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The ripple discussed above is not caused by an edge effect since there is no discontinuity in the angular direction; instead, it is due to the mutual coupling among the elements on this nonplanar geometry The embedded-element pattern is given by a superposition of the isolated-element patterns of all elements when excited through mutual coupling When added together, the interference between the different contributions will result in an oscillating behavior As we see in Figure 621 (a), the interference may add out of phase (d = 06 ) or add in phase (d = 07 ) The ripple is reduced by reducing the element spacing To provide another way of looking at the sometimes very fast changes of the element pattern when changing the geometry slightly, two additional examples are considered Figure 6.

2.4 (a) See Bjorken and Drell(1965), 816.12; or Mandl (1959), Ch. 5 and Ch. 8; see also Exercise 2.9b. (b) Use [ H ,I I ( x ,t ) ] = i6H/64(x,t ) , the definition of

20 30 [degrees]

To find reference details for the attributes of an HTML tag, a JavaScript object, or a CSS style rule included on a Web page, open Code view and select the code in question prior to choosing Shift+F1 or clicking the Reference button on the toolbar.

22 shows the gain (E plane) for two cases with very different results obtained by only changing the element spacing for a fixed radius of 6 In Figure 622 (a), the element spacing is 06 and in Figure 622 (b) it is increased by one-tenth of a wavelength to 07 Figure 622 shows the gain and element excitations (amplitude and phase) The excitation (obtained from the mutual coupling analysis) is shown for the elements located within 90 with respect to the actively fed element denoted as element number 0 The phase of the elements is shown with respect to the fed element Together with the original excitation, a projected excitation is obtained This projected excitation is the excitation of the elements on the curved surface when projected on a planar surface in front of the cylinder.

preparation, you re going to waste a lot of time and effort. With it, you can usually tell with merely a glance at the rst image whether or not it s worth your while to dig into the rest of the artist s offerings.

Next, add pedestrian lights between the trees (Fig. 6-32). Place the light between two trees (approximate). Array three more lights into the model between the trees using the Move/Copy command. Continue to import more detail (such as benches, cars, and people) into the scene. Experiment by using the various tools to adjust size, rotation, and location (Fig. 6-33, Fig. 6-34). Make sure to place all component types onto an appropriate layer.

is a constant of motion,

3

Hence, this equivalent planar array becomes an array with nonuniform element spacing The new excitations are found by adding a phase corresponding to the distance between the element position on the curved surface and the new position on the planar surface Studying the excitation data, now from a planar array point of view, we can more easily explain why the embedded-element patterns look like they do For the smaller element spacing [Figure 622 (a)], there is a large change in phase among the elements closest to the excited element For these elements, the element spacings are almost equal on the projected plane If a planar analysis is applied, we get a pattern similar to the embedded-element pattern shown in Figure 622 (a) The contributions from the elements closest to the.

This query uses the previous query (without the ORDER BY clause) as a subquery and joins it to the Product table to get the product group: Figure 9-3 shows number of households that have made a purchase and the proportion that are one-time-only within each category. By this measure, the worst product group is APPAREL, where over half the purchasers are onetime only. The best is FREEBIE, with less than 1%. That is presumably because the FREEBIE products are typically included in bundles with other products.