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To find a drink recipe, just choose the category and then choose Search By Liquor or Search By First Letter. If you know one of the main liquors in a drink recipe or simply want to browse through a list of vodka drinks, Search By Liquor is your best bet. If you know the name of the drink you want (for example, Bloody Mary), just enter the first letter of the drink name and then scroll down the list until you find the drink you are looking for. Figure 10-24 shows the Search By First Letter option in action.

Marshalling and unmarshalling of request parameters is performed by the dynamic invocation interface, client stubs and implementation skeletons, which are C O RBA s server stubs. Client stubs and server skeletons are generated by an IDL compiler, which is an integral component of every C O RBA product. The dynamic invocation interface supports the

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The use cases described in this chapter exemplify the potential for innovative applications and services when they can benefit from capabilities that are abstracted from individual characteristics of specific hardware and software environments. These Grids require a flexible environment that can be directly manipulated as opposed to one that compromises the potential of the application. They require access to repositories of resources that can be gathered, integrated, and used on demand, and which can be readjusted dynamically, in real time. An essential requirement is that the control and management of these resources be decentralized, in part, because constant interactions with centralized management processes generate unacceptable performance penalties and cannot scale sufficiently. These requirements are further described in the next chapter.

For several values of interconnection material resistivity, load voltage waveforms in the time range 0 150 ps are shown in Fig 3419 while the dependences of delay time and rise time on resistivities in the range 1 500 m cm are shown in Fig 3420 For several values of driving source resistance, load voltage waveforms in the time range 0 150 ps are shown in Fig 3421 while the dependences of delay time and rise time on source resistance in the range 10 1000 are shown in Fig 3422 Load voltage waveforms for several values of load capacitance in the time range 0 150 ps are shown in Fig 3423 while the dependences of delay time and rise time on load capacitance in the range 10 2000 fF are shown in Fig 3424.

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As expected, the propagation delays in the driving interconnection increase with increases in material resistivity, load capacitance, or source resistance and vice versa Figure 3425 shows the dependences of delay time and rise time on the thickness of the GaAs substrate in the range 10 500 mm For several values of interlevel distance, that is, the distance between the top level containing the driven interconnection and the second level containing the crossing interconnections, load voltage waveforms in the time range 0 150 ps are shown in Fig 3426 while the dependences of delay time and rise time on interlevel distance in the range 01 10 mm are shown in Fig 3427 As expected, the effect of crossing lines on the propagation delays in the driven line decreases as the distance between the two levels increases.

1.5 Wavelength ( m)

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The relative effects of coupling of the driven interconnection with its two neighbors on each side on the top plane and with the crossing lines in the second level are shown by the load voltage waveforms in Fig 3428 For several values of the number of crossing lines, load voltage waveforms in the time range 0 150 ps are shown in.