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wind and fall, ultimately, to about 55 cents. There was plenty of time to pro t from selling this stock short or owning puts on it. Every stock chart tells a different story, and even though patterns often play out with similar directional movements, the speed of those movements varies quite a bit. Figure 9.26 provides a nice contrast to the LU graph. We see the classic signs of a rounded top: the well-de ned support line, the break beneath support, and the subsequent recovery up to the former support level. Unlike Lucent, however, this stock subsequently only took about a week to wipe out virtually all of its equity value. Those who entered short positions at the recovery level of about $7 would have enjoyed very rapid pro ts in this case. Another crucial aspect of rounded tops is that, to be pro table, they need to be preceded by a meaningful ascent in price. If a stock has traded between $10 and $12 for years, and then it creates a rounded top between $12 and $13, it s not going to matter very much if it falls beneath its support level. The reason is that there is already a huge mass of buyers from $10 to $12 to support it. A more exciting pattern would be for a stock that has gone from $1 to $80 and forms a rounded top between $80 and $90. In that instance, the stock has plenty of room to fall. Take Ipsco (symbol IPS) as an example, shown in Figure 9.27. There is a rounded top over the span of about two-and-a-half months starting in March and ending in mid-May. In less than a year the stock has risen from

(18.56)

(18.57)

2. Rescaling. Restore the cutoff to A by increasing the unit of length by a factor b, by changing the variable of integration to

(18.58)

Click the Home tab on the Ribbon. Click an indent button. You can click the Decrease Indent button ( ) to decrease the indentation. You can click the Increase Indent button ( ) to increase the indentation.

(18.59)

3. Normalization. Restore the standard normalization of the order parameter, i.e., make the coefficient of the k,2 term in (18.59) equal to !. This can be done by replacing m(k) by

m'( k') ==

Solvent: no' Solute: 0

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former support line. This is the ideal low risk/high reward scenario. Figure 1.8 is an example of just this circumstance, with Ariba (symbol ARBA) forming a very nice head and shoulders pattern from July through November. Once prices broke beneath the neckline, the stock went from about $600 to $300. But for the rst couple of weeks of December, buyers pushed the stock back to about $550, still below the neckline. (Note: these prices are adjusted for reverse stock splits.) This is a test of the pattern. The pattern has already established itself, and the chart is bearish, but buyers are still trying to push the stock higher. You can almost picture the bulls and bears in a tug-of-war with the neckline being in the middle of the battle. In this case, shorting the stock at $550 would have been brilliant, because after testing the pattern, the price started to sink virtually without pause until almost all the equity was wiped out. Take a look at Figure 1.9, which is a very similar chart. Broadcom (symbol BRCM) managed to survive the initial burst of the NASDAQ bubble in the rst half of 2000. By October of that year, it broke beneath the neckline in a very well-formed head and shoulders pattern, and it didn t stop once to test that level again. The stock plummeted from $130 to under $10 per share in a couple of years.

ture and the total volume of the composite system held fixed. Then n a suffers a change dna, and no suffers a change -dna, for, as far as the pure solvent is concerned, the membrane is nonexistent. The volume of the solution changes by the amount va dn o' The work done by the entire composite system is

dW = P'vo dna (2,47)

According to the second law this is equal to the negative of the change in free energy dA, given by (2,48) Therefore

Since n1/n a 1, however, V = n ova is just the volume occupied by the solution. Hence (2,49) It is easy to see that the boiling point of a solution is higher than that of the pure solvent, on account of osmotic pressure. To deduce the change in boiling point, let us first find the difference between the vapor pressure of a solution and that of a pure solvent. This can be done by considering the arrangement shown in Fig. 2.14, which is self-explanatory. Under equilibrium conditions the difference between the pressures is the difference between the pressures of the vapor at B and at C. The pressure at C, however, is the same as that at A, because the vapor is at rest. Hence (2.50) where p' is the mass density of the vapor. On the other hand, the osmotic pressure is by definition equal to the pressure exerted by the column of solution of height h:

(2.51)

Click the Home tab on the Ribbon. Click the corner group button ( ) in the Paragraph group. The Paragraph dialog box appears.

Fig. 2.14 Aid in the derivation of the difference in vapor pressure of a solution and the pure solvent.

(2.52)

(2.53)

FIGURE 1.9 Broadcom, one of the hottest stocks of the Internet bubble, collapsed after a head and shoulders pattern in late 2000.

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