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The transitions between idle mode and UTRA connected mode are illustrated in Figure 4.10. The UTRAN connected mode is entered when an RRC connection is established. The RRC connection is de ned as a PTP bidirectional connection between RRC peer entities in the UE and UTRAN. A UE has either zero or one RRC connection. The RRC connection establishment procedure can only be initiated by the UE sending an RRC connection request message to the RAN. The event is triggered either by a paging request from the network or by a request from upper layers in the UE. The establishment of an RRC connection may include cell reselection, admission control, and Layer 2 signalling link establishment. When the RRC connection is established, the UE is assigned a radio network temporary identity (RNTI) to be used as its own identity on common transport channels. The release of an RRC connection can be initiated by a request from higher layers to release the last signalling connection for the UE or by the RRC layer itself in case of RRC connection failure. In case of connection loss, the UE requests re-establishment of the RRC connection. When the RRC connection is released, the signalling link and all radio bearers between the UE and the UTRAN are released [22]. As depicted in Figure 4.10, the RRC states are (a description of the physical channels can be found in Section 4.2.5.3):

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1614 MHz, respectively, for antennas 3 and 4. For antenna 4, the center frequency is lowered by about 22% compared to that of the reference antenna. This suggests that an antenna size reduction of about 40% can be obtained by using the present design at a xed frequency. Good radiation patterns of antennas 3 and 4 have been observed. 5.8.3 With a Triangular Patch Figure 5.69 shows three promising CP designs with a tuning stub for triangular microstrip antennas. By simply loading a tuning stub of proper length at the triangular tip or at the center of the bottom edge of the triangular patch [see Figures 5.69(a) and 5.69(b)], two orthogonal near-degenerate resonant modes can easily be excited for

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Thomas, Electronic Processing of Moire Fringes: Application to Moire Topography and Comparison with Photogrammetry, Appl Opt, 18, 563 574 (1979) Post D, Developments in Moire Interferometry, Opt Eng, 21, 458 467 (1982) Post D, B Han and P Ifju, High Sensitivity Moire: Experimental Analysis for Mechanics and Materials, Springer, 1997 Powell R L and K A Stetson, Interferometric Vibration Analysis by Wavefront Reconstruction, J Opt Soc Am, 55, 1593 1598 (1965) Proll K-P, J-M Nivet, V Voland and H J Tiziani, Application of Liquid Crystal Spatial Light Modulator for Brightness Adaptation in Microscopic Topometry, Applied Optics 39, 6430 6435 (2003) Pryputniewicz R J and K A Stetson, Holographic Strain Analysis: Extension of FringeVector Method to Include Perspective, Appl Opt, 15, 725 728 (1976) Pryputniewicz R J and K A Stetson, Measurement of Vibration Patterns Using ElectroOptic Holography, Proc.

B = diag(1 A ) .

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SPIE, 1162, 456 467 (1989) Pryputniewicz R J, Speckle Metrology Techniques and their Applications, Proc SPIE, 556, 90 98 (1985) Reich C, R Ritter and J Thesing, 3D Shape Measurement of Complex Objects by Combining Photogrammetry and Fringe Projection, Optical Eng 39, 224 231 (2000) Reid G T, Moire Fringes in Metrology, Opt Lasers Eng, 5, 63 93 (1984a) Reid G T, R C Rixon, and H I Messer, Absolute and Comparative Measurements of Three Dimensional Shape by Pulse Measuring Moire Topography, Opt Laser Tech, 16, 315 319 (1984b) Righi, A, Sui Fenomeni Che si Producono colla Sovrapposizione dei Due Reticoli e sopra Alcune Lora Applicazioni: I, Nuovo Cim, 21, 203 227 (1887) Ritter R and R Hahn, Contribution to Analysis of the Re ection Grating Method, Optics Lasers Eng 4, 13 24 (1983) Robinson D W and D C.

Figure 7-15

Wiillams, Digital Phase Stepping Speckle Interferometry, Opt Commun, 57, 26 30 (1986) Rowe S H Projected Interference Fringes in Holographic Interferometry, J Opt Soc Am, 61, 1599 1603 (1971) Rowe S H and W T Welford, Surface Topography of Non-Optical Surfaces by Projected Interference Fringes, Nature, 216 (5117), 786 787 (1967)..

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Summary

FIGURE 5.52 Measured input impedance for the antenna shown in Figure 5.51; r = 4.4, h = 1.6 mm, L = 48 mm, W y = 7.2 mm ( 0.15L), and feed at point A. (a) Antenna 1: = W = 5.1 mm, L = 4.7 mm, and (x p , y p ) = (5.8, 6.6 mm); (b) antenna 2: W = 1.4 mm, L = 5.0 mm, and (x p , y p ) = (5.5, 6.5 mm). (From Ref. 16, C 1999 John Wiley & Sons, Inc.)

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convert tiff to pdf c# itextsharp

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convert tiff to pdf c# itextsharp

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