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Small molecules, calculations

Table 2-5. Average dipole polarizabilites (in atomic units) of noble-gas atoms and small molecules calculated using different exchange-correlation potentials and the reference data (benchmark wave-function calculations or experimental).83... Table 2-5. Average dipole polarizabilites (in atomic units) of noble-gas atoms and small molecules calculated using different exchange-correlation potentials and the reference data (benchmark wave-function calculations or experimental).83...
Pubchem [32] Pubchem is a database maintained by the National Center for Biotechnology Information (NCBI), which is part of the US National Institutes of Health (NIH). PubChem can be freely accessed through a web user interface or is downloadable by File Transfer Protocol (FTP) at http //pubchem.ncbi.nlm.nih.gov. Pubchem is organized into three main parts substances ( 126 million entries of compound mixtures, extracts, etc.), pure compounds (48 million unique structures), and bioassays (-740,000 records). Users can search the database by name, Pub-Chem identifiers, structures of molecules to retrieve small molecules, calculated physicochemical data, and experimental biological data. Structure-activity relationship tools are available for further analysis of the extracted results. [Pg.114]

With respect to AG the results of polymer solutions may be used as they are. If the entropy of mixing is written as AS and the enthalpy of mixing as AH , then AG = AH - T AS where AS is the change of entropy when j solvent molecules and 2 polymer chains mix and form a homogeneous solution [3]. At this point, unlike in the case of mixing of small molecules, calculation issues are involved because the sizes of solvent and solute molecules are extremely different. As well, a number of polymer conformations must be taken into account. However, the results based on a lattice model can be expressed in the following simple form ... [Pg.67]

The monolayer amount adsorbed on an aluminum oxide sample was determined using a small molecule adsorbate and then molecular-weight polystyrenes (much as shown in Ref. 169). The results are shown in the table. Calculate the fractal dimension of the oxide. [Pg.674]

Shelton D P and Rice J E 1994 Measurements and calculations of the hyperpolarizabilities of atoms and small molecules in the gas phase Chem. Rev. 94 3... [Pg.211]

Shifts can also be predicted ftom basic theory, using higher levels of computation, if the molecular structure is precisely known [16], The best calculations, on relatively small molecules, vary from observation by little more than the variations in shift caused by changes in solvent. In all cases, it is harder to predict the shifts of less coimnon nuclei, because of the generally greater number of electrons in the atom, and also because fewer shift examples are available. [Pg.1450]

Several ideas have been put forward to calculate tire diffusion coefficient of small molecules in polymers. Glasstone et al [M] proposed an expression based on transition-state tlieory... [Pg.2536]

Atomistically detailed models account for all atoms. The force field contains additive contributions specified in tenns of bond lengtlis, bond angles, torsional angles and possible crosstenns. It also includes non-bonded contributions as tire sum of van der Waals interactions, often described by Lennard-Jones potentials, and Coulomb interactions. Atomistic simulations are successfully used to predict tire transport properties of small molecules in glassy polymers, to calculate elastic moduli and to study plastic defonnation and local motion in quasi-static simulations [fy7, ( ]. The atomistic models are also useful to interiDret scattering data [fyl] and NMR measurements [70] in tenns of local order. [Pg.2538]

Molecular mechanics calculations are a very useful tool for the spatial and energetic description of small molecules as well as macroscopic systems like proteins or DMA. [Pg.398]

Besides the aforementioned descriptors, grid-based methods are frequently used in the field of QSAR quantitative structure-activity relationships) [50]. A molecule is placed in a box and for an orthogonal grid of points the interaction energy values between this molecule and another small molecule, such as water, are calculated. The grid map thus obtained characterizes the molecular shape, charge distribution, and hydrophobicity. [Pg.428]

OPTS (Optim i/.ed Potentials for Liquid Simulations) is based on a force field developed by the research group of Bill Jorgensen now at Yale University and previously at Purdue University. Like AMBER, the OPLS force field is designed for calculations on proteins an d nucleic acids. It in troduces non bonded in leraclion parameters that have been carefully developed from extensive Monte Carlo liquid sim u lation s of small molecules. These n on-bonded interactions have been added to the bonding interactions of AMBER to produce a new force field that is expected to be better than AMBER at describing simulations w here the solvent isexplic-... [Pg.191]

For small molecules, the accuracy of solutions to the Schrtidinger equation competes with the accuracy of experimental results. However, these accurate a i initw calculations require enormous com putation an d are on ly suitable for the molecular system s with small or medium size. Ah initio calculations for very large molecules are beyond the realm of current computers, so HyperChern also supports sern i-em p irical quantum meclian ics m eth ods. Sem i-em pirical approximate solutions are appropriate and allow extensive cliem ical exploration, Th e in accuracy of the approxirn ation s made in semi-empirical methods is offset to a degree by recourse to experimental data in defining the parameters of the method. [Pg.217]

In some cases the atomic charges are chosen to reproduce thermodynamic properties calculated using a molecular dynamics or Monte Carlo simulation. A series of simulations is performed and the charge model is modified until satisfactory agreement with experiment is obtained. This approach can be quite powerful despite its apparent simplicity, but it is only really practical for small molecules or simple models. [Pg.207]

Ihe allure of methods for calculating free energies and their associated thermod)mai values such as equilibrium constants has resulted in considerable interest in free ene calculations. A number of decisions must be made about the way that the calculatior performed. One obvious choice concerns the simulation method. In principle, eit Monte Carlo or molecular dynamics can be used in practice, molecular dynamics almost always used for systems where there is a significant degree of conformatio flexibility, whereas Monte Carlo can give very good results for small molecules which either rigid or have limited conformational freedom. [Pg.593]

We envision a potential energy surface with minima near the equilibrium positions of the atoms comprising the molecule. The MM model is intended to mimic the many-dimensional potential energy surface of real polyatomic molecules. (MM is little used for very small molecules like diatomies.) Once the potential energy surface iias been established for an MM model by specifying the force constants for all forces operative within the molecule, the calculation can proceed. [Pg.98]

QSPR methods have yielded the most accurate results. Most often, they use large expansions of parameters obtainable from semiempirical calculations along with other less computationally intensive properties. This is often the method of choice for small molecules. [Pg.114]


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