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Wait, J.R. The Receiving Loop with a Hollow Prolate Spheroidal Core. Can J Tech Vol. 31, June 1953b, pp. 132 137. Walser, R.M. Electromagnetic Metamaterials. In Complex Mediums II: Beyond Linear Isotropic Dielectrics, Lakhtakia, A. Werner, S.W. Hodgkinson, I.J., Eds. Proc SPIE Vol. 4467, 2001, pp. 1 15. Wanselow, R.D. and Milligan, D.W. A Compact, Low Pro le, Transmission Line Antenna Tunable over Greater than Octave Bandwidth. Trans IEEE Vol. AP-14, Nov. 1966, pp. 701 707. Wegstein, J. Algorithm 2. CACM Vol. 3, Issue 2, 1960, p. 74. Wheeler, H.A. Fundamental Limitations of Small Antennas. Proc IRE Vol. 35, Dec. 1947, pp. 1479 1484. Wheeler, H.A. The Spherical Coil as an Inductor, Shield, or Antenna. Proc IRE, Vol. 46, Sept. 1958, pp. 1595 1602. Wheeler, H.A. Transmission-Line Propagationerties of Parallel Strips Separated by a Dielectric Sheet. Trans IEEE Vol. MTT-13, Mar. 1965, pp. 172 185. Wheeler, H.A. Small Antennas. Trans IEEE Vol. AP-23, July 1975, pp. 462 469. Wong, J.L. and King, H.E. Height-Reduced Meander Zigzag Monopoles with Broad-Band Characteristics. Trans IEEE Vol. AP-34, May 1986, pp. 716 717. Wu, T.T. and King, R.W.P. The Cylindrical Antenna with Nonre ecting Resistive Loading. Trans IEEE Vol. AP-13, May 1965, pp. 369 373; correction Nov. 1965 p. 998. Yaghjian, A.D. and Best, S.R. Impedance, Bandwidth, and Q of Antennas. Trans IEEE Vol. AP-53, April 2005, pp. 1298 1324. Zhu, J. and Engheta, N. Peano Antennas. IEEE Ant Wireless Propagation Lett Vol. 3, 2004, pp. 71 74. Zhu, J., Hoorfar, A., and Engheta, N. Bandwidth, Cross-Polarization, and FeedPoint Characteristics of Matched Hilbert Antennas. IEEE Ant Wireless Propagation Lett Vol. 2, 2003, pp. 2 5. Ziolkowski, R.W. and Kipple, A.D. Application of Double Negative Materials to Increase the Power Radiated by Electrically Small Antennas. Trans IEEE Vol. AP-51, Oct. 2003, pp. 2626 2640.

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Appendix C ensure adequate personnel to meet the needs of the system; (b) all sources of funding, both public and private, are used and maximized to ensure the fiscal support necessary to provide adequate services; (c) all employees have adequate technology, clerical services, and a physical work environment; and (d) employees have adequate personnel benefits necessary to support the work of the unit including continuing educational professional development. 3.1 School psychological services units assume the professional responsibility and accountability for services provided through the recruitment of qualified and diverse staff and the assurance that staff members function only in their areas of competency. 3.2 School psychological services units support recruitment and retention of qualified staff by advocating for appropriate ratios of school psychology services staff to students. The ratio of staff to students should not exceed one staff person for every 1000 sttudents. 3.3 School psychological services units utilize advanced technologies (e.g., computer-assisted) in time management, communication systems, data management systems, and service delivery. 3.4 School psychological services unit have access to adequate clerical assistance, appropriate professional work materials, sufficient office and work space, adequate technology support (e.g., e-mail, computer) and general working conditions that enhance the delivery of effective services. Included are test materials, access to private telephone and office, secretarial services, therapeutic aids, and professional literature.

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An early version is in SMG 385/97, the last version is in SMG 111/99. SMG 302/97.

Here, A is the electrode area, C and D are the concentration and the diffusion coefficient of the electroactive species, DE and x(= 2pf) are the amplitude and the angular frequency of the AC applied voltage, t is the time, and j = nF (Edc E1/2)/RT. For reversible processes, the AC polarographic wave has a symmetrical bell shape and corresponds to the derivative curve of the DC polarographic wave (Fig. 5.14 (b)). The peak current ip, expressed by Eq. (5.24), is proportional to the concentration of electroactive species and the peak potential is almost equal to the half-wave potential in DC polarography: ip n2 F 2 AC xD 1=2 DE 32 1=2 RT 5:24

Note that processes placed in the background are given a job ID number (in this case, 1). By placing a percentage sign in front of the number (for example, %1) you can identify a particular background process to the bg and fg commands or simply type the number

12.5 MOMENTS Moments are widely used in shape analysis tasks. Shape normalization, shape encoding (characterization), shape matching, and shape identi cation are just some examples where moments techniques are successfully applied. To be precise, by shape moments we mean geometric moments. The geometric moment mp,q (S) of a given planar shape S is de ned by mp,q (S) =

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