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Pattern generators

Fig. 11. Computer-simulated recirculating patterns in a mixing tank with full baffles (a) elevation view shows circulation patterns generated by turbine blades (b) plane view shows the effect of the baffle on the radial velocity vectors above the turbine blades. Fig. 11. Computer-simulated recirculating patterns in a mixing tank with full baffles (a) elevation view shows circulation patterns generated by turbine blades (b) plane view shows the effect of the baffle on the radial velocity vectors above the turbine blades.
Figure 7. Tangential flow pattern generated by a paddle mixer. Figure 7. Tangential flow pattern generated by a paddle mixer.
This chapter reviews the various types of impellers, die flow patterns generated by diese agitators, correlation of die dimensionless parameters (i.e., Reynolds number, Froude number, and Power number), scale-up of mixers, heat transfer coefficients of jacketed agitated vessels, and die time required for heating or cooling diese vessels. [Pg.553]

Figure 1.3 shows a few examples of the kinds of space-time patterns generated by binary (k 2) nearest-neighbor (r = 1) in one dimension and starting from random initial states. [Pg.13]

We recall, from equations 2.8 and 2,9, that only 32 so-called legal rules (out of the 256 total possible rules that can be defined), leave the zero-state a — 0 unchanged and are such that reflection-symmetric local states - 100 and 001 , for example - yield the same values. We now examine the patterns generated by these types of rules. [Pg.54]

Patterns of this third class in fact demonstrate a complex form of scale-invariance by their self-similarity, in the infinite time limit, different magnifications observed at the same resolution are indistinguishable. The pattern generated by rule R90, for example, matches that of the successive lines in Pascal s triangle ai t) is given by the coefficient of in the expansion of (1 - - xY modulo-tv/o (see figure 3.2). [Pg.55]

While the patterns generated by rules R18 and R218 are essentially the same as... [Pg.55]

Defining T(n) to be the density of triangular clearings with base length n , it has been found that, for large n and for patterns generated from disordered initial states, T(n) behaves as... [Pg.75]

For additive rules, which we recall from chapter two are those obeying an additive superposition principle, the difference at time t is equal to the step in the evolution of the initial difference.thus counts the number of I s appearing in the t row of the characteristic fractal patterns generated from single seeds (see figure 3.1). For Rule R90, for example, it is easy to show that H t) is given explicitly by H(t) = where ffi(t) is the number of times the digit 1 appears in the bi-... [Pg.79]

Figures 3.38 and 3.39 show typical space-time patterns generated by a few r = 1 reversible rules starting from both simple and disordered initial states. Although analogs of the four generic classes of behavior may be discerned, there are important dynamical differences. The most important difference being the absence of attractors, since there can never be a merging of trajectories in a reversible system for finite lattices this means that the state transition graph must consist exclusively of cyclic states. We make a few general observations. Figures 3.38 and 3.39 show typical space-time patterns generated by a few r = 1 reversible rules starting from both simple and disordered initial states. Although analogs of the four generic classes of behavior may be discerned, there are important dynamical differences. The most important difference being the absence of attractors, since there can never be a merging of trajectories in a reversible system for finite lattices this means that the state transition graph must consist exclusively of cyclic states. We make a few general observations.
Ii89] Li, W., Complex patterns generated by next nearest neighbor cellular automata, Computers and Graphics 13 (1989). [Pg.773]

Includes Pattern generator, photo-repeater, electron-beam lithography and contact printer... [Pg.323]

Interference pattern The pattern generated when two or more waves interact with one another. [Pg.120]

Figure 3.2 The cumulative pattern generated by photons sent one by one through a two-slit interferometer. Number of photons (a) 10, (b) 100, (c) 3000, (d) 20,000, and (e) 70,000. (Reproduced with permission from Tonomura et al, Amer. J. Phys. 57, i 17, 1987.)... Figure 3.2 The cumulative pattern generated by photons sent one by one through a two-slit interferometer. Number of photons (a) 10, (b) 100, (c) 3000, (d) 20,000, and (e) 70,000. (Reproduced with permission from Tonomura et al, Amer. J. Phys. 57, i 17, 1987.)...
The Malvern particle sizer is one of the most widely used, most effective, simple, and reliable methods commercially available for rapid measurements of ensemble characteristics of a spray. It is able to handle high droplet concentrations. It is easy to use and does not require comprehensive knowledge of its basic principles for operation. The primary advantage of the system is the speed of data acquisition and analysis. In addition, measurements of droplet size distributions can be made at any droplet velocities due to the fact that the diffraction patterns generated by droplets are independent of the... [Pg.427]


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