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surements. In Figure 6.59, the normalized E- and H-plane patterns are shown for the experimental antenna shown in Figure 6.46. The result is for the element located in the center of the array calculated at f = 5.4 GHz. As shown, the agreement between theory and measurements is quite good both in the E and the H planes. The small differences that can be observed in the E plane around = 20 is due to the air gap in the measurements, as has been verified in [Sipus and Kildal 2003]. In [Thors et al. 2003], it was shown that the corresponding E-plane radiation pattern for an isolated element in this array is very broad. However, when the element is placed in an array environment, the radiation pattern is changed considerably due to the mutual coupling. The oscillations in the theoretical H-plane results are a consequence of interference between rays creeping around the cylinder. These oscillations are not observed in the measurement since the experimental antenna was truncated in the azimuthal direction, as shown in Figure 6.46. As shown in Figure 6.59 (a), the E-plane embedded-element pattern is very oscillatory. The origin of the ripples can be attributed to the mutual coupling and the rather large 0.67 at f = 5.4 GHz). azimuthal element spacing in the experimental antenna (R This was discussed in Section 6.2.4. The most practical way to avoid the problem is to reduce the element spacing. Similar oscillations are not observed in Figure 6.59 (b). This can be understood by realizing that the H-plane coupling is much weaker than the E-plane coupling.

Figure 11-27 Regimes of gas liquid mass transfer with reaction. (From Middleton, 1997; reproduced by permission of Butterworth-Heinemann.)

Performance of Computer Communication Systems: A Model-Based Approach. Boudewijn R. Haverkort Copyright 1998 John Wiley & Sons Ltd ISBNs: 0-471-97228-2 (Hardback); 0-470-84192-3 (Electronic)

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100 ; -- r ed position <= ball-x-reg + x-delta-reg when refr-tick= l e l s e ball-x-reg ; ball-y-next <= ball-y-reg + y-delta-reg when refr-tick= l e l s e ball-y-reg ; -- new b a l l v e l o c i t y p r o c e s s (x-delta-reg , y-delta-reg , ball-y-t , ball-x-1 , ball-x-r , ball-y-t,ball-y-b,bar-y-t,bar-y-b) begin x-delta-next < = x-delta-reg; y-delta-next <= y-delta-reg ; i f ball-y-t < 1 t h e n -- r e a c h t o p y-delta-next <= BALL-V-P ; e l s i f ball-y-b > (MAX-Y-1) t h e n -- r e a c h b o t t o m y-delta-next <= BALL-V-N; e l s i f ball-x-1 <= WALL-X-R t h e n -- r e a c h w a l l x-delta-next < = BALL-V-P ; -- b o u n c e b a c k e l s i f (BAR-X-L<=ball-x-r) and (ball-x-r <=BAR-X-R) t h e n __ r e a c h x o f r i g h t b a r i f (bar-y-t <=ball-y-b) and (ball-y-t <=bar-y-b) t h e n x-delta-next < = BALL-V-N ; --hit , b o u n c e bac k end i f ; end i f ; end p r o c e s s ;

A combination corner point is a point where a curved segment and a straight segment meet each other. At this corner point, there s one control handle coming from the anchor point from the side where the curved segment is located, and on the other side, there s no control handle, indicating a straight segment. To create a combination corner point with the Pen tool, draw a few curved segments and then go back to the last anchor point. You should see two linked control handles displayed at this point. Simply click once on the anchor point, and one of the two control handles disappears. The next segment then starts out straight.

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