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The feed position is chosen at point A for right-hand CP radiation It is seen that, when the tuning stub is at the bottom edge, the required tuning-stub length (about 03 times the patch s side length) for CP radiation is much larger than that in the design with the tuning stub at the triangle tip This suggests that the effect of the tuning-stub loading is more prominent at the triangle tip than at the bottom edge 5833 Design with a Tuning Stub and a Cross-Slot of Equal Slot Lengths [Figure 569(c)] Compact CP design with three different cross-slot sizes (antennas C1 C3) has been studied The obtained CP performance is listed in Table 518 It is observed that the CP center frequency decreases with increasing cross-slot length.

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because the ends of the string cannot be displaced. De ne as the function that describes the displacement at any point along the wave; the solutions to the wave equation, , are called the wave functions. It follows, by de nition, that the waves that are generated by plucking such string constrained at both ends can be described by solving the wave equation for . The classical mechanics wave equation in three dimensions is [453] 2 (x, y, z) where 2 is the Laplacian operator: 2 2 x2 2 y2 2 z2 (2 / )2 (x, y, z) (D.1)

For antenna C3, the center frequency is lowered to 1708 MHz, which is about 88% times that (1937 MHz) of the regular-size CP design (antenna A2) This lowering of the center frequency corresponds to an antenna size reduction of about 22% using.

Vgd sin cos Vgs (3.84)

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P1: KOA WY050-02 WY050-Ulick-v4 September 19, 2004 10:56

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For typical designs in the E = 10 GeV range, U, is in the neighborhood of 10 MeV. To allow for straight sections, let s put p / R : Then w, = 19 keV, . that is, in the hard x-ray part of the spectrum. Let 0 = 0 (separated function lattice). If the dispersion function is on the order of 2 m and the amplitude function is on the order of 40 m in the bending regions, then ( Z )= (2 mI2/40 m = 0.10 m. So the equilibrium emittance and energy spread for our example would be E , = 2500 mm mrad and u E / E = 0.8 X The contribution to the horizontal beam size from the transverse emittance , = would be u = (pX~X/y)l/z 2.2 mm. The total horizontal beam size is u = ( p , ~ , / y D 2 z / E 2 ) 1 / 2 2.7 mm. u = Our idealized results imply that the vertical beam size is zero. In reality, some portion of the transverse emittance will be coupled into the vertical degree of freedom, as will some small part of the horizontal dispersion. Though the vertical beam size will not be zero, for a corrected lattice it will be an order of magnitude or more smaller than the horizontal beam size. As a result, the words ribbon beam are often applied to describe the transverse bunch cross section.

3 explained basic concepts of relational databases such as tables, tuples, rows, and columns. (If you don t remember 3, go back and skim through it quickly to refresh your memory.) Converting semantic object models and ER diagrams into a relational version isn t too dif cult once you know how the concepts described in 3 map to those described so far in this chapter. The following table shows the how key terms from 3 map to the terms used in semantic object models and ER diagrams. Theory Relation Tuple Attribute Database Table Row Column File File Record Field SOM Class Object Attribute ER Entity Set Entity Attribute

Figure 6-1 A network operation center (NOC) is used to resolve problems or escalate them to the appropriate personnel.

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