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utoCAD and AutoCAD LT offer many ways to integrate your drawings with the Internet. You can open drawings from a Web site, hyperlink objects to anywhere on the Web, and publish drawings in DWF format on a Web site. When you access a Web site (perhaps your company s intranet), you can find blocks or other data, and drag them into your drawing. This chapter covers all of the ways to connect your drawings with the Internet. You can share your 3D drawings in the 3D DWF format. The DWF format is not only for use on the Internet; your colleagues can also view your DWF files using the Autodesk DWF viewer.



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hree different cadres deserve recognition for their parts in this book:

First, look at each report you ve roughed out for your database. For the CollectibleMiniCars database, start with the customer data and list the data items, as shown in Table 33-1. As you can see by comparing the type of customer information needed for each report, there are many common elds. Most of the customer data elds are found in both reports. Table 33-1 shows only some of the elds that are used in each report those related to customer information. Because the related row and the eld names are the same, you can easily make sure that you have all the data items. Although locating items easily is not critical for this small database, it becomes very important when you have to deal with large tables containing many elds.

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Return Loss (dB)

(3.10)

2 k!1

the edge yields the edge spread function of the system. To compute the line spread function of the system, it is only necessary to take the rst derivative of the edge spread function. Figure 2.5C depicts the experimental setup to obtain the edge spread function. 2.5.1.4 Modulation Transfer Function (MTF) Now substitute the edge phantom with a high-contrast line pair phantom with different spatial frequencies, and repeat the preceding experiment. In the image receptor, an image of the line pair phantom will form. From this image, the output amplitude (or gray level) of each spatial frequency can be measured. The modulation transfer function (MTF) of the imaging system, along a line perpendicular to the line pairs, is de ned as the ratio between the output amplitude and the input amplitude expressed as a function of spatial frequency MTF(u) = Output amplitude Input amplitude (2.9)

Lk (t) dt + Rm (tn+1 ),

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back to the laser diode array From an experimental and practical point of view, this con guration is attractive since a large fraction of the radiated energy can be extracted from the laser system As the re ectivity of the PCM is built up, the output far- eld lobe grows at the expense of the injection lobe To achieve single-lobe operation, it is often necessary to open the spatial lter slightly so that more energy will reach the PCM in order to start the self-pumped conjugator After a few minutes the distance between the two razor blades can then be diminished again Figure 96a shows the far eld of the laser array when it runs freely at a drive current of 2ith Figures 96b and 96c display the far eld for a drive current of 2ith and 3ith, respectively, when the FSPCF is applied.

In the plane perpendicular to the junction the far eld is close to the diffraction limit and has a Gaussian shape that is unaffected by the number of oscillating spatial array modes It is the lobe at the negative angles (the injection lobe) that is fed back to the laser diode array The peak of the output lobe is centered at 238 and 228 for 2ith and 3ith, respectively The most ef cient performance of the system always takes place with an emission around 238 The edges of the two razor blades that form the spatial lter are positioned at 2198 and 2258 The FWHM of the output beam is measured to 0758 at 2ith and 0928 at ith, corresponding to 14 and 17 times the diffraction limit, respectively.

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The total power radiated from the laser diode array is increased by approximately 5% with the phase conjugate feedback compared with the power of the freely running laser diode array..

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