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with the solution formally given by x = A 1f More details about the procedure can be found in any of the numerous references in this area; see, for example [Kantorovich and Krylov 1964, Vorovbyev 1965, Harrington 1968, Adams 1974, Poggio and Miller 1973, Miller and Burke 1992, Wang 1991] The MoM procedure is general and applicable to conformal antennas located at arbitrarily shaped surfaces Unfortunately, both calculating the elements in A and solving the matrix equation can be cumbersome if the number of unknowns is large This is a general problem when using the MoM, but it can be much more pronounced for conformal antennas If the appropriate Green s function cannot be found, as is the case in many conformal antenna applications, the free space Green s function must be used, resulting in an increased number of unknowns.

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At higher frequencies and/or for electrically large surfaces, the MoM becomes impractical in many cases Despite these complications, the MoM has found widespread use in the analysis of conformal antennas It is often used in combination with other techniques such as spectral domain and asymptotic techniques in order to simplify the analysis In the references cited below, several examples are found in which the MoM has been used, sometimes combined with other methods Slots in (coated) PEC surfaces are considered in Peterson and Mittra [1989] and Sipus et al [2001a b] Microstrip patch antennas have been studied extensively; see for example, [Habashy et al 1990; Silva et al 1991; Wong et al 1993; Gottwald and Wiesbeck 1994; da Silva and Lacava 1995; Vecchi et al 1997a b; Bertuch et al 1999; Raffaelli et al 2001, 2005; Sipus et al.

1998; Sipus 2003; Svezhentsev and Vandenbosch 2001; Svezhentsev 2003; Jakobus and van Tonder 2003] A perturbed microstrip antenna is considered in Thiel and Dreher [1999]; see also [Thiel and Dreher 2001a c, 2002; Thiel 2002] A conformal spiral antenna is studied in Nakayama et al [1999] Boulder Microwave Technologies was offering a commercial software for analysis of conformal microstrip-patch antennas, called Clementine [Hall and Wu 1996] in the late 1990s This software is based on a mixed-potential integral equation (MPIE) model However, to our knowledge, this software is no longer available 434 Finite Difference Time Domain Methods (FDTD).

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Fig. 14.14 Development in equal time steps of the projected center-of-mass baryon density at three different impact parameters b, obtained from a threedimensional relativistic hydrodynamic model. The equivalent laboratory beam energy is 800 MeV per nucleon (Kapusta and Strottman, 1981).

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You may want to turn specific plug-ins on and off as needed rather than have them in the way all the time. A good way to do this is to create plug-in sets that you can then switch among. I recommend you create a set of plug-ins called Standard Plugs (at first, it would be the same as the All Plug-ins set, including everything that comes with InDesign out of the box). Then, before you add any new plug-ins, first create a new set named after the new plug-in and activate it in the Set menu. Then quit InDesign and install the new plug-ins. You can decide whether to switch between this plug-in set and Standard plug-ins using the Set pop-up menu or to save this new set as Standard Plug-ins, making the new plug-in part of your standard plug-in set.

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