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4 May 2013 ... Please try this project: http://www.codeproject.com/Articles/5887/Generate- Thumbnail - Images -from- PDF -Documents. The related key code ... As an alternative, if you have these packages available on CD-ROM, you can type the following commands to identify the location of the packages and install them from that location: An active star architecture (also known as a double star) reduces the total ber deployed, and hence lowers costs through feeder ber sharing In the active star, a remote node is deployed between the CO and the subscriber s premises Each OLT port and the feeder ber between the CO and the remote node is shared by anywhere from four7 to a thousand8 homes (the split ratio) via dedicated distribution links from the remote node [1], see Figure 85 The remote node in the active star network can be either a multiplexer or switch The remote node switches signals in the electrical domain, and hence OEO conversions are necessary at the remote node [1] Since the feeder bandwidth is shared among multiple end points, the maximum sustained capacity available to each home both upstream and downstream is typically less with an active star architecture than with home run ber . . . . . . . . . . . . 132 133 In the previous section, following the geometric approach used by Craig to obtain the form of Q(x) given in (4.2), we derived a representation of the two-dimensional joint Gaussian Q-function [see (4.7)] which has similar desirable properties; however, the integrand is not purely exponential in the integration variable, and furthermore the argument of the exponential in the integrand is not as simple as in (4.2). Applying a clever transformation to (4.2), Simon [26] was able to arrive at a simpler form for Q(x1 , y1 ; ) that dispenses with the trigonometric factor that precedes the exponentials in its integrands and furthermore results in an exponential argument that is precisely in the same simple form as that in the Craig representation of Q(x) of (4.2). As such, the entire dependence of Q(x1 , y1 ; ) on now appears only in the limits of integration. We now present a brief summary of the results in Ref. 26. Consider applying to the integrals in (4.7) the change of variables = tan 1 It can easily be shown that d = 1 2 d 1 sin 2 (4.11) tan (4.10) 833 Passive star (passive optical network PON) c# pdf to image pdfsharp Convert PDF Page to Image in C# - E-Iceblue
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