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How could such a loss have been avoided How could we have at least preserved a portion of the pro ts after that initial 150 percent increase Every chart is different, of course, but in this case, it probably would have been best to monitor the stock for its series of higher highs and higher lows. As long as the stock was ascending with a pattern of higher highs and higher lows, it would be a solid hold. When the price cut beneath one of the prior lows, however, it would have been a good time to get out. In this instance, it would have meant a pro t of about 50 percent (instead of 150 percent), but that s certainly a lot better than the loss that would have ensued if the position had simply been held in spite of its price action. One of the most popular securities on the market is the QQQ, often referred to as the cubes and with the ticker symbol QQQQ. This ETF tracks the performance of the NASDAQ 100 stocks, and the chart in Figure 10.21 shows the QQQ with a well-formed cup with handle and a resistance level of about $40.20. At the time of this chart, the price pushed cleanly past this resistance level, portending good times for this security. Look at the longer-term price perspective in Figure 10.22, however. The price breakout is indicated by the arrow, and as you can see, the price



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{z. (E~2 )

H~O)*} =Re {-~COSBi dk~W(ki.l - k~)Mee(ki.1,k~)}

<Pi)

(1.1.62)

FIGURE 17-6 The end view displays the complexity inherent in extending the two-hinged arch to the bearing point without interrupting the bottom chord.

[k~ cos2(<p~ -

+ ~~ sin2(<p~ - <Pi)]

Note that since only the real part contributes to power, only the propagating waves contribute in the plane wave spectrum. Note that (1.1.62) is a negative contribution making the coherent reflectivity lower than that of a flat surface. Putting (1.1.61) and (1.1.62) into (1.1.58), after making the transformation of dk -l to angular integrals, the coherent reflectivity is

(-Ss . Z coherent A)

FIGURE 10.22 In spite of the cup with handle pattern and the subsequent price action above resistance, QQQQ ultimately fell well below its former resistance level.

( 21/ )

cosO;

3 . /2 0

d<ps W(ku - k-l)

. [ cosBs cos (<Ps - <Pi)





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(1.1.63)

47f 0

+ 'Yvh)

r d<PsW(k-l- k u )

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moved up to $42, sank back down to the former resistance level, pushed higher once again to $43.50, and sank once again to the resistance level, ascending yet again (but not as high as the last time), and then nally gave up and fell hard. This certainly wasn t the result expected. The QQQ seemed to cling to the $40.20 line and fell to that level repeatedly. On its fourth fall down to that level, it no longer had the support from buyers that it needed, and it sank far beneath the initial breakout point. A person steadfastly holding onto this position would have had a substantial loss. The higher highs/higher lows would also have been helpful here. It would not take long to see that no such pattern was forming, and the position could be closed. At a minimum, however, a stop price should always be set just beneath the former resistance level. In this instance, any price action below $40.20 would be cause to immediately close out the position. Even if it means sacri cing former pro ts, at least you keep your losses to an absolute minimum.

. [cos 2 (<Ps - <Pi) cos2 Bs + sin 2 (<Ps - <Pi)]

(1.1.64)

Thus combining (1.1.63) and (1.1.64) indicates that energy conservation is exactly obeyed. The incoherent scattering intensity due to first order fields exactly balance the intensity of the second order coherent field to obey energy conservation. To calculate the second-order intensity, we need to calculate

(5.3.106)

1. Richard Sanders Allen, Covered Bridges of the Middle Atlantic States. (Brattleboro, Vermont: The Stephen Green Press, 1959). 2. C. Daniel Crews, Villages of the Lord: The Moravians Come to Carolina (Winston-Salem: Moravian Archives, 1995). 3. Susan M. Zacher, The Covered Bridges of Pennsylvania (Harrisburg, PA: Commonwealth of Pennsylvania and Museum Commission, 1994).

Using the results of (5.3.102) and (5.3.105), the momentum representation of T can be calculated from the mixed representation. In the low frequency limit we have

T p(15l,152)

= (15IITI152) = jdre-iPl.T(rITI152) =

[G~\15) -

This chapter discusses two new, related subjects: how to emphasize particular parts of a chart with highlighting and text, and how to recognize and pro t from multiple tops and bottoms. When a chart is in the process of creating a multiple top or bottom, it is helpful to be able to highlight these zones as it is happening.

[pp( _k 2 + fT,n) + (p2 - k 2 - fTm)(iJpiJp + ~p~p)]

(5.3.107b)

with f = novo as the volume fraction occupied by the particles. The solution for the effective propagation ]{ is

](2 =

(5.3.108a)

American Wooden Bridges (New York: American Society of Civil Engineers, 1976).

(5.3.108b)

Quasi-crystalline Approximation (QCA)

Cp(15l,152)

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