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More recently, a package called X.Org has come onto the Linux scene. It too provides an open-source software implementation of the X Windows system, but in a much more user-friendly way. It uses a combination of scripts and utilities to attempt to automatically detect the core input and output devices on a workstation, then creates the configuration file based on its findings. X.Org is becoming increasingly popular, and many Linux distributions are starting to use it instead of the older XFree86 system. Ubuntu uses the X.Org package to produce the graphical X Windows you see for your desktop. When you install Ubuntu, it goes through a series of steps to detect the input and output devices on your workstation (see 3, Installing Ubuntu ). During the installation you may notice a time when it scans your video card and monitor for supported video modes. Sometimes this causes your monitor to go blank for a few seconds. Because there are many types of video cards and monitors out there, this process can take a little while to complete. Unfortunately, sometimes Ubuntu can t autodetect what video settings to use, especially with some of the newer, more complicated video cards. If this happens, Ubuntu reverts to a default, safe X.Org configuration. The safe configuration assumes a generic video card and monitor and usually will produce a graphical desktop, although not at the highest resolution possible on your system. If this happens in your installation, don t worry. Usually you can use the Screen Resolution utility (discussed in The Screen Resolution Utility section later in this chapter) to set the proper video mode for your setup. If all else fails, you can manually enter the settings in the X.Org configuration file.

where Tk is the noise temperature of module k. This can be referred to the input of the module by dividing it by the module gain: pnoise,k+1 kT0 B (3.7a) pn@in,k = gk or pn@in,k = kBTk . (3.7b)

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BPO has managers around the world asking what it can do for them and what it might do to them They are excited about the potential for BPO to help them manage costs and improve their balance sheets Under constant pressure from analysts to control headcount, outsourcing back-office activities to contract laborers in remote corners of the world can provide welcome and quick relief Whether the labor source is in India, Pakistan, China, or some other international port, the prevalence of high-speed Internet provides opportunities for real-time back-office support regardless of location At the same time as these new possibilities are opening up as a result of the BPO revolution, new questions are being asked and new challenges in organizational design and leadership are arising Many organizational leaders remain skeptical about BPO because of the lingering aftereffects of the tech bubble burst.

The value of Cms can be calculated from the difference Zsn between Zsn and Zsn , that is xdp Zsn = Zsn Zsn = ( jxsn ) jxsn = j ( xsn + xsn ) = j rsn + xsn . rdp Cms = 1 xdp r rsn + xsn dp (4.19)

A . .

r,=1.05

Notice, the PDF of the field intensity at the beam peak is slightly different from a Gaussian function. For I R , the PDF can be approximated as a Gaussian function with mean R and standard deviation R . Typically, that happens if becomes very small. In other situations fV V deviates from a Gaussian PDF. In Figure 14.4 we plot fV V versus V at the beam peak of an array of 20 uniformly excited elements. The standard deviation of the element amplitude, An , is assumed as 0.8 (80%) and the standard deviation of the element phase, , is assumed as 0.67 rad. We plot three different PDFs. The solid line corresponds to (14.46) and the dashed line (nondistinguishable) corresponds to (14.54). This essentially verifies the accuracy of the approximation in (14.54). The dots correspond to a standard Gaussian PDF with mean R and standard deviation R . Evidently, fV V in (14.54) is a better approximation than the Gaussian PDF. PDF for R = I We now consider another special case. We notice from Figure 14.2 that, except at bore sight and at a few other locations, R and I are very close to each other. If we assume R = I , the integral of (14.45) reduces to a closed form. Using R = I in (14.45) and with straightforward algebraic manipulation, we obtain fV V = V

is the phase delay due to the propagation inside the deposited layer. As the form of Equation (3.1.13) is the same for s and p polarizations, the subscripts are omitted in it. Re ection loss due to the surface roughness is accounted for in r in the form of a Debye Waller factor exp[ 2(2 sin / )2 ] (3.1.15)

Do not delete any of the named dimensions in a normal or revised Hole Wizard hole. SolidWorks has a checking mechanism that looks for these names, and it will display an error if the named dimension is not there. If there is no use for the dimension, it still has to be there, although it does not need to be used for its original use. You could rename another dimension with the name or simply dimension the centerline or an otherwise unused construction line. It does not matter about the function of the dimension, as long as there is a dimension with that name in the sketch. You should also name any new dimensions that you may want to change. These dimensions will have more meaning when you are placing the feature if they have names.

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