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Initial temperature

The analysis of the heat exchanger network first identifies sources of heat (termed hot streams) and sinks (termed cold streams) from the material and energy balance. Consider first a very simple problem with just one hot stream (heat source) and one cold stream (heat sink). The initial temperature (termed supply temperature), final temperature (termed target temperature), and enthalpy change of both streams are given in Table 6.1. [Pg.160]

Finally, sulfur has a negative effect on the performance of the catalyst itself. One sees for example in Figure 5.23 that the initiation temperature increases with the sulfur level in the diesel fuel, even between 0.01% and 0.05%. Yet, in the diesel engine, characterized by relatively low exhaust temperatures, the operation of the catalyst is a determining factor. One can thus predict an ultimate diesel fuel desulfurization to levels lower than 0.05%. [Pg.255]

The initial condition for the dry gas is outside the two-phase envelope, and is to the right of the critical point, confirming that the fluid initially exists as a single phase gas. As the reservoir is produced, the pressure drops under isothermal conditions, as indicated by the vertical line. Since the initial temperature is higher than the maximum temperature of the two-phase envelope (the cricondotherm - typically less than 0°C for a dry gas) the reservoir conditions of temperature and pressure never fall inside the two phase region, indicating that the composition and phase of the fluid in the reservoir remains constant. [Pg.102]

The initial temperature of a gas condensate lies between the critical temperature and the cricondotherm. The fluid therefore exists at initial conditions in the reservoir as a gas, but on pressure depletion the dew point line is reached, at which point liquids condense in the reservoir. As can be seen from Figure 5.22, the volume percentage of liquids is low, typically insufficient for the saturation of the liquid in the pore space to reach the critical saturation beyond which the liquid phase becomes mobile. These... [Pg.102]

Equation (A3.3.57) must be supplied with appropriate initial conditions describing the system prior to the onset of phase separation. The initial post-quench state is characterized by the order parameter fluctuations characteristic of the pre-quench initial temperature T.. The role of these fluctuations has been described in detail m [23]. Flowever, again using the renomialization group arguments, any initial short-range correlations should be irrelevant, and one can take the initial conditions to represent a completely disordered state at J = xj. For example, one can choose the white noise fomi (i /(,t,0)v (,t, 0)) = q8(.t -. ), where ( ) represents an... [Pg.739]

C - INITIALIZE TEMPERATURE SECOND IWARIANT OF RATE OF DEFORMATION TENSOR... [Pg.224]

In the heating phase (assuming t is non-zero), the velocities are periodically rescaled to change the system temperature from the initial temperature Tj to the simulation temperature T2 in increments of the temperature step AT. The heating period for rescaling the velocities, P, is defined by ... [Pg.314]

Berendsen et al. [H. I. C. Berendsen, I. P. M. Postma, W. F. van Gun-steren, A. di Nola, and I. R. Haak, J. Chem. Phys. 81, 3684 (1984)] have described a simple scheme for constant temperature simulations that is implemented in HyperChem. You can use this constant temperature scheme by checking the constant temperature check box and specifying a bath relaxation constant t. This relaxation constant must be equal to or bigger than the dynamics step size D/. If it is equal to the step size, the temperature will be kept as close to constant as possible. This occurs, essentially, by rescaling the velocities used to update positions to correspond exactly to the specified initial temperature. For larger values of the relaxation constant, the temperature is kept approximately constant by superimposing a first-order relaxation process on the simulation. That is ... [Pg.317]

A constant force is applied to an ideal elastomer, assumed to be a perfect network. At an initial temperature Tj the length of the sample is Ij. The temperature is raised to Tf and the final length is If. Which is larger Ij or If (remember F is a constant and Tf > Tj) Suppose a wheel were constructed with spokes of this same elastomer. From the viewpoint of an observer, the spokes are heated near the 3 o clock position-say, by exposure to sunlight-while other spokes are shaded. Assuming the torque produced can overcome any friction at the axle, would the observer see the wheel turn clockwise or counterclockwise How would this experiment contrast, in magnitude and direction, with an experiment using metal spokes ... [Pg.193]

For simplicity, we further assume h = 1. Let some initial temperature distribution be given ... [Pg.200]

R. C. Strittmater, E. M. Wineholt, and M. E. Holmes, The Sensitivity of Double Base Propellant Burning Rate to Initial Temperature, MR-2593, BRL, Aberdeen, Md., 1976. [Pg.54]

Linear Low Density Polyethylene. Films from linear low density polyethylene (LLDPE) resias have 75% higher tensile strength, 50% higher elongation-to-break strength, and a slightly higher but broader heat-seal initiation temperature than do films from LDPE. Impact and puncture resistance are also improved over LDPE. Water-vapor and gas-permeation properties are similar to those of LDPE films. [Pg.452]

Fig. 6. Phase diagram showing the composition pathway traveled by the casting solution during precipitation by cooling. Point A represents the initial temperature and composition of the casting solution. The cloud point is the point of fast precipitation. In the two-phase region tie lines linking the... Fig. 6. Phase diagram showing the composition pathway traveled by the casting solution during precipitation by cooling. Point A represents the initial temperature and composition of the casting solution. The cloud point is the point of fast precipitation. In the two-phase region tie lines linking the...
Volumetric heat generation increases with temperature as a single or multiple S-shaped curves, whereas surface heat removal increases linearly. The shapes of these heat-generation curves and the slopes of the heat-removal lines depend on reaction kinetics, activation energies, reactant concentrations, flow rates, and the initial temperatures of reactants and coolants (70). The intersections of the heat-generation curves and heat-removal lines represent possible steady-state operations called stationary states (Fig. 15). Multiple stationary states are possible. Control is introduced to estabHsh the desired steady-state operation, produce products at targeted rates, and provide safe start-up and shutdown. Control methods can affect overall performance by their way of adjusting temperature and concentration variations and upsets, and by the closeness to which critical variables are operated near their limits. [Pg.519]

Table 17. Approximate Initial Temperature, °C, at which Refractories React ... Table 17. Approximate Initial Temperature, °C, at which Refractories React ...
Amines and other bases cataly2e the exothermic decomposition of molten maleic anhydride [108-31-6] at temperatures above 150°C, accompanied by the rapid evolution of gaseous products (44,45). The rate of reaction reportedly increases with the basicity of the amine and higher initial temperatures. The reaction mixture can become explosive. [Pg.43]

Operating Temperature. The operating temperature needed to achieve a particular VOC destmction efficiency depends primarily on the species of pollutants contained in the waste stream, the concentration of the pollutants, and the catalyst type (14). One of the most important factors is the hydrocarbon species. Each has a catalytic initiation temperature which is also dependent on the type of catalyst used (14). [Pg.506]

Various numerical and graphical methods are used for unsteady-state conduction problems, in particular the Schmidt graphical method (Foppls Festschrift, Springer-Verlag, Berhn, 1924). These methods are very useful because any form of initial temperature distribution may be used. [Pg.557]

Heating with Internal Coil from Initial Temperature for Specified Time... [Pg.1050]

Heating with External Coil from Initial Temperature for Specified Time The temperature of the dead-air space is obtained from... [Pg.1050]

Values of enthalpy constants for approximate equations are not tabulated here but are also computed for each stage based on the initial temperature distribution. [Pg.1289]

The use of the internal baffle permits operation of the ciystaUizer at a slurry consistency other than that naturally obtained by the cooling of the feed from the initial temperature to the final mother-liquor temperature. The baffle also permits fines removal and destruction. [Pg.1665]

Tr = temperature of reactants at relief set pressure To = aUowable temperature following complete quench To = initial temperature of the quen fluid = specific heat of the quench fluid Cr = specific heat of the reac tants (consistent Enghsh or SI units)... [Pg.2299]

The problem of flame arrestment, either of deflagrations or detonations, depends on the properties of the gas mixture involved plus the initial temperature and pressure. Gas mixture combustion properties cannot be quantified for direc t use in flame arrester selection and only general charac teristics can be assigned. For this reason, flame arrester performance must be demonstrated by realistic testing. Such... [Pg.2301]

Various types of rapid, adiabatic compressions have caused explosions. With propane at an initial temperature of 25°C, To = 432°K (I59°C) for compression and specific heat ratios of 25 and I.I3, respectively. Assume that now air enters a compressor to bring propane into the flammable range at 5 percent by volume. The mixture then will be mostly air with k = 1.47. The same compression ratio of 25 will elevate the final temperature T2 to 834°K (56I°C), i.e., above the published autoignition temperature of 450°C for propane and perhaps high enough to cause an explosion. [Pg.2317]

FIG. 27-13 Available heats for some typical fuels. The fuels are identified by their gross (or higher) heating values. All available heat figures are based upon complete combustion and fuel and air initial temperature of 288 K (60 F). To convert from MJ/Nm to Btii/ft, multiply by 26.84. To convert from MJ/dm to Btii/gal, multiply by. 1588. [Pg.2380]

Control temperature of heating media below expected initiation temperature... [Pg.71]

Q = initial temperature rise of the machine above the ambient in °C... [Pg.58]


See other pages where Initial temperature is mentioned: [Pg.2355]    [Pg.317]    [Pg.317]    [Pg.317]    [Pg.558]    [Pg.569]    [Pg.203]    [Pg.180]    [Pg.65]    [Pg.49]    [Pg.511]    [Pg.265]    [Pg.291]    [Pg.209]    [Pg.392]    [Pg.215]    [Pg.109]    [Pg.517]    [Pg.517]    [Pg.518]    [Pg.443]    [Pg.1137]    [Pg.2293]   
See also in sourсe #XX -- [ Pg.10 ]




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Doses and Temperatures to Initiate Explosives by Pulsed High-Energy Electrons

Effect of Initial Temperature

Effect of Temperature and Concentration Non-uniformity on Shock-Free Detonation Initiation

Effects of Initial Temperature and Non-combustible Gases on Detonation Parameters

Initial Bed Temperature

Initial and final temperatures

Initial decomposition temperature

Initial deformation temperature

Initial exotherm temperature

Initial methanation temperature

Initial oxidation temperature

Initial softening temperature

Initial stage temperature

Initiation by high temperatures

Initiation temperature

Initiation temperature

Initiator half-life temperature

Initiators high temperature

Initiators low temperature

Process parameters initial temperature

Self-propagating high-temperature synthesis initiation

Temperature control radical initiators

Temperature of initiation—

Thermally Initiated cationic temperatures

Using Initiator Combinations with Designed Temperature Profile

Velocity — Temperature (Initial) of Charge Relationship

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