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cognitive psychology, 63, 101 cognitive task analysis, 116, 379 cognitive task analysis approach, 102 column generation, 426 command, management, 156 commitment abstraction, 152 CommonKADS, see: KADS communication, 16 human and system, 236 multisite scheduling, 296 representation types, 148 communication model, 396 complete state-action table, 309 composition based reuse, 211 computational complexity, 4, 256, 465 computational equivalence, 144 concept/concept abstraction, 151 concept/individual abstraction, 152 conceptual representations, 150 con ict, multi-actor system, 166 connectionism, 15 constraint propagation, 396 constraint relaxation, 127 Constraint Satisfaction Programming (CSP), 394 constraints, 6, 225 levels of description, 105 planning environment, 17 shunting, 386, 403 constraints-based scheduling, 284 content, representation, 106 content constraints, 6 context conditions, 47 contracts, 159 control, 16 controller, 388 cooperation, 141, 153 bene ts and costs, 167 coordinated action, 141,154 coordination, 16 multisite scheduling, 296 coordination efforts, 168 coordinative structures, 42 cost functions, 167 e.v., 358 crisis management, 80, 87 cultural differences, 125 e.v. data model of scheduling system, 233 debative cooperation, 153 decentralized planning, 139 e.v. decision aids, 480 decision making, 5, 108 air-traf c control, 90 decomposition, 184





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Another variation (Hariharan, 1975) of the basic parallel plate interferometer uses two plates whose separation may be adjusted to expand the range of the possible shear. In Figure 4.35, one of the plates is mounted on a movable platform so that the air gap is variable and, hence, variable shear is obtained without plate rotation. The inside surfaces of these plates are uncoated so that about 4% re ection occurs there. The outer surfaces are treated with high quality antire ection coatings to minimize re ections. The plate mounting may be equipped with additional degree of freedom so that it can be rotated orthogonally to introduce tilt. The physical separation of two plates makes this system sensitive to disturbances and fragile in handling. The stability of the fringe system depends on the quality of mechanical mounts, their design, fabrication, and environmental conditions. The lateral shearing interferograms displayed in Figures 4.4 4.11 were generated employing a laser shearing interferometer laid out in Figure 4.32. An uncoated glass plate with a laser source results in a suf ciently intense fringe pattern, projected on a ground glass in a dimly illuminated room. An exposure time of only a fraction of a second is suf cient to photograph the fringes. With the currently available CCD detector arrays, the experimental work is even simpler.

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Hence, one can imagine a beam of protons, each particle having suffered various random deflections due to scattering from gas molecules, intrabeam scattering, perturbations in magnetic fields, power supply noise, mechanical vibrations, and so on. So long as the various events are random and uncorrelated among the various particles, the distribution function describing the position of a particle which has been subjected to all of these random processes will be Gaussian, to good approximation. At the beginning of this chapter it was mentioned that discussion of electron beam emittance would be left to 8. There we will see that the dominant source of emittance fluctuation is the emission of photons due to synchrotron radiation, an inherently random process. Since the ensuing damping times are, in general, short, one would expect that even correlated processes such as injection errors might be swamped by the synchrotron radiation effects. Thus, electron beams in circular accelerators are certainly expected to have Gaussian distributions, and that is what is observed. The fact that proton beams in large synchrotrons also typically appear Gaussian suggests that the central limit theorem is at work here as well.

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