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A number of the following examples will be drawn from extremely large Fibonacci fans which span many decades. The chart shown in Figure 13.19 is just a portion of the Dow Jones Industrial Average on which a 70-year-old fan has been drawn. The rectangle has been drawn to highlight how the price action is not only bounded by two fan lines but also, for many years, tends to cling to one of the lines. This particular section is following the dramatic crash of 1987. In spite of all the chaos and tumult surrounding that crash, the prices continue their orderly motion between and along the fan lines. One should pause to consider how simply remarkable this is. The fan lines were drawn from the depths of the Great Depression to the peak of the Internet bubble (1932 to 2000). The market had no awareness at least none of which it was conscious of these boundaries. Over the decades, billions upon billions of individual decisions are made that move this index up and down every day. And in spite of all of these variables,



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+ k iz )1 2 )

(3.6.26)

The last equality in (3.6.26) is a result of using (3.6.19) and (3.4.23). The sum of (3.6.23) and (3.6.26) gives the intensity of the incoherent first-order scattered fields ('l/Jy) ('F)'l/Jjl)*(r' )). We note from (3.6.24) and (3.6.25) that Hp(p) is usually negative because 9p(r) = 0 for Irl < dmin so that the correlation of scattering between different clusters decreases incoherent scattering. The decrease of incoherent scattering is associated with an increase in the coherent forward scattering which, as we saw earlier, does not contribute to extinction. Thus the scattering effect of gp is to decrease





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extinction. From (3.6.16), we note that 9s is positive so that (lJ(p) (k p , k z )1 2 ) is usually larger than N s 111 2 . This means that clustering due to 9s generally increases the scattering cross section above that of independent scattering. Thus 9p and 9s have opposite effects on extinction. The overall scattering of a random collection of scatterers depends on the interplay between the two pair functions 9p and 9s, namely, the pair function between different clusters and the pair function within a cluster. Without the second-order coherent field, the outgoing power from the slab is analogous to (3.4.33). From (3.6.11), (3.6.14), (3.6.23), and (3.6.26) we have

f dsn . 1m 1,im_ \7 [VJinc(r)'I/)7ncCr') + 'l/Jinc('F) ('I/)s(1) (r')) + ('I/)s(1) (r) )'I/)7nc(r')

= A{ -ImU)41fn o D + 1112 (21f~;;;D)2

7r 2 /

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The relocation of the Cape Hatteras Lighthouse utilized technology known to few people, mostly in the structural moving industry, to lift, transport, and set the 4,800-ton lighthouse. The uni ed hydraulic system allowed the structure to be uniformly supported while traversing a support system consisting of beams, mats, and compacted soils. Structural issues involved vertical support of the lighthouse as its base was incrementally removed by mining, support during transport by a system of cross beams and main beams, and temporary and permanent support at the new location. The inherent stability of the lighthouse dictated that once supported on steel the lighthouse would remain stable. The 5-inch double extra strong steel pipe shoring towers had to be laterally braced to resist wind and seismic forces.

d<jJ(lf(P)(k p - kip, -k z + k iz )1 2)

FIGURE 13.19 Prices will often become bound between the support and resistance provided by fan lines.

127r

+ Dkn~(21f)3

7r/2

d<jJHp(k p - kip, -k z + k iz )

(3.6.27)

. IU(P)(k p - kip, k z + k iz ))\2 }

We can see that, in (3.6.27), the second term is from ('I/)s(1)) ('I/)s(1)*) , the third and fourth terms are the outgoing incoherent intensities from the boundary, and the fifth and sixth terms are the outgoing incoherent intensities from the top boundary. The second-order coherent scattered field can be calculated as follows. We use (3.4.19). The double summation of L:l L:#l is decomposed into the sum of scattering from two different scatterers in the same cluster and from two scatterers in two different clusters. Thus taking the average of (3.4.19)

FIGURE 13-15 Temporary support shoring posts consisting of 5 x-strong pipes had to be laterally braced.

(3.6.28) By using the plane wave representation of Green's functions in (3.6.28), one can show that the coherent scattered field is only appreciable in region 2. By considering the transmitted intensity associated with the second-order coherent field, one gets

-z .J,i~r 1m [\l'l/Jinc(f)('l/;S(2)(f')) + \l (-~;S(2)('F))'l/;tnAf')]

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