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where tn is the per-cell time to compute the numerics (i.e., governing equations), tb is the per-cell time to compute the embedded boundary, and to is a small overhead incurred by each patch. For example, a patch that does not intersect the boundary, and hence has no cut cells, will incur the cost of the numerics (tn times the total number of cells on the patch) plus a small overhead to for calling patchCubes to determine that no cut cells were found on the patch. Patches that do intersect the boundary and have cut cells incur the additional cost of computing the information on those cells (tb times the number of cut cells). The sum of these gives an estimate of the computational cost on a patch. Of course, the values of tn , tb , and to will depend on the characteristics of the machine and the algorithms used for the numerics and the embedded boundary construction but will be largely problem independent. We determined values of tn , tb , and to using a least squares t from statistics gathered from a computation of a plume evolution around buildings in Salt Lake City. For this calculation, we recorded the total number of cells on the patch, the number of cut cells on the patch, and the computation time on that patch. From these data, we computed tn and to by considering patches that contained no cut cells, and tb by additionally considering those patches that did.

Kissileff and Thornton, 1987), a combination of ephedrine and caffeine (Astrup et al., 1992), and thyroxine. All induce a degree of weight loss by enhancing sympathetic activity and thus energy expenditure, but all are non-selective

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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 (1053 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.

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A direct consequenceof the particular form of the log-likelihood function (5.59)is described by the following theorem:

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Figure 6.18 An example of the gamma probability distribution function and its characteristic function.

The design of TrueType fonts enable the type designer the ability to prevent font embedding. These fonts can be moved to the Always Embed list, but if designed without embedding permissions, they will fail to embed in the PDF. Font embedding errors are reported in the log file that can be viewed in a text editor. If a PDF is produced, you can choose File Document Properties Fonts to determine whether the font was embedded.

The rest of the corners are created in exactly the same way, except that the function either adds or subtracts $curveDepth from $x1, $y1, $x2, and $y2 as appropriate to get the correct center points for each arc. Also remember that the start and end positions of the arcs change for each corner.

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 5441 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 18 Np corresponding to a small signal ampli cation of 62 At this laser gain, up to 32-J pulses are extracted with a injected seed energy of *100 mJ The plot in Fig 519a 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.

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