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Energy from

Solution gas drive occurs in a reservoir which contains no initial gas cap or underlying active aquifer to support the pressure and therefore oil is produced by the driving force due to the expansion of oil and connate water, plus any compaction drive.. The contribution to drive energy from compaction and connate water is small, so the oil compressibility initially dominates the drive energy. Because the oil compressibility itself is low, pressure drops rapidly as production takes place, until the pressure reaches the bubble point. [Pg.186]

It is the indication of a transfer of energy from a distance between the solenoid and the conductor material. The cause of the variation of impedance observed is the modification of the magnetic flow through the solenoid. The flow varies in amplitude and in phase. [Pg.349]

The use of air-bome ultrasound for the excitation and reception of surface or bulk waves introduces a number of problems. The acoustic impedance mismatch which exists at the transducer/air and the air/sample interfaces is the dominant factor to be overcome in this system. Typical values for these three media are about 35 MRayls for a piezo-ceramic (PZT) element and 45 MRayls for steel, compared with just 0.0004 MRayls for air. The transmission coefficient T for energy from a medium 1 into a medium 2 is given by... [Pg.840]

Typically, the ratio of this to the incident flux detennines the transition probability. This infonnation will be averaged over the energy range of the initial wavepacket, unless one wants to project out specific energies from the solution. This projection procedure is accomplished using the following expression for the energy resolved (tune-independent) wavefunction in tenns in tenns of its time-dependent counterpart ... [Pg.981]

The tenn (E-E ) is tire sum of states at the transition state for energies from 0 to E-E. Equation (A3.12.15) is the RRKM expression for the imimolecular rate constant. [Pg.1013]

Modem photochemistry (IR, UV or VIS) is induced by coherent or incoherent radiative excitation processes [4, 5, 6 and 7]. The first step within a photochemical process is of course a preparation step within our conceptual framework, in which time-dependent states are generated that possibly show IVR. In an ideal scenario, energy from a laser would be deposited in a spatially localized, large amplitude vibrational motion of the reacting molecular system, which would then possibly lead to the cleavage of selected chemical bonds. This is basically the central idea behind the concepts for a mode selective chemistry , introduced in the late 1970s [127], and has continuously received much attention [10, 117. 122. 128. 129. 130. 131. 132. 133. 134... [Pg.1060]

Figure Bl.24.5. Backscattering spectrum of a thin Ni film (950 A) with near monolayers ( 30 x 10 at cm of An on the front and back surfaces of the Ni film. The signals from the front and back layers of An are shown and are separated in energy from each other by nearly the same energy width as the Ni signal. Figure Bl.24.5. Backscattering spectrum of a thin Ni film (950 A) with near monolayers ( 30 x 10 at cm of An on the front and back surfaces of the Ni film. The signals from the front and back layers of An are shown and are separated in energy from each other by nearly the same energy width as the Ni signal.
A liquid serves as the calorimetric medium in which the reaction vessel is placed and facilitates the transfer of energy from the reaction. The liquid is part of the calorimeter (vessel) proper. The vessel may be isolated from the jacket (isoperibole or adiabatic), or may be in good themial contact (lieat-flow type) depending upon the principle of operation used in the calorimeter design. [Pg.1903]

When the initial and final internal states of the system are not well-separated in energy from other states then the closed-coupling calculation converges very slowly. An effective strategy is to add a series of correlation temis involving powers of the distance r. between internal particles of projectile and target to the tmncated close-coupling expansion which already includes the important states. [Pg.2050]

Figure C2.17.12. Exciton energy shift witli particle size. The lowest exciton energy is measured by optical absorjDtion for a number of different CdSe nanocrystal samples, and plotted against tire mean nanocrystal radius. The mean particle radii have been detennined using eitlier small-angle x-ray scattering (open circles) or TEM (squares). The solid curve is tire predicted exciton energy from tire Bms fonnula. Figure C2.17.12. Exciton energy shift witli particle size. The lowest exciton energy is measured by optical absorjDtion for a number of different CdSe nanocrystal samples, and plotted against tire mean nanocrystal radius. The mean particle radii have been detennined using eitlier small-angle x-ray scattering (open circles) or TEM (squares). The solid curve is tire predicted exciton energy from tire Bms fonnula.
Once prepared in S q witli well defined energy E, donor molecules will begin to collide witli batli molecules B at a rate detennined by tire batli-gas pressure. A typical process of tliis type is tire collision between a CgFg molecule witli approximately 5 eV (40 000 cm or 460 kJ mor ) of internal vibrational energy and a CO2 molecule in its ground vibrationless state 00 0 to produce CO2 in tire first asymmetric stretch vibrational level 00 1 [11,12 and 13]. This collision results in tire loss of approximately AE= 2349 cnA of internal energy from tire CgFg,... [Pg.2999]

Sharma R D and Brau C A 1969 Energy transfer in near-resonant molecular collisions due to long-range forces with application to transfer of vibrational energy from the mode of CO2 to N2 J. Chem. Phys. 50 924-30... [Pg.3015]


See other pages where Energy from is mentioned: [Pg.204]    [Pg.314]    [Pg.45]    [Pg.181]    [Pg.216]    [Pg.343]    [Pg.70]    [Pg.280]    [Pg.281]    [Pg.347]    [Pg.348]    [Pg.638]    [Pg.77]    [Pg.88]    [Pg.97]    [Pg.126]    [Pg.193]    [Pg.357]    [Pg.393]    [Pg.405]    [Pg.894]    [Pg.905]    [Pg.915]    [Pg.934]    [Pg.1312]    [Pg.1322]    [Pg.1811]    [Pg.2317]    [Pg.2531]    [Pg.2815]    [Pg.2955]    [Pg.2997]    [Pg.2999]    [Pg.3007]    [Pg.3010]   
See also in sourсe #XX -- [ Pg.448 ]

See also in sourсe #XX -- [ Pg.448 ]




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Activation energies from Arrhenius equation

Activation energy determining, from experimental

Activation energy from diffusion

Activation, energy differentiated from

Activity coefficient from excess Gibbs energy

Agricultural thermal energy from

Analysis of Band Gap Energies from UV-Vis Spectra

Application of Complete Energy Expression to Results Obtained from the Hard-Sphere Potential

Atomic Energies from ONETEP

Biomass energy from

Biomass energy production from

Bond dissociation energy enthalpy change calculation from

Bond dissociation energy from thermochemical data

Bond energies from electron-transfer

Bond energies from spectra

Born-Oppenheimer energy surface from molecular vibrations

Calculated surface energies from pull-off data

Carbohydrates energy from

Carbonyl groups energy transfer from

Catabolism energy from

Catalysis for Renewables: From Feedstock to Energy Production

Characteristics of Type I ELM Energy and Particle Losses from the Core Plasma

Chemical Energy from Carbohydrates

Clean fuels, from fossil energy sources

Cohesive energies from monolayer

Cohesive energies from monolayer desorption

Combustion energy recovery from wood

Contributions of textile materials to reduce the operational energy demand, and comparisons with examples from nature

Direct fuel cells , from FuelCell Energy

Disposal methods energy recovery from

Dissociation energy determination from

ENERGY CAN BE HARNESSED FROM SUNLIGHT

Effective atomic number from ionization energy

Eigenfunctions extracted from wavepacket dynamics Energy screening

Electric power generation from geothermal energy

Electrical Energy from Nuclear Fission

Electrical Energy from Oxidation-Reduction Reactions

Electrical energy from thermal

Electrical energy from thermal conversion

Electricity production from nuclear energy

Electrode potentials, standard calculating free energy changes from

Electrolysis, hydrogen from Proton Energy Systems

Electron-phonon coupling energies from experimental data

Electronegativities from bond energies

Electrons secondary from high energy radiation

Endurance exercise energy from protein

Energies calculated from different

Energies calculated from different techniques

Energy Conservation by Heat Recovery from Flue Gases

Energy Transfer from

Energy Transfer from Photosensitive Polymers to SWNTs

Energy Transfer to and from Carotenoids in Photosynthesis

Energy Variation Under Transition from Bulk to Clusters

Energy Yield from Fatty Acid Oxidation

Energy Yield from Glucose Oxidation

Energy Yields from Oxidative Phosphorylation

Energy amount released from fission

Energy and Charge Distribution Changes from Orbital Interaction

Energy aromaticity from

Energy bands from atomic levels

Energy calculation from wavefunction

Energy collisional, from excited

Energy deviations from full

Energy dissipation resulting from chain

Energy dissipation resulting from chain extension

Energy expansion, property derivatives from

Energy flow to and from a system

Energy from ATP hydrolysis

Energy from Earths Two Great Fluids in Motion

Energy from Glucose

Energy from Moving Water

Energy from agricultural residues

Energy from an Approximate Wave Function

Energy from biomass-derived

Energy from bismuth

Energy from carbon oxidation

Energy from cerium

Energy from chromium

Energy from combustion reactions

Energy from displacement reactions

Energy from electrostatic discharges

Energy from fission products

Energy from foods

Energy from fuels

Energy from human activity

Energy from incineration

Energy from inorganic reactions

Energy from nuclear fission reaction

Energy from nuclear reactions

Energy from oxidative phosphorylation

Energy from partition function

Energy from thallium

Energy from the sun

Energy from unimolecular reactions

Energy from waste conversion

Energy from waste conversion process

Energy from wood

Energy generation, from biomass

Energy insight from past

Energy loss from stationary nuclei

Energy matter distinct from

Energy of Activation from Chemical Stress Relaxation Times

Energy of Particles Backscattered from Thin and Thick Targets

Energy of adsorption from

Energy of dissociation from continuous absorption

Energy of the Ideal Gas from State Functions

Energy percentage from carbohydrates

Energy percentage from fatty acids

Energy percentage from protein

Energy production from fossil fuels

Energy production from nuclear power

Energy production from petroleum products

Energy recovery from high-pressure streams

Energy recovery from high-temperature reactors

Energy recovery from vent gases

Energy recovery from waste gasification

Energy recovery from waste solvent

Energy recovery from wastes

Energy recovery savings from

Energy sources extract order from

Energy sources pollution from

Energy total, from self-consistent electron density

Energy transfer from irradiated solids

Energy transfer from probe

Energy transfer from sensitizer singlet

Energy transfer from sensitizer singlet states

Energy transfer from surface

Energy transfer from transition metal ions

Energy transfer from transition metal ions elements

Energy transfer, from donor to acceptor

Energy, activation from inorganic compounds

Energy, recovery from pump turbines

Energy-level diagram, derived from molecular

Enthalpy change estimation from bond dissociation energy

Enthalpy reaction from bond energies

Entropy extract, from energy

Estimation of Crack-Driving Force G from Energy Loss Rate (Irwin and Kies

Exact exchange energy density functional from Fock operator

Excitation energy transfer from fucoxanthin

Excitation energy, first from correlation potentials

Excited states, energy dissipation from

FERs from VB Studies of Free Energy Changes for PT in Condensed Phases

Fatty acid metabolism energy yield from

Fatty acids energy from

Fatty acids energy yield from

Fission products energy release from

Fluorescein energy transfer from coumarin

Fluorescein energy transfer from coumarin derivatives

Fluorescence energy transfer from phenyl group

Force derived from potential energy

Forster energy transfer experiments from Trp residues to calcofluor white

Forster energy transfer from quantum dots to organics

Fossil fuel combustion energy from

Fourth-order energy from coupled-cluster doubles

Free Energies from Histograms

Free Energies from Transition Path Sampling Simulations

Free energies and enthalpies of formation from the elements

Free energy calculating electromotive force from

Free energy calculating from electrode potentials

Free energy changes from oxidation/reduction

Free energy from carbon oxidation

Free energy from ionic fluctuations

Free energy from radioactivity

Free energy from simulations

Free energy landscape from metadynamics

Free energy of formation from the

Free energy of formation from the elements

Free energy surfactants transferred from

Free-energy barrier for escape of water molecules from protein hydration layer

From Bond Energies to Heats of Reaction

From Delocalisation Energies

From Plastic Waste to Feedstocks and Energy by Means of Fluidized-bed Pyrolysis

From molecular potential energy to rates of reaction

Fuels from Energy Crops

Gaseous wastes energy recovery from

Generating energy from catabolism

Gibbs energy change on transfer of ions from water to organic

Gibbs energy from heat capacity

Gibbs energy from partition function

Gibbs energy, hydrocarbons from liquid

Grain plant, energy production from

Helium atom energy from perturbation theory

Helmholtz Free Energy from the CS Approximation

Helmholtz energy from partition function

Helmholtz free energy from heat capacity

Helmholtz free energy from partition function

How Scientists Learned to Distinguish Energy from Force (Brief Historic Review)

Hydroelectric Power Comes from the Kinetic Energy of Flowing Water

Hydrogen Produced from Wind Energy

Hydrogen from Nuclear Energy

Hydrogen from Water Using Renewable Energy

Hydrogen from solar energy

Incandescent objects, energy from

Industry sector, thermal energy from

Intelligent Energy process from

Internal energy I From statistics and quantum mechanics

Internal energy from measurables

Internal energy from partition function

Iodine excited, energy transfer from

Ionization energies determination from emission

Iron energy from reaction

Kinetic Energies Calculated from Density Gradient Expansion

Kinetic energy lost from

Lattice energy estimates from an electrostatic model

Lattice energy estimates from electrostatic model

Lattice energy from point-charge model

Liquid wastes energy recovery from

Maximum Obtainable Useful Energy from a System

Measurement of energy transfer efficiency from Trp residues to TNS

Metabolism energy production from

Methanogenesis energy yield from

Mixing Rules from Models for Excess Gibbs Energy

Mixture Properties from Helmholtz Energy Equations of State

Molecular orbitals chemical bond energy from

Nitric energy transfer from

Nuclear energy from fission reactors

Nuclear energy from fusion reactors

Nuclear energy hydrogen production from

Nuclear energy waste from

Nuclear fission energy production from

Nuclear fusion energy production from

Pair production, from high energy radiation

Perturbation Theory Energies from the Coupled Cluster Hamiltonian

Petroleum energy production from

Phonon electron coupling energies from

Polymers energy recovery from

Potential Energy Curves from Electronic Band Spectra

Potential Energy Surfaces from Correlated Wavefunctions

Potential energy surface, parameters reaction rates from

Potential energy surfaces determination from high resolution

Potential energy, distortion from vibronic

Potential energy, distortion from vibronic interaction

Power plants energy production from

Principal Considerations Related to Energy Transfer from Charged Particles

Production of Energy from Biomass

Prospects, Challenges, and Opportunities for Energy Recovery from Wastes

Protocol for Free Energy Estimates from Nonequilibrium Work Averages

Quantum Mechanical Force Fields from Ab Initio Data The Theory of Energy Derivatives

Quantum energy flow dynamical corrections to RRKM from

Quenching energy loss from excited species

Radiant energy transfer from flames

Radiation calculating energy from wavelength

Radiation energy from

Rate of energy transfer from the

Resonance energies from thermochemistry

Restrictions on the conversion of energy from one form to another

Risk from various energy sources

Separation energy recovery from

Side effects, energy transfer from

Skewing Momenta Distributions to Enhance Free Energy Calculations from Trajectory Space Methods

Solar energy, hydrogen production from

Solid wastes energy recovery from

Sorption energy from

Spectroscopic excited state energy from redox

Spectroscopic excited state energy from redox potentials

Statistical thermodynamics energy levels, calculations from

Strain energy from equilibrium constants

Sulfur energy from

Surface energy from solubility changes

Surface free energy from cleavage experiments

Switching from Entropy to Free Energy

System energy flow to and from

The Chemical Bond Energy from Molecular Orbitals

The Energy from Fatty Acids

The Relative Energies of Atomic Orbitals from Electronegativity

The link from energy supply to economic development

Thermal energy from agricultural residues

Thermal energy from wood

Thermodynamic Properties from Helmholtz Energy Equations of State

Total Energies from Many-Body Theory

Translational energy releases from photoion—photoelectron coincidence (PIPECO)

Triplet excited states energy transfer from

Typical energy losses from a mains frequency coreless induction furnace

UV Energy from the Sun

Unimolecular reactions, energy disposal from

Variations in adsorption energies from one metal to the next

Waste management energy recovery from

Where does all that energy come from

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