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Furthermore, an (uniform) asymptotic solution is not unique, but the difference between two solutions is usually small* However, a general formulation is very desirable for efficient analyses of various realistic conformal antennas The work by Robert Kouyoumjian and his group at the ElectroScience Laboratory at Ohio State University has been successful and their solution is valid for different types of convex surfaces The solution is known as the uniform theory of diffraction (UTD), which is a raybased theory We have chosen to concentrate the discussion about high-frequency methods on this UTD formulation since we think it is a very powerful concept used worldwide Furthermore, this concept (in addition to, eg, the solution by [Lee 1978]) is well suited to study arbitrary surfaces since UTD is explicit in its way of describing the different effects that govern the behavior of wave propagation along curved surfaces.

The Consumer component s selector property filters messages based on values in message headers. The Producer and Consumer components implement a subtopic property that can be used to filter messages based on arbitrary topic names. The MultiTopicProducer and MultiTopicConsumer components enable you to send and receive messages that are filtered for multiple arbitrarily named topics.

a(z) = q 1 (z)b(z) + rl(z) (6.13)

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One of the trickiest types of documents to print is a folded booklet because you can t simply print the pages in sequence and have them end up on the right location on the final sheets of paper. When you fold them, the page order is rearranged because of the folding, especially in two-sided documents. The tried-and-true approach is to use a booklet template that essentially provides a map of where pages should be so when they are printed and folded, they end up in the right place and then arrange your pages in that order via the Pages panel. Figure 30.7 shows the natural order (1 8) that you typically think a booklet has, as well as the actual page order (8,1; 2,7; 6,3; and 4,5) that it must be printed as, so after it is folded and stapled it appears to the reader in the sequence of 1 through 8.

(3.7-6) where the integration proceeds along the path dl from point pl to point p2. Substituting Eq. (3.7-5) into Eq. (3.7-6) and integrating gives (3.7-7) The potential decreases as llr moving away from the charge. However, if the plasma is allowed to react to a test charge placed in the plasma, the potential has a different behavior than predicted by Eq. (3.7-7). Utilizing Eq. (3.2-7) for the electric field in Eq. (3.2-1) gives Poisson's equation:

A Sub-summary part is displayed in Browse mode, in Preview mode and print (or PDF) output, when the records are sorted according to the corresponding field (the break field associated with the Sub-summary part). You may create multiple Sub-summary parts, each coming into play only if the current found set is sorted by an associated field.

have mechanisms that allow users and resource owners to select policies that t particular security and performance needs, as well as meet local administrative requirements Global namespace: The lack of a global namespace for accessing data and resources is one of the most signi cant obstacles to wide-area distributed and parallel processing The current multitude of disjoint namespaces greatly impedes developing applications that span sites All Grid objects must be able to access (subject to security constraints) any other Grid object transparently without regard to location or replication Fault tolerance: Failure in large-scale Grid systems is and will be a fact of life Hosts, networks, disks and applications frequently fail, restart, disappear and behave otherwise unexpectedly Forcing the programmer to predict and handle all these failures signi cantly increases the dif culty of writing reliable applications Fault-tolerant computing is a known, very dif cult problem.

Even though the UTD concept is a general approach, there are minor differences; for example, when a coated or noncoated surface is considered as well as if the far field radiation problem or the surface field problem is considered There are also differences if the surface is convex or concave Due to space limitations, this book will only consider smooth convex surfaces For concave surfaces, the interested reader is referred to the available literature Conformal antennas have been convex in most of their applications and will probably be so in the future as well However, concave surfaces can find use on spacecraft and some RF lenses (see 9) An asymptotic (ray-based) theory can be used also for concave structures, but there are some additional features to consider such as caustics and whispering gallery modes [Inami et al 1982; Felsen and Green 1976; Ishihara and Felsen 1978, 1988; Tomasic et al.

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