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2 is the capability to mark objects as being potential candidates for garbage collection while still referencing them These so-called weak references complicate the garbage-collection process and are not supported by the CLDC..

2 presents both mode sets (Am and Cm) for the circular array pattern of Figure 101 (b) The next step is to find the element excitation V( ) expressed in the near field (excitation) modes according to Equation (104) Sampling the continuous excitation V( ) at the element positions n gives the element excitation values [Figure 103 (a)] Has the discrete excitation we found solved the problem From 2 we know that additional spurious modes are generated (distortion terms) and we have to make sure that they are sufficiently attenuated We notice from Figure 103 (b) that the pattern computed from the discrete element excitation has an increased side lobe level compared to the design goal of 25 dB, possibly due to spurious effects Let us take a closer look at the relevant design criteria.

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Dreamweaver enjoys a tight integration with its sister graphics program, Adobe Fireworks. To empower Dreamweaver with Fireworks capabilities, such as Launch and Edit, Dreamweaver has to know where Fireworks is installed. If you install Studio 8, the path to Fireworks is prefilled for you and shown in this option. If you install Fireworks separately, you ll need to click Browse and locate the Fireworks executable.

You can readjust the 3D components that you inserted into the imported block/components. When you enter the component instance, you can delete the inserted 3D component and exchange it with a different version. Because the elements within the model can be edited easily, SketchUp is very versatile; this versatility can be utilized to convey design intent (Fig. 19-28 through Fig. 19-31).

First of all, the number of modes used (we had nine) must be less than or equal to the number of elements (we had ten) in order to avoid aliasing of the phase-mode spectrum (cf Table 21) Second, in order to radiate the useful unambiguous mode spectrum the number of phase modes must be less than about 2kR (cf Figure 212) A commonly stated limit is 2kR + 1 [Taylor 1952]; in our case we had 2kR + 1 = 9 With 11 elements instead of 10, we would get 2kR + 1 = 98, which is more on the safe side Using this number, we get the pattern shown in Figure 104 Now we have obtained a result that is very close to the ideal Chebyshev pattern However, this is a narrowband solution since kR cannot be allowed to vary much.