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We shall illustrate the numerical results of the effective propagation constants and backscattering coefficients using parameters of snow. The results are illustrated with the Rayleigh size distribution, which is a special case of the modified gamma size distribution. The size distribution is represented by n(a), which is the number of particles per unit volume with radii between a and a + da. The Rayleigh size distribution is given by 7f fa (7fa ) n(a) = 16(a)5 exp - 4(a)2

(6.3.52)



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where (a) is the mean radius. The fractional volume j, the mean radius (a), and the mode radius am are defined by

1 4;





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The follow-up to Figure 12.70 is shown in Figure 12.71, which illustrates the four-fold increase in price of the stock for Fred s, Inc. You can plainly see the retracement return the price to its neckline level several months after the breakout, followed by a virtually uninterrupted increase in equity value. The exchange-traded fund for the Russell 1000 index (symbol IWD) is illustrated in Figure 12.72. In this instance, you would be faced with the decision about where to draw the neckline, since the price doesn t quite come up as high in January as it did the prior August. In cases like this, you should place the neckline at the highest point, since that is the resistance level. A breakout cannot really occur until all the recent high prices have been bested. The effects of an inverted H&S breakout can last for years, or even decades. For symbol IWD, the price moved higher for several years following the breakout (Figure 12.73). Knowing where to place the neckline isn t as obvious as the earlier examples in this chapter would suggest. Of course, if guring out the placement of the neckline is too hard, perhaps the pattern is not well-de ned in

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a 3 n(a)

All structural engineers should obtain a copy of The Secretary of the Interior s Standards for Rehabilitation. Under these standards, rehabilitation means the process of returning a property to a state of utility, through repair or alteration, which makes possible an ef cient contemporary use while preserving those portions and features of the property that are signi cant to its historic, architectural, and cultural value. Minimum alteration of the building, its environment, and its distinguishing architectural qualities is required for a project to qualify as a certi ed rehabilitation bene ting from the provisions of the tax act. Archeological resources must be protected, as well as signi cant historical, architectural, or cultural material. An understanding of the historical signi cance of a building must be obtained to enable the engineer to provide an acceptable solution to a particular design problem while following the secretary s standards. The guidelines for applying The Secretary of the Interior s Standards for Rehabilitation recommend recognition of the special problems inherent in the structural system of historic buildings, especially where there are visible signs of cracking, de ection, or failure. In addition, stabilization and repair of weakened structural members and systems when damaged or inadequate are recommended. Historically important structural members are to be replaced only when necessary. 1

(6.3.53) (6.3.54) (6.3.55)

.::...:;;-;OO:;;C---:-,.-

Jooo daan(a)

fo dan(a)

am = [g(a)

In (6.3.55), am is the mode radius at which the size distribution is at a maximum. Thus, given the fractional volume j, the Rayleigh size distribution contains only one parameter, namely, the mean radius. In the numerical calculations, we discretize the Rayleigh size distribution into 20 different equally spaced sizes (Le., L = 20 species). The pair distribution functions for a medium with 20 sizes are then calculated by the Percus-Yevick approximation as given in 8 of Volume II. The maximum size for these 20 sizes is chosen such that at least 99.7% of the scattering contributions and the fractional volume of particles are included. That usually occurs around 2.5 to 3 times the mean radius. Comparison will be made between the scattering of a medium with Rayleigh size distribution of a specified value of (a) and the case of monodisperse particles with radii equal to that same value. The results of QCA will also be compared with that of independent scattering. For the case of independent scattering, the extinction rate is ( lie ) independent -

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