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If you want to specify the file to recover, select Specify source file. FileMaker Pro opens a dialog displaying a list of files. Choose the file you want to recover. Choose Perform without dialog if you don t want the user to have the choice of which file to recover or to see the summary alert at the end of the recovery process. However, if you select Perform without dialog but do not specify a file, the Open Damaged File dialog will still open when this script step is executed because FileMaker Pro won t know which file to recover.

Excel can display values in many different formats. Later in this chapter, you see how different format options can affect the display of numerical values (see Applying Number Formatting ).

If positive integers x and y in ZN can be found so that 1 , d gcd{x 2 y, N} , N, then d is a factor of N. Pairs (x, y) can be found by random trials, hence the name Monte Carlo; accordingly, a random function f mapping the integers in ZN 2 {0} into themselves is selected. The sequence x1, x2, . . . is determined by the rule & x1 1 xi f (xi 1 ); for 2 i , n:

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7. Optional: If you want the field to be a repeating field, enter a value greater than 1 in the Number of repetitions text box, specifying the maximum number of repetitions you want the field to have. See Repeating fields, later in this chapter, for more information. 8. Optional: To set indexing or storage options for the results of the calculation, click the Storage Options button. 9. Click OK. FileMaker Pro evaluates the formula and reports any errors it detects. When the formula is syntactically correct, it returns you to the Define Database dialog. 10. You can define additional fields by repeating Steps 1 9, or you can click OK to dismiss the dialog.

The concept of phase modes finds use also in the analysis of spherical arrays [Witte et al 2003] 85 POLARIZATION For ordinary planar arrays, the radiation function can be divided into a (vector) element factor and a (scalar) array factor The radiating elements carry the polarization information Since the element part can generally not be factored out for conformal arrays, the analysis of the polarization becomes a complicated issue It is also a complicated practical design issue, since polarization control at the element level often becomes necessary The fundamental problem is well illustrated in Figure 826 for a slot array on a conical structure The slots in the figure are oriented for linear polarization in the axial direction, but they will clearly generate a depolarized pattern in other directions.

Even if the radiating elements themselves are free of cross polarization, the curvature of the antenna structure can give rise to cross polarization If the curvature varies across the array, then the cross polarization contributions from different elements will also change However, with independent control of two orthogonal radiating components at the element level it is possible to synthesize the radiation pattern for low cross polarization [Douchin and Lemorton 1997] It has been shown [Gobert and Yang 1974] that the radiation function for an arc or ring array can be written in terms of and components whose amplitudes depend on scalar expressions involving a normalized array factor and its derivatives The patterns of cylindrical, conical, and spherical arrays can, therefore, be constructed from a superposition of arc patterns However, the method leads to complicated expressions and is furthermore limited to certain canonical-element types like Hertzian dipoles.

The selector is an expression that can be used to match speci c elements within HTML documents. Its simplest form is an element s name, such as h1, which would match all h1 elements. At its most complex, the selector expression can be used to match individual sub-elements of particular elements or to specify text to include before or after matched elements.

1. On the Layers panel, click the Background layer. 2. Click the New Sublayer button. 3. Rename the new layer ShoppingCart. 4. Position the new sublayer just below the TopNav sublayer (see Figure 19.50).

Today, it appears more practical to employ direct numerical methods in the analysis 851 Polarization Definitions Polarization is defined by the direction of the radiated electric-field vector [IEEE 1993] Usually, polarization characteristics are referenced to a particular coordinate system The classical Ludwig definitions [Ludwig 1973] are shown in Figure 827 Definition 2 (Figure 827) can be applied throughout all space, with the exception of the two singular directions along the Y axis The Definition 2 is the most common.

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