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Draws an arc using a system of X,Y displacement and bulge using the syntax X-displacement, Y-displacement, and bulge. These three codes can range from 127 to +127. The X and Y displacements just specify the endpoint of the arc. The bulge equals ((2 * H/D) * 127) where D is the chord length (the distance from the start point to the endpoint) and H is the height measured from the midpoint of the chord to the circumference of the arc. The bulge should be negative if the arc is drawn clockwise. Continued

Time (min)

[;(l+pz)]j,



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Figure 17.11 Effects of sibutramine and placebo on body weight during the 2-year STORM study (Bray et al., 1996).

FIGURE 5.41 Geometry of a compact circularly polarized square microstrip antenna with slits and a chip resistor. (From Ref. 11, C 1999 John Wiley & Sons, Inc.)





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connection. Thus not only do you lose range during attenuation, but you lose throughput. Below a certain point, the wireless connection drops out completely. When maximum attenuation is calculated, a formula called EIRP (Equivalent Isotropically Radiated Power) is used. For information on measuring the amount of acceptable loss using EIRP, go to www.wi-fiplanet.com/tutorials/ article.php/1431101. It is important to understand that attenuation isn t a linear function. The further away from the wireless source that you put a barrier, the more effect it has on dropping the signal strength. Thus, a single wall close to the source will have considerably less impact on the signal strength than the same wall would have a couple of rooms away. Of course, what the wall is made of is important, too. The following estimates of attenuation are offered for common building features: Plasterboard: 3dB Office window: 3dB Concrete or cinder block walls: 4dB Glass wall in a metal frame: 6dB Metal door: 6dB Metal door in brick wall: 12.4dB The type of wireless protocol you are using affects the attenuation of a signal through the same media. The higher frequencies and larger ranges of the 802.11g devices you might use suffer more degradation of their signal than an 802.11b device.

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Armed with the conceptual framework presented in Part One of the book, and with the development process concepts introduced in this chapter, we can now discuss the three remaining parts of setting up a business component factory. 8 discusses the technical architecture and the business component virtual machine and 9 the application architecture required to produce industrial-strength business components and business component systems . Finally in 10 we conclude the factory set-up by discussing what is required to scale the production to very large teams .

Once the rst-order Kirchhoff s equation has been solved and the rst-order terms have been found, the second-order Kirchhoff s equation can be written as C dvss,2 (t) 2 + g1 (t) vss,2 (t) + g2 (t) vss,1 (t) = 0 dt (7.22)

Figure 5.25. (a) The heterodyne beat between a sample of a 500-ns high-energy output pulse and a single-frequency 1053-nm diode-pumped CW laser. (b) The analysis of the beat pro le demonstrates a peak-to-valley variation of the cumulative phase error of ,0.1l. When the SBS loop is blocked, returning the SBS mirror to the single-focus geometry, the heterodyne beat becomes very unstable and exhibits the large temporal phase steps that have been observed by other researchers [49].

Figure 17-1: Nobody s perfect, and neither is the best of scanned photos (left). You can modify colors in an image to achieve special effects (middle) or simply fix the image with a few well-targeted color corrections (right). Too bad Photoshop hasn t delivered on its promised Remove Excessive Jewelry filter.

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