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Temperature profile, calculation

Figure 2. Sorption of i-octane on 13X at U03 K temperature profiles calculated by the present model. Figure 2. Sorption of i-octane on 13X at U03 K temperature profiles calculated by the present model.
For a case that one stable steady state exists transient temperature profiles calculated agree satisfactorily with the measurements. For a case of three steady states the situation is quite complicated. The model used describes propagation of the fronts however, apparently cannot describe front multiplicity. A detailed calculation of the two-dimensional steady state equations including also the radial dispersion terms indicates that the onedimensional model is a very rough approximation for the diffusion" regime. We expect that dynamic calculations with the one-phase two-dimensional model could explain multiplicity of the fronts. [Pg.93]

Fig. 13 Optimal temperature profile calculated from a first-principle model for maximizing the mean crystal size for unseeded crystallization of paracetamol in water and the simulated change in mean crystal size during crystallization. Fig. 13 Optimal temperature profile calculated from a first-principle model for maximizing the mean crystal size for unseeded crystallization of paracetamol in water and the simulated change in mean crystal size during crystallization.
Tunnel pasteurisers are divided into zones where water is sprayed at different temperatures, with the total transit time and temperature profile calculated to provide the required degree of pasteurisation. It is common in practice to have a superheat zone before the holding zone to ensure the required tanperature has been reached. Heat recovery is important to ensure maximum energy efficiency and minimise costs. Each zone of the tunnel pasteuriser will contain a water tank, a pump and a water distribution system. Heat recovery is achieved by water being moved to different zones where its temperature is appropriate. [Pg.260]

Figure 4. Example of heat flux and temperature profiles calculated by model... Figure 4. Example of heat flux and temperature profiles calculated by model...
Nonisothermal Gas Absorption. The computation of nonisothermal gas absorption processes is difficult because of all the interactions involved as described for packed columns. A computer is normally required for the enormous number of plate calculations necessary to estabUsh the correct concentration and temperature profiles through the tower. Suitable algorithms have been developed (46,105) and nonisothermal gas absorption in plate columns has been studied experimentally and the measured profiles compared to the calculated results (47,106). Figure 27 shows a typical Hquid temperature profile observed in an adiabatic bubble plate absorber (107). The close agreement between the calculated and observed profiles was obtained without adjusting parameters. The plate efficiencies required for the calculations were measured independendy on a single exact copy of the bubble cap plates installed in the five-tray absorber. [Pg.42]

Why not put new lyrics to an old tune This is an excellent idea, and many have done this very thing. Rice" started w ith the Smith-Brinkley raethod" used to calculate distillation, absorption, extraction, etc., overhead and bottoms compositions, and developed distillation equations for determining the liquid composition on any tray. This together with bubble point calculations yield a column temperature profile useful for column analysis. [Pg.403]

A common process task involves heating a slurry by pumping it through a well-stirred tank. It is useful to know the temperature profile of the slurry in the agitated vessel. This information can be used to optimize the heat transfer process by performing simple sensitivity studies with the formulas presented below. Defining the inlet temperature of the slurry as T, and the temperature of the outer surface of the steam coil as U then by a macroscopic mass and energy balance for the system, a simplified calculation method is developed. [Pg.519]

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]

The exact procedure is to estimate a temperature profile from top to bottom of the column and then calculate a for each theoretical tray or stage by assuming a temperature increment from tray to tray. For many systems this, or some variation, is recommended to achieve good separation calculations. [Pg.25]

This approach was applied to data obtained by Hausberger, Atwood, and Knight (17). Figure 9 shows the basic temperature profile and feed gas data and the derived composition profiles. Application of the Hougen and Watson approach (16) and the method of least squares to the calculated profiles in Figure 9 gave the following methane rate equation ... [Pg.23]

No differences in operability and catalyst behavior (activity and deactivation) in the two plants were discernible. The expected catalyst lifetime in a commercial plant, calculated from the movement of the temperature profile down the catalyst bed with time, in both cases will be more than 16,000 hrs under the design conditions. [Pg.127]

Clearly, the temperature profile is linear. The activation parameters are the sums shown in general, a sum of entropies and enthalpies is the result when constants are multiplied. If values of AS% and Aare known independently, from the temperature dependence of Ka for example, one can then calculate AS and AH by difference. [Pg.162]

The heat transfer problem which must be solved in order to calculate the temperature profiles has been posed by Lee and Macosko(lO) as a coupled unsteady state heat conduction problem in the adjoining domains of the reaction mixture and of the nonadiabatic, nonisothermal mold wall. Figure 5 shows the geometry of interest. The following assumptions were made 1) no flow in the reaction mixture (typical molds fill in <2 sec.) ... [Pg.152]

Fig. 2 Time-series of annual mean water temperature in the San Reservoir (Spain) and air temperature in the Ter River watershed. The series start in 1964, after the first filling of the reservoir. Annual means are based on monthly measures of the volume weighted mean temperature. Only years with at least 10 temperature profiles were included in the figure. The air temperatures are annual means for the whole Ter River watershed, calculated from data collected in several meteorological stations in the basin, and weighted according to their area of influence... Fig. 2 Time-series of annual mean water temperature in the San Reservoir (Spain) and air temperature in the Ter River watershed. The series start in 1964, after the first filling of the reservoir. Annual means are based on monthly measures of the volume weighted mean temperature. Only years with at least 10 temperature profiles were included in the figure. The air temperatures are annual means for the whole Ter River watershed, calculated from data collected in several meteorological stations in the basin, and weighted according to their area of influence...

See other pages where Temperature profile, calculation is mentioned: [Pg.316]    [Pg.688]    [Pg.109]    [Pg.866]    [Pg.869]    [Pg.323]    [Pg.159]    [Pg.746]    [Pg.315]    [Pg.72]    [Pg.389]    [Pg.781]    [Pg.305]    [Pg.316]    [Pg.688]    [Pg.109]    [Pg.866]    [Pg.869]    [Pg.323]    [Pg.159]    [Pg.746]    [Pg.315]    [Pg.72]    [Pg.389]    [Pg.781]    [Pg.305]    [Pg.29]    [Pg.29]    [Pg.31]    [Pg.147]    [Pg.1296]    [Pg.216]    [Pg.424]    [Pg.158]    [Pg.56]    [Pg.158]    [Pg.89]    [Pg.108]    [Pg.113]    [Pg.98]    [Pg.199]    [Pg.201]    [Pg.324]    [Pg.700]   
See also in sourсe #XX -- [ Pg.121 ]




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