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Console.WriteLine(FormatDateTime(d, DateFormat.GeneralDate)) ' Returns 5/15/2001 Console.WriteLine(FormatDateTime(d, DateFormat.LongDate)) ' Returns Tuesday, May 15, 2001 Console.WriteLine(FormatDateTime(d, DateFormat.LongTime)) ' Returns 10:30:00 AM Console.WriteLine(FormatDateTime(d, DateFormat.ShortDate)) ' Returns 5/15/2001 Console.WriteLine(FormatDateTime(d, DateFormat.ShortTime)) ' Returns 10:30

Notice that the names for the files are long and somewhat difficult to read. This would also apply for files that use sequential numbers for the file name instead of a descriptive name.

The fontsizer.js library, available for download from the Web site associated with this book, contains the scripting logic associated with this makeover. Along with fontsizer.css, copy this file into the css subfolder of your Web site. Next, to reference it in your HTML file, enter the following code in the head element:

In fully depleted SO1 MOSFET, the transconductance can be obtained from in a similar way:

As explained earlier in this chapter, RRAS installs when you set up Windows Server 2003, but you need to enable and con gure the service. The wizard offers a handful of options to help you automatically con gure the service.

Formulas (6.87) - (6.91) remain valid with the following changes:

where (5.22)

(9.32)

There are a few different settings you can play with here to help out with printer administration:

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The sequence 3, 10, 21, 36, ... consists of every other triangular number, missing out 1, 6, 15, 28, .... The sequence of numbers immediately to the left of the equality signs is 4, 12, 24, 40, .... This is just four times the triangular numbers, and the sequence of pairs sandwiching the equality signs, 4-5, 12-13, 24-25 are the same pairs met in Problem G. Taking the third line as an example, we get 212 = 25 2 - 242 + 26 2 - 23 2 + 272 - 222 or

electronics of BaBar vertex detector Nucl Instrum Methods A 377, 459 464 (1996) Berger, MJ, Hubbell, JH, Seltzer, SM, Coursey, JS and Zucker, DS, XCOM: Photon Cross Section Database (version 12), Available: http://physicsnistgov/xcom National Institute of Standards and Technology, Gaithersburg, MD (1999) Originally published as Berger, MJ and Hubbell, JH Photon Cross Sections on a Personal Computer, NBSIR 87 3597; and as Berger, MJ and Hubbell, JH, NIST X-ray and Gamma-ray Attenuation Coef cients and Cross Sections Database, NIST Standard Reference Database 8 National Institute of Standards and Technology, Gaithersburg, MD (1987) Bertuccio, G, Fasoli, L and Sampietro, M, Design criteria of low-power low-noise charge ampli ers in VLSI bipolar technology IEEE Trans Nucl Sci 44, 1708 1718 (1997) Besch, HJ, Radiation detectors in medical and biological applications Nucl.

Figure 4.17 Return loss of transformer balun for group 3 UWB system (S11, S22, S33) in simulation 3: transformer balun with two added parts.

Each item in the list has an onclick event trigger. In the highlight() function, you have a single statement that adds a class to the li tag:

Instrum Methods A 419, 202 216 (1998) Bielajew, AF, Hirayama, H, Nelson, WR and Rogers, DWO, History overview and improvements of EGS4, SLAC Report, SLAC-PUB-6499 (1994) Breibach, J, Lubelsmeyer, K, Masing, Th and Rente, C, Investigation of a bump bonding interconnect technology for GaAs pixel detectors Nucl Instrum Methods A 470, 571 575 (2001) Cederstr m, B, Danielsson, M, Lundqvist, M and Nygren, D, o High-resolution X-ray imaging using the signal time dependence on a double-sided silicon detector Nucl Instrum Methods A 423, 135 145 (1999) Chen, J, Geppert, R, Irsigler, R, Ludwig, J, P ster, J, Plotze, T, Rogalla, M, Runge, K, Schafer, F, Schmid, Th, Soldner-Rembold, S and Webel, M, Beam test of GaAs strip detectors Nucl Instrum Methods A 369, 62 62 (1996).

Par.17 Originationlndicator (one octet). This integer indicates the destinations allowed to be called by the mobile: Value 2 3 4 5 6 Meaning No originations allowed Local calls only Calls to selected area codes only Calls to selected area codes and local calls Calls to area codes of all destinations in world zone 1 (see Section 1.3.3) and local calls

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