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Beyond the resources available from the FileMaker, Inc., Web site, resources and mailing lists are available via the membership-based programs (TechNet and the FileMaker Business Alliance) offered to developers and businesses working with FileMaker. Through these resources, users and developers around the globe stay abreast of news, changes, updates, and new releases of the software, and exchange notes with each other and the Developer Relations contacts at FileMaker, Inc. Other resources, such as white papers and technical briefs, are available exclusively to members of FileMaker developer organizations.

This query is very similar to the query for the overall calculation, with the addition of the aggregation by market. The results in Table 3-8 make it clear that the stop rate for Smallville is different from the stop rate for Gotham and Metropolis. The 95% confidence interval for Smallville does not overlap with the confidence intervals of the other two markets, as shown in Figure 3-7. This is a strong condition. When the confidence intervals do not overlap, there is a high confidence that the ratios are different.

The Sound Effect action allows you to play an imported sound. When you select this action, the Select Asset dialog box appears (even though you are not selecting anything visual), displaying the assets in your library. Previously imported sounds will be in the Media folder. If you have not imported sounds, you can click the Import button to do so now.

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the orifice and the discharge current) and can be affected by the anode location and design [46]. As the discharge current is increased for a given cathode orifice size and gas flow rate, the noise in the discharge voltage and in probe signals from the plasma increases [70], and the cathodes produce ions with energies significantly in excess of the discharge voltage and produce significant keeper and cathode orifice erosion. This leads to the keeper and cathode life issues discussed above associated with plume-mode behavior and often determines the cathode geometry and operation conditions selected for any given thruster. Figure 6-54 shows the discharge voltage versus current for a 1.5-cm-diameter dispenser hollow cathode with a 2.1 -mm orifice for several different flow rates [6]. In this case, two different anode geometries were used: one was a 45-deg conical anode and the second was a 5-cm-diameter cylindrical anode. The maximum current in the plot that could be achieved at a given gas flow was due to the onset of strong discharge voltage oscillations of greater than 55 V. The small cylindrical anode permitted significantly higher discharge currents to be obtained before the oscillation limits and also reduced the discharge voltage at all currents. This is due to the increased gas pressure near the cathode exit increasing the plasma generation in the cathode plume, which could only be achieved with the conical anode by injecting significant amounts of gas directly into the anode region. It is clear that the onset of the oscillations and the transition to plume mode is an anode-plasma effect, which will be discussed further later.

[15]

Figure 2.18 Cation and anion exchange chromatography. (a) Anion exchange columns carry a positive charge and bind negatively charged analyte molecules. Cation exchange columns carry a negative charge and bind positively charged analyte molecules; (b) Target analyte molecules are eluted by increasing the ionic strength, I, of the eluant from low I to high I. In order to monitor this process, absorbance (A) at a given wavelength is observed as a function of elution volume (V ) or time (t ).

Framesets, much like tables, are made up of columns and rows. The columns and rows attributes (cols and rows) are lists of comma-separated values. The number of values indicates the number of either columns or rows, and the values themselves establish the size of the columns or rows. Thus, a <frameset> tag that looks like this

which has no apparent reflection symmetry. In fact, the symmetry is there because the original Lagrangian possessed such a symmetry, but it has been hidden. For small oscillations about the classical vacuum

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