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Geometry absorption

Thioxanthone MP2 CASPT2 Geometry, absorption spectra 2006JPH(179)298... [Pg.732]

Much of his work, discussed in Chapter 8 of this book, is important because chemical actinometry is the only way of truly measuring the absorbed dosage of the incident radiation. A chemical actinometer corrects for container problems such as reflection, refraction, geometry, absorption, internal reflections, etc. [Pg.18]

The influences on the IMPS response of the illumination geometry, absorption coefficient, and electron recombination lifetime predicted for the diffusion controlled case are illustrated in Fig. 46 and Fig. 47. Two cases are considered corresponding to interband excitation and to dye sensitisation. In the first the penetration depth of the light is chosen to be much smaller than the film thickness. The calculated IMPS responses for illumination from the electrolyte and from the substrate side are contrasted in Fig. 46a and 46b respectively. The first thing to note is that the imaginary component of the IMPS response is negative under most conditions. This contrasts... [Pg.153]

Although it is possible in principle to theoretically calculate the element concentrations on the basis of this equation (taking into account the incident beam intensity, instrument geometry, absorption effects, detector efficiencies, etc.) (see e g., Bos and Vrielink 1998 Jenkins 1999 Hansteen et al. 2000), this is almost never done because of the inherent uncertainties in the numerous parameters. Instead various forms of standardization are utilized in an attempt to reduce the number of dependent variables. There are two general approaches (1) use a standard for each element of interest and (2) use an internal standard element. [Pg.440]

In order to measure a Mossbauer spectrum one has to detect recoilless absorption or emission of a selected y radiation as a function of the Doppler velocity of the sample and a reference material relative to each other. In the most common case of transmission geometry, absorption of the y rays is measured, and the reference material is a standard source, which is moved. Thus, the most important components of a Mossbauer spectrometer are a Doppler velocity drive system and an energy selective y detection chain with appropriate recording system. [Pg.1428]

Electron attachment energies at neutral ground state geometry Eva vertical excitation energy at the anion ground state geometry Absorption maxima in acetonitrile/water... [Pg.527]

Figure Bl.22.10. Carbon K-edge near-edge x-ray absorption (NEXAFS) speetra as a fiinotion of photon ineidenee angle from a submonolayer of vinyl moieties adsorbed on Ni(lOO) (prepared by dosing 0.2 1 of ethylene on that surfaee at 180 K). Several eleetronie transitions are identified in these speetra, to both the pi (284 and 286 eV) and the sigma (>292 eV) imoeeupied levels of the moleeule. The relative variations in the intensities of those peaks with ineidenee angle ean be easily eonverted into adsorption geometry data the vinyl plane was found in this ease to be at a tilt angle of about 65° from the surfaee [71], Similar geometrieal detenninations using NEXAFS have been earried out for a number of simple adsorbate systems over the past few deeades. Figure Bl.22.10. Carbon K-edge near-edge x-ray absorption (NEXAFS) speetra as a fiinotion of photon ineidenee angle from a submonolayer of vinyl moieties adsorbed on Ni(lOO) (prepared by dosing 0.2 1 of ethylene on that surfaee at 180 K). Several eleetronie transitions are identified in these speetra, to both the pi (284 and 286 eV) and the sigma (>292 eV) imoeeupied levels of the moleeule. The relative variations in the intensities of those peaks with ineidenee angle ean be easily eonverted into adsorption geometry data the vinyl plane was found in this ease to be at a tilt angle of about 65° from the surfaee [71], Similar geometrieal detenninations using NEXAFS have been earried out for a number of simple adsorbate systems over the past few deeades.
Zaera F, Fischer D A, Carr R G and Gland J L 1988 Determination of chemisorption geometries for complex molecules by using near-edge X-ray absorption fine structure ethylene on Ni(IOO) J. Chem. Rhys. 89 5335-41... [Pg.1798]

On e type of single point calculation, that of calculating vibration al properties, is distinguished as a vihmiions calculation in Ilyper-Chein. A lufcratilrui.s calculation predicts fun dam en tal vibrational frecinencies, m frared absorption in tensities, and norm al modes for a geometry optimized molecular structure. [Pg.16]

Beyond sueh eleetronie symmetry analysis, it is also possible to derive vibrational and rotational seleetion rules for eleetronie transitions that are El allowed. As was done in the vibrational speetroseopy ease, it is eonventional to expand if (R) in a power series about the equilibrium geometry of the initial eleetronie state (sinee this geometry is more eharaeteristie of the moleeular strueture prior to photon absorption) ... [Pg.411]

Thermodynamic properties (71,72), force constants (73), and infrared absorption characteristics (74) are documented. The coordinatively unsaturated species, Ni(CO)2 and Ni(CO)2, also exist and the bonding and geometry data have been subjected to molecular orbital treatments (75,76). [Pg.11]

Infrared spectroscopy has broad appHcations for sensitive molecular speciation. Infrared frequencies depend on the masses of the atoms iavolved ia the various vibrational motions, and on the force constants and geometry of the bonds connecting them band shapes are determined by the rotational stmcture and hence by the molecular symmetry and moments of iaertia. The rovibrational spectmm of a gas thus provides direct molecular stmctural information, resulting ia very high specificity. The vibrational spectmm of any molecule is unique, except for those of optical isomers. Every molecule, except homonuclear diatomics such as O2, N2, and the halogens, has at least one vibrational absorption ia the iafrared. Several texts treat iafrared iastmmentation and techniques (22,36—38) and thek appHcations (39—42). [Pg.314]

In the foregoing discussion polymers have been used as a medium for smaU molecules in comparison with the crystalline state. It has also been observed that there are changes in polymeric geometry and various rotational motions introduced by pressure (10—14). These are at times reflected in the absorption spectmm (usuaUy in the ultraviolet) or in the emission spectmm and are a form of piezochromism. [Pg.168]

To determine the mass-transfer rate, one needs the interfacial area in addition to the mass-transfer coefficient. For the simpler geometries, determining the interfacial area is straightforward. For packed beds of particles a, the interfacial area per volume can be estimated as shown in Table 5-27-A. For packed beds in distillation, absorption, and so on in Table 5-28, the interfacial area per volume is included with the mass-transfer coefficient in the correlations for HTU. For agitated liquid-liquid systems, the interfacial area can be estimated... [Pg.606]


See other pages where Geometry absorption is mentioned: [Pg.240]    [Pg.47]    [Pg.240]    [Pg.47]    [Pg.20]    [Pg.105]    [Pg.571]    [Pg.1243]    [Pg.1781]    [Pg.1791]    [Pg.1792]    [Pg.1792]    [Pg.507]    [Pg.157]    [Pg.216]    [Pg.378]    [Pg.288]    [Pg.18]    [Pg.161]    [Pg.199]    [Pg.122]    [Pg.420]    [Pg.494]    [Pg.128]    [Pg.4]    [Pg.167]    [Pg.167]    [Pg.168]    [Pg.168]    [Pg.170]    [Pg.407]    [Pg.90]    [Pg.201]    [Pg.604]    [Pg.135]    [Pg.423]    [Pg.208]    [Pg.212]   
See also in sourсe #XX -- [ Pg.80 ]

See also in sourсe #XX -- [ Pg.80 ]




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