Elliott Wave Principle : Chapter 4
Chapter 4
Elliott Applied
4.1 Ratio Analysis and Fibonacci Time Sequences
Ratio analysis is
the assessment of the proportionate relationship, in time and amplitude, of one
wave to another. In discerning the working of the Golden Ratio in the five up
and three down movement of the stock market cycle, one might anticipate that on
completion of any bull phase, the ensuing correction would be three-fifths of
the previous rise in both time and amplitude. Such simplicity is seldom seen.
However, the underlying tendency of the market to conform to relationships
suggested by the Golden Ratio is always present and helps generate the right
look for each wave.
The study of wave
amplitude relationships in the stock market can often lead to such startling
discoveries that some Elliott wave practitioners have become almost obsessive
about its importance. Although Fibonacci time ratios are far less common, years
of plotting the averages have convinced the authors that the amplitude (measured
either arithmetically or in percentage terms) of virtually every wave is
related to the amplitude of an adjacent, alternate and/or component wave by one
of the ratios between Fibonacci numbers. However, we shall endeavor to present
some evidence and let it stand or fall on its own merit.
The first data
reflecting time and amplitude ratios in the stock market come from, of all
suitable sources, the works of the great Dow Theorist, Robert Rhea. In 1934,
Rhea, in his book The Story of the Averages, compiled a consolidated
summary of market data covering nine Dow Theory bull markets and nine bear
markets spanning a thirty-six-year time period from 1896 to 1932. He had this
to say about why he felt it was necessary to present the data despite the fact
that no use for it was immediately apparent:
Whether
or not [this review of the averages] has contributed anything to the sum total
of financial history, I feel certain that the statistical data presented will
save other students many months of work.... Consequently, it seemed best to
record all the statistical data we had collected rather than merely that
portion which appeared to be useful.... The figures presented under this
heading probably have little value as a factor in estimating the probable
extent of future movements; nevertheless, as a part of a general study of the
averages, the treatment is worthy of consideration.
One of the
observations was this one:
The
footings of the tabulation shown above (considering only the industrial
average) show that the nine bull and bear markets covered in this review
extended over 13,115 calendar days. Bull markets were in progress 8,143 days,
while the remaining 4,972 days were in bear markets. The relationship between
these figures tends to show that bear markets run 61.1 percent
of the time required for bull periods.
And finally,
Column
1 shows the sum of all primary movements in each bull (or bear) market. It is
obvious that such a figure is considerably greater than the net difference
between the highest and lowest figures of any bull market. For example, the
bull market discussed in Chapter II started (for Industrials) at 29.64 and
ended at 76.04, and the difference, or net advance, was 46.40 points. Now this
advance was staged in four primary swings of 14.44, 17.33, 18.97, and 24.48
points respectively. The sum of these advances is 75.22, which is the figure
shown in Column 1. If the net advance, 46.40, is divided into the sum of
advances, 75.22, the result is 1.621, which gives the percent shown in Column 1. Assume
that two traders were infallible in their market operations, and that one
bought stocks at the low point of the bull market and retained them until the
high day of that market before selling. Call his gain 100 percent. Now assume
that the other trader bought at the bottom, sold out at the top of each primary
swing, and repurchased the same stocks at the bottom of each secondary reaction
— his profit would be 162.1, compared with 100 realized by the first trader.
Thus the total of secondary reactions retraced 62.1 percent of
the net advance. [Emphasis added.]
So in 1934 Robert
Rhea discovered, without knowing it, the Fibonacci ratio and its function
relating bull phases to bear in both time and amplitude. Fortunately, he felt
that there was value in presenting data that had no immediate practical
utility, but that might be useful at some future date. Similarly, we feel that
there is much to learn on the ratio front, and our introduction, which merely
scratches the surface, could be valuable in leading some future analyst to
answer questions we have not even thought to ask.
Ratio analysis has
revealed a number of precise price relationships that occur often among waves.
There are two categories of relationships: retracements and multiples.
Retracements
Occasionally, a correction retraces a Fibonacci percentage of the preceding wave. As illustrated in Figure 4-1, sharp corrections tend more often to retrace 61.8% or 50% of the previous wave, particularly when they occur as wave 2 of an impulse, wave B of a larger zigzag, or wave X in a multiple zigzag. A leading diagonal in the wave one position is typically followed by a zigzag retracement of 78.6% (ϕ√ϕ). Sideways corrections tend more often to retrace 38.2% of the previous impulse wave, particularly when they occur as wave 4, as shown in Figure 4-2.

|
Figure 4-1 |
Figure 4-2 |
Retracements come in all sizes. The ratios shown in Figures 4-1 and 4-2 are merely tendencies. Unfortunately, that is where most analysts place an inordinate focus because measuring retracements is easy. Far more precise and reliable, however, are relationships between alternate waves, or lengths unfolding in the same direction, as explained in the next section.
Motive Wave Multiples
Chapter 2 mentioned that when wave 3 is extended, waves 1 and 5 tend towards equality or a .618 relationship, as illustrated in Figure 4-3. Actually, all three motive waves tend to be related by Fibonacci mathematics, whether by equality, 1.618 or 2.618 (whose inverses are .618 and .382). These impulse wave relationships usually occur in percentage terms. For instance, wave I from 1932 to 1937 gained 371.6%, while wave III from 1942 to 1966 gained 971.7%, or 2.618 times as much. Semilog scale is required to reveal these relationships. Of course, at small degrees, arithmetic and percentage scales produce essentially the same result, so that the number of points in each impulse wave reveals the same multiples.

|
Figure 4-3 |
Figure 4-4 |
Figure 4-5 |
Another typical
development is that wave 5’s length is sometimes related by the Fibonacci ratio
to the length of wave 1 through wave 3, as illustrated in Figure 4-4, showing
an extended fifth wave. .382 and .618 relationships occur when wave five is not
extended. In those rare cases when wave 1 is extended, it is wave 2, quite
reasonably, that often subdivides the entire impulse wave into the Golden
Section, as shown in Figure 4-5.
Here is a generalization that subsumes some of the observations we have already made: Unless wave 1 is extended, wave 4 often divides the price range of an impulse wave into the Golden Section. In such cases, the latter portion is .382 of the total distance when wave 5 is not extended, as shown in Figure 4-6, and .618 when it is, as shown in Figure 4-7. Real life examples are shown in Figures 6-8 and 6-9. This guideline is somewhat loose in that the exact point within wave 4 that effects the subdivision varies. It can be its start, end or extreme countertrend point. Thus, it provides, depending on the circumstances, two or three closely clustered targets for the end of wave 5. This guideline explains why the target for a retracement following a fifth wave often is doubly indicated both by the end of the preceding fourth wave and the .382 retracement point.

|
Figure 4-6 |
Figure 4-7 |
Corrective Wave Multiples
In a zigzag, the
length of wave C is usually equal to that of wave A, as shown in Figure 4-8,
although it is not uncommonly 1.618 or .618 times the length of wave A. This
same relationship applies to a second zigzag relative to the first in a double
zigzag pattern, as shown in Figure 4-9.
In a regular flat correction, waves A, B and C are, of course, approximately equal, as shown in Figure 4-10. In an expanded flat correction, wave C is often 1.618 times the length of wave A. Sometimes wave C will terminate beyond the end of wave A by .618 times the length of wave A. Each of these tendencies is illustrated in Figure 4-11. In rare cases, wave C is 2.618 times the length of wave A. Wave B in an expanded flat is sometimes 1.236 or 1.382 times the length of wave A.

|
Figure 4-8 |
Figure 4-9 |

Figure 4-10

Figure 4-11
In a triangle, we have found that at least two of the alternate waves are typically related to each other by .618. I.e., in a contracting or barrier triangle, wave e = .618c, wave c = .618a, or wave d = .618b, as illustrated in Figure 4-12. In an expanding triangle, the multiple is 1.618.

Figure 4-12
In double and triple
corrections, the net travel of one simple pattern is sometimes related to
another by equality or, particularly if one of the threes is a triangle, by
.618.
Finally, wave 4
quite commonly spans a gross and/or net price range that has an equality or
Fibonacci relationship to its corresponding wave 2. As with impulse waves,
these relationships usually occur in percentage terms.
4.2 Applied Ratio Analysis
Elliott himself, a
few years after Rhea’s book, was the first to realize the applicability of
ratio analysis. He noted that the number of DJIA points between 1921 and 1926,
encompassing the first through third waves, was 61.8% of the number of points
in the fifth wave from 1926 to 1928 (1928 is the orthodox top of the bull
market according to Elliott). Exactly the same relationship occurred again in
the five waves up from 1932 to 1937 (for reference, see Figures 2-11 and 2-12).
A. Hamilton Bolton,
in the 1957 Elliott Wave Supplement to the Bank Credit Analyst,
gave this price forecast based on expectations of typical wave behavior:
The
powerhouse that will be building up if the market consolidates for another year
or so along orthodox lines, it seems to us, will offer the probability that
Primary V could be quite sensational, taking the DJIA to 1000 or more in the
early 1960s in a wave of great speculation.
Then, in The Elliott
Wave Principle — A Critical Appraisal, reflecting on examples cited by
Elliott, Bolton stated,
Should
the 1949 market to date adhere to this formula, then the advance from 1949 to
1956 (361 points in the DJIA) should be completed when 583 points (161.8% of
361 points) have been added to the 1957 low of 416, or a total of 999 DJIA.
Alternatively, 361 over 416 would call for 777 in the DJIA.
Later, when Bolton
wrote the 1964 Elliott Wave Supplement, he concluded,
Since
we are now well past the 777 level, it looks as if 1000 in the averages could
be our next target.
The year 1966 proved
those statements to be the most accurate prediction in stock market history,
when the 3:00 p.m. hourly reading on February 9th registered a high at 995.82
(the "intraday" high was 1001.11). Six years prior to the event, then,
Bolton was right to within 3.18 DJIA points, less than one third of one percent
error.
Despite this
remarkable portent, it was Bolton’s view, as it is ours, that wave form
analysis must take precedence over the implications of proportionate
relationships. Indeed, when undertaking a ratio analysis, it is essential that
one understand and apply the Elliott counting and labeling method to determine
from which points the measurements should be made in the first place. Ratios
between lengths based on orthodox pattern termination levels are reliable;
those based on nonorthodox price extremes generally are not.
The authors
themselves have used ratio analysis, often with satisfying success. A.J. Frost
became convinced of his ability to recognize turning points by catching the
"Cuban crisis" low in October 1962 the hour it occurred and
telegraphing his conclusion to Hamilton Bolton in Greece. Then, in 1970, in a
supplement to The Bank Credit Analyst, he determined that the bear
market low for the Cycle wave correction in progress would probably occur at a
level .618 times the distance of the 1966 decline below the 1966 low, or 572.
Four years later, the DJIA’s hourly reading in December 1974 at the exact low
was 572.20, from which the explosive rise into 1975-76 occurred.
Ratio analysis has
value at smaller degrees as well. In the summer of 1976, in a published report
for Merrill Lynch, Robert Prechter identified the fourth wave then in progress
as a rare expanding triangle, and in October used the 1.618 ratio to determine
that the maximum expected low for the eight-month pattern should be 922 on the
Dow. The low occurred five weeks later at 920.63 at 11:00 on November 11,
launching the year-end fifth-wave rally.
In October 1977,
five months in advance, Mr. Prechter computed a probable level for the 1978
major bottom as "744 or slightly lower." On March 1, 1978, at 11:00,
the Dow registered its low at exactly 740.30. A follow-up report published two
weeks after the bottom reaffirmed the importance of the 740 level, noting that:
...the
740 area marks the point at which the 1977-78 correction, in terms of Dow
points, is exactly .618 times the length of the entire bull market rise from
1974 to 1976. Mathematically we can state that 1022 - (1022-572).618 = 744 (or
using the orthodox high on December 31st, 1005 - (1005-572).618 = 737). Second,
the 740 area marks the point at which the 1977-78 correction is exactly 2.618
times the length of the preceding correction in 1975 from July to October, so
that 1005 - (885- 784)2.618 = 742. Third, in relating the target to the internal
components of the decline, we find that the length of wave C = 2.618 times the
length of wave A if wave C bottoms at 746. Even the wave factors as researched in the April
1977 report mark 740 as a likely level for a turn. At this juncture then, the
wave count is compelling, the market appears to be stabilizing, and the last
acceptable Fibonacci target level under the Cycle dimension bull market thesis
has been reached at 740.30 on March 1st. It is at such times that the market,
in Elliott terms, must "make it or break it."
The three charts from that report are reproduced here as Figures 4-13 (with a few extra markings to condense comments from the text), 4-14 and 4-15. They illustrate the wave structure into the recent low from Primary down to Minuette degree. Even at this early date, 740.30 seems to be firmly established as the low of Primary wave ② in Cycle Wave V.

Figure 4-13

Figure 4-14

Figure 4-15
The 740 level has
proved important other times in the past as well, quite possibly because while
the 1974 low at 572.20 lies exactly 423.60 points under the 1966 peak at
995.82, 740.30 lies approximately 261.80 points under the 1004.65 level, the
orthodox top in 1976. Both of these distances are expressions of Fibonacci
ratios. Mr. Prechter further discussed the 740 level as follows:
It
is certainly not coincidence that the 740 level has proved of some importance
in the past. In 1961, the intraday Dow peak at 741.30 accompanied the highest
market P/E ratio in history; in 1966, the intraday low of 735.74 marked the end
of the first slide to the measuring low in the Cycle wave IV bear market (the
point which was 61.8% of the entire decline of Cycle wave IV); in 1963, 1970,
1974 and 1975, breaks through 740 in each direction accompanied extreme
violence; in 1978, the 740 level corresponds with long term trendline support.
Furthermore, the Wave Principle holds that the limit of any market correction
is the bottom of the previous fourth wave of lesser degree. When the first wave
in a five-wave sequence extends, however, the limit of the ensuing correction
is often the bottom of the second wave of that five-wave sequence. Given this
guideline, the recent low on March first at 740.30 was a remarkable level at
which to stop. A check with the hourly back figures as printed in the Wall
Street Journal reveals that on March 25,
1975 the DJIA bottomed at 740.30 to complete the pullback of the second wave.
[See note on Figure 4-13.]
In addition to the
more traditional Elliott forecasting methods, Mr. Prechter has begun to
research mathematical wave factors in terms of both time and price, of which
motive waves have been found to be whole number multiples and corrective waves
Fibonacci ratio multiples. The approach was discussed recently in several
reports for Merrill Lynch.
Undoubtedly to some
it will seem that we are patting ourselves on the back, which we most certainly
are! Truthfully, though, we are hoping that an account of the successes which
we have personally experienced with Elliott will inspire others to strive for
similar achievements using this approach. To our knowledge, only the Wave
Principle can be used to forecast with such accuracy. Of course, we have
experienced failures as well, but nevertheless we feel that any drawbacks in
the Elliott wave approach have been grossly overstated in the past, and that
when expectations with regard to the market are not fulfilled, the Wave
Principle warns the analyst in plenty of time to chart the next most likely
course and to avoid losses by letting the market itself dictate his course of
action.
We have found that
predetermined price objectives are useful in that if a
reversal occurs at that level and the wave count is acceptable, a doubly
significant point has been reached. When the market ignores such a level or
gaps through it, you are put on alert to expect the next calculated level to be
achieved. As the next level is often a good distance away, this can be
extremely valuable information. Moreover, targets are based upon the most satisfying
wave count. Thus, if they are not met or are exceeded by a significant margin,
in many instances you will be forced in a timely manner to reconsider your
preferred count and investigate what may be rapidly developing as a more
attractive interpretation. This approach helps keep you one step ahead of nasty
surprises. It is a good idea to keep all reasonable wave interpretations in
mind so you can use ratio analysis to obtain additional clues as to which one
is operative.
4.3 Multiple Wave Relationships
Keep in mind
that all
degrees of trend are always operating in the market at the same time.
Therefore, at any given moment, the market will be full of Fibonacci ratio
relationships, all occurring with respect to the various wave degrees
unfolding. It follows that future levels that will create several Fibonacci
relationships have a greater likelihood of marking a turn than a level that
will create only one.
For instance, if a .618 retracement of Primary wave ① by Primary wave ② gives a particular target, and within it, a 1.618 multiple of Intermediate wave (A) in an irregular correction gives the same target for Intermediate wave (C), and within that, a 1.00 multiple of Minor wave 1 gives the same target yet again for Minor wave 5, then you have a powerful argument for expecting a turn at that calculated price level. Figure 4-16 illustrates this example.

Figure 4-16
Figure 4-17 is an
imaginary rendition of a reasonably ideal Elliott wave, complete with parallel
trend channel. It has been created as an example of how ratios are often
present throughout the market. In it, the following eight relationships hold:
② = .618 x ①;
④ = .382 x ③;
⑤ = 1.618 x ①;
⑤ = .618 x Ⓞ → ③;

Figure 4-17
② = .618 x ④;
in ②, (A) = (B) = (C);
in ④, (A) = (C);
in ④, (B) = .382 x (A).
If a complete method of ratio analysis could be successfully resolved into basic tenets, forecasting with the Elliott Wave Principle would become more scientific. It will always remain an exercise to determine probability, however, not certainty. Nature’s laws governing life and growth, though immutable, nevertheless allow for an immense diversity of specific outcome, and the market is no exception. All that can be said at this point is that comparing the price lengths of waves frequently confirms, often with pinpoint accuracy, that Fibonacci ratios are a key determinant of where waves will stop. It was awe-inspiring, but no surprise to us, for instance, that the advance from December 1974 to July 1975 traced just over 61.8% of the preceding 1973- 74 bear slide, and that the 1976-78 market decline traced exactly 61.8% of the preceding rise from December 1974 to September 1976. Despite the continual evidence of the importance of the .618 ratio, however, our basic reliance must be on form, with ratio analysis as evidence to support or challenge what we see in the patterns of movement. Bolton’s advice with respect to ratio analysis was, "Keep it simple." Research may still achieve further progress, as ratio analysis is still in its infancy. We are hopeful that those who labor with the problem of ratio analysis will add worthwhile material to the Elliott approach.
Fibonacci
Time Sequences
There is no sure way
of using the time factor by itself in forecasting. Elliott said that the time
factor often "conforms to the pattern," for instance with regard to
trend channels, and therein lies its primary significance. Frequently, however,
durations and time relationships themselves reflect Fibonacci measurements.
Exploring Fibonacci numbers of time units appears to go beyond an exercise in
numerology, fitting wave spans with remarkable accuracy. They serve to give the
analyst added perspective by indicating possible times for a turn, especially
if they coincide with price targets and wave counts.
In Nature’s Law, Elliott gave the following examples of Fibonacci time spans between important turning points in the market:

In Dow Theory Letters on November 21, 1973, Richard Russell gave some additional examples of Fibonacci time periods:

Walter E. White, in
his 1968 monograph on the Elliott Wave Principle, concluded that "the next
important low point may be in 1970." As substantiation, he pointed out the
following Fibonacci sequence: 1949 + 21 = 1970; 1957 + 13 = 1970; 1962 + 8 =
1970; 1965 + 5 = 1970. May 1970, of course, marked the low point of the most
vicious slide in thirty years. Taken in toto, these distances appear to be a bit more than
coincidence.
The progression of years from the 1928 (possible orthodox) and 1929 (nominal) high of the last Super cycle produces a remarkable Fibonacci sequence as well:

A similar series has begun at the 1965 (possible orthodox) and 1966 (nominal) highs of the third Cycle wave of the current Super cycle:

Thus, we foresee
some interesting possibilities with respect to DJIA turning points in the near
future. These possibilities are further explored in Chapter 8.
Besides their
significant frequency, there is reason to believe that Fibonacci numbers and
ratios of time units in the stock market are something other than numerology.
For one thing, natural time units are related to the Fibonacci sequence. There
are 365.24 days in a year, just shy of 377. There are 12.37 lunar cycles in a
year, just shy of 13. The ratios between these actual numbers and Fibonacci
numbers are .9688 and .9515. When the Earth’s orbit and rotation were faster,
these numbers would have been concurrently quite close to actual Fibonacci
numbers. (Might the solar system have begun its periodicities at those
frequencies?) Music of the spheres, indeed.
There are also 52.18
weeks in a year, just shy of 55. Weeks may not be natural time units, but the
fact that there are four weeks in a month forces weeks into a near-Fibonacci
relationship with months because Fibonacci numbers x 4.236 yield other
Fibonacci numbers. Any duration of a Fibonacci number of months will be close
to a Fibonacci number of weeks as well. For example, 13 months = 56 (55 + 1)
weeks. There is no reason to believe that man-made time constructs such as
minutes and centuries should follow Fibonacci time sequences, but we have not
investigated such durations.
We have noted that the longer the duration of a wave sequence, the further it tends to deviate from a Fibonacci number of time units. The range of deviation itself appears to create a Fibonacci progression as the durations increase. Here are the typical time durations of wave sequences in natural units of time (days, weeks, months, years), along with their ranges of deviation:

In applying
Fibonacci time periods to the pattern of the market, Bolton noted that time
"permutations tend to become infinite" and that time "periods
will produce tops to bottoms, tops to tops, bottoms to bottoms or bottoms to
tops." Despite
this reservation, he
successfully indicated within the same book, which was published in 1960, that
1962 or 1963, based on the Fibonacci sequence, could produce an important
turning point. 1962, as we now know, saw a vicious bear market and the low of
Primary wave ④, which preceded a virtually uninterrupted advance lasting nearly
four years.
In addition to this
type of time sequence analysis, the time relationship between bull and bear as
discovered by Robert Rhea has proved useful in forecasting. Robert Prechter, in
writing for Merrill Lynch, noted in March 1978 that "April 17 marks the
day on which the A-B-C decline would consume 1931 market hours, or .618 times
the 3124 market hours in the advance of waves (1), (2) and (3)." Friday,
April 14 marked the upside breakout from the lethargic inverse head and
shoulders pattern on the Dow, and Monday, April 17 was the explosive day of
record volume, 63.5 million shares (see Figure 1-18). While this time
projection did not coincide with the low, it did mark the exact day when the
psychological pressure of the preceding bear was lifted from the market.
4.4 Benner's Theory
Samuel T. Benner was
an ironworks manufacturer until the post-Civil War panic of 1873 ruined him
financially. He turned to wheat farming in Ohio and took up the statistical
study of price movements as a hobby to find, if possible, the answer to the
recurring ups and downs in business. In 1875, Benner wrote a book
entitled Business
Prophecies of the Future Ups and Downs in Prices. The forecasts
contained in his book are based mainly on cycles in pig iron prices and the
recurrence of financial panics. Benner’s forecasts proved remarkably accurate
for many years, and he established an enviable record for himself as a
statistician and forecaster. Even today, Benner’s charts are of interest to
students of cycles and are occasionally seen in print, sometimes without due
credit to the originator.
Benner noted that the highs of business tend to follow a repeating 8-9-10 yearly pattern. If we apply this pattern to high points in the Dow Jones Industrial Average over the past seventy-five years starting with 1902, we get the following results. These dates are not projections based on Benner’s forecasts from earlier years, but are only an application of the 8-9-10 repeating pattern applied in retrospect.

With respect to economic low points, Benner noted two series of time sequences indicating that recessions (bad times) and depressions (panics) tend to alternate (not surprising, given Elliott’s rule of alternation). In commenting on panics, Benner observed that 1819, 1837, 1857 and 1873 were panic years and showed them in his original "panic" chart to reflect a repeating 16-18-20 pattern, resulting in an irregular periodicity of these recurring events. Although he applied a 20-18-16 series to recessions, or "bad times," less serious stock market lows seem rather to follow the same 16-18-20 pattern as do major panic lows. By applying the 16-18-20 series to the alternating stock market lows, we get an accurate fit, as the Benner-Fibonacci Cycle Chart (Figure 4-18), first published in the 1967 supplement to the Bank Credit Analyst, graphically illustrates.

Figure 4-18
Note that the last
time the cycle configuration was the same as the present was the period of the
1920s, paralleling both the Kondratieff picture, which we discuss in Chapter 7,
and the last occurrence of a fifth Elliott wave of Cycle degree.
This formula, based upon Benner’s idea of repeating time series for tops and bottoms, has fit most of this century’s stock market turning points. Whether the pattern will always reflect future highs is another question. These are fixed cycles, after all, not Elliott. Nevertheless, in our search for the reason for its fit with reality, we find that Benner’s theory conforms reasonably closely to the Fibonacci sequence in that the repeating series of 8-9-10 produces Fibonacci numbers up to the number 377, allowing for a marginal difference of one point, as shown below.

Our conclusion is that Benner’s theory, which is based on different rotating time periods for bottoms and tops rather than constant repetitive periodicities, falls within the framework of the Fibonacci sequence. Had we no experience with the approach, we might not have mentioned it, but it has proved useful in the past when applied in conjunction with a knowledge of Elliott wave progression. A.J. Frost applied Benner’s concept in late 1964 to make the inconceivable (at the time) prediction that stock prices were doomed to move essentially sideways for the next ten years, reaching a high in 1973 at about 1000 DJIA and a low in the 500 to 600 zone in late 1974 or early 1975. A letter sent by Frost to Hamilton Bolton at the time is reproduced on the following page. Figure 4-19 is a reproduction of the accompanying chart, complete with notes. As the letter was dated December 10, 1964, it represents yet another long term Elliott prediction that turned out to be more fact than fancy.


Figure 4-19
Although we have been able to codify ratio analysis
substantially as described in the first half of this chapter, there appear to
be many ways that the Fibonacci ratio is manifest in the stock market. The
approaches suggested here are merely carrots to whet the appetite of
prospective analysts and set them on the right track. Parts of the following
chapters further explore the use of ratio analysis and give perspective on its
complexity, accuracy and applicability. Obviously, the key is there. All that
remains is to discover how many doors it will unlock.