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Molecules calculation

The film pressure of a myristic acid film at 20°C is 10 dyn/cm at an area of 23 A per molecule the limiting area at high pressures can be taken as 20 A per molecule. Calculate what the film pressure should be, using Eq. IV-36 with / = 1, and what the activity coefficient of water in the interfacial solution is in terms of that model. [Pg.157]

Consider the case of an emulsion of 1 liter of oil in 1 liter of water having oil droplets of 0.6 /rm diameter. If the oil-water interface contains a close-packed monolayer of surfactant of 18 per molecule, calculate how many moles of surfactant are present. [Pg.527]

For both types of orbitals, the coordinates r, 0 and cji refer to the position of the electron relative to a set of axes attached to the centre on which the basis orbital is located. Although STOs have the proper cusp behaviour near the nuclei, they are used primarily for atomic- and linear-molecule calculations because the multi-centre integrals which arise in polyatomic-molecule calculations caimot efficiently be perfonned when STOs are employed. In contrast, such integrals can routinely be done when GTOs are used. This fiindamental advantage of GTOs has led to the dominance of these fimetions in molecular quantum chemistry. [Pg.2170]

In our hydrogen molecule calculation in Section 2.4.1 the molecular orbitals were provided as input, but in most electronic structure calculations we are usually trying to calculate the molecular orbitals. How do we go about this We must remember that for many-body problems there is no correct solution we therefore require some means to decide whether one proposed wavefunction is better than another. Fortunately, the variation theorem provides us with a mechanism for answering this question. The theorem states that the... [Pg.71]

TIk experimentally determined dipole moment of a water molecule in the gas phase is 1.85 D. The dipole moment of an individual water molecule calculated with any of thv se simple models is significantly higher for example, the SPC dipole moment is 2.27 D and that for TIP4P is 2.18 D. These values are much closer to the effective dipole moment of liquid water, which is approximately 2.6 D. These models are thus all effective pairwise models. The simple water models are usually parametrised by calculating various pmperties using molecular dynamics or Monte Carlo simulations and then modifying the... [Pg.235]

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]

Organic molecule calculations can be done routinely to good accuracy on workstation-class hardware. It is advisable to examine tabulations of results in order to choose a method with acceptable accuracy and computational time for the property of interest. The trend toward having microcomputer versions of computational chemistry codes is making calculations on small organic molecules even more readily accessible. [Pg.284]

Eor small and medium-sized molecules, calculate all nonbonded interactions. [Pg.104]

Size consistency the results given for a system of molecules infinitely separated from one another ought to equal the sum of the results obtained for each individual molecule calculated separately. Another way of describing this requirement is that the error in the predictions of any method should scale roughly in proportion to the size of the molecule. When size consistency does not hold, comparing the properties of molecules of different sizes will not result in quantitatively meaningful differences. [Pg.8]

Run your NMR calculations at the HF/6-31G(d) level here are the structures of the three molecules calculated at the B3LYP/6-31G(d) level ... [Pg.29]

For each molecule, calculate the overall energy barrier for ring inversion in each direction. Use this barrier to calculate the half-life (t./,) of an individual molecule at 298 K (use equation 2). Which molecule inverts most rapidly Most slowly Why (Hint What geometrical changes are required for inversion )... [Pg.81]

Another factor to consider is the energy required to break solid MH into individual molecules. Calculate the dissociation energies for sodium hydride dimer and potassium hydride dimer, i.e. [Pg.123]

Problem 2.9 Organic phosphate groups occur commonly in biological molecules. Calculate formal charges on the four O atoms in the methyl phosphate dianion. [Pg.42]

Nakamura, T., Ohno, K., Kotani, M., and Hijikata, K., Progr. Theoret. Phys. Kyoto) 8, 387, Interaction of -electrons in the acetylene molecule/ Calculations using both MO-CI and HL with ionic-homopolar resonance. [Pg.333]

B.14 (a) Determine the total number of protons, neutrons, and electrons in one carbon tetrafluoride molecule, CF4, assuming that all atoms are the most common isotopes of that element, (b) What is the total mass of protons, of neutrons, and of electrons in one carbon tetrafluoride molecule Calculate three masses. [Pg.46]

Curve 1 shows the electronic energy of the hydrogen molecule neglecting interelectronic interaction (from Burrau s solution for the molecule-ion) curve 2, the electronic energy empirically corrected by Condon s method and curve 3, the total energy of the hydrogen molecule, calculated by Condon s method. [Pg.53]

Carbon Tetrachloride.—By the usual visual method and by other methods involving microphotometer records, we have assigned8 to the carbon tetrachloride molecule the value 1.760 0.005 A. for the C-Cl distance, a value supported by other recent work.9 The radial distribution function for this molecule calculated by Equation 6, using the ten terms for which data are given in Table I, is shown in Fig. 1. [Pg.628]

In Tabled theoretical magnetic anisotropies AK for selected molecules, calculated assuming the bond lengths shown in Fig. 5, are listed (in units of d.Kbenzene) d Compared with the experimental exaltations reported by Dauben et a/. . Theoretical values are in good agreement... [Pg.34]

C07-0118. Neutrons, like electrons and photons, are particle-waves whose diffraction patterns can be used to determine the structures of molecules. Calculate the kinetic energy of a neutron with a wavelength of 75 pm. [Pg.498]

Clog P Calculated hydrophobicity of the whole molecule (calculated logarithm of partition coefficient (P) in M-octanol/water) ji Calculated hydrophobicity of the substituent... [Pg.44]

Pparaceii = permeability coefficient accounting for molecular size restricted diffusion independent of the charge on the molecule calculated from Eq. (47). [Pg.266]

In complex organic molecules calculations of the geometry of excited states and hence predictions of chemiluminescent reactions are very difficult however, as is well known, in polycyclic aromatic hydrocarbons there are relatively small differences in the configurations of the ground state and the excited state. Moreover, the chemiluminescence produced by the reaction of aromatic hydrocarbon radical anions and radical cations is due to simple one-electron transfer reactions, especially in cases where both radical ions are derived from the same aromatic hydrocarbon, as in the reaction between 9.10-diphenyl anthracene radical cation and anion. More complex are radical ion chemiluminescence reactions involving radical ions of different parent compounds, such as the couple naphthalene radical anion/Wurster s blue (see Section VIII. B.). [Pg.69]


See other pages where Molecules calculation is mentioned: [Pg.157]    [Pg.158]    [Pg.329]    [Pg.466]    [Pg.46]    [Pg.64]    [Pg.228]    [Pg.237]    [Pg.341]    [Pg.27]    [Pg.631]    [Pg.310]    [Pg.182]    [Pg.47]    [Pg.121]    [Pg.12]    [Pg.283]    [Pg.393]    [Pg.619]    [Pg.46]    [Pg.73]    [Pg.105]    [Pg.5]    [Pg.35]   
See also in sourсe #XX -- [ Pg.80 , Pg.81 , Pg.82 , Pg.83 ]




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Ab Initio Calculations on Molecules containing Five or Six Atoms

Ab initio and DFT Calculations on Diatomic Molecules

Ab initio calculations, for molecules

Approaches to the Problem of Solvation Calculations in Polar and Charged Molecules

Basis Sets for Relativistic Calculations of Molecules

Calculating a Molecules Degree of Unsaturation

Calculating absorption maxima aromatic molecules

Calculation for small molecules

Calculation of NMR Tensors Application to Small-Molecule Pharmaceutical Solids

Calculations counting molecules

Calculations on Diatomic Molecules

Closed-shell molecule, self-consistent field configuration, calculation

Diatomic molecules coupling calculations

Dirac-Hartree-Fock calculations large molecules

Electronic Calculations on Large Molecules

Electronic calculations for molecules

Free Energy Perturbation Calculations for Small Molecules

Geometries of simple polyatomic molecules from KRHF calculations

Gonzdlez-Ferez and W. Schweizer Propagator calculations for large molecules Determination of transition

Ground-state calculations hydrogen molecules

H. Stoll, Electronic structure calculations for molecules containing lanthanide atoms

HMO Calculations on Some Simple Molecules

Hartree-Fock calculations, molecules

Heteronuclear diatomic molecule molecular orbital calculations

Homonuclear diatomic molecules molecular orbital calculations

Hydrogen molecule minimum basis set calculation

Hydrogen molecule simple calculations

Hydrogen molecule, calculations

Hydrogen-bonded molecules calculation protocol

Molecular orbital calculations ethylene molecules

Molecule calculating number

Molecule mass, calculation

Molecules finite-difference calculations

Molecules fraction that ionize, calculation

Molecules, small electron-correlated calculations

Non-Born-Oppenheimer calculations diatomic molecules

Organic molecules electron-correlated calculations

PRESENT STATUS OF NMR CALCULATIONS ON MOLECULES

Polyatomic Molecules Method of Calculation

Properties of Molecules by Direct Calculation

Quantum Mechanical Calculations on Small Molecules

Relativistic Ab-Initio Model Potential Calculations for Molecules and Embedded Clusters

Rovibrational spectra - an example of accurate calculations atom - diatomic molecule

Self-consistent field calculations molecules

Semi-empirical Calculations on Molecules

Semiempirical Calculations on Larger Molecules

Small molecules, calculations

Structure calculations polyatomic molecules

The LiH molecule approximate molecular orbital calculations

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