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By using (6.2.52) through (6.2.58), the conditional average of the exciting field can be solved. Equations (6.2.52) and (6.2.53) are homogeneous linear equations for the coefficients y;,}M) and y;,}N). For a nontrivial solution to exist, the determinant must vanish giving the dispersion equation from which K is determined. The solution for K is the same as that for normal incidence as in Section 1. There is also an eigenvector associated with the solution of J( with an arbitrary constant multiplying the eigenvector. That arbitrary constant is then determined by using the single inhomogeneous equation of (6.2.58). The values of y,}M) and y,}N) are then uniquely determined. The conditional-averaged exciting field is then given by (6.2.47) and (6.2.48). To calculate the coherent reflected field, substitute (6.2.47) and (6.2.48) in (6.2.45). The Mj integration can be carried out readily. It follows that 2 ';-11.+1_ ( - ) iK :1'7f,,/mn" ik :1'- ( ) (6.2.59a) MjMmnkrrje d J=k'_(K k)e' CmnBi, i zJ<O k zz Z + 'lZ n iK /.1' 27f"/mn i ik :;:- ( ) ( ) MjNmn krrj e ' J = - kk- (K k-) e ' B mn Bi, i 6.2.59b Note that because of statistical translational invariance in the horizontal plane, the integration of dfj over the lower half-space in (6.2.59a) and (6.2.59b) gives a specularly reflected wave for the coherent field. Substituting (6.2.59a) and (6.2.59b) into (6.2.45), we have the coherent reflected field as



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1 - (-) 1

27fn + _ --J..-)(} (E s -)\ = kk'-(K o i k._)e ik,.:;: ""'(_1)1n (2n 1 1) {T(Mly(MlClnn (() ll,/-,l td (r i L..t ( +) n 11. 'lZ Z + lZ n n lnn

FIGURE 12.32 The typical movement seen here is a break beneath the neckline followed by a strengthening of the stock back to a point just underneath the same line.

. C- mn (7f - ()t, i)

+ Tl~Nly,}Nl Bmn(()i, i)fJtd B- mn (7f - ()t, i)} (6.2.60)

Next, we make use of the vector addition theorem of (6.2.55a) and (6.2.55b). For this case B = B-i , = i, B' = 7f - ()t, and ' = i, so that (r . r') = - cos Bi cos Bt + sin Bi sin Bt = - cos( Bi + Bt}. The final result for the coherent reflected field is

(EsC-f))





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= fJ i 27fn o eik,.:;:_'f_

Historic structures provide the best laboratories for basic research in materials. The service life of a material or system can best be observed in an installation that has experienced cycles of thermal and moisture changes, long periods of sunlight, and gravitational force. Accumulated knowledge in preservation technology offers a broader palette of solutions. For example, a structural system to replace a historic hammer-beam truss in a church could be a steel frame clad in wood, a glued laminated timber frame with bolted connections and steel side plates, or a traditional timber frame with dovetail and mortise-andtenon connections, or multiple leaves of prefabricated nail plate trusses. The structural system could be built with precast concrete or extruded aluminum box sections, or the frame could consist of ber-reinforced plastic resin structural elements simply grained to look like wood. The nal decision should depend on what is most appropriate for the project, rather than what is most comfortable for the engineer. Unfortunately, there is little incentive for the construction-material industry to spend money on historic-materials research. Basic research focuses on

+Kz)

L( _1)n (2n + 1) {Y,}M)TfVI)

n(n + 1)

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Pl~ (cos(Bi + Bt )) + y(N)T(N) [cot(B . n 11. sm (B i + Bt ) + n(n + l)Pn (cos(Bi + ()t))]}

which is somewhat unusual, but the downtrend was orderly as the stock lost about 60 percent of its value after the break. Many of the examples used in this chapter are from companies that perhaps you had not heard of before. Important technical patterns such as the H&S certainly are not restricted to small stocks, however. In Figure 12.34, General Electric s stock price carved out a very good H&S pattern with predictable results. Even though the H&S pattern is widely recognized, the vast majority of traders even those involved with gigantic stocks like GE do not understand its power and application. On some occasions you will see an H&S pattern form above a price gap. A price gap is an instance, in this case, where a stock s price opens at a price far above the prior day s close and whose trading remains at or higher than the opening price, thus creating a gap in the price graph between where the previous day s price has closed and where the current day s price had opened. An H&S pattern will usually form a neckline at or above the high point of the gap. An example of this is shown in Figure 12.35, where the $78 neckline is just above the price gap. It is not surprising that this level

+ () )pl (cos(B + () ))

(6.2.61)

where k i = k(sin ()i cos ix+sin ()i sin dJ+cos ()iZ) denotes the upward propagating direction that is specularly related to the downward incident wavevec-

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