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17. IEEE, IEEE Standardfor VHDLRegister TransferLevel (RTL)Synthesis (IEEEStd 107661999), Institute of Electrical and Electronics Engineers, 2000. 18. IEEE, IEEE Standard VHDL Synthesis Packages (IEEE Std 1076.3-1997), Institute of Electrical and Electronics Engineers, 1997. 19. IEEE, IEEE Standard Multivalue Logic System for VHDL Model Interoperability (IEEE Std 1164-1993),Institute of Electrical and Electronics Engineers, 1993. 20. Integrated Silicon Solution, Data Sheet of IS61LV25616AL SRAM, Integrated Silicon Solution, Inc. 21. R. H. Katz and G. Borriello, Contemporary Logic Design, 2nd ed., Prentice Hall, 2004. 22. M. Keating andP. Bricaud, Methodology Manualfor System-on-a-ChipDesigns, 3rded., SpringerVerlag, 2002. 23. C. M. Maxfield, The Design Warrior s Guide to FPGAs, Newnes, 2004. 24. Mentor Graphics, ModelSim Tutorial, Mentor Graphics Corporation. 25. S. Palnitkar, Verilog HDL, 2nd ed., Prentice Hall, 2003. 26. D. A. Patterson and J. L. Hennessy, Computer Organization and Design: The Hardware/Software Interface, 3rd ed., Morgan Kaufmann, 2004. 27. J. M. Rabaey, Digital Integrated Circuits, 2nd ed., Prentice Hall, 2002. 28. J. F. Wakerly, Digital Design: Principles and Practices, Prentice Hall, 2002. 29. W. Wolf, FPGA-Based System Design, Prentice Hall, 2004. 30. Xilinx, DS099 Spartan-3 FPGA Family: Complete Data Sheet, Xilinx, Inc. 3 1. Xilinx, ISE 8.1 i Quick Start Tutorial, Xilinx, Inc. 32. Xilinx, ISE In-Depth Tutorial, Xilinx, Inc. 33. Xilinx, PicoBlaze 8-bit Embedded Microcontroller User Guide, Xilinx, Inc. 34. Xilinx, Spartan-3 Starter Kit Board User Guide, Xilinx, Inc.

Jm(kR), which governs the transformation from excitation-phase modes to radiation-phase modes when the elements are isotropic; compare Eq (225) As expected, Jm also approaches zero for m > 3 For the reflection coefficient, a feed-line impedance of 73 ohms was assumed Jones and Griffiths describe an analysis of a four-element circular array using quarterwavelength monopoles on a ground plane The element spacing was /6, corresponding to a kR value of 066 Thus, phase-mode orders beyond the m = 0 and m = 1 would be strongly attenuated The active phase-mode resistance for the array was calculated to be about 90 ohms, 12 ohms, and about 2 ohms when the array was excited with the zeroth, first, and second phase mode, respectively [Jones and Griffiths 1988, 1989] We got for the same case (assuming monopoles) 120 ohms, 12 ohms, and 06 ohms respectively.

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All the icon set examples in this section are available on the companion CD-ROM. The workbook is named icon set examples.xlsx.

Hanging out in San Diego, California, Gareth Pursehouse s single most favorite thing to do is practice Capoeira, which is considered, by some, a type of martial art. Capoeira blends dance, music, rituals, acrobatics, and fighting. This blend originates in Brazil, where it is played like a game. We wouldn t be surprised if Gareth conquered Flash ActionScript with the help of some good mojo from Capoeira. He earned his Flash recognition with one of his first Flash sites, www.infinovation.com.

and plaintext x(7(t N k)); x(7(t N k 1)); . . . ; x(7(t N 1)) | {z }

For linear and planar arrays, the active impedance is sometimes presented as a function of scan angle, typically assuming a large or infinite array with uniform amplitude excitation In this way, the useful scan range for a maximum acceptable reflection coefficient can be illustrated The corresponding reference case for a circular array is the phase mode impedance, demonstrating the range of useful phase-mode orders It should be remembered, however, that in practice a combination of phase-mode orders are used in order to synthesize a particular beam pattern [Josefsson and Persson 2005]; compare Section 104 Each single phase mode produces an omnidirectional pattern in the azimuth, but with reduced radiation at high elevation angles when m > 0 This has found use in antifading antennas for long- and medium-wave broadcasting systems, where it is desired to suppress the reflected signal from the ionosphere (Section 24).

The design correlation is based on experiments in which the blend time required to reach 95% homogeneity were measured. The blend time required to reach another degree of homogeneity can be calculated because the blending process is rst order (i.e., the concentration uctuations which are being smoothed as

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If a(z) k02l k01lz k01lz 2 k03lz 3, then the transformation Ta : b(z ) ! a(z ) b(z ) (modulo(1 z 4 ))

Since these designs typically use a small-diameter array (in wavelengths), the radiation resistance can become quite.

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