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Type edge on the command line. At the Specify edge of 3dface to toggle visibility or [Display]: prompt, select a visible edge that you want to make invisible. AutoCAD repeats the prompt so that you can select additional edges. Press Enter to make the edges invisible. Although a visible edge might actually be two edges belonging to two adjacent 3D faces, EDGE makes them both invisible. To make invisible edges visible, choose the Display option. AutoCAD displays all the edges in dashed lines and shows the Enter selection method for display of hidden edges [Select/All] <All>: prompt. Press Enter to display all the edges or use the Select option to select 3D faces (you can use windows for selection). Either way, you see the edges of the 3D face that you want to edit. AutoCAD then repeats the Specify edge of 3dface to toggle visibility or [Display]: prompt. You can now select the edge that you want to make visible. Press Enter to end the command and make the edge visible.

As you saw in 3, home routers operate as both a DHCP client and as a DHCP server. The router may also act as a DNS server for the PCs on the LAN. Figure 9-1 shows how the router, client PCs, and your ISP work together to provide DHCP and DNS services for the client PCs on your LAN. Here s the explanation for the steps shown in Figure 9-1. 1. When your router first powers up, it sends a DHCP request to the ISP. 2. The DHCP server at the ISP responds to the request, sending back an IP address, the address of the gateway router at the ISP, and the address of one or more DNS servers. The router assigns the IP address to the router s WAN interface, and it stores the gateway and DNS server addresses in its memory.

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Figure 12-13: Donny Valiante, the drummer from Midnight Sun Music, in a project using the Chroma Key Type

FIGURE 10.6 This birthday party photo from the 1960s was quickly color balanced with one click. With the Gray Point eyedropper on the Levels command, I clicked the blade of the saw the boy (me) is holding, neutralizing any colorcasts in the gray blade and the rest of the photo.

since they are independent. The observation vector x is a linear function of s, so that its probability density function is given in terms of W = H 1 by pX (x; W , r) = det |W | r(W x). (10.8)

Equation (9.38) indicates aliasing of spectral components separated by the range cN/2Z Ndl. Aliasing is unlikely to be an issue for the continuous scan integrate approach, however, because the spectrum is lowpass- ltered by the sampling function. Typically, we assume that ^(n) sinc(Dt n), meaning that terms in the series p are substantially attenuated for jn0 n00 Nj . N=2. Since we are exclusively interested in values of Sn for positive n, this means that we obtain on the order of one spectral value for every two samples (although samples near the band edge will be severely attenuated). In practice, sampling at the rate of vDt lmax/4 may be advisable. With the multiplex spectrometer, the spectral values nc/2Z span the range from DC (n 0) to nmax . In practice, of course, DC values are not part of the optical spectrum. If we consider an instrument spanning the range from l 2 20 mm, then 90% of the spectral range from DC to lmax contains useful information. On the other hand, an instrument in the visible spanning the range l 500 700 nm must collect over six measurements per data value. This potential sampling inef ciency puts interferometric systems at a disadvantage to dispersive systems in using detector P arrays. Substituting Eqn. (9.38) in Eqn. (9.31) and assuming that G(0) n Sn , the measurement model for an FT spectrometer becomes ! N=2 1X nn0 gn Sn0 1 cos 2p 2 n0 0 N

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