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Composition profile atmosphere

Noble, C. A., and K. A. Prather, Real-Time Size Measurement of Correlated Size and Composition Profiles of Individual Atmospheric Aerosol Particles," Environ. Sci. Technol., 30, 2667-2680 (1996). [Pg.430]

Figure 8. Two depth composition profiles obtained by AES a 304 stainless steel surface exposed to commercial vapor degreasing, then exposed to atmosphere for 15Oo h (a), and a stainless steel surface as received (b). Key O (Xl) ... Figure 8. Two depth composition profiles obtained by AES a 304 stainless steel surface exposed to commercial vapor degreasing, then exposed to atmosphere for 15Oo h (a), and a stainless steel surface as received (b). Key O (Xl) ...
The present work involves measurement of k in a 0.1 atmosphere, stoichiometric CH -Air flame. All experiments were conducted using 3 inch diameter water-cooled sintered copper burners. Data obtained in our study include (a) temperature profiles obtained by coated miniature thermocouples calibrated by sodium line reversal, (b) NO and composition profiles obtained using molecular beam sampling mass spectrometry and microprobe sampling with chemiluminescent analysis and (c) OH profiles obtained by absorption spectroscopy using an OH resonance lamp. Several flame studies (4) have demonstrated the applicability of partial equilibrium in the post reaction zone of low pressure flames and therefore the (OH) profile can be used to obtain the (0) profile with high accuracy. [Pg.375]

Thermogravimetry (TG) or thermogravimetric analysis (TGA). In this technique, the mass of a sample is followed as a function of temperature or time. The amount and rate of mass change with temperature or time in a controlled atmosphere are obtained. Such information can tell us about thermal stability as well as the compositional profile of a variety of elastomers and polymers. It is an excellent quantitative technique but qualitatively there may be some doubt as to what material is lost during heating. [Pg.236]

The burning velocity, and the temperature and composition profiles in a low temperature, fuel-rich hydrogen—nitrogen—oxygen flame at atmospheric pressure having an unbumt gas composition 2, u = 0.1883, A N2,u 0.7657 and Aqj.u = 0.0460, with = 336 K, were measured by Dixon-Lewis et al. [156] while the burning velocities of a number of flames having compositions not too far from this were also examined by Dixon-Lewis and co-workers [158, 159]. In a number of these flames the main reaction zone extended from approximately 600—1060 K, and the predominantly recombination zone from about 1060—1080 K. The maxi-... [Pg.84]

Noble CA, Prather KA (1996) Real-time measurement of correlated size and composition profiles of individual atmospheric aerosol particles. Environ Sci Technol 30 2667-2680... [Pg.344]

Cetin B, Odabasi M (2008) Atmospheric concentrations and phase partitioning of polytaominated diphenyl ethers (PBDEs) in Izmir, Turkey. Chemosphere 71 1067-1078 Chen S-J, Hsieh L-T, Hwang P-S (1996) Concentration, phase distribution, and size distribution of atmospheric polychlorinated biphenyls measured in southern Taiwan. Environ Int 22 411-423 Chen L-G, Mai B-X, Bi X-H et al (2006) Concentration levels, compositional profiles, and gas-particle partitioning of polybrominated diphenyl ethers in the atmosphere of an urban city in South China Environ Sci Technol 40 1190-1196 Chuang JC, Mack GA, Kuhlman MR et al (1991) Polycyclic aromatic hydrocarbons and then-derivatives in indoor and outdoor air in an eight-home study. Atmos Environ B 25 369-380 Cotham WE, Bidleman TF (1995) Polycyclic aromatic hydrocarbons and polychlorinated biphenyls in air at an urban and a rural site near Lake Michigan. Environ Sci Technol 29 2782-2789... [Pg.357]

Decreasing the evaporation or transfer rate of the aroma components to the environment (modifying composition, profile, intensity) during all processing operations and storage, depending on temperature/heat water content (a, atmosphere), and duration... [Pg.836]

Fig. 39. Micro-EDX analysis of Ndl23 crystals grown by the modified TSSG method in low-Po, atmosphere from contamination-firee Nd Oj crucibles with different post-growth heat treatments. In all the cases final oxygenation at 340°C in oxygen was applied. The picture demonstrates (a) tweed structure formation and (b) nanoscale composition fluctuations in crystals with the anomalous peak effect on a magnetization curve. Note that the composition profile for heavy atoms (Ba/Nd ratio) is similar to wave-like fluctuations typical for demixing behavior or a spinodal homophase decomposition rather than for a heterophase decomposition with the formation of a boundary between the crystal matrix and the precipitated phase (M. Nakamura et al. 1996c). Fig. 39. Micro-EDX analysis of Ndl23 crystals grown by the modified TSSG method in low-Po, atmosphere from contamination-firee Nd Oj crucibles with different post-growth heat treatments. In all the cases final oxygenation at 340°C in oxygen was applied. The picture demonstrates (a) tweed structure formation and (b) nanoscale composition fluctuations in crystals with the anomalous peak effect on a magnetization curve. Note that the composition profile for heavy atoms (Ba/Nd ratio) is similar to wave-like fluctuations typical for demixing behavior or a spinodal homophase decomposition rather than for a heterophase decomposition with the formation of a boundary between the crystal matrix and the precipitated phase (M. Nakamura et al. 1996c).
Although the basic principles of the retrieval of vertical composition profiles from infrared measurements by inversion of the radiative transfer equation are the same as the retrieval of temperature profiles discussed in Section 8.2, the composition problem is usually more difficult to deal with in practice. The optical depth at a given level in the atmosphere is determined by an integration over the optically active gas profile from that level to the effective top of the atmosphere. Calculation of the radiance at the top of the atmosphere then requires an integration of the source function over all optical depths from the lower boundary to the top of the atmosphere. Thus the desired abundance profile is embedded within a double integration. [Pg.372]

Figure 6.30 shows the grand composite curve plotted from the problem table cascade in Fig. 6.186. The starting point for the flue gas is an actual temperature of 1800 C, which corresponds to a shifl ed temperature of (1800 — 25) = mS C on the grand composite curve. The flue gas profile is not restricted above the pinch and can be cooled to pinch temperature corresponding to a shifted temperature of 145 C before venting to the atmosphere. The actual stack temperature is thus 145 + 25= 170°C. This is just above the acid dew point of 160 C. Now calculate the fuel consumption ... Figure 6.30 shows the grand composite curve plotted from the problem table cascade in Fig. 6.186. The starting point for the flue gas is an actual temperature of 1800 C, which corresponds to a shifl ed temperature of (1800 — 25) = mS C on the grand composite curve. The flue gas profile is not restricted above the pinch and can be cooled to pinch temperature corresponding to a shifted temperature of 145 C before venting to the atmosphere. The actual stack temperature is thus 145 + 25= 170°C. This is just above the acid dew point of 160 C. Now calculate the fuel consumption ...
As with the steam turbine, if there was no stack loss to the atmosphere (i.e., if Qloss was zero), then W heat would he turned into W shaftwork. The stack losses in Fig. 6.34 reduce the efficiency of conversion of heat to work. The overall efficiency of conversion of heat to power depends on the turbine exhaust profile, the pinch temperature, and the shape of the process grand composite. [Pg.197]

The temperature profile of a planetary atmosphere depends both on the composition and some simple thermodynamics. The temperature decreases with altitude at a rate called the lapse rate. As a parcel of air rises, the pressure falls as we have seen, which means that the volume will increase as a result of an adiabatic expansion. The change in enthalpy H coupled with the definition of the specific heat capacity... [Pg.212]

With emission source chemical signatures and corresponding aerosol or rainwater sample measurements PLS can be used Co calculate a chemical element mass balance (CEB). Exact emission profiles for the copper smelter and for a power plant located further upwind were not available for calculation of source contributions to Western Washington rainwater composition. This type of calculation Is more difficult for rainwater Chan for aerosol samples due Co atmospheric gas to particle conversion of sulfur and nitrogen species and due Co variations In scavenging efficiencies among species. Gatz (14) has applied Che CEB to rainwater samples and discussed Che effect of variable solubility on the evaluation of Che soil or road dust factor. [Pg.47]

The boron isotope approach to pC02 estimation relies on the fact that a rise in the atmospheric CO2 concentration will increase pC02 of the surface ocean which in turn causes a reduction of its pH. By measuring the boron isotope composition of planktonic foraminifera Pahner et al. (1998) and Pearson and Palmer (2000) have reconstructed the pH-profile of Eocene sea water and estimated past atmospheric CO2 concentrations. However, Lemarchand et al. (2000) argued that 5 B records of planktonic foraminifera partly reflect changes in the marine boron isotope budget rather than changes in ocean pH. [Pg.172]

We emphasize the line shape problem perhaps a little more than usual in the spectroscopic literature. Collision-induced spectra have little structure. Yet, the diffuse line and band spectra extend over wide frequency bands and must often be subtracted, say from the complex spectra of planetary or stellar atmospheres, for a more detailed analysis of other, less well known components. The subtraction requires accurate knowledge of the profile and its variation with temperature, composition, etc., often over frequency bands of hundreds of cm-1. [Pg.19]

The flue gas at the NH3 injection location can be assumed to have the following composition (vol) NO = 200 ppm, CO = 100 ppm (peak 500 ppm), O2 = 3.0%, CO2 = 12.0%, H2O = 15.0%. The pressure is atmospheric. The residence time can be estimated from Fig. 16.12, assuming that there is about 0.5 s from the rebum fuel injector level to the rebum overfire air ports below the wing walls. An estimated temperature profile for the furnace indicates that the temperature can be assumed to be constant, around 950°C, from the upper OFA level until the flue gas reaches the wing wall. Mixing of NH3 with the flue gas is assumed to be instantaneous. [Pg.684]

Chemistry is a foundation for many other disciplines, (a) Biochemists analyzing DNA profiles, (b) Meteorologist releasing weather balloon to study the chemistry of the upper atmosphere, (c) Technicians conducting DNA research, (d) Paleontologists preparing fossilized dinosaur bones for transport to laboratory for chemical analysis, (e) Astronomer studying the composition of asteroids. [Pg.2]


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