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Building a portable Nintendo Entertainment System is a great way to relive some fun gaming memories of the past, and building it by hand is within the technical and financial reach of most gamers. In this chapter, you Built a custom case for the NES portable by hand, using thin engraving plastic and strips of aluminum. Wired up new custom built-in controllers using printed-circuit boards and integrated circuits from old NES controllers. Attached a PSOne screen for use with a NES. Installed a NES motherboard (that you modified in 6) into your custom case. Connected all these components together, along with a battery, in order to make the unit portable. The end result is that you now have a portable NES that you can take wherever you go. Have fun with it and show all your friends, but keep these pointers in mind: Don t drop the unit or allow it to get crushed the hand-built case or the screen may get damaged. A small case, such as a camcorder or camera bag, makes a great portable transporter ( portable transporter ... that s certainly a redundant M bius strip of a phrase). If you take this thing on an airplane, remove it from its bag, as you would a laptop computer, when you put it through the scanner. Be ready to turn it on and play it if they ask questions. Imagine how confusing the rat s nest of wiring inside must look on an X-ray. You can use a car power adapter to run the unit just follow the same guidelines as for the DC wall power adapter.



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SECTION FOUR: PRODUCT INFORMATION (EQUITY)





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A key observation is that if a convolutional encoder at the transmitter is followed by an interleaver, then the convolutive effects experienced as the signal traverses through the channel act like a second convolutional encoder, so the overall scheme acts like a serially concatenatedcode, with an interleaverbetween them. It is thus amenable to turbo decoding. Figure 14.19 shows the general framework for a system that can employ turbo decoding. The interleaver serves to decorrelate the values, so that extrinsic information computed in the decoder is nearly independent of the input values and can be used as a prior. In practice, the length of the interleaver is on the order of the length of the channel response. In the turbo decoder, the channel response is first accounted for using a MAP equalizer, which produces information about the bits in the form of log likelihood ratios, h(xt Ir). The prior information is subtracted, leaving an extrinsic information that is passed through the interleaver and on to the convolutionaldecoder, where it is employed as a prior probability. The output of the decoder is again bit information in the form of log likelihood ratios h(xl Ir). The prior information associated with this is subtracted off, then the resulting extrinsic information is sent back to the equalizer for another iteration. All elements of this equalizer should by now be familiar, with the possible exception of the MAP equalizer, which is described via an example. Suppose fl-valued bits emerging from the convolutional encoder are denoted as fit (where, for the moment, we simply think of these as a string of bits, without regard to which are message bits and which are parity bits). The modulated bits are af = f i z z . Suppose

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but not to the ller alternatives. In this case, the suspect fails the test, which is the correct decision. It is also possible that a guilty suspect shows similar responses to all alternatives, or shows a speci c response to a ller alternative. In this case, the suspect will pass the test, which is an incorrect decision. An innocent suspect may show similar responses to all alternatives or a speci c response to a ller alternative. In this case, the suspect will pass the test, which is the correct decision. However, an innocent suspect may show a speci c response to the critical item. This time the suspect fails the test, which is an incorrect decision.

+ Lc*rj2' + A(&).

in a number of attempts of account takeover being prevented by the telephone operators. Two months later, despite our efforts and xing control gaps, we were still unable to nd the internal perpetrator. We were no longer losing money to this scheme but attempts to steal from our clients were still being made. It was clear that the problem would not go away by itself.

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Figure 7.27 Models of extension involving frictional-plastic (brittle) strain softening at (a) low extensional velocities (Vext = 0.6 mm a 1) and (b) high extensional velocities (Vext = 100 mm a 1). Models also show rift sensitivity to (c) a weak and (d) a strong middle and lower crust at Vext = 3 mm a 1 (images provided by R. Huismans and modi ed from Huismans & Beaumont, 2007, with permission from the Geological Society of London). t, time elapsed in millions of years; x amount of horizontal extension. Vertical and horizontal scales are in kilometers.

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Many of the areas described above have continued to receive ongoing development and advancement. This section reviews some the recent progress. Building elements Davies (1999) gives a review of practice in building element conduction problems contrasting transfer methods (i.e. response factor-type approaches see Section 1.3), with numerical ( nite difference) methods (see Section 2.1) and exact analytical methods (i.e. conventional time domain methods see Section 1.3). Wang & Chen (2001) use frequency domain regression methods to estimate Laplace transfer function-based transient wall conduction

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1 0.9 0.8 0.7 0.6 0.5 0.4 0.3 0.2 0.1 0

Figure 17-4: Opera supports generated content, as demonstrated by the generated quotes around the <blockquote> paragraph.

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