Big Chemical Encyclopedia

Chemical substances, components, reactions, process design ...

Articles Figures Tables About

Structures energy used

The electronic energy, as detennined from must be added to tire ion-ion interactions to obtain the structural energies. This is a straightforward calculation for confined systems. For extended systems such as crystals, the calculations can be done using Madelimg summation techniques [2]. [Pg.97]

Many phenomena in solid-state physics can be understood by resort to energy band calculations. Conductivity trends, photoemission spectra, and optical properties can all be understood by examining the quantum states or energy bands of solids. In addition, electronic structure methods can be used to extract a wide variety of properties such as structural energies, mechanical properties and thennodynamic properties. [Pg.113]

Marchut L, Buck T M, Wheatley G H and McMahon C J Jr 1984 Surface structure analysis using low energy ion scattering Surf. Sc/. 141 549-66... [Pg.1825]

Very early force fields were used in an attempt to calculate structures, enthalpies of formation, and vibrational spectra, but it was soon found that accuracy suffered severely in either the structure-energy calculations or the vibrational spectra. Force constants were, on the whole, not transferable from one field to another. The result was that early force fields evolved so as to calculate either structure and energy or spectra, but not both. [Pg.161]

Figure 6 Steps in automated assignment. (1) Select the lowest energy structures from iteration / — 1 that are used to interpret the spectra. (2) For each peak, list all possible assignments compatible with the resonances within a frequency mnge. (3) Extract a distance for each assignment possibility from the ensemble of structures. (4) Use the distances to assign ambiguous NOEs. (5) Calibrate the peak volumes to obtain distance restraints. (6) Calculate structures based on the new restraints. Figure 6 Steps in automated assignment. (1) Select the lowest energy structures from iteration / — 1 that are used to interpret the spectra. (2) For each peak, list all possible assignments compatible with the resonances within a frequency mnge. (3) Extract a distance for each assignment possibility from the ensemble of structures. (4) Use the distances to assign ambiguous NOEs. (5) Calibrate the peak volumes to obtain distance restraints. (6) Calculate structures based on the new restraints.
L Chiche, LM Gregoret, FE Cohen, PA Kollman. Protein model structure evaluation using the solvation free energy of folding. Proc Natl Acad Sci USA 87 3240-3244, 1990. [Pg.310]

Fine structure extending several hundred eV in kinetic energy below a CEELS peak, analogous to EXAFS, have been observed in REELS. Bond lengths of adsorbed species can be determined from Surface Electron Energy-Loss Fine Structure (SEELFS) using a modified EXAFS formalism. [Pg.328]

Figures Quantitative high depth resoiution profile of a complex Ai Ga. j As laser diode test structure obtained using electron-gas SNMS in the direct bombardment mode, with 600-V sputtering energy. The data have been corrected for relative ion yield variations and summed to Al + Ga = 50%. The 100-A thick GaAs layer is very well resolved. Figures Quantitative high depth resoiution profile of a complex Ai Ga. j As laser diode test structure obtained using electron-gas SNMS in the direct bombardment mode, with 600-V sputtering energy. The data have been corrected for relative ion yield variations and summed to Al + Ga = 50%. The 100-A thick GaAs layer is very well resolved.
Electronic structure methods use the laws of quantum mechanics rather than classical physics as the basis for their computations. Quantum mechanics states that the energy and other related properties of a molecule may be obtained by solving the Schrodinger equation ... [Pg.5]

Determine which of the minima are connected by this transition structure and predict the activation barriers for the reactions. Run your frequency and IRC calculations at the HF/6-31G(d) level, and compute final energies using the MP4 method with the same basis set. [Pg.200]

Figure 2. The structural energy difference (a) and the magnetic moment (b) as a function of the occupation of the canonical d-band n corresponding to the Fe-Co alloy. The same lines as in Fig. 1 are used for the different structures. In (b) the concentration dependence of the Stoner exchange integral Id used for the spin-polarized canonical d-band model calculations is shown as a thin dashed line with the solid circles. The value of Id for pure Fe and Co, calculated from LSDA and scaled to canonical units, are also shown in (b) as solid squares. Figure 2. The structural energy difference (a) and the magnetic moment (b) as a function of the occupation of the canonical d-band n corresponding to the Fe-Co alloy. The same lines as in Fig. 1 are used for the different structures. In (b) the concentration dependence of the Stoner exchange integral Id used for the spin-polarized canonical d-band model calculations is shown as a thin dashed line with the solid circles. The value of Id for pure Fe and Co, calculated from LSDA and scaled to canonical units, are also shown in (b) as solid squares.
The structure and energy use of post-World War II commercial buildings was re defined as a direct result of air conditioning. [Pg.191]

The trends dcinoiistratc the capability of industiy to improve energy efficiency when it has the incentive to do so. Energy requirements can be cut by new process development. In addition, the amount of raw materials demanded by a society tends to decline as countries reach certain stages of industrial development, which leads to a decrease in industrial energy use. The accounting of trends in structural shift, material intensity, and technical energy efficiency... [Pg.749]

Howarth, R. B. Schipper, L. Duerr, P. A. and Strom, S. (1991). Manufacturing Energy Use in Eight OECD Countries, Decomposing the Impacts of Changes in Output, Industry Structure, and Energy Intensity. Energy Economics 13 135-142. [Pg.757]

In order to explore mechanism a, or any other mechanism, we have to start by defining the most important resonance structures and calibrating their energies using the relevant experimental information for the reference system in solution. The key resonance structures for the formation of t in mechanism a are... [Pg.173]

The smaller cluster ions 83", 84" and 85 + have been examined by Zakrzewski and von Niessen at the HF/6-3H-G level [82]. The lowest cationic states are predicted to be 82, and A" for 83 (Cyv), 84 (I>4h) and (Cs), respectively. The ionisation processes may result in significant structural relaxation leading to the sequence of states different from that of the vertical states. The calculated lowest adiabatic ionisation energies, using the GI method with a very large ANO basis set, are 9.53, 8.05, and 8.20 eV for 83, 84 and 85 , respectively. [Pg.18]


See other pages where Structures energy used is mentioned: [Pg.440]    [Pg.338]    [Pg.55]    [Pg.137]    [Pg.654]    [Pg.680]    [Pg.289]    [Pg.166]    [Pg.55]    [Pg.111]    [Pg.267]    [Pg.281]    [Pg.288]    [Pg.306]    [Pg.403]    [Pg.459]    [Pg.212]    [Pg.300]    [Pg.93]    [Pg.16]    [Pg.227]    [Pg.231]    [Pg.147]    [Pg.319]    [Pg.14]    [Pg.14]    [Pg.365]    [Pg.449]    [Pg.204]    [Pg.463]    [Pg.749]    [Pg.757]    [Pg.765]    [Pg.132]    [Pg.620]   
See also in sourсe #XX -- [ Pg.22 , Pg.267 ]




SEARCH



Energy structure

Energy use

Structural Simulation using Pair Potentials Energy Calculation

© 2024 chempedia.info