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of limited precision effects on filter performance also appears in Cioffi (1987) and Shenvood and Bershad (1987). Further results for LMS, NLMS, and sign-regressor LMS appear in Chang and Willson (1995), Bermudez and Bershad (1996ab), Eweda, Yousef, and El-Ramly (1998), and Eweda, Younis, and El-Ramly (1998). In the works by Bermudez and Bershad (1996ab), the authors develop a model to account for nonlinearities in the quantization process, including the occurrence of underflow, and use the model to study the performance of quantized LMS. The extension of the energy conservation approach to the case of finite precision implementations can be found in Yousef and Sayed (2000b,2003) and Sayed (2003, Ch. 8). Drift problem. The fact that the LMS filter can produce unbounded weight estimates in some situations is illustrated in Prob. IV.39. This so-called drift problem has been described in several references including, for example, Gitlin, Meadors, and Weinstein (1982), Ioannou and Kokotovic (1984), Cioffi and Werner (1985), Sethares et al. (1986), Cioffi (1987), and Rupp (1995). The reference Ioannou and Kokotovic (1984) provides an analysis in the adaptive control context. The reference Sethares et al. (1986) studies the drift problem in a deterministic infinite-precision setting, while the references Cioffi and Werner (1985) and Cioffi (1987) consider finite-precision effects. They show that even with zero noise, unbounded growth (i.e., drift) of the weight estimates can happen due to finite-precision arithmetic errors. Such unbounded growth of the LMS estimates usually happens if two conditions are satisfied:



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11.2 Sketch a phaser representation of an abc-sequence bal anced three-phase V-connected source, including Vall' V b", and V eil ifV UI, = 120 / 15 V rm s. 11 3 Ske tch a ph asor represent ati on o f a ba lanced three-phase system containin g both phase vo ltages and line voltages if V ab = 208 / 60 0 V rms. Label all ph asors and assume 11.8 Find the equi vale nt Z of the network in Fi g. P 11.8.





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Combustion of fossil fuels is the most important anthropogenic source of atmospheric Be, Co, Hg, Mo, Ni, Sb, Se, Sn and V; it also contributes to emissions of As, Cr, Cu, Mn and Zn [6] Industrial metallurgical processes produce the largest emissions of As, Cd, Cu, Ni and Zn Exhaust emissions from gasoline- and diesel-fuelled vehicles contribute to atmospheric Pb, Fe, Cu, Zn, Ni and Cd, while tyre-rubber abrasion to Zn [8] In the last decade, the use of new automobile catalytic converters also contributes to the emissions of Pt, Pd and Rh [9, 10] The composition of aerosols depends on the occurrence of metals in combustion processes and their volatility as well as on their amount produced by decomposition of continental and oceanic surfaces Thus, the size distributions of different metals depend on the balance of different sources..

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This two-line script works fine in Acrobat 6 through 8; however, there are problems executing the script properly in earlier versions of Acrobat. Be certain to use the script with six lines of code and specify all attributes of the spawned page and you can be certain the script works in all versions of Acrobat. You can also use an action type to instruct Acrobat to go to the newly created page. By default, spawned pages are created at the end of the PDF document. When pages are spawned, the page containing the button used to spawn a new page remains in view. To help a user navigate to the new spawned page, you can add another line of code to go to the new page. Add the following script after the last line of code used to spawn a page:

Show Length MP3 Bit Depth 32 kbps mono 96 kbps stereo 112 kbps stereo 128 kbps stereo 5 Min. 1.2 MB 3.6 MB 4.2 MB 4.8 MB 10 Min. 2.4 MB 7.2 MB 8.4 MB 9.6 MB 20 Min. 4.8 MB 30 Min. 7.2 MB 60 Min. 14.4 MB

RESEARCH METHOD MATTERS Efforts to explain prosocial behavior, especially its seemingly anomalous aspects, have raised thorny issues about research methods that, though not speci c to this area, ourish here.

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= 2 s) = 10 V in th e circuit in Fi g. P6. 19, find the e ne rgy stored in the capac itor a nd the power suppli ed by the source at I = 6 s .

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