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are in a position, you should stay in that position so long as the prices stay within the boundaries (Figure 8.8). And if you are not in a position, you may want to wait until the price breaks above (bullish) or below (bearish) the channel before taking action. You should also keep in mind that breakouts are more potent if they are contrary to the primary trend of the channel. In other words, a breakout above a descending channel is especially bullish, and a breakdown below an ascending channel is especially bearish, because in each case, the breakout is in opposition to the former trend. As mentioned before, channel patterns are unusual, but they do happen, and the longer they last, the more meaningful they are. Any price trend will eventually change, so as a channel gets progressively old, the likelihood of its staying within that channel diminishes, and the potency of the move once it escapes that channel increases. As Figure 8.9 shows, it is hazardous to try to anticipate the breakout from a channel until is actually happens, since prices can stay within the con nes of a channel for months or even years.



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(4.1.52) For the case kma 1, the correlation function C(r - rl) is sharply peaked at l' = rl. Hence, for the nonlinear approximation we have

M(G(r))C(r)

FIGURE 15-3 The deteriorated members in the Utica Road Covered Bridge were replaced in kind. (See color insert.)

(4.1.53)

Assuming (G(r))

= exp(iKr)/41TT and C(r) = Jk:~exp(-r/a), 2 K ~ k~ + Jk:~a2(1 + 2'iKa)

(4.1.54)





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Next we compare the result of bilocal approximation of (4.1.34) with that of nonlinear approximation of (4.1.54). Suppose k m is real, then Re(I{2) are the same for both approximations. The imaginary part of K2 is related to the attenuation rate due to scattering. The two results for the imaginary part are different since one is 2Jk:~a3 while the other is 2Jk~:K a3. Since Re(K) is much greater than Im(K), the attenuation rates based on the two approximations will be essentially the same if Re(K) is approximately equal to k m . This is usually the case for a tenuous medium with small J. Under the circumstances where J 1, the results of bilocal approximation and nonlinear approximation are roughly the same.

In Section 1, Dyson's equation for the mean field is derived by renormalization, i.e., re-summing the averaged Neumann series for the field. In a similar fashion, an equation governing the second moment of the field can be derived by using the diagrammatic method. We consider a random medium with permittivity (4.2.1) The solution to the scattering of electromagnetic waves in terms of dyadic Green's functions is given in the previous section.

=(0)

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When prices do nally leave their channels and they always will, eventually those holding positions in those securities are wise to close them out, and those looking for an entry point should examine the chart as an opportunity. Figure 8.10 illustrates typical action after a channel is broken. In this instance, prices were trending slowly lower, making a series of lower highs and lower lows. A person exploiting this channel may have seized on opportunities to buy the stock when it was at the lower support line and sell the stock short when it was at the upper resistance line. But as the chart shows, the fourth time it touched the support line, it subsequently broke it, and the downfall in price from there was fast and powerful. Prices can move out of a channel in either direction, of course. Figure 8.11 shows a channel made of two horizontal, parallel trendlines. This also happens to be an inverted head and shoulders pattern, which you will read about in 12. After prices moved above resistance, they swiftly more than doubled, and a person purchasing this stock after the

=(0)

(r,rJ)Q(rJ) G(rj,r o)

With modern computers, the analysis of the Burr arch-truss can be accomplished in elegant ways to mimic its actual action.

(4.2.2)

where Q(1') =

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