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Frames can be tricky to print. It s hard, if not impossible, to ensure that your entire frameset will print when the user chooses the print command. If a user clicks within a frame, that may well be the frame that prints. Users may end up with a printout of your navigation bar, rather than the information desired, or else your information may print, but without your site s identification. There s no way to force the entire frameset to print. If you intend for your site s content to be printed, you will have to either create printready pages that open outside of the frameset, or create a PDF (Adobe Acrobat) file and then link to that for viewing or download. On the other hand, if your site doesn t really provide material that lends itself to being printed, you may not share this concern. Just in case, though, check that the files are print-presentable.

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In the above gain loss expression, the frequency-independent element pattern is assumed. In Figure 1.15 we have plotted the gain loss versus scan angle for a 20-element linear array with element spacing of 1 0 . We used frequency deviations of 3 and 5%, respectively, above the center frequency. Expectedly, the more the frequency deviation, the more is the beam deviation and subsequent gain loss. Also, the gain loss increases with increasing array size. The gain loss limits the bandwidth of a scan beam array. For N > 7, the 3-dB-gain-loss bandwidth can be shown to be 2 f 0 88 f0 L sin

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SYMMETRY AND STRUCTURAL PARAMETERS Structural parameters (bond lengths, bond angles, dihedral angles) must be the same in a molecule when they are interconvertible by a symmetry operation, that is, congruent. Conversely, structural parameters cannot be the same in a molecule when they are not congruent. If the structural parameters are not congruent, it is not possible to use symmetry arguments to predict the magnitude of the di erence. Some relationships between the bond lengths and angles of nominally tetrahedral molecules are shown below. The notation a and b denote groups which are di erent in some way. The point groups shown denote the molecular point group. For the relationships to hold exactly, the structures of a and b must be such as to preserve the overall symmetry. The relationships may be approximately obeyed if the denoted point groups are a fair representation of the local symmetry. For example, the rst structure will have exactly Td symmetry if a is H, Cl, or Me but not if a is Et, since the ethyl group does not have a threefold axis of symmetry. Equation (1.1) de nes the tetrahedral angle. Equation (1.2) may be handy for relating the internal bond angle of a threefold symmetric species, such as ammonia, to the out-of-plane angle of the bonds. Equation (1.3) applies to molecules like methylene chloride (CH2 Cl2 ) or cyclopropane.

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15 10 5 0 Gain, dBi 5 10 15 20 25 0 10 20 30 40 , deg (b) 50 60 70 80 90 Cross-pol, D-plane a1 = b1 = 0.55 0 a2 = b2 = 1.49 0 a = b = 1.5 0, square grid Length = 2.0 0

Our philosophy of PACS design and implementation is that regardless of the scale of the PACS being planned, we should always leave room for future expansion, including integration with the enterprise PACS and ePR with image distribution. Thus, if the planning objective is to have a large-scale PACS now, the PACS architecture should allow for its future growth to an enterprise PACS with ePR image distribution features. On the other hand, if only a PACS module is being planned, consideration of the connectivity and compatibility of this module with future modules or a larger scale PACS is essential. The terms we discussed in previous chapters, namely open architecture, connectivity, standardization, portability, modularity, and IHE work ow pro les, should be included in the PACS design. 18.1.1 Cost Analysis

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