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The Log-MAP algorithm requires forward and backward recursions through the entire sequence of symbols in the received burst in order to evaluate theforward and backward transition probability of Equation l 1.11 and 1 1.12, before calculating thePosteriori LLR values a C, ( c k ) . Therefore, effectively the computation of the a posteriori LLRs C, ( c k ) is performed on a burst-by-burst basis. The RBF based equaliser, however, performs the evaluation the of a posteriori LLRs Cp(ck) on a symbol-by-symbol basis. Therefore, in order to reduce the associated computational complexity, the RBF based TEQ may skip evaluating the symbol LLRs according to Equation 11.8 in the current iteration, when the symbol has a low error probability or high a priori LLR magnitude I ( c k )I after channel decodingin the previous C : iteration. If, however this isnot the case,the equaliser invokes a further iteration attempts and to improve the decoder's reliablility estimation of the coded bits. The output & , , ( v k ) of the RBF equaliser provides the likelihoodof the ith symbol at instant IC. The log-likelihood values of the ith symbol provided by the channel decoder in the previous iteration obey an approximately linear relationship versus the log-likelihood values from the equaliser in the current iteration, as demonstrated in Figure 1 1.1 I for the BPSK mode over a three-path, symbol-spaced fading channel equal CIR tap weights,where the Rayleigh fading statistics of obeyed a normalized Doppler frequency of 1.5 x lop4. Therefore, the logarithmic domain output In v k ) of the RBF equalisercan be estimated based onthisnear-linearrela( tionship portrayed in Figure 1 1.1according to: 1

+ (y - Hw)*W(y - Hw)

5

(8.14)

you an idea of how this works. As the dots get closer to one another, they begin to form a line. When you zoom out, the individual dots disappear. (It s similar to the idea of getting ink dots close together on a printer (dpi).

This formula converts the date in D19 to a text, three-letter month abbreviation; joins that with a line break, CHAR(13); and finally appends a two-letter abbreviation for the year. Using the CHAR(13) in concatenated text is a useful trick in many text situations. 15, Text Based Dashboards, provides more examples of how to concatenate (join) text, numbers, or dates.

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For this exercise, use the Desk.obj file found in the Photoshop CD containing the bonus content. To access this file, insert the bonus content CD and navigate to Goodies 3D models Desk.

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When using the Make Opacity Mask function, all the objects in the mask are automatically grouped together.

namely, for the k-th entries:

Modern stakeholder doctrine is relatively recent. It represents a signi cant shift in business governance paradigm (Clarke and Clegg, 1998; Jones and Wicks, 1999) from mainstream management principles ( Jonker and Foster, n.d. 2002). The origins of modern stakeholder

10. Type 10, 20, 30, and 40 in each column. a. In the topmost, leftmost aqua shape, type 10. b. Select the 10 you just typed and press Ctrl+C to copy it. c. Select the next shape in that row and press Ctrl+V. Repeat two more times so that all of the shapes in the rst turquoise row have 10 in them. d. Repeat the process to put 20 in the next row, 30 in the next, and then 40 in the bottom row.

surements. In Figure 6.59, the normalized E- and H-plane patterns are shown for the experimental antenna shown in Figure 6.46. The result is for the element located in the center of the array calculated at f = 5.4 GHz. As shown, the agreement between theory and measurements is quite good both in the E and the H planes. The small differences that can be observed in the E plane around = 20 is due to the air gap in the measurements, as has been verified in [Sipus and Kildal 2003]. In [Thors et al. 2003], it was shown that the corresponding E-plane radiation pattern for an isolated element in this array is very broad. However, when the element is placed in an array environment, the radiation pattern is changed considerably due to the mutual coupling. The oscillations in the theoretical H-plane results are a consequence of interference between rays creeping around the cylinder. These oscillations are not observed in the measurement since the experimental antenna was truncated in the azimuthal direction, as shown in Figure 6.46. As shown in Figure 6.59 (a), the E-plane embedded-element pattern is very oscillatory. The origin of the ripples can be attributed to the mutual coupling and the rather large 0.67 at f = 5.4 GHz). azimuthal element spacing in the experimental antenna (R This was discussed in Section 6.2.4. The most practical way to avoid the problem is to reduce the element spacing. Similar oscillations are not observed in Figure 6.59 (b). This can be understood by realizing that the H-plane coupling is much weaker than the E-plane coupling.

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