Radio Science, Volume 7, Number 3, pages 351-353, March 1972
Fifty-megahertz Es, 1964-1970
Patrick J. Dyer
Office of Telecommunications, Institute for Telecommunication Sciences
Boulder, Colorado 80302
(Received October 28, 1971.)
Using amateur signals in the 50-MHz band to indicate the presence of oblique-incidence
Es paths, the diurnal, seasonal, and magnetic relationships of the phenomena for the years
1964-1970 were examined. Summer double diurnal peaks were found along with 'off-season'
meteor shower influences.
INTRODUCTION
Using commonly available amateur equipment for
50-MHz, observations of Es phenomena were con-
ducted in the period 1964-1970.
In general, receiver sensitivities were on the order
of 1 µv, although the equipment used varied through
the years of study. Antenna systems also underwent
some variation, with the average gain realized in the
7-9 db range. The receiving terminal point was still
another unfixed item. Observations were conducted
from San Antonio, Texas, from January 1964
through early August 1966 and again from No-
vember 1969 through the end of December 1970.
In the period between August 1966 and November
1969, observations were conducted from Austin,
Texas (some 85 miles northeast of San Antonio).
Equipment outage caused the loss of September-
November 1966 data.
MONITORING PRACTICES
The detection of all instances of 5O-MHz Es-
propagated signals was noted for onset and dropout
time (with 5-min resolution). A 30-min fadeout
period was defined as terminating a given 'opening.'
As no automatic recording devices were available,
the time that could be spent monitoring 50 MHz
varied greatly during the year. The summer periods,
however, can in many ways be considered near con-
tinuous.
Close monitoring of the 30-50-MHz region for
Es enabled the observations on 50 MHz proper to
be either intensified or relaxed depending on condi-
tions noted. This type of "back-up" system did not
come into use until September of 1967. A frequency
of 27 MHz (with some 2,000,000 transmitters in
this country) was often used, especially at night, to
indicate the lack of any Es likely to reach 50 MHz
MUF.
The 50-MHz Es openings were not rated accord-
ing to strength, quality, distance, bearing, etc. The
wide variations found in those parameters are thus
not reflected in these data. As 50-MHz signal sources
(amateur stations) are not evenly distributed in time
or space, the data are strongly influenced by that
factor.
DATA ANALYSIS
Much of the following data analysis is patterned
after earlier amateur radio work [Monroe and Mon-
roe, 1962, 1964].
Seasonal. Figure 1 shows the totals of 50-MHz
Es minutes observed each month summed for 1964-
1970. The definite minimum occurs in March with
an equally definite peak in June (although July
of a given year may have exceeded June). A sec-
ondary maximum is evident in the month of De-
cember. This agrees with the long-known seasonal
trends.
![[Figure 1]](rs72fig1.gif)
Figure 2 presents the yearly sums of 50-MHz
Es. No clear relationship to the sunspot cycle is
visible, although the largest value in 1965 cor-
responded to a period of low solar activity and the
smallest value in 1969 came during high solar levels.
The large value in 1968 with high sunspot epoch
does not agree with the trend found during the down-
swing of cycle 19 [Monroe and Monroe, 1962].
![[Figure 2]](rs72fig2.gif)
Diurnal. Figure 3 is a sum of the diurnal varia-
tions of the summer months (May-August) for each
of the 7 years and a sum of those together. Note
the different scale in the last graph. The double-
hump maxima show very nicely through these years.

Figure 4, for December, shows marked contrast
to the summer diurnal curves. Only those days are
included when both forenoon and afternoon mon-
toring were possible in order to avoid biasing the
evening results. Even then the preference for De-
cember Es to be an after-dark event is strikingly
evident.
![[Figure 4]](rs72fig4.gif)
In considering the diurnal behavior (all CST),
it must be kept in mind that the actual solar time
at the Es patch itself could vary by some two hours
since the data make no distinction between clouds
east or west of the observer. The 700-mile radio
horizon during December, however, is all well into
darkness by the time of the peak in Figure 4.
Magnetic relationships. At the suggestion of
some who attended the 1970 ESSA in-house Es
seminar, attempts were made to relate the 3-hour
Kp indices to the termination of an Es event in prog-
ress. Very inconclusive results were found with Es
commencing when Kp's were as high as 7. The 24-
hour Kp sum is a much more meaningful parameter
to use.
Figure 5 compares the daily 50-MHz Es sums
with the 24-hour (CST base) Kp sum for May-July
of 1965. During this period the most intense mag-
netic storm of the IQSY took place, In the period
around the storm (June 15-22) one can easily see
the depressing effect on Es, followed by a tremen-
dous level of Es during the quiet period after. For
3 of 4 days the daily Es sum ran over 800 min., a
level not elsewhere duplicated in the 7 years of the
study.
![[Figure 5]](rs72fig5.gif)
Meteor influences. Figure 6 shows the October-
December daily sums for 1964-197O combined. The
abrupt rise in levels in mid-December relates very
well to the Geminid meteor shower. Later December
effects may be attributable to the Ursids. Likewise
the mid-November rise is likely tied to the Leonid
shower. Less strong peaks in early and late October
may be linked to the Draconids and the Orionids,
respectively.
![[Figure 6]](rs72fig6.gif)
CONCLUSIONS
By using relatively inexpensive equipment to
monitor a VHF band highly populated with signals,
many of the commonly observed behavior patterns
of an oblique path agree with well-established varia-
tions of Es deduced from other modes of radio prob-
ing (e.g., vertical incidence, backscatter). Use of the
large numbers of active 50-MHz stations should al-
ways be kept in mind when considering any Es, in-
vestigations related to VHF propagation.
REFERENCES
Monroe, M., and D. Monroe (1962), 50 Mc propagation
effects, CQ, 18 (6), 37-42.
Monroe, M., and D. Monroe (1964), 50 Mc propagation
effects, CQ, 20 (11), 82-87.
Copyright © 1972 by the American Geophysical Union
Page modified: February 14, 2000
December 15, 2003