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over time in technical education, which has now also translated into fewer U.S. students seeking college degrees in technical fields. Exhibit 1.3 compares the relative numbers of U.S. and Asian students pursuing science and engineering disciplines at the collegiate level. As illustrated in the exhibit, Asian students are increasing their engineering expertise in a world that increasingly appreciates and utilizes their new abilities. Of the nearly 590,000 foreign students enrolled in U.S. higher education in 2002, more than 20 percent came from India or China. Ironically, the United States is not only relocating its coveted technical jobs to these foreign locations, but it is also preparing many of the workers who fill those jobs. The following list provides some sobering statistics on technical education EXHIBIT 1.3

her may even be feeling a mixture of astonishment and anger, as if to exclaim, How can you leave someone as sweet as me Damn you for accepting all my goodwill!

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Boyd, J P 1986 Solitons from sine waves: Analytical and numerical methods for nonintegrable solitary and cnoidal waves Physica 21D:227 246 Branstator, G, and S E Haupt 1998 An empirical model of barotropic atmospheric dynamics and its response to forcing J Climate 11:2645 2667 Cartwright, H M, and S P Harris 1993 Analysis of the distribution of airborne pollution using GAs Atmos Environ 27A:1783 1791 Chambers, L (ed) 1995 GAs, Applications, Vol 1 New York: CRC Press Davidor, Y 1991 GAs and Robotics River Edge, NJ: World Scienti c Davis, L 1991 Handbook of GAs New York: Van Nostrand Reinhold Fausett, L 1994 Fundamentals of Neural Networks: Architectures, Algorithms, and Applications Upper Saddle River, NJ: Prentice Hall Hagan, M T, H B Demuth, and M Beale 1995 Neural Network Design Boston: PWS Hasselmann, K 1976 Stochastic climate models Part I: Theory Tellus 28:473 485 Haupt, R.

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L 1995 An introduction to GAs for electromagnetics IEEE Ant Propagat Mag 37:7 15 Haupt, S E 1988 Solving nonlinear wave problems with spectral boundary value techniques PhD dissertation University of Michigan, Ann Arbor Haupt, S E, and J P Boyd 1988a Modeling nonlinear resonance: A modi cation to the Stokes perturbation expansion Wave Motion 10:83 98 Haupt, S E, and J P Boyd 1988b Double cnoidal waves of the Korteweg De Vries equation: Solution by the spectral boundary value approach Physica 50D:117 134 Holland, J H 1992 Genetic Algorithms Sci Am 267:66 72 Karr, C L 2003 Minimization of sonic boom using an evolutionary algorithm Paper AIAA 2003-0463 40st AIAA Aerospace Sciences Meeting and Exhibit, Reno, NV Karr, C L, I Yakushin, and K Nicolosi 2001 Solving inverse initial-value, boundaryvalue problems via GA Eng Appl Art Intell 13:625 633 Kirkpatrick, S, C D.

Figure 8.14 Temporal masking phenomenon shows how long it takes for the auditory system to realize that there is a test tone. This delay time depends on the level of the test tone. The louder the test tone, the sooner the ear detects it. In other words, the ear thinks that the masking tone is still there, even though it has been removed.

Gelatt, and M P Vecchi 1983 Optimization by simulated annealing Science 220:671 680 Koza, J R 1992 The Genetic Programming Paradigm: Genetically Breeding Populations of Computer Programs to Solve Problems In B Soucek (ed), Dynamic, Genetic, and Chaotic Programming: The Sixth Generation New York: J Wiley, pp 203 321 Loughlin, D H, S R Ranjithan, J W Baugh, Jr, and E D Brill Jr 2000 Application of GAs for the design of ozone control strategies J Air Waste Manage Assoc 50:1050 1063 Michalewicz, Z 1992 Genetic Algorithms + Data Structures = Evolution Programs New York: Springer-Verlag Obayashi, S, D Sasaki, Y Takeguchi, and N Hirose 2000 Multiobjective evolutionary computation for supersonic wing-shape optimization IEEE Trans Evol Comput 4:182 187 Pack, D, G Toussaint, and R Haupt 1996 Robot trajectory planning using a GA Int Symp on Optical Science, Engineering, and Instrumentation.

SPIE s Annual Meeting, Denver, CO Penland, C 1989 Random forcing and forecasting using principal oscillation pattern analysis Mon Weather Rev 117:2165 2185..

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where FL is the reflection coefficient of an array element under Floquet exci= FL , which follows from (4.34), one can see that tation. Since FL Smn = Snm . 4.4 ARRAY OF MULTIMODAL SOURCES For many applications the array element may be excited with more than one mode at the input level. For instance, if a square horn array has to radiate a circularly polarized wave, the input waveguide must contain the TE10 and TE01 modes

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