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In a simple telephone system, the voice signal is transmitted in its original baseband form, over copper wires, from transmitter to receiver. Such a case does not involve modulation. If, however, the same voice signal is to be transmitted by wireless, then some kind of modulation of a high-frequency carrier wave is required. Regardless of the type of modulation used, the result is always the production of a band of side-band frequencies, clustered symmetrically about the carrier. Since the original signal information is contained in this band of frequencies, it s desirable that the entire band be passed through circuits having a reasonably good band-pass characteristic, such as is illustrated in Fig. 240.

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your menus and navigation features; no matter how attractive and easy-to-use you believe your GUI to be, you ll still have points deducted if you don t follow standard conventions.

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Menus are a powerful (and necessary) part of almost all GUIs. We focus our attention on the most common implementation of menus, the menu bar. An application s main menu bar is almost always located at the top of the display sometimes directly under an application s title bar, and sometimes separate from the application s main window and docked to the top of the display. You re familiar with the standard menu bar. Several of its more consistent entries are typically located toward the left end of the bar and include File, Edit, and View. Each entry in the menu bar represents a collection of related capabilities. Clicking on one of the entries on the menu bar will cause a specially formatted widget (a menu) that resembles a list widget to appear beneath the menu bar entry. The entries

First, by note 6:

in these lists each represent a system capability. The most common capabilities available through menu entries are

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Fourth-order lter schematic and impedance response. CDAMPRDAMPMaximum 4.20000e-005 4.20000e-005 4.20000e-005 4.20000e-005 4.20000e-005 4.20000e-005 4.20000e-005 4.20000e-005 4.20000e-005 4.20000e-005 4.20000e-005 4.20000e-005 5.60000e-005 5.60000e-005 5.60000e-005 5.60000e-005 5.60000e-005 5.60000e-005 5.60000e-005 5.60000e-005 5.60000e-005 5.60000e-005 8.00000e-001 1.00000e+000 1.20000e+000 1.40000e+000 1.60000e+000 1.80000e+000 2.00000e+000 2.20000e+000 2.40000e+000 2.60000e+000 2.80000e+000 3.00000e+000 8.00000e-001 1.00000e+000 1.20000e+000 1.40000e+000 1.60000e+000 1.80000e+000 2.00000e+000 2.20000e+000 2.40000e+000 2.60000e+000 2.507 2.215 2.027 2.024 2.083 2.133 2.285 2.458 2.627 2.791 2.950 3.103 1.799 1.716 1.659 1.727 1.820 1.979 2.158 2.334 2.505 2.670

A navigational command such as Close (close the current document),

Trigonometric Identity for (sin x sin y)

Print (move to the Print display to initiate a print session), or Exit (end the application)

In the above equation, replace y with y; then, since (section 5.3) cos y cos y and sin y sin y, eq. (I) becomes cos x y cos x cos y sin x sin y hence cos x y cos x cos y sin x sin y Lastly, addition of eqs. (I) and (II) gives the identity we are after, thus sin x sin y 1 cos x y cos x y 2 II

An action command such as Spell Check (invoke the built in spell checker)

or Copy (copy the currently highlighted data to the clipboard)

23 24 25 26 27 28 29 30 31 32 33 34 35 36

Consider a coil of TWO TURNS in which each turn, considered by itself, has L henrys of inductance. If there were NO COUPLING WHATEVER between the two turns the total inductance Lt would simply be the sum of the inductances of the individual turns; thus If, however, some amount of coupling does exist between the two turns, then, as we found in problem 198, the total inductance would be equal to Lt L L 2M or, by eq. (371) Lt L L 2kL Hence, for the ideal case in which there is COMPLETE COUPLING between the two turns (k 1), eq. (16-A) becomes Lt L L 2L 17-A

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