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Flow rates initial guess

Table I lists the values of the rate coefficients used to simulate the transient response experiments shown in Figs. 3 through 8. These values were obtained in the following manner (29). Starting from a set of initial guesses, the values of k were varied systematically to obtain a fit between the predicted product responses and those obtained from experiments in which H2 was added suddenly to a flow of NO. These experiments while not described here were identical to that presented in Fig. 9, with the exception that only l NO was used. Because of the large number of parameters in the model, only a rough agreement could be achieved between experiment and theory even after 500 iterations of the optimization routine (30). The parameter values obtained at this point were now used to calculate the responses expected during the reduction of adsorbed NO. These computations produced responses similar to those observed experimentally (i.e., Fig. 3) but the appearance of the product peaks in time did not coincide with those observed. To correct for this, the values of kg, ky, and kg were adjusted in an empirical manner. Table I lists the values of the rate coefficients used to simulate the transient response experiments shown in Figs. 3 through 8. These values were obtained in the following manner (29). Starting from a set of initial guesses, the values of k were varied systematically to obtain a fit between the predicted product responses and those obtained from experiments in which H2 was added suddenly to a flow of NO. These experiments while not described here were identical to that presented in Fig. 9, with the exception that only l NO was used. Because of the large number of parameters in the model, only a rough agreement could be achieved between experiment and theory even after 500 iterations of the optimization routine (30). The parameter values obtained at this point were now used to calculate the responses expected during the reduction of adsorbed NO. These computations produced responses similar to those observed experimentally (i.e., Fig. 3) but the appearance of the product peaks in time did not coincide with those observed. To correct for this, the values of kg, ky, and kg were adjusted in an empirical manner.
Input data on the column size, components, physical properties, feeds, and initial conditions (liquid compositions, liquid flow rates, and initial guesses of temperatures on all trays). [Pg.140]

The model equations can be solved by a shooting technique start with an initial guess X for the conversion x(l), calculate the recycle flow rate/j from Eq. (4.37) and reactor-inlet concentration from Eq. (4.38), integrate the PFR Eqs. (4.34) and (4.35), check and update the guess X. This implies that it is theoretically possible to reduce the model to one equation with one variable ... [Pg.120]

Procedure. The apparatus and general procedures of the capillary IGC experiment are described elsewhere (1.2.36-). Each measurement was conducted at three different earner gas flow rates (between 2 to 20 cm/s). For each experiment, an estimate of a and B was obtained using moment analysis and used as an initial guess for the Fourier domain fitting. The values of B2 at the three different earner gas flow rates were plotted versus 1/tc. Using equation (31), x2/D was estimated from the slope of B2 versus 1/tc, using a linear least-squares. [Pg.97]

Multiobjective optimization of the SMB and Varicol processes by a non-dominated sorting genetic algorithm (NSGA) which does not require any initial guess of the optimum solution was carried out by Zhang et al. [80] who used in that process an objective function that maximizes the feed flow rate (maximum throughput). [Pg.925]

An initial guess for K,V/L is based on the temperatures and flow rates of the feed streams ... [Pg.409]

Finally, a second column C2 is added in the normal way. A 22-stage column is specified with feed on Stage 11 and operating at 1 atm. The final flowsheet with all the pumps and valves installed is shown in Figure 5.22. Note that neither of the recycles streams is connected. The two streams that we have made some initial guesses of flow rates and compositions are REFLUX and RECYCLE. The two streams that have been calculated and should be approximately the same as these two are ORGREF and D2CALC. ... [Pg.112]

The initial guessed value of the reflux ratio in the second column was 2. The bottoms purity was very high. The reflux ratio was reduced to about RR = 0.2 without affecting the bottoms purity significantly. A second Design Spec/Vary is set to maintain the ethanol composition of the bottoms of the second column at 0.1 mol% by varying the bottoms flow rate B2. [Pg.114]

In theory, the next and final step is to close the organic reflux loop. The stream labeled ORGREF is deleted, the stream REFLUX connected to the summer Ml and REFLUX is defined as a TEAR stream. Unfortunately, this loop does not converge even though the initial values of the guessed and calculated values are very close in both composition and flow rate. An alternative way to converge this system using dynamic simulation will be discussed in Chapter 8 after we have discussed the details of dynamic simulation. [Pg.114]

Initial guesses were made of the flow rates of the distillate, stripper bottoms and sidestream, and the RR of the main column. [Pg.287]

The final job in the steady-state design is to achieve the desired specification of an ASTM 95% point of 375 °F (ASTM D-86). An initial guess of 20,000 B/D for the liquid distillate flow rate gives an ASTM 95% point of 353 °F. This is lower than the specification, which indicates that more material can be taken overhead. Increasing the flow rate carries more higher-boiling material into the naphtha product. To display the TBP and ASTM boiling point values for the process streams, go to Setup, Report Options, Stream, Property Sets and select Petro. [Pg.325]

Unfortunately, when one first starts the calculation with the initial guesses for all tenperatures, vapor, and liquid flow rates, the energy balance, component mass balance, and equilibrium functions will not equal zero. The Newtonian method is used to develop new values for the variables to calculate enthalpies and K values. To use the Newtonian method, Naphtali and Sandholm developed derivatives for the changes in all variables. Note that the energy balance (and component mass balances and equilibrium relationships) on plate j depend only on the variables on plates j-1, j and j+1. For the energy balance (EB) function on... [Pg.259]


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See also in sourсe #XX -- [ Pg.220 ]




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