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Figure 6.3.2 Effective loss tangent 2Kd K r of QCA as a function of fractional volume. Frequency is at 37 GHz. The permittivity of the particles is E = {3.2 + iO.OOl)Eo. Two cases s of Rayleigh size distributions are considered with (a) = 0.05 cm and (a) = 0.09 cm.

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Figure 6.3.3 Normalized phase velocity k/ K r of QCA as a function of fractional volume. Frequency is at 37 GHz. The permittivity of the particles is E = {3.2 + iO.OOl)Eo, Two cases s of Rayleigh size distributions are considered with (a) = 0.05 cm and (a) = 0.09 cm.

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horizontal shear, are the three qualities that are normally determined during the process of selection we call design Because timber is available in certain standard lumber sizes, the designer selects from those available, the size, grade, and species that most economically meets the preordained standards for bending stress, de ection, and horizontal shear When the engineer reviews the capacity of an existing member, many parameters complicate this process Size, span, and spacing of members are dictated by the existing structure It is the engineer s task to determine the size, orientation, species, grade, and end condition of all the structural elements in a building that already exists The freedom of choice afforded by design is therefore reduced in the review process Often, the structural engineer must pass judgment on a structure that has served far beyond what we consider to be a normal period of service.

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In all the many, many years I ve been learning and performing technical analysis, there is no set of studies which has interested me more than those of Fibonacci. In both JavaCharts and ProphetCharts, there are four kinds of Fibonacci studies available: retracements, fans, time zones, and arcs. In this chapter we will explore each of these, as always, with actual examples from the recent past. But rst, let us learn a little about the namesake of these studies.

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Figure 6.3.4 Backscattering coefficient (jhh (in decibels) of QCA a.s a function of fractional volume. Frequency is at 37 GHz. The permittivity of the particles is ts = (3.2 + W.OOl)tQ. Two cases of Rayleigh size distributions are considered with (a) = 0.05 cm and (a) = 0.09 cm. The layer thickness is d = 3 cm and incident angle is 30 .

In Figs. 6.3.5, 6.3.6, and 6.3.7, we show the coherent wave attenuation rates for a smaller mean grain radim; of 0.035 cm. The corresponding mode radius is 0.0279 cm. Figure 6.3.5 compares the extinction rate 2Ki between independent scattering and QCA. We note that attenuation rate of independent scattering is larger than QCA. The results show that the extinction rate first increases rapidly with frequency as in Rayleigh scattering. Then it departs from Rayleigh scattering around 20 GHz and starts to gradually level off. This indicates the importance of including Mie scattering effects beyond 20 GHz for (a) = 0.035 cm. Figure 6.3.6 compares the results of QCA between the extinction rates of monodisperse particles with radii = 0.035 cm and the case of Rayleigh size distribution with (a) = 0.035 cm. We note that the case of Rayleigh size distribution has a considerably larger scattering rate than monodisperse case. This indicates the importance of including size distribution in modeling scattering from realistic geophysical terrain when grain sizes are small. The numerical results indicate that the extinction rate is at 1.056 cm- 1 based on Rayleigh size distribution at frequency = 95 GHz, meaning that there is strong multiple scattering of incoherent waves at such high frequency even for moderate snow layer thicknesses. Figure 6.3.7 shows the results of HH backscattering coefficient for a layer thickness of d = 10 em.

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