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where the channel s frequency-domain transfer functionH ( f ) is the Fourier transform the of impulse response h ( t ) :



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Xunming describes two components of working hard: working smart and pooling resources to achieve a vision His company is pursuing a solar niche Its thin- lm sheets are meant not for homes but for factories and retail centers They will carpet large, at roofs that cannot sustain the weight of traditional glass solar panels, as most houses can Xunming, Xunlight s president and CEO, and Liwei, its vice president of nance and administration, initially expect to export most of their product to Europe, until solar energy takes hold in America They envision manufacturing more than $200 million worth of solar cells each year That will require more physicists and chemists, but also traditional business people and rank-and- le factory workers They also plan to stay in Toledo, and not only because their daughter likes her high school.





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Y ( t + At) - & ( Y ( tt) A t ) = O(Atp+'). ,,

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Calculated controls are based on expressions, such as functions or calculations. Calculated controls are unbound because they don t directly update table elds. An example of a calculated control is =[SalePrice] - [Cost]. This control calculates the total of two table elds for display on a form but is not bound to any table eld. The value of an unbound calculated control may be referenced by other controls on the form or used in an expression in another control on the form or in VBA in the form s module.

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If you want to create your own custom preset, you copy an existing preset, modify the settings, and save it as a new preset. Because modifying a video processing filter is covered in 10, this example uses a factory preset for preprocessing, but shows you how to modify an encoding preset. As per preceding examples, we ll encode a 300 kbps file, with 32 kbps audio. We ll target MPEG-4 this time:

=DATE(YEAR(TODAY()),7,4)

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7.2.2.2 Array Mutual Coupling. Unfortunately, doubly curved arrays are not as symmetrical as singly curved surfaces. Thus, the analysis of doubly curved arrays is more time-consuming than singly curved arrays. Often, an element-by-element approach is needed and all combinations of element locations must be calculated. For example, about 500 apertures are required to fully cover the experimental antenna with elements (14 rings and 0.75 element spacings in a triangular lattice); see Section 8.5.3.1 and Figure 8.33. Here, we will limit ourselves to the array mutual coupling along the principal y axis of the experimental antenna (Figure 7.1). All results presented are measured at the frequency f = 8.975 GHz. Several cases are included with different positions of the source along the y axis. During the measurements, the elements along the principal axis were terminated in matched loads (Figure 7.19), except the two between which the coupling was measured. The elements away from the y axis were all covered with metallic tape [Lanne and Josefsson 2002]. Both E- and H-plane array couplings are considered. For each polarization, three sets of measurements were made. The first set is when element y11 is fed and the array coupling is measured to the elements away from this element in the positive y axis direction. This set is named Case A for E-plane coupling and Case B for H-plane coupling. In the next set, element y6 is fed instead and this set is called Case C for Eplane coupling and Case D for H-plane coupling. Finally, the element at the vertex is fed and the array coupling is measured along the positive y axis. This set is called Case E for E-plane coupling and Case F for H-plane coupling. The results are shown versus

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