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FIGURE 9.35 Compare this chart of Owens Illinois to Figure 9.2. In spite of the initial gains, the stock eventually weakened and went on to a substantial loss.

~p~p) - no(Tp(p,p))st]

Larger concrete dead men with earth anchors were installed to resist the pull of the stays on the end towers. The needle beams provided a perfect support for a rail and rolling hoist.

(5.3.23)



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We note that the effective field approximation is valid for a sparse concentration of particles so that the coherent effective propagation constant is close to k. We then look for the solution of p that is close to k in (5.3.23). The arguments of T pin (5.3.23) can be replaced by kp. The first term in (5.3.23) is much larger than the terms that have the (p2 - k 2) factor. Thus, the determinant of (5.3.23) is approximately equal to _k 2 times the determinant of the 2 x 2 matrix formed by Op and ~p components. Hence, the dispersion relation is

3.2 Effective Field Approximation (EFA, Foldy's Approximation)

-noOp ' (Tp(kjJ, kjJ))st . P p2 - k 2 -::- nJJp . (~p(k~, kP)),st . Op { p2 _ k 2 - no p' (Tp(kp, kp)}st . p -no<pp' (Tp(kp, kp))st . ()p





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(5.3.24) Using the relation between F and T in (5.1.44), the dispersion relation can be expressed in terms of the F dyad for propagation in the direction ki Note that iJ corresponds to v and that corresponds to h.

(5.3.25)

with Vi and hi (vertical and horizontal polarizations) as the basis for (5.3.25). In (5.3.25), (fo.(3)st denotes averaging over the state (e.g., orientation and size). The eigenvalues for K in (5.3.25) are the effective propagation constants, and the corresponding eigenvectors give the characteristic wave polarizations associated with the propagation constants. Let

i21fn o M a(3 ((}i, <pd = (fo.(3((}i, <Pi; (}i, <pd)st-y;-

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not guarantee future results. They simply aid in predicting short-term direction. To close this topic as well as this chapter, let us look at one nal stock example: Avalon Bay (symbol AVB), which helps illustrate again how much protection technical analysis can provide when used properly. Figure 9.36 shows a rounded top that would thrill most individuals hoping to sell the stock short. Everything about the top seems proper, and using traditional measurement techniques, one could conclude this stock was going to fall from $28 to $18, generating a handsome pro t for those who were short the stock or long put options. The fact is, however, that even though the stock did indeed sink below $28, it didn t stay there for long. It paused there brie y and then began moving higher. That would have been the signal for bears to close their positions at once for a very small loss. If a stock in this kind of pattern can muster the kind of strength to shake off a pattern of this size, the stock buyers are far too strong for the sellers (Figure 9.37). It is wise to move out of the way quickly. In this instance, once the stock recomposed itself, it moved higher many hundreds of percent. Those short the stock who refused to cover their position would have been wiped out.

(5.3.26)

This enabled the long glued laminated timber chord replacement members and other materials to be pulled into the bridge.

Solving (5.3.25) gives values of K2 and since K is close to k, the two effective coherent propagation constants are K 1 and K 2 with

[Mvv + Jvhh {(Mvv - Mhh)2 + 4MvhlYhv} 1/2]

(5.3.27)

and the associated eigenvectors are, for Mvh, Mhv ={; 0,

(Ev ) 2Mv h (5.3.28) (Eh) -Mvv + lYhh {(Mvv - Mhh)2 + 4MvhMhv} 1/2 where (Ev )/ (Eh) is the ratio of vertical to horizontal polarization in the

characteristic wave. Note that there are only two propagation constants and characteristic waves for a specified direction of propagation. For the case (fvh)st = (fhv)st = 0, when there is no coupling between the two polarizations, the eigensolutions are

(5.3.29)

FIGURE 9.36 This chart of Avalon Bay (symbol AVB) appears to be breaking beneath support and on its way to a major fall.

(5.3.30)

FIGURE 16-5 Glued laminated timber was used for chord replacement material, oor beams, and bolster beams.

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