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If you have AutoCAD LT: Follow the prompts:
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Figure 6-6: The Convert Multi-page PDF to PSD command enables conversion of several pages within a PDF file to be acquired in Photoshop.
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As with Opacity, you can select a blend mode from the keyboard when a selection or navigation tool is active. Press Shift+plus to advance incrementally down the list; press Shift+minus to inch back up. You can also press Shift+Alt and a letter key to select a specific mode. For example, Shift+Alt+M selects the Multiply mode. Shift+Alt+N restores the mode to Normal.
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where h is the average liquid height, g the gravitational constant and the density of the solution. Since viscosity measurements of the solvent alone ( o ) and of various concentrations of the particle ( ) are carried out under identical experimental conditions, they may be conveniently expressed as relative viscosity, r , of the solution/suspension; r = t = o to o (7.4)
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Here s an example that uses the Date variable type and displays it in a message box:
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>>> s = socket(AF_INET,SOCK_STREAM) >>> s.connect(( 127.0.0.1 ,44444))
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where and are the mean and standard deviation and USL and LSL are the upper and lower speci cation limits, respectively, for a product quality measurement. Process capability indices are useful for process improvement studies because they transform diverse measures of quality (e.g., weight, concentration, rate) into dimensionless units, thereby allowing investigators to pinpoint major sources of variation in a process (operations which have the lowest Cpk scores) when many measurement systems and quality attributes are involved. The process capability index, Cpk, is related to the so-called process sigma such that a 6 process corresponds to a Cpk of exactly 2.00, or 2.0 defective parts per billion (PPB), assuming N (0, ) quality variance distribution (can alternative calculation for process sigma estimates 3.4 defective parts per million for a 6 process). Examples of the correspondence between Cpk, process sigma, and defect rate for N(0, ) distributions are shown in Figure 2. The process capability (based on observed yield) of pharmaceutical manufacturers has been cited by some benchmark studies to be roughly 0.7 (2.1 ) [28]. While industrial benchmarks clearly indicate that pharmaceutical manufacturers have many opportunities to improve quality control, direct comparison with other industries may be somewhat misleading. As opposed to such industries as semiconductor manufacturing, where defective parts are often readily apparent at some
At the pump levels required for generating 30 J in 500 ns, the laser ampli er system can be safely operated at a pulse repetition frequency of up to 3 Hz without risk of thermal fracture of the Nd:glass ampli er slab. We have demonstrated an average power of 96 W (32 J at 3 Hz) at 1 v (1.053 mm). This is reduced from the 150 W reported earlier for the same glass ampli er with 15-ns pulses [29] due to the inherently lower extraction ef ciency of the long pulse ampli er. The SBS phase conjugated mirror accurately reverses both (a) the static wavefront distortions arising from errors introduced by optical components and (b) those introduced by the thermally loaded glass ampli er. As a result, just as with the short pulse ampli er, the output beam characteristics of pulse energy, pulse shape, beam quality, pointing stability, and coherence length are essentially unchanged from single shot to full average power operation. 5.4.4.1 Long-pulse output energy and pulse shape To amplify pulses with durations from 500 1000 ns, the laser ampli er slab is operated with a singlepass gain of 1.8 Np corresponding to a small signal ampli cation of 6.2. At this laser gain, up to 32-J pulses are extracted with a injected seed energy of *100 mJ. The plot in Fig. 5.19a shows the temporal pro le of an ampli ed 500-ns output pulse. An oscillator pulse is shown temporally aligned to the output pulse as it would be recorded after a full optical transit through the ampli er system without gain. Note that the bulk of the output pulse results from the ampli cation of the exponentially rising leading edge of the input pulse. This provides the somewhat counterintuitive result of the ampli cation of a 200-ns FWHM injected pulse to the full-energy, 500ns output pulse. Just as the log of the input power, shown in Fig. 5.18b, begins to roll over from linear, the ampli ed output abruptly falls off. Also note that although 100 mJ is injected from the oscillator/preampli er, less than half of the energy from the rst part of the input pulse substantially contributes to the output pulse. Figure 5.19b shows a progression of output pulse temporal pro les that readily illustrate the simple extraction theory presented earlier. Using a constant input seed pulse energy, as the gain in the ampli er is increased, the peak power of the ampli ed output pulses increases until a maximum value of 60 MW is reached. A further increase in ampli er gain beyond this point does not increase the peak power but only increases the pulse duration. In this manner, controlled extraction of long pulses is achieved from the ampli er resulting in near-rectangular, constant power output pulses. 5.4.4.2 Long-pulse beam quality As described earlier, the output beam from the ampli er system is approximately 25 25 mm2. Figure 5.20 illustrates a near- eld pro le imaged at the input to the doubler assembly. Figure 5.21 shows the corresponding measured far- eld pro le for this beam. Although nearly square in
Figure 5-8: The results of sharpening the car with the pressure set to 50 percent (top) and 100 percent (bottom).
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To negate the sense of a character class that is, to match a character that is not one of the characters in the set place a caret (^) symbol at the start of the list:
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90 0 j 0.05 0.2 0.5 1 2 5 150 1 120 2 j 5
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