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One nice feature of breakouts is that they often give traders a second chance to get in after the breakout. This temporary softening in prices after the breakout is known as a pullback, and it is caused by a portion of the owners of the stock anxious to bank their pro ts on their stock s newfound price activity. Imagine a hypothetical group of 1,000 people, each of whom owned shares in a company that had been trading between $10 and $12 for years. If the stock nally breaks out and hits $15, you can understand the excitement of these owners, since they have been holding a do-nothing stock for years and it is nally showing signs of life. Although most of these owners may be patient enough to let their pro ts build, there is going to be a subset of this group that will want to get out of the stock immediately and take their pro ts. The psychology behind this group is understandable too after all, their stock has done absolutely nothing, and now it is giving them an opportunity to get out with some extra cash. So some people let s say 100 out of the group of 1,000 immediately place orders to sell the stock at the current market price. This in ux of selling is going to cause the price to soften, at least temporarily. It usually will head back to the upper end of its former trading range, at which point selling will dry up since any newfound pro ts

When t = 0, this reduces to p = - 3v 3/2 for small v, which shows that the critical isotherm is an odd function about the critical point. For t < 0, the same approximation gives

which shows that the isotherm is a odd function about a point displaced from the critical point by 8t/3 along the p axis. Therefore, the Maxwell construction will yield coexisting volumes VI' V; that are symmetrically placed about the critical volume V = 1:

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(17.57)

we obtain (17.58)

x=20

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Hence f3 = !. The specific heat cannot be calculated because (17.50) is determined only up to a function of the temperature. Assuming it to be such as to give ideal gas behavior at large V, we obtain a = 0. In summary, the critical exponents have "classical" values. If we were interested only in the neighborhood of the critical point, we would write down a mean field theory identical to (17.37), with m identified with VI - v 2 , the specific-volume difference of the coexisting phases, and H with P - 1. We would arrive at the same critical exponents, although the model would be quite different. In the model we just discussed, VI - V 2 is a calculated quantity, and not a free variable. Mean-field theory, as we can see, has many guises, but they lead to the same critical exponents for theories of the same class.

(17.59)

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