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view of the computing requirements, parallel computing and improved accurate and flexible meshes need to be investigated.

or, employing Eq. ( 15.51 ),

TABLE 8.2 Bits 0000 0001 0101 0101 0101 0101 0101 0101 0101 0101 0101 0110 0110 0110 0110 0110 0110 0111 0111 0111

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display name [org.springframework.context.support.ClassPathXmlApplicationContext ... INFO [org.springframework.beans.factory.support.DefaultListableBeanFactory] Pre-instantiating singletons in factory [org.springframework.beans.factory.support.DefaultListableBeanFactory defining beans [xfire.customEditorConfigurer,xfire.serviceRegistry, xfire.transportManager,xfire, xfire.typeMappingRegistry,xfire.aegisBindingProvider, xfire.serviceFactory,xfire.servletController, xfire.messageServiceFactory,xfire.messageBindingProvider, emailValidationClient]; root of BeanFactory hierarchy] response for email id naveen@yahoo.com : VALID response for email id naveen@abc.com : NOT_VALID Web services client executed

FIGURE 8.10 Measured return loss for the antenna shown in Figure 8.9; R = 35 mm, h = 13.6 mm, d = 6.5 mm, = 7 mm, H1 = 10 mm, H2 = 30 mm, t = 3.5 mm, and ground-plane size = 100 100 mm2 . (a) H-slot coupled feed (port 1); (b) gap-coupled probe feed (port 2). (From Ref. 6, C 2000 John Wiley & Sons, Inc.)

In this paragraph, the special formulations that the nonlinear analysis methods described in 1 assume for autonomous circuits are described, together with the main problems connected with their use for circuit analysis and design. In 1, several numerical approaches have been brie y described, namely time-domain direct numerical integration, harmonic and spectral balance, Volterra series

Figure 4-10

Total weight required [kg] for exposure (C) 186 231 367 529

1 noise component in active devices being up-converted f from very low frequency to near the oscillation frequency. Both mechanisms can be implemented in a nonlinear simulator and are accurately predicted, provided noise sources are accurately modelled. Frequency conversion from baseband to near the carrier is essentially a secondorder nonlinear effect (see Section 1.3.1). Therefore, its magnitude depends very much on the importance of second-order nonlinearities. A qualitative measure of second-order nonlinearities is the amplitude of the recti cation of the oscillating signal, generating an increase of the DC bias currents and voltages. Therefore, a low-noise oscillator should exhibit a fairly constant DC bias current with and without oscillation, to within a few percent of the static unperturbed current. Generation of current and voltage harmonics has been treated in detail in 4, and the reader can refer to that approach for a correct procedure while designing an oscillator as in Section 5.3. It can be noted that, while third-order (or odd-order in general) nonlinearities are required for the saturation of the signal in an ampli er, and therefore for the achievement of the steady-state amplitude of the oscillation, second-order nonlinearities can be avoided by careful design without affecting the proper performances of the oscillator, especially when emphasis is put on noise instead of ef ciency. Another parameter related to the noise performances of the oscillator is the oscillation frequency shift with bias voltages. A rst qualitative indicator is the frequency

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Frequency (MHz)

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