changing the number of atoms. In this study we compare the performance of linear and several nonlinear transformation methods, among them separation shifted “soft core” scaling, for a popular test system, the hydration free energy of an amino acid side chain. All the nonlinear methods yield similar results if extensive sampling is performed, but soft core scaling provides smooth λ curves that are best suited for commonly used numerical integration schemes. Additionally, results from a more flexible solute, hexane, will also be discussed.
    Type of Medium: Online Resource
    ISSN: 0021-9606 , 1089-7690
    Language: English
    Publisher: AIP Publishing
    Publication Date: 2007
    detail.hit.zdb_id: 3113-6
    detail.hit.zdb_id: 1473050-9
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  • 4
    Online Resource
    Online Resource
    AIP Publishing ; 2021
    In:  The Journal of Chemical Physics Vol. 154, No. 10 ( 2021-03-14)
    In: The Journal of Chemical Physics, AIP Publishing, Vol. 154, No. 10 ( 2021-03-14)
    Type of Medium: Online Resource
    ISSN: 0021-9606 , 1089-7690
    Language: English
    Publisher: AIP Publishing
    Publication Date: 2021
    detail.hit.zdb_id: 3113-6
    detail.hit.zdb_id: 1473050-9
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  • 5
    Online Resource
    Online Resource
    AIP Publishing ; 1985
    In:  The Journal of Chemical Physics Vol. 83, No. 11 ( 1985-12-01), p. 5792-5796
    In: The Journal of Chemical Physics, AIP Publishing, Vol. 83, No. 11 ( 1985-12-01), p. 5792-5796
    Abstract: Relativistic molecular orbital calculations in the multiple scattering approximation are reported for NpF6, and the results are used to calculate the molecular g tensor and hyperfine parameters for the Np and F nuclei. Core spin-polarization effects are estimated from quasirelativistic spin-unrestricted calculations, which are corrected in an approximate fashion for the effects of spin-orbit mixing. The calculated results (with experimental values in parentheses) are: g=−0.700 (−0.604); A(237Np)=−2.02 GHz (−2.00); a∥(19F)=−103 MHz (−132); and a⊥(19F)=−43 MHz (−42). These results are among the first nonempirical calculations of magnetic resonance parameters for actinide complexes. The calculations predict that the unpaired electron in NpF6 has 4% to 5% fluorine p character.
    Type of Medium: Online Resource
    ISSN: 0021-9606 , 1089-7690
    Language: English
    Publisher: AIP Publishing
    Publication Date: 1985
    detail.hit.zdb_id: 3113-6
    detail.hit.zdb_id: 1473050-9
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  • 6
    Online Resource
    Online Resource
    AIP Publishing ; 2006
    In:  The Journal of Chemical Physics Vol. 125, No. 18 ( 2006-11-14)
    In: The Journal of Chemical Physics, AIP Publishing, Vol. 125, No. 18 ( 2006-11-14)
    Abstract: The path-integral molecular dynamics and centroid molecular dynamics methods have been applied to investigate the behavior of liquid water at ambient conditions starting from a recently developed simple point charge/flexible (SPC/Fw) model. Several quantum structural, thermodynamic, and dynamical properties have been computed and compared to the corresponding classical values, as well as to the available experimental data. The path-integral molecular dynamics simulations show that the inclusion of quantum effects results in a less structured liquid with a reduced amount of hydrogen bonding in comparison to its classical analog. The nuclear quantization also leads to a smaller dielectric constant and a larger diffusion coefficient relative to the corresponding classical values. Collective and single molecule time correlation functions show a faster decay than their classical counterparts. Good agreement with the experimental measurements in the low-frequency region is obtained for the quantum infrared spectrum, which also shows a higher intensity and a redshift relative to its classical analog. A modification of the original parametrization of the SPC/Fw model is suggested and tested in order to construct an accurate quantum model, called q-SPC/Fw, for liquid water. The quantum results for several thermodynamic and dynamical properties computed with the new model are shown to be in a significantly better agreement with the experimental data. Finally, a force-matching approach was applied to the q-SPC/Fw model to derive an effective quantum force field for liquid water in which the effects due to the nuclear quantization are explicitly distinguished from those due to the underlying molecular interactions. Thermodynamic and dynamical properties computed using standard classical simulations with this effective quantum potential are found in excellent agreement with those obtained from significantly more computationally demanding full centroid molecular dynamics simulations. The present results suggest that the inclusion of nuclear quantum effects into an empirical model for water enhances the ability of such model to faithfully represent experimental data, presumably through an increased ability of the model itself to capture realistic physical effects.
    Type of Medium: Online Resource
    ISSN: 0021-9606 , 1089-7690
    Language: English
    Publisher: AIP Publishing
    Publication Date: 2006
    detail.hit.zdb_id: 3113-6
    detail.hit.zdb_id: 1473050-9
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  • 7
    Online Resource
    Online Resource
    AIP Publishing ; 2022
    In:  The Journal of Chemical Physics Vol. 156, No. 1 ( 2022-01-07)
    In: The Journal of Chemical Physics, AIP Publishing, Vol. 156, No. 1 ( 2022-01-07)
    Abstract: The solvent can occupy up to ∼70% of macromolecular crystals, and hence, having models that predict solvent distributions in periodic systems could improve the interpretation of crystallographic data. Yet, there are few implicit solvent models applicable to periodic solutes, and crystallographic structures are commonly solved assuming a flat solvent model. Here, we present a newly developed periodic version of the 3D-reference interaction site model (RISM) integral equation method that is able to solve efficiently and describe accurately water and ion distributions in periodic systems; the code can compute accurate gradients that can be used in minimizations or molecular dynamics simulations. The new method includes an extension of the Ornstein–Zernike equation needed to yield charge neutrality for charged solutes, which requires an additional contribution to the excess chemical potential that has not been previously identified; this is an important consideration for nucleic acids or any other charged system where most or all the counter- and co-ions are part of the “disordered” solvent. We present several calculations of proteins, RNAs, and small molecule crystals to show that x-ray scattering intensities and the solvent structure predicted by the periodic 3D-RISM solvent model are in closer agreement with the experiment than are intensities computed using the default flat solvent model in the refmac5 or phenix refinement programs, with the greatest improvement in the 2 to 4 Å range. Prospects for incorporating integral equation models into crystallographic refinement are discussed.
    Type of Medium: Online Resource
    ISSN: 0021-9606 , 1089-7690
    Language: English
    Publisher: AIP Publishing
    Publication Date: 2022
    detail.hit.zdb_id: 3113-6
    detail.hit.zdb_id: 1473050-9
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  • 8
    Online Resource
    Online Resource
    AIP Publishing ; 2014
    In:  The Journal of Chemical Physics Vol. 141, No. 22 ( 2014-12-14)
    In: The Journal of Chemical Physics, AIP Publishing, Vol. 141, No. 22 ( 2014-12-14)
    Abstract: A new method is introduced to compute X-ray solution scattering profiles from atomic models of macromolecules. The three-dimensional version of the Reference Interaction Site Model (RISM) from liquid-state statistical mechanics is employed to compute the solvent distribution around the solute, including both water and ions. X-ray scattering profiles are computed from this distribution together with the solute geometry. We describe an efficient procedure for performing this calculation employing a Lebedev grid for the angular averaging. The intensity profiles (which involve no adjustable parameters) match experiment and molecular dynamics simulations up to wide angle for two proteins (lysozyme and myoglobin) in water, as well as the small-angle profiles for a dozen biomolecules taken from the BioIsis.net database. The RISM model is especially well-suited for studies of nucleic acids in salt solution. Use of fiber-diffraction models for the structure of duplex DNA in solution yields close agreement with the observed scattering profiles in both the small and wide angle scattering (SAXS and WAXS) regimes. In addition, computed profiles of anomalous SAXS signals (for Rb+ and Sr2+) emphasize the ionic contribution to scattering and are in reasonable agreement with experiment. In cases where an absolute calibration of the experimental data at q = 0 is available, one can extract a count of the excess number of waters and ions; computed values depend on the closure that is assumed in the solution of the Ornstein–Zernike equations, with results from the Kovalenko–Hirata closure being closest to experiment for the cases studied here.
    Type of Medium: Online Resource
    ISSN: 0021-9606 , 1089-7690
    Language: English
    Publisher: AIP Publishing
    Publication Date: 2014
    detail.hit.zdb_id: 3113-6
    detail.hit.zdb_id: 1473050-9
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  • 9
    Online Resource
    Online Resource
    AIP Publishing ; 1965
    In:  The Journal of Chemical Physics Vol. 43, No. 3 ( 1965-08-01), p. 1067-1068
    In: The Journal of Chemical Physics, AIP Publishing, Vol. 43, No. 3 ( 1965-08-01), p. 1067-1068
    Type of Medium: Online Resource
    ISSN: 0021-9606 , 1089-7690
    Language: English
    Publisher: AIP Publishing
    Publication Date: 1965
    detail.hit.zdb_id: 3113-6
    detail.hit.zdb_id: 1473050-9
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  • 10
    In: The Journal of Chemical Physics, AIP Publishing, Vol. 136, No. 13 ( 2012-04-07)
    Abstract: A joint experimental-theoretical study has been carried out on electronic states of propadienylidene (H2CCC), using results from negative-ion photoelectron spectroscopy. In addition to the previously characterized \documentclass[12pt]{minimal}\begin{document}${\tilde{X}}^1A_1$\end{document}X̃1A1 electronic state, spectroscopic features are observed that belong to five additional states: the low-lying \documentclass[12pt] {minimal}\begin{document}${\tilde{a}}^3B_1$\end{document}ã3B1 and \documentclass[12pt]{minimal}\begin{document}${\tilde{b}}^3A_2$\end{document}b̃3A2 states, as well as two excited singlets, \documentclass[12pt] {minimal}\begin{document}${\tilde{A}}^1A_2$\end{document}Ã1A2 and \documentclass[12pt]{minimal}\begin{document}${\tilde{B}}^1B_1$\end{document}B̃1B1, and a higher-lying triplet, \documentclass[12pt] {minimal}\begin{document}${\tilde{c}}^3A_1$\end{document}c̃3A1. Term energies (T0, in cm−1) for the excited states obtained from the data are: 10 354±11 (\documentclass[12pt]{minimal}\begin{document}${\tilde{a}}^3B_1$\end{document}ã3B1); 11 950±30 (\documentclass[12pt] {minimal}\begin{document}${\tilde{b}}^3A_2$\end{document}b̃3A2); 20 943±11 (\documentclass[12pt]{minimal}\begin{document}${\tilde{c}}^3A_1$\end{document}c̃3A1); and 13 677±11 (\documentclass[12pt] {minimal}\begin{document}${\tilde{A}}^1A_2$\end{document}Ã1A2). Strong vibronic coupling affects the \documentclass[12pt]{minimal}\begin{document}${\tilde{A}}^1A_2$\end{document}Ã1A2 and \documentclass[12pt] {minimal}\begin{document}${\tilde{B}}^1B_1$\end{document}B̃1B1 states as well as \documentclass[12pt]{minimal}\begin{document}${\tilde{a}}^3B_1$\end{document}ã3B1 and \documentclass[12pt] {minimal}\begin{document}${\tilde{b}}^3A_2$\end{document}b̃3A2 and has profound effects on the spectrum. As a result, only a weak, broadened band is observed in the energy region where the origin of the \documentclass[12pt]{minimal}\begin{document}${\tilde{B}}^1B_1$\end{document}B̃1B1 state is expected. The assignments here are supported by high-level coupled-cluster calculations and spectral simulations based on a vibronic coupling Hamiltonian. A result of astrophysical interest is that the present study supports the idea that a broad absorption band found at 5450 Å by cavity ringdown spectroscopy (and coincident with a diffuse interstellar band) is carried by the \documentclass[12pt] {minimal}\begin{document}${\tilde{B}}^1B_1$\end{document}B̃1B1 state of H2CCC.
    Type of Medium: Online Resource
    ISSN: 0021-9606 , 1089-7690
    Language: English
    Publisher: AIP Publishing
    Publication Date: 2012
    detail.hit.zdb_id: 3113-6
    detail.hit.zdb_id: 1473050-9
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