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To de ne the encipherment process, some additional notation is needed; the position of a pin-wheel for the encipherment of the jth letter is denoted as folIows:

If you want to use a custom symbol in more than one document, simply select the check box in the Convert to Symbol dialog box to save the symbol to the Common Library rather than the Document Library.

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45 TWO EXAMPLES 451 Introduction In this section, we will discuss two examples in order to provide some more information about how to proceed when analyzing conformal antennas The approach is based on the integral equation formulation, solved by the method of moments (MoM) As will become clear, the general analysis is not any different from the planar case However, it is much more difficult to find the field representation outside a curved surface In some cases, a high-frequency solution must be used to find the field, that is, a hybrid UTD-MoM approach is used We will discuss this briefly in Section 452 The two cases are the waveguide-fed aperture antenna array and the microstrip-patch antenna array These two canonical examples will also be discussed extensively in the following chapters, where several numerical examples illustrate the characteristics of conformal antennas 45.

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(v) tomographic scan of phantom (vi) projection imaging of point source. 5 True or false: In assessing the results of the center of rotation test, a deviation of the measured position of the source of less than two pixels from the expected position does not need further investigation.

2 The Aperture Antenna An aperture antenna can, generally speaking, be any of the following types: slits, slots, waveguide openings, horns, reflectors, and lenses However, in this context we consider an aperture antenna in the form of a waveguide aperture flush mounted on or integrated into a curved surface (see Figure 413) The cross section can be of any kind, but from a practical point of view rectangular and circular cross sections are common Aperture antennas can be flush mounted on a surface and are therefore very suitable for conformal antenna applications Furthermore, the opening can be covered with a dielectric material for protection without disturbing the overall shape of the surface This is very important when considering, for example, aircraft, in which the aerodynamic profile is important Figure 4.

13 shows the waveguide-fed aperture problem (for aperture m out of M apertures) with the computational domain divided into two regions: the exterior and interior regions Here, a noncoated PEC surface is assumed, but the formulation is equivalent if a coating is present The main idea of the solution presented here is to start with an exact formulation in terms of an integral equation for the boundary between the exterior and the interior regions By using the field equivalence theorem [Harrington 1961, page 106] an equivalent (exterior) problem is obtained by covering the apertures with a perfectly conducting surface and introducing unknown equivalent magnetic current moments on the surface These infinitesimal magnetic current moments then radiate in the presence of a perfectly conducting surface..

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