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How closely does the output of an LFSR whose characteristic polynomial is p(z) cN cN21z c1z N21 c0z N with initial state s(0) = (0)N resemble a random sequence A run of 0 s (resp. of l s) of length k occurs in the LFSR output sequence s0(0), s0(1), s0(2), . . . starting at time t if (s0 (t 1), s0 (t), s0 (t 1), . . . , s0 (t k 1)), | {z }

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vector<Cost<SpecAbsoluteCost> > c(p.size(), transactionCost); unsigned int nContracts = 1; Strategy Strategy cout << << << << << for(size_t cout ru(potential_profit_ralg(p, c, nContracts)); lu(potential_profit_lalg(p, c, nContracts)); setw(8) << "Price" << " " setw(8) << "Cost" << " " setw(3) << "R" << " " setw(3) << "L" << " " endl; i = 0; i < p.size(); i++) { << setw(8) << p[i] << " " << setw(8) << c[i].cost() << " " << setw(3) << ru[i] << " " << setw(3) << lu[i] << " " << endl;

which can be considered as a drop size. One would expect this to depend only on the ow regime (elongational or shearing) and the viscosity ratio. Grace (1982) showed that such a relationship exists for drops broken up in laminar ow in a four-roll mill. Mutsakis et al. (1986) showed that a similar relation could be obtained for a motionless mixer. This relation and work are shown in Figure 7-27. Note that the breakup of drops only seems to occur at dispersed/continuous viscosity ratios of less than about 4. At this and higher ratios the droplets do not seem to break in shear ow. At low viscosity ratios the exponent on the viscosity ratio is between 0.33 and 0.5. Some authors give a theoretically derived viscosity ratio effect, q + 16 (7-37) q + 19 where q is the viscosity ratio, dispersed to continuous. For a range of q from 1 to 0.0, this value varies from 16/19 to 17/20. This is a very minor effect and does not accurately predict the effects measured. From the above the maximum stable drop size can be estimated. There will be smaller drops, but in theory no drops larger than this. No data on distribution as yet exist for laminar breakup. Figure 7-28 compares drop size by laminar mechanisms with those calculated for turbulent ow. Smaller droplets are expected for laminar versus turbulent ow at the same energy dissipation rate.

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Google SketchUp s website offers free and very useful component bonus packs (Fig. 3-21). To effectively use this book, download and install the bonus components for SketchUp 7.

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