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on the mesh generator cubes that operates on surface triangulations and is part of the Cart3D [3] package. Eleven is a general complex geometry library that operates on ESRI shape les and is included as part of the Overture [21] package. Both packages are integrated with SAMRAI in a way that provides a fully parallel embedded boundary mesh generation capability. The particular approach used in FEM3MP to enforce the boundary is an algorithm based on the immersed boundary formulation (see Ref. [27]), which is slightly different from traditional embedded boundary approaches (see, e.g., Ref. [15]); however, it uses the geometric information provided by the embedded boundary packages. In what follows, we use the term embedded boundary to refer to any of the Cartesian grid approaches where the boundary is not body tted. SAMRAI can support either embedded or immersed boundary representations. Although the discussion in this chapter will focus on the urban modeling application using FEM3MP, the framework we have put together is general purpose and can be applied to many other problems that require AMR, complex geometries, and parallel computing. Section 6.2 gives some background on the numerics in the FEM3MP model and the particular algorithmic changes that were made to operate on an adaptive Cartesian mesh with an embedded boundary representation of the building surfaces. Section 1.3 discusses the computational infrastructures that provide the adaptive grid capability on large-scale parallel computer systems with complex geometry. Section 1.4 discusses details of the parallel implementation. Finally, Section 6.5 deals with about future improvements that could be achieved through continued use of innovative computational infrastructures.

The drawings used in the following exercise on creating and using a tool palette, ab26-c.dwg and ab26-d.dwg, are in the Drawings folder on the CD-ROM.

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When you work in Source view, an extra in-page toolbar provides buttons that show errors and help identify code. Figure 3-6 shows these buttons.

Example 49 An example of M A C frame exchanges between a station and an A P is shown in Figure 8.12. The message exchange in this example is described as follows:

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the light is absorbed by the plasmon, converted into electrical energy that propagates through the nanostructure, and eventually converted back to light [265, 294] Superprism e ects The superprism phenomenon relates to the very large angular dispersion experienced by a light beam when entering a photonic crystal This arises from the anisotropy of the photonic band structure that can be present even in systems without a complete photonic bandgap [295] These e ects can be exploited for sensing and ltering applications Subwavelength There is research interest in surface electromagnetic waves and the extraordinary light transmittance (EOT) through an phenomena and optically thick metal lm that is perforated with subwavelength-size holes EOT was rst discussed in the late 1990s plasmonic excitations and has been intensively investigated since [296] These phenomena and properties in nanoengineered structures can be used as integrated elements in various optoelectronic and photonic devices, including optical computers [297].

Figure 14.7. Types of end-of-life electronic equipment collected predominately from residential sources. Ref. 36.

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In the optical and infrared spectral ranges, the excitation of the electron density coupled to the electromagnetic eld results in a surface plasmon polariton (SPP) traveling on the metal surface At the metal air interface, the ` SPP is a wave, with the direction of the magnetic eld parallel to the metal surface In the direction perpendicular to the interface, SPPs exponentially decay in both media The SPP can propagate not only on the metal surface but also on the surface of arti cial electromagnetic crystals, for example, on wire-mesh crystals Since the SPP propagation includes rearrangement of the electron density, its speed is less than the speed of light; as a result, the SPP cannot be excited by an electromagnetic wave impinging on a perfectly at metal surface.

The combination of HALS with a UV absorber is used in lms of polypropylene and polyethylene as well as in thick sections In lms of LDPE, nickel quenchers were commonly used with a UV absorber, except in a very thin lm, in which a higher concentration of nickel stabilizer is superior to the combination The low-molecular-weight HALS are not suf ciently compatible with LDPE at the concentrations necessary, possibly as high as 2%, for the required protection Incompatibility of HALS with LDPE has been overcome with the development of polymeric HALS It is considerably better than either the UV absorber or nickel quencher or combinations of the two For thicker lms (100 200 m), the combination of a benzophenone-type UV absorber with polymeric HALS is signi cantly superior to an equivalent amount of polymeric HALS.

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