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Property Calculations

The factor enabling interpolation of reduced properties of a pure compound or mixture between two reduced properties calculated on two reference fluids merits attention in order to understand its meaning. [Pg.113]

The themiodynamic properties calculated by different routes are different, since the MS solution is an approximation. The osmotic coefficient from the virial pressure, compressibility and energy equations are not the same. Of these, the energy equation is the most accurate by comparison with computer simulations of Card and Valleau [ ]. The osmotic coefficients from the virial and compressibility equations are... [Pg.495]

The chirality code of a molecule is based on atomic properties and on the 3D structure. Examples of atomic properties arc partial atomic charges and polarizabilities, which are easily accessible by fast empirical methods contained in the PETRA package. Other atomic properties, calculated by other methods, can in principle be used. It is convenient, however, if the chosen atomic property discriminates as much as possible between non-equivalent atoms. 3D molecular structures are easily generated by the GORINA software package (see Section 2.13), but other sources of 3D structures can be used as well. [Pg.420]

Tie first consideration is that the total wavefunction and the molecular properties calculated rom it should be the same when a transformed basis set is used. We have already encoun-ered this requirement in our discussion of the transformation of the Roothaan-Hall quations to an orthogonal set. To reiterate suppose a molecular orbital is written as a inear combination of atomic orbitals ... [Pg.108]

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]

Ah initio methods are applicable to the widest variety of property calculations. Many typical organic molecules can now be modeled with ah initio methods, such as Flartree-Fock, density functional theory, and Moller Plesset perturbation theory. Organic molecule calculations are made easier by the fact that most organic molecules have singlet spin ground states. Organics are the systems for which sophisticated properties, such as NMR chemical shifts and nonlinear optical properties, can be calculated most accurately. [Pg.284]

The functionality available in MedChem Explorer is broken down into a list of available computational experiments, including activity prediction, align/ pharmacophore, overlay molecules, conformer generation, property calculation, and database access. Within each experiment, the Web system walks the user through a series of questions that must be answered sequentially. The task is then submitted to a remote server, where it is performed. The user can view the progress of the work in their Web browser at any time. Once complete, the results of the calculation are stored on the server. The user can then run subsequent experiments starting with those results. The Web interface includes links to help pages at every step of the process. [Pg.355]

The property calculation experiment offers a list of 34 molecular properties, including thermodynamic, electrostatic, graph theory, geometric properties, and Lipinski properties. These properties are useful for traditional QSAR activity prediction. Some are computed with MOPAC others are displayed in the browser without units. A table of computed properties can be exported to a Microsoft Excel spreadsheet. [Pg.356]

Critical Temperature The critical temperature of a compound is the temperature above which a hquid phase cannot be formed, no matter what the pressure on the system. The critical temperature is important in determining the phase boundaries of any compound and is a required input parameter for most phase equilibrium thermal property or volumetric property calculations using analytic equations of state or the theorem of corresponding states. Critical temperatures are predicted by various empirical methods according to the type of compound or mixture being considered. [Pg.384]

The treatment of electrostatics and dielectric effects in molecular mechanics calculations necessary for redox property calculations can be divided into two issues electronic polarization contributions to the dielectric response and reorientational polarization contributions to the dielectric response. Without reorientation, the electronic polarization contribution to e is 2 for the types of atoms found in biological systems. The reorientational contribution is due to the reorientation of polar groups by charges. In the protein, the reorientation is restricted by the bonding between the polar groups, whereas in water the reorientation is enhanced owing to cooperative effects of the freely rotating solvent molecules. [Pg.399]

In such cases the expression from fii st-order perturbation theory (10.18) yields a result identical to the first derivative of the energy with respect to A. For wave functions which are not completely optimized with respect to all parameters (Cl, MP or CC), the Hellmann-Feynman theorem does not hold, and a first-order property calculated as an expectation value will not be identical to that obtained as an energy derivative. Since the Hellmann-Feynman theorem holds for an exact wave function, the difference between the two values becomes smaller as the quality of an approximate wave function increases however, for practical applications the difference is not negligible. It has been argued that the derivative technique resembles the physical experiment more, and consequently formula (10.21) should be preferred over (10.18). [Pg.241]

In order to address the possible influence of positional disorder, we have chosen to analyze the way basic operations such as translations and rotations affect the properties calculated for highly symmetric configurations. This approach could provide guidelines to prevent the loss of significant optical coupling between the ground state and the lowest excited state, and hence the quenching of luminescence in the solid state. [Pg.65]

Table A4.5 summarizes the equations for calculating anharmonicity and nonrigid rotator corrections for diatomic molecules. These corrections are to be added to the thermodynamic properties calculated from the equations given in Table A4.1 (which assume harmonic oscillator and rigid rotator approximations). Table A4.5 summarizes the equations for calculating anharmonicity and nonrigid rotator corrections for diatomic molecules. These corrections are to be added to the thermodynamic properties calculated from the equations given in Table A4.1 (which assume harmonic oscillator and rigid rotator approximations).
In Table 3, a comparison of several properties calculated by model I and model III are presented. For the calculation of individual molecular properties, both models provide very similar values. A comparison of the CCSD second-... [Pg.164]

Table 3 Second Order Properties Calculated by EOM-CCSD Methods... Table 3 Second Order Properties Calculated by EOM-CCSD Methods...
During an experiment, a chemist may measure physical quantities such as mass, volume, and temperature. Usually the chemist seeks information that is related to the measured quantities but must be found by doing calculations. In later chapters we develop and use equations that relate measured physical quantities to important chemical properties. Calculations are an essential part of all of chemistry therefore, they play important roles in much of general chemistry. The physical property of density illustrates how to apply an equation to calculations. [Pg.38]

Total number of spin and symmetry adapted configurations Number of spin and symmetry adapted configurations selected by second-order perturbation theory and treatedvariationally Property calculated with respect to the center of mass. [Pg.322]

A force field is considered transferable from an arbitrary molecule A to another molecule B if the agreement of properties calculated fori (geometrical, vibrational, thermochemical, and other properties) with the respective experimental values is as good as for A. In our calculations we are dealing with force fields which describe entire families of molecules. Within these families, properties of only a fraction of their members are known experimentally while it is our aim to predict the others computationally. It is therefore clear that the problem of transferability is of decisive importance for force field calculations of unknown systems or those with unknown properties or. Traditional vibrational spectroscopic force fields in most cases reproduce well the frequencies of a single molecule or a family of closely related molecules however, they are not transferable to molecules of different strain. Subsequently we comment on this point in somewhat more detail. [Pg.171]

Another property calculated in the XH3—Y series is the X—Y bond dissociation energy. For this purpose the MP2 optimized geometries for the XH3 and Y (doublet spin) radicals were obtained using the unrestricted HF (UHF) method. For comparison to experiment, the electronic energy differences for the reaction... [Pg.32]

It should be kept in mind that quantum chemical calculations of structures and magnetic properties generally are done for the isolated carbocation without taking into account its environment and media effects such as solvent, site-specific solvation or counterion effects. This is a critical question since NMR spectra of carbocations with a few exceptions are studied in superacid solutions and properties calculated for the gas-phase species are of little relevance if the electronic structure of carbocations is strongly perturbed by solvent effects. Provided that appropriate methods are used,... [Pg.159]

INDPROP, The molecular properties calculation package developed at the Theoretical Chemistry Group, Department of Chemistry, University of Pune, Pune, India. See also Bapat, S. V., Shirsat, R. N., and Gadre, S. R. Chem. Phys. Lett. 1992, 200, 373. See also Balanarayan, P. and Gadre, S. R. J. Chem. Phys. 2003, 115, 5037. [Pg.70]


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ASPEN properties, calculable

Additive property, calculation

Adsorption properties, calculation

Analytic Methods for Calculation of Partial Molar Properties

Approximate Quantum Mechanical Calculation of Thermodynamic Properties

Basic Calculations of Physical Properties

Basis Sets for the Calculation of Molecular Properties

Basis sets effect upon calculated properties

Calculate Properties push button

Calculated Molecular Properties and Multivariate Statistical Analysis in Absorption Prediction

Calculated molecular properties

Calculated properties to improve CASE

Calculated properties, polarizabilities

Calculating Molecular Properties Using ab initio Quantum Mechanics

Calculating Properties by Integration

Calculating Thermodynamic Properties Using a Force Field

Calculating properties of chemical bonding

Calculating thermodynamic properties

Calculation of Atomic Properties

Calculation of Magnetic Properties

Calculation of Rare-Earth Excited-State Absorption Properties

Calculation of Simple Thermodynamic Properties

Calculation of Spectroscopic Properties

Calculation of nonlinear properties

Calculation of properties from response theory

Calculation of thermodynamic properties

Calculations Using Colligative Properties

Calculations of species properties

Calculations spectroscopic properties

Chemical property bonding calculations

Chemical property calculator

Comparative molecular field analysis property calculations

Computational quantum mechanics calculating properties

Computer simulations fluid property calculations

Critical properties calculation methods

Density-functional Perturbation Theory and the Calculation of Response Properties

Detonation Properties calculation

Diagrams property calculators

Electrical response property calculations

Empirical Approaches to the Calculation of Properties

Equilibrium geometries property calculations

Equilibrium properties, calculation

Filtering candidates by calculated properties

Fluids property calculations

Integration calculating properties

Intermolecular interaction property based potential model calculations

Inverse micelle size calculated from the dielectric property

LCAO Calculations of Perfect-crystal Properties

Lattice calculations polymer surface properties

Lipinski property calculation systems

Magnetic properties in DKH calculations of electronic g values

Magnetic properties programs calculating

Magnetic properties, calculation

Molecular orbital theory properties calculable

Molecular properties calculating

Molecular properties, calculation

Monte Carlo simulation integration, calculating properties

New Schemes for Calculation and Analysis of Properties

Nonlinear optical properties calculation

Partial molar properties calculation

Partial properties calculation

Physical Properties with Results of HMO Calculations

Physical property calculator

Prediction and Calculation of Molecular Properties

Prediction of properties other than equilibrium geometries from Hartree-Fock-Roothaan calculations

Properties and Calculated Parameters of Representative

Properties from Quantum Mechanical Calculations

Properties of Molecules by Direct Calculation

Property Values for Burning Rate Calculations

Property based potential model calculations

Property calculations/calculators

Property calculations/calculators

Property derivatives calculation techniques

Second-order properties, calculation

Software for Calculating Thermodynamic Properties

Some Calculated Properties of Tetrahedrane

Structural properties, calculating

Structure property calculator

Symmetric properties calculation

The Calculation of Time Correlation Functions and Static Properties

Theoretical methods chemical property bonding calculations

Theoretical methods thermodynamic property calculations

Thermodynamic properties, calculated

Thermodynamic properties, calculation

Transport properties computer calculation

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