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The Sheet Set Manager has three tabs: Sheet List contains the sheets that you create for the sheet set. You use this tab to manage and organize the sheet set. You can set properties for the sheet set, for subsets (categories), and for individual sheets. You can use this tab to add and remove sheets, and to import a layout from another drawing as a sheet. You can also use it to plot, publish, eTransmit, or archive an entire sheet set or a selection of sheets, to rename and renumber sheets, and to close the sheet set. You can also open any sheet, which is the same as opening the drawing. Figure 26-19 shows the Sheet List tab. Sheet Views contains a list of paper space views, which are viewports on a layout. A layout can have more than one viewport. You can create view categories, such as elevation and floor plan. You can display the view from this tab. You also use this tab to rename and renumber your views within a layout, as well as to place label blocks that label a view and callout blocks that reference other views. See Figure 26-20 on the left. Model Views lists the drawings that are the source of your sheets, as well as their model space views, as shown in Figure 26-20 on the right.

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Fig. 13.3 Flow regimes This allows the local superficial gas velocity and a local void fraction be used to describe the local flow pattern. The flow regime map is shown on Fig. 13.4 for these co-ordinates and has been constructed from the main flow regimes that were observed during experimental tests, (3). To model the conditions in the annulus, four flow regimes were believed to have a dominant effect; mist flows, churn flows, thin film flows, and thick film flows. The regions in which these regimes are believed to exist are shown on Fig. 13.4. Region A and B are parts of the flow map that are not expected to be encountered. To ensure that the calculations will not fail due to the lack of closure laws, Region A defaults to the mist regime and Region B defaults to the chum regime if the solution falls in these regions. The mist flow regime accounts for all the dispersed flows that might occur during the flooding process and at this stage in the modelling process also accounts for regimes where the liquid may be partly wall based, i.e. film-mist type flows. The modelled churn flow regime describes a chaotic flow pattern observed in the annulus but only describes the conditions where a co-current flow of liquid and gas is expected. The modelled film flow regimes actually accounts for observed liquid film flows but also accounts for churn flows

0, the discriminant is non(C.10)

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FIGURE 5.8 Measured radiation patterns for the antennas studied in Figure 5.6. (a) Antenna 1 at 1916 MHz, (b) antenna 2 at 1880 MHz, (c) antenna 3 at 1768 MHz. (From Ref. 3, C 1999 IEEE, reprinted with permission.)

The reference tristimulus values are then transformed to tristimulus values for the second viewing condition using Equation 13.24 with an A matrix calculated for the second viewing conditions. X X ref Y = (RAM) 1 Yref Z Z ref

By clicking the arrow to the left of the tag you can see the details of the object, as shown in Figure 3-10. When you re designing in Layout view you can see the HTML code behind your page without having to read between all the HTML code. But this is still a bunch of HTML tags. So, how does it really help if you don t already know the tags Say, for example, you want to understand the code that renders a table. You ve looked into source code but all those <td> and <tr> tags are confusing. While in Layout mode, because you want to know the exact tag for the actual table, select the entire table. Then, with the table selected, switch to Outline. As demonstrated in Figure 3-11, the actual table tag stands out. For one thing, it s selected by a black box around it, and for another, the attributes of the table are visible. You know they re a part of the table tag because they appear indented, like any subsection of a heading does in any outline.

Time 1:30 2:30 3:45 1:30 2:15 3:30 2:00 3:30

7. Stimulated Brillouin Scattering Pulse Compression and Its Application in Lasers G. A. Pasmanik, E. I. Shklovsky, and A. A. Shilov 7.1 7.2 7.3 7.4 7.5 7.6 7.7 7.8 Introduction Phenomenological Description of Brillouin Compression Theoretical Analysis of Brillouin Pulse Compression Numerical Simulation Characterization of Materials Used for SBS Compressors Experimental Study of Brillouin Pulse Compression Application of SBS Pulse Compression to Diode-Pumped Solid-State Lasers with High Pulse Repetition Rate Conclusion References