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, 47(8), 20 23 6 Brzozowski, C (2004), Tags, tickets & labels: New technologies emerge, Printing News, 153(3) 7 Ranky, P G, An integrated PM approach, including: Process modeling, requirements analysis, risk analysis, statistical tools and 3D multimedia, presented at the Project Management Institute (PMI), New Jersey Jan 2006 8 Ranky, P G, Focus on RFID (radio frequency identi cation) methods, technologies and education, presented as part of the NCME Mission (National Center for Manufacturing Education), sponsored by NSF (National Science Foundation, USA) and industry, Jan 2006 9 Flaherty, M, Ranky, P G, Ranky, M F, Sands, S, and Stratful, S (1999, Mar), An engineering multimedia approach to servo pneumatic positioning, ADAM (Adv Des Manufacturing), available: http://wwwcimwareukandusacom, listed and indexed by the Association of Research Libraries, Washington DC, and the Edinburgh Engineering Virtual Library, United Kingdom, Vol 1 10 Glidden, R.



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, Bockorick, C, etal (2004), Design of ultra-low-cost UHF RFID tags for supply chain applications, IEEE Commun Mag 42(8), 140 151 11 Graham-Rowe, D (2004), Tags to banish forgetfulness, New Scientist, 183(2460), 19 12 Graham-Rowe, D (2004), Who s keeping tabs on your tags New Scientist, 183(2462), 22 13 Ho, K L, and Ranky, P G (1999, Mar), An object oriented approach to exible conveyor system design, ADAM (Adv Des Manufacturing), available: http://www cimwareukandusacom, listed and indexed by the Association of Research Libraries, Washington DC, and the Edinburgh Engineering Virtual Library, United Kingdom, Vol 1..

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Figure 8.10 IPILab research networks consist of three major networks: (A, right; light purple) Connection between IPILab research facility with the USC PACS internal networks (to be described in 16: Enterprise PACS), data from outside the USC passes the USC network rewall through two ber-channel switches (upper green and upper purple). The switch in the upper green connects to a second set of switches protected by the IPILab rewall; data transmits to a second set of switches, which distribute it to the light blue and light yellow columns. (B , middle column; light blue) projects servers, and (C , left; light yellow) personal devices in the laboratory.

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Figure 5-18: A 100-pixel diameter brush shown as it appears when set to a variety of Hardness percentages. I changed the background pixels below from white to black so that you can see the actual diameter of each brush shape. The tick marks indicate 10-pixel increments.

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general radiographic procedures. Tissue thickness (cm) Absorption factor (AF) versus HVL (mm Al) 1.5 0 3 6 8 10 12 14 16 20 25 30 35 1.00 2.10 4.35 6.41 9.35 13.7 20.0 28.6 63.0 165 440 1150 2.0 1.00 1.81 3.13 4.42 5.99 8.20 11.2 15.4 29.5 65.5 146 330 3.0 1.00 1.54 2.50 3.42 4.61 6.25 8.55 11.8 22.0 49.0 108 240 4.0 1.00 1.35 2.12 2.90 3.82 5.18 7.04 9.52 17.3 36.5 78.0 166 5.0 1.00 1.17 1.80 2.40 3.20 4.30 5.70 7.00 13.7 27.8 57.0 118

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culation on any system which does not have equal numbers of alpha and beta electrons should be of the UHF type THE BASIS SET (STO-3G, 6-31G*, AND ALL THAT) Molecular orbitals will be very irregular three-dimensional functions with maxima near the nuclei since the electrons are most likely to be found there and falling o toward zero as the distance from the nuclei increases There will also be many zeros de ning nodal surfaces that separate phase changes These requirements are satis ed by a linear combination of atom-centered basis functions The basis functions we choose should describe as closely as possible the correct distribution of electrons in the vicinity of nuclei since, when the electron is close to one atom and far from the others, its distribution will resemble an AO of that atom.

And yet they should be simple enough that mathematical operations required in the solution of the Fock equations can actually be carried out e ciently The rst requirement is easily satis ed by choosing hydrogenic AOs as a basis set Unfortunately, the exponential radial dependence of the hydrogenic functions [see equation (A62) and Figure 22a] makes the evaluation of the necessary integrals exceedingly di cult and time consuming for general computation, and so another set of functions with approximately the same behavior is now universally adopted These are Cartesian Gaussian functions, centered on nuclei The correct radial behavior of the hydrogenlike AO is as a simple exponential Orbitals based on this radial dependence are called Slater-type orbitals (STOs) Gaussian functions are rounded at the nucleus and decrease faster than desirable (Figure 22b).

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