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7. Choose Last Break on the Debug toolbar to jump to the error in the source code. 8. To place a break point in the code, place the cursor after (princ (chr 40)). Press F9. Visual LISP marks the break with a red box. 9. Place another break point after (princ (car aList)). Finally, place a third break point after the closing parenthesis on the line that follows (princ item 1). Your code should look like Figure 36-3. 10. After the code produces an error, you need to reset. Click Reset on the Debug toolbar. 11. Click the Visual LISP Editor window and reload the function into Visual LISP. (Choose Load Active Edit Window on the Tools toolbar.) 12. Type the same expression that produced the error in the Console:

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java oracle.xml.xsql.XSQLCommandLine file:///java/xsql/newsletter.xsql xml-stylesheet=file:///java/xsql/newsletter.xsl email=test2@momnpup.com | mail -t test2@momnpup.com -s Newsletter

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In most cases changes in spectra as a result of environmental effects are obvious on inspection. It is also possible to plot a difference spectrum which may be obtained by subtracting one spectrum (A) from the other (B), that is A B or A A A B versus wavelength or frequency (Figure 3.15). This facilitates identi cation of wavelengths

10 20

The rest of Section 2.4 is loosely based on references [19] and [26].

The makefile([mode[, bufsize]]) method returns a file-like object wrapping this socket, so that you can then pass it to code that expects a file argument (or maybe you prefer to use file methods instead of send and recv). The optional mode and bufsize parameters take the same values as the built-in open function.

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1. Open ab24-g.dwg from the CD-ROM. 2. Save the file as ab24-10.dwg in your AutoCAD Bible folder. You see a bushing, in 2D and 3D, as shown in Figure 24-32. The 3D bushing has been exploded into simple geometry otherwise, you wouldn t be able to use it to extend the 2D lines.

To flush the cache manually, type the following at the command prompt:

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In the following guide we'll create a local report ( RDLC file) which features barcoding capabilities by using Bytescout Barcode SDK. Follow these steps:.

You cannot place a grid next to a table. That is, you can t do so directly on a page. But you can achieve a similar effect by placing a grid within any cell in a table. You cannot start a line with text, and then add a grid to that line, or type text after a grid on the same line. However, no reason really exists for wanting to do this because you can put your text on the grid instead, and gain full control over its placement. However, you can do one of the following with grids: Place one grid beneath another. You might do this if some of your material spans the entire width of a page (or much of it) and other material above or below only spans a narrow area. You might also do this if some material needs to be on one side while other stuff should be on the other. In that case, one grid can be left-aligned and the other right-aligned. Place a grid within a table cell. The common scenario for this is when certain graphics (such as buttons) need to remain tightly grouped. Those graphics are placed in one table cell, while the grid is placed in another cell, enabling items to be freely placed within the gridded cell s area. For example, you might create a two-column table with no visible borders and then place a navigation bar in the left column and a grid in the right. Figure 7-1 shows an example of this. (You can also find the live version of Figure 7-1 at www.golivebible.com.)

An effective, and somewhat clever, method of determining the fraction of thermal neutrons in a beam is to take advantage of the high neutron absorption property of cadmium. As shown in Figure 14-1, cadmium effectively removes all neutrons of energy below about 0.4 eV and is completely transparent to neutrons above about 1 eV. If a foil such as indium or gold is irradiated bare and an identical one is wrapped in a cadmium foil 0.1 0.2 in thick and irradiated under the same conditions, the activity of each is a measure of the number of thermal and fast neutrons in the beam. The activity of the bare foil is due to thermal plus fast neutrons while the activity of the cadmium-covered foil is due only to fast neutrons since essentially all the thermal neutrons will be absorbed by the cadmium. The ratio of thermal to fast neutrons is given by the cadmium ratio:

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