Impressive profits can be accumulated just by staying with a position during a trend. We would all be
millionaires if only we could identify the trend early in its onset. While the trends are obvious in
retrospect, it's another matter altogether to identify the trend in the heat of battle. Not only that, there may
not be a trend at all at the time we expect one.
If we make a reasonable mathematical model of the market we can examine it parametrically. The
conclusions we draw from this model can help us establish our entry points and strategies for trading the
trends. We will view the market as a random walk problem to create our model.
Random walk for the market
In the same way that water can only flow downstream, time cannot be reversed in trading. In addition,
prices can only be higher or lower in the same way that the river can only bend to the right or left. These
elements constrain the random walk problem to a special form that mathematicians call "drunkard's
walk." In the simplest form of this walk, the "drunk" steps only into a square diagonally to the right or
into a square diagonally to the left as he steps forward. He must make a new decision with each step. To
make the decision random, he flips a coin to determine the direction he will take. Repeated many times,
the overlay of paths that he follows will look like a smoke plume. The question of the drunkard's
destination can be answered through a well-known partial differential equation called the Diffusion
Equation. The density of the smoke particles in the plume is analogous to the probability of the
drunkard's location. A multiple-exposure photograph of the drunkard's walk repeated over and over
would show its randomness. This photograph would show the composite paths to have a uniform density, widening from the initial position. The uniform density would make the sum of the paths look like smoke
plume.
Further, random walk does not necessarily mean chaos. A minor variation of the drunkard's walk problem
is to allow the random coin-flip decision to control the change of direction rather than the direction
itself— that is, the random variable becomes momentum instead of direction. The partial differential
equation describing this condition is known as the Telegrapher's Equation. The equation describes
electric waves along telegraph wires, among other subjects. You can picture the result as the drunk
reeling back and forth. He overcorrects around a general direction trying to reach an objective. This
formulation of the problem, expressed in terms of physics, accurately portrays the river and explains why
the river meanders. In a multiple-exposure photograph the paths are still randomly distributed.
Nevertheless, the cycles are apparent in the shorter case of a single path. By analogy, the market has
short-term cycles when the appropriate conditions prevail.
If enough traders ask themselves whether the market will go up today, the random variable is direction.
Thus, conditions are established for the solution of the Diffusion Equation. On the other hand, if enough
traders ask themselves whether the trend will continue, the random variable now becomes momentum.
You could then expect the conditions to be established for the solution of the Telegrapher's Equation. The
market is ripe for short-term cycle activity.
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