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What the slicing process really does is divide your image into different pieces, which are described in HTML as a table. Figure 19.25 shows an example of such a table. Each cell of the table contains a different image, optimized as you specify with or without a link. Because a cell must be rectangular, you must also make all slices rectangular. When the table is rendered in a Web browser, the image looks like a complete graphic.

152. Environrnental Catalysis, ACS Symp. Ser., Vol. 552, J. Armor, ed., American Chemical Society, Washington, DC, 1994. 153. Applied Catalysis, B: Environrnental was launched in 1992.

Both correlations collapse to the Chen and Middleman result in the inviscid limit. According to eqs. (12-21), (12-24), and (12-25), the dependency of drop size 2 1 on max or P/V varies from the 5 to the 4 power as d or Vi increases. The ideas discussed earlier about scale-up and application to other impeller types still

For very viscous mixtures, the viscosity is likely non-Newtonian. For shearthinning uids that can be represented by a power law exponent (n); power = D3 N1+n (16-2)

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The intersection of the rulers in the upper-left corner of the page is called the zero point. Known as the ruler origin in other applications, this is the starting place for all horizontal and vertical measurements. If you need to place items in relation to another spot on the page (for example, from

FIGURE 10.21 Assigning a Tab Control to the layout tab order so it can be selected via the keyboard.

the close button (the X button) in the upper left corner of the Keywords window, or simply click the Keywords button in the middle of the toolbar.

Slit-Illumination Beam Forming our discussion about diffraction ( 6), we found that diffraction efficiency varies with the square of modulation. It s necessary to split the total available dynamic range of the material among the number of exposures made-to record N different exposures into a single hologram without overexposing any part, we must reduce the exposure (and thus the modulation) of each by N , which in turn reduces diffraction efficiency by N2. Another reason for the 1-over-N nature of holographic exposure is a problem known as bias buildup . If we make a simple hologram of multiple points, the fringe patterns that represent each point combine coherently to form the resulting holographic fringe pattern, usually combined with some base exposure due to the brightness of the reference beam. Coherent exposure means that the patterns from individual points can add to and cancel each other out in some places, reducing as well as adding to the base exposure amount and achieving more efficiency. In contrast, incoherent exposures can only add to previously made exposures; there s no way to reduce any exposure that s already been made. With each exposure, this base exposure builds, biasing the meaningful part of the fringe pattern and minimizing the dynamic range it can have. The order effect amendment to the one-over-N law Even beyond the diffraction-efficiency cost of multiple exposures, there is more bad news. Peculiarities of the physics of the silver halide process cause the first exposure to dominate in holographic effect. If three equal sub-hologram exposures are given to a composite hologram, the first-exposed sub-hologram will be brighter than the second, which will be brighter than the third. An approximate compensation can be made by giving them unequal exposures in the ratios of