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by normalization with the instantaneous d32 (t). This is shown in Figure 12-13. Therefore, the instantaneous DSD can be described by eq. (12-29), where X(t) = d/d32 (t) and the mean and the volume standard deviation are de ned similarly. Chang found that his data for a RDT were well correlated by X = 1.07 and V = 0.27 for both inviscid and viscous drops with d 0.140 Pa s. This is essentially the same result as for the equilibrium DSD of Section 12-2.3.2, as should be expected. Therefore, for dilute systems, a single correlation describes the time evolution of the DSD provided that d32 (t) is known. The correlation also ts the data of Narsimhan et al. for a at-blade turbine. Chang (1990) used a population balance framework (discussed in Section 12-4) to develop correlations for d32 (t). For nonviscous oils dispersed in water, he obtained d32 (t) = d 32 3.8 103 Nt

The shaded bands are generated by a bar chart series with eight data points (in the range D2:E9). The bar chart series uses the value axis at the bottom of the chart, and each bar has been manually formatted to display a graduated color effect. Because the chart plots transformed data, the chart can be used for any data set without modification.

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Option Explicit tells VBE that anytime you use a new variable within your code, you must specify whether that variable is a string, a number, a range, or whatever.

1. Create a smooth point along a path. See the last set of steps to learn how to do so. 2. Select the newly created smooth point with the Direct Selection tool. For more on using the selection tools, see 6. 3. Click and drag the control handle again. 4. Adjust the angle for both control handle lines and the length for the new control handle line that you re dragging. Note that as you drag out this control handle line, the other control handle line wobbles to the angle that you re dragging. This happens because on any smooth point, the control handle lines must be at the same angle, and as you drag out the new control handle line, you re simultaneously changing the angle for both control handle lines.

The interface circuit in Section 8.4 returns the make code of the last released key and thus ignores the typematic condition. An alternative approach is to consider the typematic condition. The keyboard interface circuit should return a key s make code repeatedly when it is held down and ignore the final break code. For simplicity, we assume that the extended keys are not used. Design the new interface circuit, resynthesize the verification circuit, and verify operation of the new interface circuit.

be assumed for a given gas rate, and this allows reasonable estimates to be made of the combined gas and vapor ow loading the impeller. When an existing boiling reactor is sparged, the sparged gas rate can be corrected using the vapor pressure of the liquid at the temperature measured. Assuming that the partial pressure of the vapor pv is then known, the total volumetric rate, QGV , is given by QGV p0 = QG p0 pv (11-14)

In Listing 9-26, the first thing is the ENTRY_RE constant, which has been given the regular expression composed during the planning stage of this scraper. The way this string is put together in the Python source code is a little strange. Rather than using a multi-line string, this one is built from a series of concatenated strings. This is a tradeoff to retain some clarity in the Python source code, yet to keep errant whitespace and carriage returns out of the regular expression. Although there is a re.VERBOSE compilation flag that s supposed to help out with this, it didn t seem to work very well when used here. You may want to tinker with this in your own code. Things get a little interesting in Listing 9-27, where this class gets wrapped up.

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