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If your original shape and/or the extruded portion uses spot colors, the Use Full Color Range option might help you get where you want to go. Deselecting it has the effect of limiting the color variations caused by light sources to only those percentages of the spot colors defined in both your original object and its extruded portion. Unfortunately, deselecting this option limits color depth and diminishes the effects of the lighting you apply, but it results in a print-legal spot color tint, as opposed to the normal color space of RGB that you see onscreen. This means that if your objects are filled with spot color, you should consider unchecking the Use Full Color Range check box.
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Double-click to return the Color Palette to its default docked location Click-drag to move Close Palette
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The method of using Riemann sums to approximate an integral is sometimes called the method of rectangles. It is adequate, but it does not converge very quickly and it begs more ef cient methods. In this subsection we consider the method of approximating by trapezoids. Let f be a continuous function on an interval [a, b] and consider a partition P = {x0 , x1 , . . . , xk } of the interval. As usual, we take x0 = a and xk = b. We also assume that the partition is uniform.
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The MonthNumberOfYear function takes a date input_parameter and returns the number of the month (1 12) for that date.
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A distinction needs to be made between physical and logical topologies. A physical topology describes how components are physically cabled together. For instance, 10BaseT has a physical star topology and FDDI has a physical dual ring topology. A logical topology describes how components communicate across the physical topology. The physical and logical topologies are independent of each other. For example, any variety of Ethernet uses a logical bus topology when components communicate, regardless of the physical layout of the cabling. This means that in Ethernet, you might be using 10BaseT with a physical star topology to connect components together; however, these components are using a logical bus topology to communicate. Token Ring is another good example of a communication protocol that has a different physical topology from its logical one. Physically, Token Ring uses a star topology, similar to 10BaseT Ethernet. Logically, however, Token Ring components use a ring topology to communicate between devices. This can create confusion when you are trying to determine how components are connected together and how they communicate. FDDI, on the other hand, is straightforward. FDDI s physical and logical Be able to match up the topologies are the same: a ring. Table 1-2 shows topologies used in Table 1-2 to a given common media types and their physical and media type. logical topologies.
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Regional geologic and tectonic history needs to be reviewed. Interaction between earth structures and bridges needs to be considered. Selecting deep versus shallow foundations for seismic resistance: Deep foundations and those well anchored into the soil are more stable against seismic forces than shallow foundations.
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Except for new, delete, >, >*, and the comma operators, the other C++ operators are overloaded in the same way as those shown in the preceding examples. Overloading new and delete requires special techniques, a complete description of which is found in 17, where exception handling is discussed. The >, >*, and comma are specialty operators that are beyond the scope of this book. The interested reader is directed to my book, C++: The Complete Reference (McGraw-Hill/Osborne), for additional examples of operator overloading.
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The Main Word Lists are predefined by Corel and cannot be edited by CorelDRAW. However, they can be edited by the WordPerfect suite s Spell Utility if you happen to have a copy. Main Word Lists contain only words used by the Spell Checker no QuickCorrect word pairs are included. The Main Word Lists dialog is shown here. If you don t own a copy of WordPerfect but you d really like to edit and create word lists, download the trial copy of WordPerfect. You ll have 30 days to use the Spell Utility and explore the merits of WordPerfect.
IP: Unlike constructors, destructors cannot have parameters. The reason for this is easy to understand: There is no means by which to pass arguments to an object that is being destroyed. Although the situation is rare, if your object needs access to some run-time-defined data when its destructor is called, you will need to create a specific variable for this purpose. Then, just prior to the object s destruction, set that variable to the desired value.
Specifying the crystal in its series resonant mode will not require the above formula, and even a parallel crystal will be fine for most applications without this CL specification unless extreme frequency accuracy is required. Obtain the crystal s motional capacitance (CM), motional inductance (LM), series resistance (RS), and parallel plate capacitance (CP) from the manufacturer for the crystal s frequency of operation, type of holder, and cut (typically AT). This will allow us to utilize the equivalent circuit of Fig. 4.9 to model the crystal in the linear circuit open-loop simulation program as a simple LCR circuit. The Pierce oscillator is meant to work only on the crystal s fundamentalmode series resonance, but can function with overtone crystals if C1 is replaced with a parallel resonant tank that is tuned midway between the desired overtone and the overtone just below it (Fig. 4.27). In this case, the crystal manufacturer must be told if the crystal is being run out of its fundamental mode. Choose a transistor with a much higher ft than required for the oscillation frequency (5ft), and with a very high gain as well. The high ft is required to assure as close to a 180 degree phase shift from the transistor s input to its output as possible, while the high gain is necessary because of this oscillator s rather high loop losses. R, C1, XTAL, and C2 of Fig. 4.26 form a 180 phase-shift network, while R is also the feedback control element employed to place less stress on the crystal. As mentioned, the Pierce oscillates just slightly above the series resonant frequency of a series crystal, so C3 is included to tune the oscillator toward the series XTAL frequency (but the oscillator can never quite reach it). By increasing C3 s capacitance, the frequency is lowered closer to the desired fr of the oscillator, while decreasing C3 increases the fr further away from the series resonance of the crystal. RVCC and CBYPASS act in the decoupling role, while Rf, RVCC, and RC are the oscillator s bias resistors. CCOUP is used to couple power out of the oscillator into a 50-ohm load without loading the oscillator down below a safe gain margin. If CCOUP is not of a high enough reactance value, the oscillator s feedback may become too low to maintain, or even begin, oscillations (see Oscillator output coupling in Sec. 4.2.5). Since the open-loop output and input impedance of a Pierce crystal oscillator are higher than 50 ohms, set the linear software simulator s termination impedances to about 300 ohms for more accurate results. Follow these design equations to complete: 1. CBYPASS 2. C1 C2 (CFACTOR 3. C3 CC 1 ohm(XC) 2 MHz; 0.8 4 MHz; 0.9 6 MHz; 1 8 MHz.)
All ground rods 10 ft 5/8 in copper clad connected together with #2 copper stranded wire (or larger).
In the U.S., bridge inspectors and structural engineers are responsible for performing inspections and preparing reports for rehabilitation (see heading number 1.2.4). The following steps are followed: 1. An inspection report is prepared describing the condition of the bridge, its past history, diagnosis of defects, methods of repair or retro t, and cost estimates. 2. Structural inventory sheets and eld data are obtained from two yearly inspections by inspection teams using the PONTIS system. Remote sensors are also used.
0.03320 0.03794 0.04309 0.04864 0.05460
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