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Just as people use holography for many different purposes, they use many different styles of analysis to understand and control the technique. Physicists tend to use three-dimensional analyses based on Green s functions, which can be hard to visualize, and don t hook into optical design thinking very well. Electrical engineers have made many contributions to the field by looking at the volume as a series of flat and parallel planes. The light signals on one plane are related to those on another by fairly simple (for them, anyway) integral transforms, or convolutions of impulse functions. For our purposes, it is much easier to concentrate on just one twodimensional surface, the x-z plane, perpendicular to the hologram plane. The sources and rays of interest will be restricted to this plane (mostly) and light will travel in the +z direction (mostly). We will find that limiting ourselves to a single plane is what makes shop math (algebra, plane geometry, trigonometry) really useful. Things that we learn by limiting the geometry to the x-z plane will cultivate many practical insights that can be generalized later on, if we feel so inclined. Actually, we will have to let the rays travel a little ways out of the x-z plane to discuss focusing properly, especially to talk about astigmatism (forewarned is forearmed!). Those of you who have already had some electrodynamics may well be skeptical of such a simplified approach, but we have many optical components to fold into our story, and the authors predict that you will be grateful for this point of view. And we will show you how to generalize the approach to the full x-y-z space before we are done, we promise.

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The first change you notice when launching Adobe Reader 8 is the welcome screen. The Beyond Adobe Reader welcome screen shown in Figure 4.1 opens when you first launch the program. Each time you launch Reader the same screen opens unless you check the box Do not show at start up. If you dismiss the screen by checking the box for all subsequent launches of Reader, you can bring the screen back any time by selecting Help Beyond Adobe Reader. Alternately, you can also bring the Beyond Adobe Reader screen back by opening

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1. If needed, move the cell pointer to cell A1 (the upper-left cell in the worksheet) by using the navigation (arrow) keys. The Name box displays the cell s address. 2. Type Month into cell A1 and press Enter. Depending on your setup, Excel either moves the cell pointer to a different cell, or the pointer remains in cell A1. 3. Move the cell pointer to B1. 4. Type Projected Sales, and again press Enter.

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assumed that the residence time in the impeller region is relatively small and that the remainder of the vessel behaves like a well-mixed tank with a much longer residence time, eq (18-55) can be used to describe the CTD Figure 18-7 also shows the cumulative CTD calculated using eq (18-55), with a mean circulation time of 12 s, for a single circulation in the STR + STR model Comparison of the experimental and calculated cumulative CTDs shows that eq (18-55) is fairly accurate in predicting the experimental CTD, and this is especially the case for the tail of the distributions Therefore, the STR + STR model is well suited to study the effects of cell residence in the poorly oxygenated bulk regions, alternated by residence in the well-aerated impeller region Detailed descriptions of the scale-down models and their operation are provided in Amanullah et al (1993a) and Amanullah (1994).

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Figure 18-8a depicts the scale-down STR + STR con guration in the laboratory Two interconnected stirred vessels 6 L (28 or 48 L working volumes) and 2 L (12 L working volume) in capacity were used Two variable speed pumps with a maximum estimated pumping capacity of 16 L/min, enabling a minimum mean circulation time of 15 s, were employed to provide the ow between the vessels Dissolved oxygen tension (DOT) was measured and controlled at 5% 05% of air saturation in the smaller vessel by means of gas blending, keeping the total ow of gas constant at 1 vvm Nitrogen was sparged at a rate of 05 vvm into the larger vessel to maintain a DOT level close to zero The mean circulation time (tc ) was varied in the range 15 to 300 s at Va /Vq of 025 and 0.

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