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To navigate to the next field for more text entry, you can make one of two choices: Click in the next field or press the Tab key on your keyboard. When you press the Tab key, the cursor jumps to the next field, according to an order the PDF author specified in Acrobat when the form was designed. Be certain the Hand tool is selected and a cursor appears in a field box when you press the Tab key. If you have any other tool selected, you can tab through the fields and type data in the field boxes; however, if you click with the mouse when another tool is selected, you make edits according to the active tool. When selecting from choices in radio button or check box fields, click in the radio button or check box. The display changes to show a small solid circle or check mark within a box or other kind of user-defined symbol from options you select for button/check box styles. When using a combo box, click the downpointing arrow in the field and select from one of several pull-down menu choices. List boxes are scrollable fields. Scroll to the choice you want to make using the up and down arrows.

You can use two sets of codes to define a shape. The first set, the length and direction codes, only allows you to draw straight line segments. You use this system to create specifications in the three-character hexadecimal format. n The first character is 0, which tells AutoCAD that the next two characters are hexadecimal values. n The second character is a length in units. The maximum is 15 units. The number values can range from 0 to 9. For values from 10 to 15, use A to F. Keep in mind that the length is measured along the nearest X or Y distance. Therefore, diagonal lengths are not true lengths. n The third character is a direction code. Figure 32.1 shows how this code works. Use the code that represents the desired direction of the line from the start point. FIGURE 32.1

Arthrobacter, Streptomyces Klebsiella, Bacillus Kluyveromyces, Saccharomyces Aspergillus, Penicillium

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equation, and to study the convergence and stability properties of the resulting continuous-time system by using, for example, Lyapunov stability methods. The convenience of this approach relies on the fact that the stability of differential equations is a well-studied subject (see, e.g., Bellman (1953)), and many results from this field could therefore be used in the study of adaptive filters. However, just like the averaging method of App. 24.A, the ODE approach is only applicable to infinitesimal step-sizes ( p = 0). Moreover, in his original work, Ljung (1977ab) only studied the case of timevariant step-sizes that tend to zero; a condition that hinders the tracking ability of an adaptive filter in steady-state. Extensions of the ODE method to deal with constant step-sizes were later developed by Kushner (1984) and Benveniste, Mttivier, and Priouret (1987). Briefly, the basic idea of the ODE method as applied to LMS is the following. Starting from the LMS update w z = wz-l pure( z ) ,with e ( i ) = d ( i ) - uzwz--l, iterating it over L iterations and we obtain

After you finish specifying options in the Displace dialog box, press Enter or Return to display the Open dialog box, which invites you to select the displacement map saved to disk. Only native Photoshop documents show up in the scrolling list.