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Chemical perturbation

Human civilization interferes more and more with the cycles that cormect land, water, and atmosphere, and pollution seriously affects water quahty. In order to assess the stresses caused to aquatic ecosystems by chemical perturbation, the distribution of pollutants and their fate in the environment must be investigated (see Air pollution). [Pg.207]

Gormin D, Kasha M (1988) Triple fluorescence in aminosalicylates. Modulation of normal, proton-transfer, and twisted intramolecular charge-transfer (TICT) fluorescence by physical and chemical perturbations. Chem Phys Lett 153 574-576... [Pg.265]

Chemical perturbations can be a useful approach to this problem. In laccase, selective replacement of the type 1 coppo- with mercury has allowed the type 1 site in laccase to be characterized stmcturally, even in the presence of three other copper atoms (27). Likewise, Simolo et al. have studied independently the a and 3 subunits in hemoglobin by preparation of the (a-M)2(P-M )2 derivaties, where M and M are different metals (28). An alternative to replacement is metal removal, for example Cu in cytochrome-c oxidase (29) or the T3 Ci in laccase (30). The concern with all of these approaches is to establish that the modified protein has the same metal-site structures as the native protein. [Pg.38]

A suitable fiuorescent probe is an organic molecule, which must change its characteristic parameters with changes in its microenvironment and the parameter must be measurable when the probe is added to the system [54]. The fluorescent probes are categorized as either extrinsic, intrinsic, or covalently bound probes. The intrinsic probes allow a system to be observed without any chemical perturbation. This occurs when the system to be characterized has an in-built fluorescent chromophore unit like tryptophan, tyrosine and phenyl alanine in protein. In some cases the fluorophore is covalently... [Pg.150]

Lelieveld, J., B. Bregman, F. Arnold, V. Burger, P. J. Crutzen, H. Fischer, A. Waibel, P. Siegmund, P. F. J. van Velthoven, Chemical Perturbation of the Lowermost Stratosphere through Exchange with the Troposphere, Geophys. Res. Lett., 24, 603-606 (3997). [Pg.717]

Simulation of the Dynamical Response of the Arctic Vortex to Aerosol-Associated Chemical Perturbations in the Lower Stratosphere, Geophys. Res. Lett., 23, 1525-1528 (1996). [Pg.726]

Figure 1. This graph shows the rapid variation of CIO and 03 as the edge of the chemically perturbed region in the Antarctic polar vortex is penetrated by the National Aeronautics and Space Administration (NASA) ER-2 high-altitude aircraft over the Palmer Peninsula of Antarctica on September 16, 1987 (5). It is one of a series of 12 snapshots, or individual flights, during the Airborne Antarctic Ozone Experiment (AAOE) that show the development of an anticorrelation between CIO and 03 that began as a correlation in mid-August. When these two measurements are combined with all the others from the ER-2 aircraft, the total data set provides a provocative picture of how such chemistry occurs and what it is capable of doing to ozone. Figure 1. This graph shows the rapid variation of CIO and 03 as the edge of the chemically perturbed region in the Antarctic polar vortex is penetrated by the National Aeronautics and Space Administration (NASA) ER-2 high-altitude aircraft over the Palmer Peninsula of Antarctica on September 16, 1987 (5). It is one of a series of 12 snapshots, or individual flights, during the Airborne Antarctic Ozone Experiment (AAOE) that show the development of an anticorrelation between CIO and 03 that began as a correlation in mid-August. When these two measurements are combined with all the others from the ER-2 aircraft, the total data set provides a provocative picture of how such chemistry occurs and what it is capable of doing to ozone.
Figure 1. Simultaneous measurements of CIO and 0 i over Antarctica on September 16, 1987, during the AAOE mission. The boundary of the chemically perturbed region at 69°S is clearly shown by the rapid increase in the CIO mixing ratio and the rapid decrease in the 03 mixing ratio. There is an anticorrelation between CIO and 03 near the boundary. Figure 1. Simultaneous measurements of CIO and 0 i over Antarctica on September 16, 1987, during the AAOE mission. The boundary of the chemically perturbed region at 69°S is clearly shown by the rapid increase in the CIO mixing ratio and the rapid decrease in the 03 mixing ratio. There is an anticorrelation between CIO and 03 near the boundary.
Figure 7. Calculated ozone production and loss rates for two different conditions from the AER two-dimensional model. Production and loss rates above 20 km are diurnally averaged loss rates for the spring equinox at 30°N. Midday loss rates are approximately two times larger. Production and loss rates for midday below 20 km are calculated for the chemically perturbed region over Antarctica on September 16,1987. The catalytic cycles responsible for the loss are explained in the text. Although ozone loss occurs at higher altitudes over Antarctica, in situ observations extend only to 19 km. Figure 7. Calculated ozone production and loss rates for two different conditions from the AER two-dimensional model. Production and loss rates above 20 km are diurnally averaged loss rates for the spring equinox at 30°N. Midday loss rates are approximately two times larger. Production and loss rates for midday below 20 km are calculated for the chemically perturbed region over Antarctica on September 16,1987. The catalytic cycles responsible for the loss are explained in the text. Although ozone loss occurs at higher altitudes over Antarctica, in situ observations extend only to 19 km.
The NOf/ values were significantly different, however, and much more NOy was removed in the Southern Hemisphere compared to the Northern Hemisphere. The curve of NOy marks the profile of NOy predicted by measurements of the N20. However, in patches and later in the mission, as much as 35% of the NOy was observed to be removed even in the Arctic. The NO abundance, not shown in Figure 9, was measured to be below the detection limit of the instrument in both chemically perturbed regions. [Pg.161]

The chemical perturbations of the nuclear levels can be divided into two classes. One effect is the electrostatic interaction between the nuclear charge and the surrounding electric charges, and the other effect is the magnetic interaction between the nuclear magnetic moment and the surrounding electron spin density. The former of these interactions will be discussed next. [Pg.130]

In the previous sections, chemical perturbations that split the nuclear energy states were discussed. These splittings result in multipeak Mossbauer spectra, and as such provide valuable catalytic information. However, from the shape and relative intensities of the various resonance peaks, additional information can be obtained, as will be discussed presently. [Pg.147]

In the previous sections it was shown that chemical perturbations of the nuclear energy states provide information useful in catalytic studies. To obtain this information, however, a source of y radiation with variable energy... [Pg.151]

In order to facilitate the modeling as well as the physical interpretation of the pressure transmission - chemical potential test, the loading is decomposed into two fundamental modes corresponding to a hydraulic and a chemical perturbation. The upstream boundary conditions at 2 0 for each of the loading... [Pg.129]

We have now seen that the effort of Parr and collaborators [8-12] to put Fukui s frontier-orbital concept of chemical reactivity on sound footing in density-functional theory through the definition of the Fukui function and the local and global softness works only for extended systems. This restriction to extended systems raises a sixth issue. In both the local softness and the Fukui function, Eqs. (54) and (53a), the orbitals at the chemical potential represent both the LUMO and the HOMO in the Fukui sense. However, there is a continuum of unoccupied KS states above the chemical potential accessible even to weak chemical perturbations any linear combination of which could in principle be selected as the LUMO, and similarly for states below fi and the HOMO. This ambiguity in the frontier-orbital concept obviously applies as well to localized systems when there is more than one KS state significantly affected by a chemical perturbation. [Pg.164]

Another source of structural information is the electrochemical response of the analyte to chemical perturbations. Changes in solution conditions have been useful in classical studies of structure-activity relationships. Exploration of a variety of solutions will help define the best conditions for particular classification problems. [Pg.109]


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See also in sourсe #XX -- [ Pg.188 ]




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Application of Perturbation Theory to Chemical Kinetic Systems

Chemical oscillators periodic perturbation

Chemical relaxation methods step perturbation

Chemical shift perturbation

Coupled-perturbed Hartree-Fock chemical shifts

Density functional perturbation theory chemical potential

Many-body perturbation theory chemical shifts

Moller-Plesset perturbation theory chemical applications

Perturbation theory chemical reactivity

Perturbation theory of chemical reactivity

Perturbations of chemical shifts

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