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Energy properties

It is then proposed that any solvent-dependent energy property, sueh as log k and AG°, ean be expressed as the sum... [Pg.440]

J. B. Foresman and H. B. Schlegel, Application of the Cl-Singles Method in Predicting the Energy, Properties and Reactivity of Molecules in Their Excited Slates in Molecular Spectroscopy Recent Experimental and Computational Advances, ed. R. Fausto, NATO-ASI Series C, Kluwer Academic, The Netherlands, 1993. [Pg.235]

Select Energy (Properties menu). Notice that it updates automatically as you go from one frame to another. This allows you to easily construct reaction energy diagrams (energy vs. frame number or vs. a specific geometrical parameter). Make such a plot for this Sn2 reaction. Note, that the reaction as written is thermodynamically favorable, i.e., it is exothermic. Note also, that only a relatively small energy barrier needs to be surmounted. [Pg.11]

This terminal point in hydrogen production can be used for refueling hydrogen-powered or hydrogen transport vehicles. There is also an option to canalize hydrogen in a natural gas (NG) pipeline provided that the distance from the WF is fairly short. Flydrogen injection in NG pipelines may improve NG energy properties [45]. [Pg.177]

According to equation 3.168, the energy properties of the four components are not mutually independent but, once the Gibbs free energy is fixed for three of them, the energy of the fourth is constrained by the reciprocal energy term... [Pg.168]

At the melt is absent and 7 and 7" coexist stably in a mechanical mixture of bulk composition C. The crystallization process in a closed system is thus completely defined at all T (and P) conditions by the Gibbs free energy properties of the various phases that may form in the compositional field of interest. [Pg.453]

Prospects for TR Electrolyte SBs. In view of the harmful effects often cited in the literature of even small traces of water on the operation of non-aqueous batteries with alkali metal anodes, it might be supposed that electrolytes of the TR composition cannot be applied in such batteries. This same idea may dominate when molten salt SBs are considered. Such a general conclusion cannot be justified. A dilute solution of water in a salt has the structure either of this salt proper or its adjacent hydrate, and the energy, properties and reactions of this water are quite different from those of pure water or of dilute solutions of various compounds in it. On the other hand, a small amount of water in the electrolyte system will decrease its melting point and increase its conductivity. Mixtures of water with such liquids as some alcohols or dioxane and other aprotic and even proton-forming substances, may open new prospects for... [Pg.288]

At the conclusion of a geometric optimization calculation, we have the equilibrium positions of all the atomic nuclei, as well as the overall electron density distributed in space (x, y, z). Many important properties, especially for an isolated single molecule at absolute zero temperature, can be obtained by solving the quantum mechanical or the molecular mechanical equations. Only the former method can produce electronic properties, such as electron distributions and dipole moments, but both methods can produce structural and energy properties. [Pg.86]

This is a question of considerable practical importance, given that optimization of equilibrium geometry can easily require one or two orders of magnitude more computation than an energy (property) calculation at a single geometry (see Chapter 11). Rephrased, the question might read ... [Pg.357]

An averaged solvent electrostatic potential, obtained by averaging over the solvent confignrations, is included in the solnte Hamiltonian and electric and energy properties are obtained. The method provides resnlts for the dipole moment and solnte-solvent interaction which agree with the experimental valnes and with the resnlts obtained by other workers (Mendoza et al., 1998). [Pg.289]

The results you obtain for Problem 1.5 should show that, since the joule (J) is a macroscopic base unit of energy, property values on the microscopic scale have extremely small magnitudes. We now explore this idea further in Worked Problem 1.3 and in Problem 1.6 to give more practice in manipulating numbers in scientific form and, more importantly, to provide further insight into size differences in the microscopic and macroscopic worlds. [Pg.14]

The quantity (a/ )-1 acquires the meaning of effective temperature, which characterizes the energy properties of the surface. It is assumed that, when the catalyst is prepared, fluctuations occur in the distribution of atoms on the surface which in fact lead to its inhomogeneity later the fluctuations freeze, and the experimenter works with a well-defined, inhomogeneous, but immutable surface. [Pg.8]

In this section we will consider the case of a multi-level electronic system in interaction with a bosonic bath [288,289], We will use unitary transformation techniques to deal with the problem, but will only focus on the low-bias transport, so that strong non-equilibrium effects can be disregarded. Our interest is to explore how the qualitative low-energy properties of the electronic system are modified by the interaction with the bosonic bath. We will see that the existence of a continuum of vibrational excitations (up to some cut-off frequency) dramatically changes the analytic properties of the electronic Green function and may lead in some limiting cases to a qualitative modification of the low-energy electronic spectrum. As a result, the I-V characteristics at low bias may display metallic behavior (finite current) even if the isolated electronic system does exhibit a band gap. The model to be discussed below... [Pg.312]

The current method of determining the energy properties of polyurethane is the Dynamic Thermal Mechanical Analyzer (DTMA). This instrument applies a cyclic stress/strain to a sample of polyurethane in a tension, compression, or twisting mode. The frequency of application can be adjusted. The sample is maintained in a temperature-controlled environment. The temperature is ramped up over the desired temperature range. The storage modulus of the polyurethane can be determined over the whole range of temperatures. Another important property closely related to the resilience, namely tan delta (8), can also be obtained. Tan (8) is defined in the simplest terms as the viscous modulus divided by the elastic modulus. [Pg.120]

It should be noted that this property of energy becoming less useful as we use it is purely a characteristic of the macroscopic realm. In the microscopic world, energy is continually transformed between kinetic and potential forms, as in a vibrating molecule, or between molecular energy and radiation, as in a molecule in a laser cavity. How microscopic systems combine to give the very different energy properties of macroscopic systems will be the subject material of Chapter 5. [Pg.85]

Therefore, biologically mediated kinetic fractionation, where the products will have more of the lighter isotope in them due to differential partitioning from higher energy properties, will result in a net depletion of the heavy isotope in the product and a more negative del value. Moreover, kinetic fractionation occurs in reactions that are unidirectional, where the reaction rates actually depend on the isotopic composition of the substrates and products. Thus, the isotopic ratio of the substrate is related to the amount... [Pg.161]

Most of the measurements discussed in this chapter deal with physical properties, such as length, volume, or weight. Measurement of these properties can be made directly. Temperature is different because it is an energy property, and energy cannot be measured directly. However, we can quantify the effect that one body s energy (in this case heat) has on the physical properties of another body, and we can measure that physical effect. [Pg.144]


See other pages where Energy properties is mentioned: [Pg.533]    [Pg.506]    [Pg.1147]    [Pg.256]    [Pg.2]    [Pg.2]    [Pg.189]    [Pg.21]    [Pg.659]    [Pg.206]    [Pg.204]    [Pg.332]    [Pg.286]    [Pg.339]    [Pg.493]    [Pg.429]    [Pg.454]    [Pg.534]    [Pg.27]    [Pg.532]    [Pg.129]    [Pg.178]    [Pg.244]    [Pg.49]    [Pg.56]    [Pg.172]    [Pg.159]    [Pg.534]   
See also in sourсe #XX -- [ Pg.115 ]




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Atomic Charges, Bond Properties, and Molecular Energies, by Sandor Fliszar

Atomic properties energy

Atomic properties ionization energy

Biomass properties energy content

Bond dissociation energy properties, table

Chemical properties high-energy radiation

Coulomb energy minimal properties

Dissociation energy properties

Donor-acceptor energy levels property, energies

Electron and Energy Transfer Properties

Energies and molecular properties

Energy Absorption Properties

Energy Band Structure, Optical Properties, and Spectroscopic Phenomena of a-BN

Energy Derivatives and Properties

Energy balances properties

Energy balances with variable properties

Energy expansion, property derivatives from

Energy levels properties

Energy particle-like properties

Energy storage, electrochemical properties

Energy transfer photochemical properties

Energy transfer properties

Energy transfer properties (thick films

Energy-dissipating properties

Energy-dissipating properties material with

Energy-harvesting system physical properties

Ethane, bond properties dissociation energies

Excess properties Gibbs energy

Excitation energies properties

Extensive property free energy

Fermi Energy and Related Properties

Fermi Energy and Related Properties Metals

Fermi Energy and Related Properties of Metals

Finite energy modelling material properties

Forster resonance energy transfer properties

Fundamental Property Relations Based on the Gibbs Energy

Gibbs energy excess-property relation

Gibbs energy fundamental property relations

Gibbs energy properties

Gibbs energy residual-property relation

Gibbs free energy properties

Homological Properties of Constant-Energy Surfaces

Inherent structure property, potential energy

Ionization energy properties

Lattice Energy and Its Effect on Properties

Link between Energy Storage and System Property

Mechanical properties fracture energy

Mechanical properties high-energy radiation

Miscellaneous Properties - UV Spectra, Ionization Energies, and Electron Affinities

Mixture Properties from Helmholtz Energy Equations of State

Molecules, properties energy levels

Nano-emulsion formation by low energy methods and functional properties

Negative-energy states properties

Optical properties energy conversion

Partial molar properties Gibbs energy

Partial molar property free energy

Periodic property ionization energy

Plasma surface energy properties

Properties Gibbs free energy of formation

Properties as Energy Derivatives

Properties of Electron Energy Band Systems

Properties of Kinetic Energy Functional

Properties of Potential Energy Surfaces

Properties of the Gibbs energy

Properties of the Helmholtz free energy

Properties of the energy

Properties of the potential energy surface relevant to transition state theory

Properties, after high-energy electron

Properties, after high-energy electron irradiation

Quantitative structure-property energy descriptors

Quantitative structure-property total interaction energy

Redox properties free energy

Relation of Bond Energies to Other Molecular Properties

Specific property kinetic energy

Spin-orbit effects on total energies and properties

State property energy

Symmetric properties energy functional form

Symmetric properties potential energy surfaces

Tear, Fracture Energy, Compression Set and Rebound Properties

The Theory and Computation of Energy Deposition Properties

Thermal energy properties related

Thermodynamic Properties from Helmholtz Energy Equations of State

Thermodynamic properties Gibbs energy

Thermodynamic properties Helmholtz energy

Thermodynamic properties energy

Thermodynamic properties internal energy

Thermodynamic properties surface energy

Total Energy and Structural Properties

Transformed Gibbs energy thermodynamic properties

Weathering properties thermal energy

Wetting Properties Surface Energy and Tension

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