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where U is the field component, and Dn and n are appropriate constants [Keller 1956, McNamara et al. 1990]. Thus, the asymptotic behavior of the cylindrical case is the same for both the E-plane and H-plane couplings, which is in contrast to the planar case. Using the dominant term only [cf. Table 6.1 and Figures 6.2 (a) and 6.3 (a)] we find that the asymptotic expressions for the circular cylinder case predict the correct decay for moderate to large distances s, whereas the asymptotic expressions for the planar case are accurate for small distances as well (not shown). The phase data in Figures 6.2 and 6.3 are shown with the phase delay corresponding to the geometrical separation subtracted. For the planar case, the phase follows almost a horizontal line, indicating that the wave is propagating as a TEM wave in free space. For the circular cylinder, there is an additional phase delay. One interpretation of this is that the wave is propagating at another radius. Analyzing the phase data gives an equivalent geo~ ~ desic length s corresponding to a radius of R R + 0.2 ; thus, the surface field can be interpreted as traveling approximately 0.2 above the curved surface. This is an interesting result when discussing the physics of the ray-based model. In this model, the surface field is assumed to travel tightly along the surface; but a different radius could have been used, as indicated in Appendix 4A.2. In fact, from Keller s surface diffraction analysis [Eq. (6.4)], the approximate solution for the Hz component (circumferential polarization) gives Hz where

(E)GPRS transmits segments of logical link control (LLC) blocks with a maximum bit rate that depends on the (M)CS utilized. The amount of LLC bits transmitted in a radio block is given by the amount of channel coding applied on each (M)CS. Table 7.1 summarizes the amount of LLC bits in a radio block of 20 ms and the peak throughput offered to the LLC layer for the different (M)CS. The maximum EGPRS peak throughput for GMSK-modulated radio blocks is given by MCS-4, which has lower peak throughput than CS-4. EGPRS may have slightly lower throughput than GPRS CS-1 4 under very good radio link conditions if MCS-5 9 cannot be used. This may happen in UL direction with certain terminals that may not be capable of transmitting with 8-PSK modulations due to transmitter limitations.

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Steiss, M. (1995). Mechanische Verfahrenstechnik, Vol. 1, 2nd ed., Springer-Verlag, Berlin, pp. 168 275. Thiel, W. J. (1982). Further comments on Suggestions on the nomenclature of powder mixtures, Powder Technol., 33, 287 288. Van den Bergh, W. (1994). Removing the uncertainty in solids mixer selection, Chem. Eng., Dec., 70 77. Weidenbaum, S. S. (1973). Solid solid mixing, in Chemical Engineers Handbook, 5th ed., J. H. Perry, ed., McGraw-Hill, New York, pp. 21 31 to 21 36. Weidenbaum, S. S. (1984). Mixing of powders, in Handbook of Powder Science and Technology, M. E. Fayed and L. Otten, eds., Van Nostrand Reinhold, New York, pp. 345 364. Weinekotter, R., and H. Gericke (1999). Mixing of Solids, Kluwer, Dordrecht, The Netherlands. Wightman, C., P. R. Mort, F. J. Muzzio, R. E. Riman, and E. K. Gleason (1995). The structure of mixtures by particles generated by time-dependent ows, Powder Technol., 84, 231 240. Williams, J. C. (1986). Mixing of particulate solids, in Mixing: Theory and Practice, Vol. III, V. W. Uhl and J. A. Von Essen, eds., Academic Press, New York, pp. 265 305. Williams, J. C., and M. I. Khan (1973). The mixing and segregation of particulate solids of different particle size, Chem. Eng. London, 269, Jan. 19. Wilms, H. (1988). Blending and homogenizing of bulk solids with the Zeppelin multi-pipe gravity blender, Bulk Solids Handl., 8(6), 733 736. Wilms, H. (1992). Blending silos: an overview, Powder Handl. Process., 4(3), 293 299. Zlokarnik, M. (1984). Scale-up in process engineering, Ger. Chem. Eng., 7(3), 150 159.

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e( 0.693/T1/2p )t e (0.693/T1/2d )t (Eq. 3-2) Fortunately this calculation can be simpli ed by classifying generators into two groups: those in which the parent half-life is 10 to 100 times that of the daughter and those in which the parent halflife is more than 100 times that of the daughter. In the rst group, the activity of the daughter during equilibrium decreases perceptibly over time. This is called transient equilibrium. On the other hand, the equilibrium segment of the curve for the second group is relatively at. This is called secular equilibrium.

Although the popupAction() and runCommand() functions are not directly useful to behavior creators because they cannot be called from within a behavior, they do enable considerable cross-pollination of Dreamweaver extensible objects. Invoking these functions calls an existing behavior or command and presents its dialog box to the user except you use these functions to call the behaviors or commands from within a custom object, command, or Property inspector. The popupAction() function takes two arguments: the name of the action file and the general function call of the action. The action chosen must be located in the Dreamweaver MX 2004\Configuration\Behaviors\Actions subfolder. For example, code to call the Play Sound behavior might look like this:

Competition (low speci city) Amensalism (variable speci city)

In fact, any object that can serialize to a String can be passed to trace(). In this example, an Array of String values is passed to trace():

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