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Signal/Noise Ratio for Short Integrated Antennas Electronics Lett Vol 11, 6 Feb 1975, pp 62 63 Maclean, TSM and Rahman, F Small Toroidal Antennas Electronics Lett Vol 14, 25 May 1978, pp 339 340 Maclean, TSM and Saini, SPS Ef ciency and Signal/Noise Ratio of Short Linear Dipoles Electronics Lett Vol 17, 9 July 1981, pp 492 494 Mandelbrot, BB Fractals: Form, Chance and Dimension WH Freeman, 1977 Mandelbrot, BB The Fractal Geometry of Nature WH Freeman, 1982 Matthaei, GL, Young, L, and Jones, EMT Microwave Filters, ImpedanceMatching Networks, and Coupling Structures McGraw-Hill, 1964, Sections 409, 410 McAllister, MW and Long, SA Resonant Hemispherical Dielectric Antenna Electronics Lett Vol 20, 2 Aug 1984, pp 657 659 McAllister, MW, Long, SA, and Conway, GL.



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with Corr(X,Z) = Corr(Y,Z) = 0 We close this section with some nal remarks. We selected discrete random variables to minimize technical requirements and simplify the exposition. All the de nitions and formulas apply to continuous random variables as well. A bit more sophistication is required to carry out computations. For discrete random variables, Corr(X,Y) = 1 is identical to the relation Y = aX + b, where a and b are constants. For those familiar with regression, a and b are regression coef cients and there is no error term. For the more general case, Y = aX + Z, a is a regression coef cient and Z is a random variable with nonzero mean. We can make this appear more like a standard regression, Y = aX + b + Z with Z = b + Z . Both a and b are regression coef cients and Z is a random variable with zero mean.





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Rectangular Dielectric Resonator Antenna Electronics Lett Vol 19, 17 March 1983, pp 218 219 McLean, JS The Application of the Method of Moments to the Analysis of Electrically-Small Compound Antennas EMC Symp Record Aug 1995, pp 119 124 McLean, JS A Re-Examination of the Fundamental Limits on the Radiation Q of Electrically Small Antennas Trans IEEE Vol AP-44, May 1996, pp 672 676 Merenda, JT Radiation Synthesizer Systems and Methods US Patent 6229494, 8 May 2001 Middleton, WM Reference Data for Engineers, Section 420 NewnesButterworth-Heinemann, 2002 Miron, DB A Study of the CTHA Based on Analytical Models Trans IEEE Vol AP-49, Aug 2001, pp 1130 1137 Mongia, RK Half-Split Dielectric Resonator Placed on Metallic Plane for Antenna Applications Electronics Lett Vol 25, 30 March 1989, pp 462 464..

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This has probably proved to be true since by May 2001 there were 500 million subscribers to GSM, far more than had been anticipated earlier As work progressed on the ASCI services, there was a desire to add the last important PMR feature, direct mode, where two terminals can communicate with each other, if in radio range, without use of a network However, this proved too dif cult for the GSM standard since it is a full duplex system and both terminals would be transmitting at the same time on the same frequency It was concluded that if this feature were really needed, there would have to be a solution outside the GSM standard Another topic studied for many years in the xed network community was known as UPT, providing them with some degree of terminal mobility.

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FS > 0 when par bond curves are upward sloping. FS < 0 when par bond curves are downward sloping. FS = NS when par bond curves are flat.

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For a system of n lossy parallel interconnection lines, the above equations lead to the 2n-port circuit model shown in Fig. 3.6.2, which consists of lossy uncoupled lines with a modal decoupling network at the input end and a complementary coupling network at the output end. The values of the linear real or complex dependent sources in the network are given by the elements of the voltage eigenvector matrix [Mv ]. The model presented in Fig. 3.6.2 differs from that presented in the last section for the lossless lines in that, in the present case, the uncoupled lines are lossy having complex impedances and propagation constants and the dependent sources are generally not in phase with the independent variables. It should be noted that, given the frequency-dependent behaviors of the impedances and propagation constants of these lossy lines, they can be represented as 2-ports consisting of lossless lines and lumped elements as shown in Fig. 3.6.3 for the skin effect losses. The time-domain response of the interconnection lines can be calculated directly using the model for linear as well as nonlinear terminations. 3.6.2 Simulation Results

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