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Isothermal regimes

The majority of polymer flow processes involve significant heat dissipation and should be regarded as nou-isothermal regimes. Therefore in the finite element modelling of polymeric flow, in conjunction with the equations of continuity... [Pg.128]

It was found that the initial reaction rate was equal to YoAo, where Yo and Ao are the initial concentrations of epoxy groups and m-phenyl diamine. Formation of hydroxyl groups during the reaction leads to self-acceleration. This prediction was confirmed by measurements carried out in an isothermal regime, because adiabatic conditions for a reaction lead to self-acceleration due to an increase in temperature (see above). Thus, the initial reaction rate vo can be expressed as... [Pg.42]

The parameters in Eq. (2.59) are usually determined from the condition that some function mean-square deviations between the experimental and calculated curves (the error function). The search for the minimum of the function Nelder-Mead algorithm.103 As an example, Table 2.2 contains results of the calculation of the constants in a self-accelerating kinetic equation used to describe experimental data from anionic-activated e-caprolactam polymerization for different catalyst concentrations. There is good correlation between the results obtained by different methods,as can be seen from Table 2.2. In order to increase the value of the experimental results, measurements have been made at different non-isothermal regimes, in which both the initial temperature and the temperature changes with time were varied. [Pg.65]

Although there is significant local recycling near the limiter blade, it is still too weak to cause substantial poloidal variations in the plasma density and temperature profiles. The plasma flow is in a simple isothermal regime, with weak influence of atomic processes, and with the power flow to the limiter being determined by the electrostatic sheath in front of the limiter [1] (and not by atomic and molecular processes). [Pg.52]

Figures 1 and 2 show an increase in during cure brings about a decrease in 0 = T — in the isothermal regime. Assuming the Arrhenius dependence of the rate constants on T, one can get a good superposition of the kinetic cilrves in the region well above and a considerable retardation of the reaction gt reaction temperatures near or below (Fig. 2). Figures 1 and 2 show an increase in during cure brings about a decrease in 0 = T — in the isothermal regime. Assuming the Arrhenius dependence of the rate constants on T, one can get a good superposition of the kinetic cilrves in the region well above and a considerable retardation of the reaction gt reaction temperatures near or below (Fig. 2).
Fig. 3. Pressure profile inside the flat slit channel in PS Keroplast melt flow (contains 0.3 (vol.) shares of a filler). Volume consumption is 1.3 mm per s. Filler-Kerogene 90 (o), shale ash ( ). light marks-isothermic regime (T = 453 K), dark-non-isothermic (reservoir temperature 453 K) [10]... Fig. 3. Pressure profile inside the flat slit channel in PS Keroplast melt flow (contains 0.3 (vol.) shares of a filler). Volume consumption is 1.3 mm per s. Filler-Kerogene 90 (o), shale ash ( ). light marks-isothermic regime (T = 453 K), dark-non-isothermic (reservoir temperature 453 K) [10]...
The values of A and AU are the physical characteristics of the material and can be easily computed from two viscosimetric experiments in the isothermal regime under different temperatures T according to the expression ... [Pg.56]

The sign in the right hand part of this expression should be chosen so that Svp (T) > at r < Ti (adiabatic regime) and the opposite inequality should take place at r > Ti (isothermal regime for the Jahn-Teller system s contribution to the elastic modulus). [Pg.761]

The reaction equipment is operated by means of a data acquisition and control program. The reactor is of stainless steel 316, with 9 mm internal diameter. It is provided with a fixed bed of catalyst diluted with alumina as inert and operates in isothermal regime. The reaction products are analysed by gas chromatography (Hewlett Packard 6890) by means of detectors based on thermal conductivity (TCD) and flame ionization (FID). The separation of products is carried out by means of a system made up of three eolumns 1) HP-1 semicapillary column for splitting the sample into two fi actions a) volatile hydrocarbon components (C4.) and polar components (ethanol, water and diethyl ether) b) remaining products (C5+). 2) SUPEL-Q Plot semicapillary column for individually separating out both volatile components and polar components, which will be subsequently analysed by TCD and FID. 3) PONA capillary column for separation of Cs+ hydrocarbons, which will be analysed by FID. [Pg.456]

Thermolysis of metal acrylates (MAcr ) was carried out in an isothermal regime in a nonisothermal reactor (at the experimental temperature Te p) the heated volume of the compound amounted to 0.03 V (where V is the reaction vessel volume the basic part of the vessel was at room temperature (T,). MAcr was studied at 350-390 °C (CoAcrj), 300-360 °C (NiAcrj), 200-370 °C... [Pg.356]

There is graduation of temperature maximums in reaction zone at rising of V and consequently Dt in spite of total polymer yield increase. Temperature dithering (quasi-isothermal regime) leads to the increasing of medium MM and narrowing of MMD of resulting product [1,58, 59]. [Pg.14]

It was revealed that the fact that liquid flows densities and viscosities change doesn t influence on reaction torch front formation is also very important (Fig. 4.2,4.3). The rise of density of flows at the expense of reduction of low bound of ratios Vi / V2 required for the formation of plan front and constancy of ratios Vi / V2 required for formation of low bound of torch front leads to the narrowing of ineffective torch regime region formation. The last fact widens possibilities of tubular turbulent apparatus exploitation in optimal quasi-plug-flow regime (quasi-isothermal regime) (Fig. 4.4). [Pg.93]

The obtained results unambiguously testify that under realization of fast exothermal processes (k > 10 1/mole Sec) in tubular turbulent apparatus of jet type in all cases removal of heat is practically possible only after processes are over (from reaction product) but not directly in reaction zone. It is very important because to reach isothermal regime directly in reaction zone when Lc = Lcooi is practically impossible even at significant decrease of Tc (Fig. 4.9). [Pg.99]

The values (Equation (38)) clearly demonstrate that crystallites grown under isothermal conditions exhibit higher interfacial energy towards surrounding amorphous phase as crystallites developed in non-isothermal regime. [Pg.114]

Studies on the thermal degradation of PE samples with different molecular masses in the isothermal regime at different temperatures have shown that the kinetic curves have linear plots up to 70% weight loss (Figure 1.2), which point to a zero-order reaction. The activation energy of thermal degradation increases with the molecular mass of the polymer from 192.3 kj/mol (molecular mass 11,000) up to 276.3 kj/mol (molecular mass 23,000) [2]. [Pg.6]

We have measured the catalytic activity of four samples of catalysts prqxued according to the above-presented procedure PA-100, PA-105, PA-110, and PA-125, calcined at temperatures 1000, 1050,1100, and 1250, respectively (Table 2). The measuremoits woe carried out in a quartz reactor of diameter 17 mm, with fluidized bed of the catalyst acting in the isothermal regime. The temperature range (720-8(X)°C) was chosen optimal for this catalyst. The air-ammonia mixture (10 % vol. NHj) was introduced into the reactor with the space velocity of 3(KXX) h . [Pg.686]

The results demonstrate that using linear heating rates, which are often employed to study calcination, and under typical catalyst preparation conditions, i.e. isothermal regimes, the reaction rate varies considerably. This is reflected in the properties (e.g. surface area and pore size) of the solid products which we have shown are highly dependent on the preparative conditions. Our results confirm Stacey s observation that the advantages of CR conditions apply equally at atmospheric pressure as well as low pressure. However, we have extended the work using smaller samples and relatively faster reaction rates over a wide range of partial pressures. [Pg.867]

The temperature stability of natural phillipsite was studied in the temperature range of 20. . . 1000 °C in a dynamic regime in air and in an isothermal regime in vacuo [91R4], The scheme of the decorr sition of... [Pg.343]

Due to the fact that the macromolecules are quite inhomogeneous with respect to their size and structure, and crystallization strongly depends on its conditions (particularly in non-isothermal regime), the final crystals exhibit different perfections. This causes that melting, which occurs in a relatively wide interval, as mentioned above. Recall that this is one of the major requirements which enables the preparation of SPCs. [Pg.680]

Isothermal regime carriers, phonons, and excitons in thermal equilibrium at lattice temperature, timescale >100 ps. [Pg.544]

Chemistry of Superheavy Elements ). The application of Monte-Carlo simulation methods in gas-phase adsorption chromatography is based on ideas given in [17]. All models use a microscopic description of the chromatographic adsorption-desorption process on the atomic scale. Hence, they are kinetic models of gas-adsorption chromatography. They can be applied to thermochromatography as well as to chromatography in the isothermal regime. To determine of the... [Pg.383]

Fig. 2.50 Isothermal regime of electrolyte flow in the porous carbon cathode blocks 1—flow in permeable pores, with dimension below critical radius (25 pm) 2— flow in permeable pores with dimensions above critical diameter of pores... Fig. 2.50 Isothermal regime of electrolyte flow in the porous carbon cathode blocks 1—flow in permeable pores, with dimension below critical radius (25 pm) 2— flow in permeable pores with dimensions above critical diameter of pores...
J. Sestak, key lecture Integration of nucleation-growth equation when considering non-isothermal regime and shared phase separation at the. 2" ESTAC (Europ. Symp. on Thermal Analysis) in Proc. Thermal Analysis (D. Dolimore, ed) Heyden. London 1981, p. 115... [Pg.433]


See other pages where Isothermal regimes is mentioned: [Pg.75]    [Pg.262]    [Pg.106]    [Pg.27]    [Pg.223]    [Pg.4]    [Pg.27]    [Pg.201]    [Pg.324]    [Pg.6]    [Pg.8]    [Pg.8]    [Pg.11]    [Pg.13]    [Pg.13]    [Pg.23]    [Pg.157]    [Pg.159]    [Pg.162]    [Pg.344]    [Pg.113]    [Pg.339]    [Pg.254]    [Pg.1305]    [Pg.259]    [Pg.152]    [Pg.375]    [Pg.356]   
See also in sourсe #XX -- [ Pg.43 , Pg.65 ]




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