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Atmosphere temperature profile

The combinations of failures and non-failed conditions define the state of the pJani at the right branches. The damage associated with these plant damage states are calculated using thermal-hydraulic analyses to determine temperature profiles that are related to critical chemical reactions, explosions and high pressure. These end-states serve as initiators fot breaking confinement that leads to release in the plant and aquatic and atmospheric release outside ol the plant,... [Pg.113]

Here a steady-state formulation of heat transfer is considered (Pollard, 1978). A hot fluid flows with linear velocity v, through a tube of length L, and diameter D, such that heat is lost via the tube wall to the surrounding atmosphere. It is required to find the steady-state temperature profile along the tube length. [Pg.261]

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]

Figure 7.11 Temperature profile of the Earth s atmosphere. (Reproduced by permission of Oklahoma Geological Society)... Figure 7.11 Temperature profile of the Earth s atmosphere. (Reproduced by permission of Oklahoma Geological Society)...
The dispersion coefficients are a function of atmospheric conditions and the distance downwind from the release. The atmospheric conditions are classified according to six different stability classes, shown in Table 5-1. The stability classes depend on wind speed and quantity of sunlight. During the day, increased wind speed results in greater atmospheric stability, whereas at night the reverse is true. This is due to a change in vertical temperature profiles from day to night. [Pg.186]

Atmospheric dispersion—The low momentum mixing of a gas or vapor with air. The mixing is the result of turbulent energy exchange, which is a function of wind and atmospheric temperature profile. [Pg.439]

Supermolecular absorption determines significant features of the atmospheres of the planets and their large moons, such as the vertical temperature profile and the high-altitude haze distribution, and offers opportunities for the determination of abundance ratios of helium and hydrogen, ortho- and para-H2, etc. [390, 396]. In certain spectral bands the spectra may sometimes be obtained by Earth-based observations. More commonly, the spectra will be obtained in space missions, such as IRIS of Voyager I and II future missions (Infrared Space Observatory) will doubtlessly enhance the available information significantly. [Pg.373]

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]

Mars is almost free of clouds and the surface can be seen from the earth through a telescope. The results of the recent space probes (1073a) reveal that the surface temperature ranges from 188 to 243 K and the Martian poles are composed of substantial amounts of water ice, seasonally covered by C02 frost. The rusty-red color of the surface is caused by the presence of substantial amounts of iron oxides. The mean surface atmospheric pressure is 7.65 0.1 mbar. The temperature profile of the Mars atmosphere is given in Fig. VIII— 12. [Pg.115]

The temperature profile of the Venus atmosphere is shown in Fig. V111— 13. The surface temperature and pressure have recently been determined by space probes to be 747 + 20°K and 88 15 bars, respectively. [Pg.117]

Fig. VIII—13. Temperature profile of the atmosphere of Venus. The surface corresponds to 6055 km from the center of Venus. (M) is the number of molecules per cm3. The surface pressure is 88 bars and the temperature is 750°K. Venus is covered with dense clouds (probably sulfuric acid droplets). After McEwan and Phillips (20), reprinted by permission of Edward Arnold Ltd. Fig. VIII—13. Temperature profile of the atmosphere of Venus. The surface corresponds to 6055 km from the center of Venus. (M) is the number of molecules per cm3. The surface pressure is 88 bars and the temperature is 750°K. Venus is covered with dense clouds (probably sulfuric acid droplets). After McEwan and Phillips (20), reprinted by permission of Edward Arnold Ltd.
Fig. VIII—1-4. Proposed temperature profile of Jupiter s Atmosphere. The tropo-pause is chosen as height reference since there is no evidence of a solid surface. The temperature at the tropopause is 9S.5°K and the number density is 2 x I01 cm 3. Contrary to the case of the upper atmosphere of earth, there appears to be no boundary between stratosphere and mesosphere. The observed cloud deck is believed to be solid ammonia. (M) signifies the number of molecules per cm3. From Hunten (490b), reprinted by permission of the American Meteorological Society. [Pg.118]

Figure 1. Temperature profile of a lean propane-air flame at atmospheric pressure (24)... Figure 1. Temperature profile of a lean propane-air flame at atmospheric pressure (24)...
Figure 2. Schematic vertical profiles (a) h (dashed) and h (solid) and (b) q (dashed) and q (solid), (c) The temperature profile, corresponding to cpT = h — gZ — Lyq, illustrates die constant lapse rate within the boundary layer and the reduced lapse rate above the boundary layer. The boundary level (1 km) is indicated by die horizontal dashed line in each panel. These profiles illustrate typical climatic values that are determined by moist convective adjustment in the free atmosphere and dry adiabatic convection in the boundary layer. [Used by permission of Geological Society of America, from Forest et al. (1999), Geol. Soc. Am. Bull., Vol. Ill, Fig. 2, p. 500.]... Figure 2. Schematic vertical profiles (a) h (dashed) and h (solid) and (b) q (dashed) and q (solid), (c) The temperature profile, corresponding to cpT = h — gZ — Lyq, illustrates die constant lapse rate within the boundary layer and the reduced lapse rate above the boundary layer. The boundary level (1 km) is indicated by die horizontal dashed line in each panel. These profiles illustrate typical climatic values that are determined by moist convective adjustment in the free atmosphere and dry adiabatic convection in the boundary layer. [Used by permission of Geological Society of America, from Forest et al. (1999), Geol. Soc. Am. Bull., Vol. Ill, Fig. 2, p. 500.]...
The vertical temperature profile of the earth s atmosphere conveniently allows it to be described as comprised of a number of vertical layers. From the earth s surface upward, these are the troposphere, stratosphere, mesosphere, and thermosphere (Mcllveen, 1992). Because 85% of the mass of the atmosphere resides in the troposphere, and most... [Pg.358]

As mentioned above, recent attempts to identify the level of atmospheric climate change have been confined to analyses of comparatively long data series on SAT, though smaller volumes of data on changes in sea ice cover extent, vertical temperature profile (radiosonde data), and results of satellite microwave sensing have also been considered (Christy et ai, 1998). However, numerical modeling results show... [Pg.439]

I ig. VIII—12. Temperature profile of the Mars atmosphere. The surface temperature oinges from 170 to 243°K and the mean atmospheric pressure is 7.65 mbar at the surface (1073a) (M) is the number of molecules per cm3. From McElroy (674c), reprinted by IK-rmission. Copyright by the American Geophysical Union. [Pg.116]


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See also in sourсe #XX -- [ Pg.214 , Pg.217 ]




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