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Stocks & Commodities V17:2 (101-106): Moving Averages, First Principles by Brian J. Millard
Copyright (c) Technical Analysis Inc.
BASIC TECHNIQUES
Moving Averages,First Principles
O
Dont quite understand moving averages, but think that you
could benefit from using them? Heres how to understand
and apply moving averages to identifying trends in stocks.
By Brian J. Millard
f all the technical indicators,
moving averages are perhaps
the most widely used andmis-
understood. Incorrectly applied,
as is usually the case, they may
be responsible for more losses
than any other indicator. Cor-
rectly applied, however, they
can be the most versatile and
powerful tools available. The
reasons for failure? First, a poor
understanding of how stock
prices move, and second, a poor understanding of the
properties of moving averages.
It is important to note that if the user does not attempt to
understand how prices move, then applying any indicator is
a haphazard affair. Indicators tend to be developed by trialand error, and without a clear understanding of how they
work, using them can lead to disappointing and disastrous
results.
STOCKPRICEMOVEMENTThe point-to-point movement modelis based partly on the
one put forward by analyst J.M. Hurst a number of years ago
and partly on my own research. In this model, stock move-
ment is considered to be composed of random point-to-point
movement and complex cyclic movement. Point-to-point
movementis simply a generalization of the sampling interval
and refers to the change between one data point and the next,
such as tick-to-tick, day-to-day, and week-to-week, aswell as others.
POINT-TO-POINTMOVEMENTPoint-to-point movement is easily extracted from stock data
by most technical analysis programs. An indicator is usu-
ally available that will give the difference between succes-
sive points; if not, such an indicator can often be created
within the program. As an alternative, stock price data can
be imported into a spreadsheet and the successive differ-
ences calculated and plotted. This method is useful, since a
spreadsheet function will be available to determine the
standard deviation of these differences, a valuable quantity
that will be discussed later.
The point-to-point differences can have negative, positive,
or zero (no change from the previous point) values. A plot of
these daily differences over a short period can be seen in
Figure 1. The vertical grids are spaced at 10-day intervals,
and the vertical scale is in dollars. A sequence of changes in
the same direction is indicated by the plot remaining on the
same side of the zero line.
A close inspection of the differences reveals that the
longest such sequence occurred between June 18 and July 2,
1998, and extended to eight successive rises. The extreme
peaks and troughs have no meaning other than they are the
maximum changes recorded. In general, a sequence of more
than 10 successive moves in the same direction in a stock
almost never occurs.
During this period of 191 trading days, there were 99 rises,
87 falls, and four no change. There was a slightly higher
probability (52%) of a rise than there was a fall. There were
102 occasions when the change was in the same direction as
the previous change and 87 occasions when it was not. There
was a slightly higher probability (54%) of a change occurring
in the same direction as the previous change.The preponderance of probabilities one way or the other
is one of the factors that produces the overall trend in the
stock price over a period. Usually, these probabilities are so
close to 50% as to offer no advantage in predicting the
direction of the price movement.
A more thorough study of these point-to-point move-
ments, however, uncovers the fact that the occurrence of
various movements in the same direction is slightly higher
than called for on a purely random basis, but this is of no help
when it comes to predicting the next move. As far as the
model is concerned, we can consider point-to-point move-
ment to be purely random.
CYCLICMOVEMENTBesides point-to-point movement, the other component of
price movement is composed of cycles of differing wave-
length, magnitude, and phase. The wavelengthis the distance
between successive peaks or troughs, and the magnitudeis
the vertical distance between a peak and the next trough or a
trough and the next peak. The phase is the relationship
between a peak and a given starting point. It is instructive to
examine just one such cycle say, the nominal 41-week
cycle in IBMstock especially for investors who do not
subscribe to cycle theory.
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Stocks & Commodities V17:2 (101-106): Moving Averages, First Principles by Brian J. Millard
Copyright (c) Technical Analysis Inc.
CHRISTINE
MORRISON 7
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5/21/98
6/4/98
6/18/98
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7/16/98
7/30/98
8/13/98
8/27/98
9/10/98
IBM (Daily differences)The nominal 41-week cycle is isolated from the weekly
closing prices in IBM, as can be seen in Figure 2 by a
method involving two moving averages. The point in
Figure 2 is that the distance between peaks and troughs
varies as we move across the plot; that is, the wavelengthis constantly changing.
Because of this, the expression nominal wavelengthis used
when referring to a particular cycle in market data, meaning
the average wavelength of an individual cycle over a period.
The other changing parameter is the magnitude the verti-
cal distance from a trough to the next peak or from a peak to
the next trough.
The phase of the cycle might also be changing, but the
effect of change in phase is to give the appearance of a change
in wavelength.In this way, phase change and wavelength
change can be lumped together as wavelength change. TheFIGURE 1: DAILY DIFFERENCES. The differences between one days closingprice and the next is plotted for IBM stock over a four-month period.
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Stocks & Commodities V17:2 (101-106): Moving Averages, First Principles by Brian J. Millard
Copyright (c) Technical Analysis Inc.
variation in wavelength is less severe than in magnitude, and
thus, the next turning point in a cycle is predictable within
fairly narrow limits.
Much wider limits must be applied to a prediction of
magnitude. In general, cycles pass though periods when their
behavior is reasonably predictable and other periods when
they are less so.Many cycles are present in the movement of an individual
stock, some of which may be universal to all stocks and others
unique to that one. The fact that some cycles are universal to
all stocks (for example, a nominal 41-week cycle can be
shown to be present in all the S&P 500 stocks by using the
moving average method used for IBMin Figure 2) does not
necessarily mean that they will pass through peaks and
troughs at the same time. They do occasionally, and it is at this
point that extreme rises and falls in the market occur.
It is debatable whether the market influence causes cycles to
come into phase with each other. Each of these cycles will go
through this variation in wavelength and magnitude, but the
variation among a group of cycles of contiguous wavelengths,covering a large band of wavelengths, can often cancel each
other out. As a result, the behavior of such a group is much
more predictable than the behavior of an individual cycle.
Now that we have a model of stock price movement,
we can investigate the properties of moving averages and
how these properties may be of use in the interpretation
of such movement.
PROPERTIESOFMOVINGAVERAGESWhile it might seem trivial, it is important to understand the
procedure by which a simple average is calculated, since
then it is possible to understand the main property of an
average. An average is derived from a running total
calculated, for example, for an n-point average by adding
up the first ndata points. The running total for the next
calculation is modified by adding the next data point and
dropping the first. Thus, the procedure is to constantly
modify the running total by adding in the (n+ 1)thpoint (the
new point) and dropping the first point (the drop point) of
the total. As each running total is calculated, the corre-
sponding average is obtained by dividing it by n.
For a regular cycle one with constant wavelength, mag-
nitude and phase, and symmetrical around a zero line we will
find that if an average of span nis applied to such a cycle with
wavelength also equal to n, the first value of the running totalwill be zero. This is because there will be a corresponding point
below the zero line for every point in the wave above the zero
line. For the next value of the running total, we find that the
point we must add in has exactly the same value as the point we
must drop. Hence, the total will remain at zero and continue to
do so as we move along the wave.
This will also happen when the span is an exact multiple of
the wavelength. Clearly, the net result is that such cycles will
be completely absent in the resulting averaged data (the out-
put). What happens if the span of the average is not the same
as the wavelength? In such cases, the magnitude of cycle will
be reduced in the averaged data, and in some instances will be
displaced in position. The various possibilities are best ad-
dressed by looking at various values of min the relationship:
8
7
6
5
4
3
2
1
0-1
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IBM (41-week cycle)
2/11/94
7/1/94
11/18/94
4/7/95
8/25/95
1/12/96
5/31/96
10/18/96
7/25/97
12/12/97
5/1/98
9/18/98
2/5/99
3/7/97
FIGURE 2:NOMINAL 41-WEEK CYCLES.The nominal 41-week cycle is plotted forIBM since early 1994. Note the moderate variation in wavelength as measured bythe horizontal successive peak-to-peak and trough-to-trough instances. The varia-tion in magnitude as measured by the vertical successive trough-to -peak and peak-to-trough distances is much more pronounced.
The running total is constructedby adding in the new point andsubtracting the drop point. Thetotal is then divided by n, the span.
When mis an exact integer, the cycle will be completely
removed from the output. When mis less than 1, the magni-
tude of the cycle will be reduced in the output. The phase of
the output (positions of peaks and troughs) will be identical
to that of the original cycle. As mdecreases, the amount of
reduction decreases.
Span = mw
Where m= a numeric value
w= wavelength
Where mlies between an even value of mand the next odd
value of m, the output will remain in phase with the original.
The magnitude will be reduced, the amount of reduction
falling to a minimum and then rising as mmoves between the
two extremes.Where mlies between an odd value of mand the next even
value of m, the phase of the output will be shifted by half a
wavelength from the original. The magnitude will be re-
duced, the amount of reduction falling to a minimum and then
rising again as mmoves between the two extremes.
CHANGEINVALUEThe running total is constructed by adding in the new point
and subtracting the drop point. The total is then divided by n,
the span. Thus, the change in the average from its previous
calculated value depends on the difference between the new
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Stocks & Commodities V17:2 (101-106): Moving Averages, First Principles by Brian J. Millard
Copyright (c) Technical Analysis Inc.
point and the drop point and also on the value of the span of
the average. For any given difference between the new point
and the drop point, the change in the average will obviously
decrease as we increase the span, because we are dividing the
total by increasingly larger numbers.
On the other hand, for any given span, the change in the
average will increase as the difference between the drop point
and the new point increases. In real terms, a kink will appear in
the averaged data not only if there is aspike,a large change in the
data at the position of the new point, but also if there is a spike
in the historical data at the position of the drop point. If there isa spike in both positions, the average will be doubly affected if
these spikes are in opposite directions. If they are in the same
direction, the kink will be greatly reduced or even absent.
11
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FIGURE 3: APPLICATION OF AVERAGES TO CYCLIC DATA.The solid sine waveis a regular cycle of wavelength of 51 weeks. The solid horizontal line at the $5 levelis the output from a 51-week average. The dashed waveform with peaks andtroughs aligned with the original sine wave is the output from the 31-week average.The dashed waveform with peaks and troughs out of phase with the original sine
wave is the output from a 75-week average.
70686664626058565452
5048464442403836343230
AT&T (daily)
12/8/94
4/27/95
9/14/95
2/1/96
6/20/96
11/7/96
3/27/97
8/14/97
5/21/98
10/8/98
2/25/99
1/1/98
706866646260585654525048464442403836343230
AT&T (daily)
12/8/94
4/27/95
9/14/95
2/1/96
6/20/96
11/7/96
3/27/97
8/14/97
5/21/98
10/8/98
2/25/99
1/1/98
706866646260585654525048464442403836343230
AT&T (daily)
12/8/94
4/27/95
9/14/95
2/1/96
6/20/96
11/7/96
3/27/97
8/14/97
5/21/98
10/8/98
2/25/99
1/1/98
FIGURE 4: NONLAGGED AVERAGES.The smooth line is the output from a 201-dayaverage plotted with no lag. The relationship between the data and the average isnot obvious.
FIGURE 5: CENTERED AVERAGES.The smooth line is the output from a 201-dayaverage plotted as a centered average, lagging by 100 days. The average can beseen as a representation of the longer-term trend.
FIGURE 6: ERROR IN NONLAGGED AVERAGES.Both the unlagged and centeredaverages are plotted on the same chart. The first two double-headed arrows showwhere the direction of the unlagged average is opposite to the true direction of thetrend. These are the places where methods based on unlagged averages are likelyto be in error. The third arrow in mid-1998 indicates a period when the direction ofthe trend is yet to be established.
APPLICATIONOFANAVERAGE
Point-to-point movement:Simply, the isolated point-to-point
movement can be considered to be truly random. In such a case,
the difference between two points is independent of their
distance apart in time and is simply a random value. Thus, the
difference between a drop point and the new point is chance.
The only factor with an effect in reducing movement in the
averaged data is the span used for the average; the greater the
span, the greater the reduction. The movement will never be
quite eliminated, but it will become unimportant once wereach spans of 50 or greater. On those occasions where the
drop point is an extreme one, and the new point is also
extreme but in the opposite manner, then there will still be a
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Stocks & Commodities V17:2 (101-106): Moving Averages, First Principles by Brian J. Millard
Copyright (c) Technical Analysis Inc.
kink in the resulting average, taking even larger spans to
reduce to an unimportant level.
If the random point-to-point movement is not isolated but
present in addition to the mixture of cycles, as is the case with
real stock market data, then we do not need such large spans
for the average to appear to eliminate this movement. It will
only represent a proportion of the total movement, and theaveraged data will have larger positive values due to the
cyclic data present, making the averaged random movement
appear insignificant.
The smaller the proportion of random movement in the
total data, the smaller the span required to reduce it to
apparent insignificance; extreme values of the drop point and
the new point will still leave a kink in the averaged data. Nine
points or less will usually suffice to smooth out the point-to-
point movement. We can use the value of standard deviation
mentioned previously to give us an idea of the proportion of
stock price movement due to randomness.
Statistically, 95.5% of the random movement will be
contained within two standard deviations either side ofthe mean, so four times the standard deviation is due to
this random movement. Dividing this by the lates t stock
price gives us an estimate of the proportion of random
point-to-point movement in that stock. For IBM, this
amounted to about 7.7% in October 1998. This does not
include the random variation in the magnitude of the
cycles present.
Cyclic movement in stocks:As we have seen for IBM, cycles
in real stock market data are not regular, since they change
randomly in wavelength and magnitude. The property of an
average that removes a cycle of the same wavelength or
multiple thereof will not apply. However, the property of
reducing the contribution of cycles of wavelengths greater or
lesser than the span will still apply, and this is what makes
moving averages so valuable.
Once we move above spans of about 9 points, there will be
a marked reduction of the point-to-point movement and of
those cycles whose wavelength is less than the span of the
average. Wavelengths longer than the span of the average are
most relevant. Roughly, cycles with wavelengths about 1.5
times the span of the average will be reduced by about 70%,
while those with twice the span will be reduced by about 50%,
but those four times the span will be reduced by only 10%.
The main effect of applying an average to stock marketdata is to remove random point-to-point movement and
reduce cycles whose wavelengths are less than about twice
that of the span of the average. All this works to leave us with
a fairly smooth average whose shape is mainly due to the
combination of all those wavelength cycles greater than
about twice the span of the average.
CENTEREDAVERAGESOne of the major reasons that moving average methods fail is
that the averages are usually plotted with no lag; that is, they
are not centered. The use of unlagged averages is so ingrained
in chartist techniques that it is no longer possible to eradicate
it. However, the properties of moving averages we have
discussed assume that averages are presented as centered.
We can demonstrate the advantages of centered averages
over unlagged averages by referring to two charts. The plot
of a 201-day average in the usual chartist mode can be seen
in Figure 4, while in Figure 5 the average is plotted as acentered average. A centered average of span nis set back in
time by:
(n- 1)/2 points
We use 201 rather than 200 days to give a lag that is an integer
(100, in this case), allowing us to center the average at the
position of a data point and not between two such points.
Plotting averages as in Figure 4 is only useful if the
crossing of the average by the data, or the crossing of two
averages, has some meaning. Plotting them as centered
averages as in Figure 5 has two main advantages. First, the
average is a better representation of the data, since short-termfluctuations and random day-to-day movement have been
almost totally removed. What is left is the net effect of all
those cycles of wavelength greater than about 400 days.
Thus, a centered average is representative of a trend, which
can be considered to be the long-term trend.
A nonlagged average, on the other hand, is in the wrong
position to be considered to be a trend, even though its shape
is identical to that of the centered average. The second and
perhaps the most vital point concerns the lag in the average,
which in this case is 100 days. We do not know how this
average moved during this period, and because we now
consider the centered average as representing the trend, we do
not know what the trend has been doing. This is something
that we will discover only when we make new calculations
over the next 100 days into the future.
This point is the source of disappointment when nonlagged
averages are used as a guide for trading decisions. The actual
trend could well have changed direction during this period, so
decisions that assume that the trend is still rising because the
average was still rising at the last calculation can go disas-
trously wrong.
This point can be illustrated by plotting both the nonlagged
and centered averages on the same chart, as seen in Figure
6. There are two places where the trend, as indicated by the
centered average, is going in the direction opposite to thatof the nonlagged average. These are marked by the first two
double-headed arrows.
The third, latest, arrow is at a point where we do not know
what the current trend is doing, so the trend might be going
in the direction opposite to that indicated by the nonlagged
average. It is at these turning points that decisions based on
nonlagged averages will come to grief.
Because the centered average is lagging by half of a
span 100 days we have two places in the plot where
the nonlagged average is in error for 100 days a total of
200 days out of 860, covering the period of the plot up to
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Stocks & Commodities V17:2 (101-106): Moving Averages, First Principles by Brian J. Millard
Copyright (c) Technical Analysis Inc.
the last position of the centered average. In addition, we
have a third place where the unlagged average will be in
error if the trend changed direction in mid-1998, although
this has yet to be established. Thus, for at least 25% of the
time, the nonlagged average indicates an incorrect direc-
tion for the long-term trend.
In those stocks with more frequent turning points, theposition will be even worse. This is unfortunate, because just
when the investor is most in need of help in deciding whether
a trend has changed direction is the time when the nonlagged
average is giving the wrong answer. However, there are ways
in which an estimation of the trend direction and whether it
has changed can be improved, and these will be discussed in
another article.
FURTHERAPPLICATIONSAnother point should be noted when a centered average is
plotted. From Figure 5, it can be seen that the excursions
of the data on either side of the average line are limited.
When a maximum distance is reached, the data reversesdirection. Boundaries can be drawn to contain this move-
ment, leading to the powerful predictive technique known S&CSee Traders Glossary for definition
as channel analysis.
My next article will show how the short-term fluctuations
that still appear in the output of simple averages can be
removed by applying a second average or a weighted aver-
age. I will also look at the use of the difference between two
averages and the difference between the average and the data
for investigating individual cycles and groups of cycles.
Brian Millard is the author of six books on technical analysis,
includingProfitable Charting Techniques,Channel Analysis
andChannels And Cycles.
RELATEDREADINGHurst, J.M. [1970]. Profit Magic of Stock Transaction Tim-
ing, Prentice-Hall.
Millard, Brian J. [1997]. Channel Analysis, second edition,
John Wiley & Sons.
_____ [1999]. Channels And Cycles: A Tribute To J.M.
Hurst, Traders Press.
_____ [1997]. Profitable Charting Techniques, second edi-tion, John Wiley & Sons.