612
XFWS-A 612 1-129(1970)
U.S. Fish Wlldl. Serv.
Spec. Scl. Rep. Fish.
The Trade Wind Zone Oceanography Pilot Study
Part VIII: Sea-Level Meteorological Properties
and Heat Exchange Processes
July 1963 to June 1965
By Gunter R. Seckel
Marine Biological Laboratory |
LIBRARY
JUNl 01971
WOODS HOLE, MASS.
SPECIAL SCIENTIFIC REPORT-FISHERIES Na 612
UNITED STATES DEPARTMENT OF THE INTERIO^^^
Walter J. Hickel, Secretary * 7 jq
Leslie L. Glasgow, Assistant Secretary
for Fish and Wildlife, Parks, and Marine Resources
Charles H. Meacham, Commissioner, U.S. FISH AND WILDLIFE SERVICE
Philip M. Roedel, Director, BUREAU OF COMMERCIAL Fisheries
The Trade Wind Zone Oceanography Pilot Study
Part VIII: Sea-Level Meteorological Properties
and Heat Exchange Processes
July 1963 to June 1965
By
GUNTER R. SECKEL
United States P^ish and Wildlife Service
Special Scientific Report — Fisheries No. 612
Washington, D, C.
June 1970
CONTENTS
Page
Introduction
Sources of data
Processing of data
Heat exchange computations.
Q(S), radiation from sun and sky_
Q(B), effective back radiation
Q(E), the heat of evaporation
Q(C), conduction of sensible heat.
Evaluation of results
Inadequacies in the distribution and quality of data
Effects of data inadequacies on the heat exchange results.
Effects of processing techniques on the heat exchange results.
Comparison with other results in the North Pacific
Interseason and interyear comparisons
Conclusion ^
Acknowledgment
Literature cited
Appendix table A
Appendix table B^ _
1
2
3
3
4
5
5
6
6
6
8
9
13
15
. 17
. 18
. 18
. 20
.105
FIGURES
1. The oceanographic and meteorological observational regions for the
Trade Wind Zone Oceanography Pilot Study ^
2. The heat of evaporation per unit difference in sea-air vapor pressure
as a function of the wind speed — —
3. Monthly heat of evaporation, cal. cmT^ day"' , lat, 25° to 29° N., long.
140° to 144° W., July 1963 to June 1965. Q{E), mean heat of evapora-
tion based on computations made for each set of meteorological obser-
vations, Q(E|), mean heat of evaporation based on daily mean meteoro-
logical properties, and Q(E2), mean heat of evaporation based on month-
ly mean meteorological properties
Page
_ 2
_ 9
Monthly net heat exchange across the sea surface (cal. cmT^ day"' )
lat. 25° to 29° N., long. 140° to 144° W., July 1963 to June 1965.
Q(N), mean net heat exchange based on computations made for each set
of meteorological observations, Q(N|), mean net heat exchange based
on daily mean meteorological properties, and Q(N2), mean net heat
exchange based on monthly mean meteorological properties
5. The heat of evaporation, Q(E), and the net heat exchange across the
sea surface, Q(N), at lat. 17° N., long. 152° W., July 1963 to June 1965
(from table B), and interpolated values from climatic charts by Wyrtki
(1966) - —
6. The heat of evaporation, Q(E), and the net heat exchange across the
sea surface, Q(N), at lat. 2° N., long. 157° W., July 1963 to June 1965
(from table B), and interpolated values from climatic charts by Wyrtki
(1966).
12
13
14
15
TABLES
Coefficients in the harmonic series for the computation of Q^ at lat. 0'
10°, 20°, 30°. and 40° N
Page
2. Heat exchange processes for each month, cal. cm7^ day"', July 1963 to
June 1965, at Christmas Island, lat. 2° N., long. 157° W.; Johnston Is-
land, lat. 16° N., long. 169° W.; and Ocean Weather Station November,
lat. 30° N., long. 140° W. Subscripts 1, exchange processes computed
daily; subscripts 2, exchange processes computed from mean monthly
meteorological processes 10
3. Differences in extremum values of Q(E|), Q(E2), Q(N|), and Q{N2), lat.
25° to 29° N., long. 140° to 144° W 16
4. Interyear comparisons of 4-month averages of Q(E|) and Q(E2), lat. 25°
to 29° N., long. 140° to 144° W.. 16
5. Interyear comparisons of 3-month averages of Q(N|) and Q(Ng), lat. 25°
to 29° N., long. 140° to 144° W 16
6. Interyear differences of Q(E) and Q(N), lat. 32° N., long. 167° W. (from
table B) 17
7. Interyear differences of Q(E) and Q(N), lat. 17° N., long. 152° W. (from
table B) 17
8. Interyear differences of Q(E) and Q(N), lat. 2° N., long. 157° W. (from
table B) 17
The Trade Wind Zone Oceanography Pilot Study
Part VIII: Sea-Level Meteorological Properties
and Heat Exchange Processes
July 1963 to June 1965
By
GUNTER R. SECKEL, Oceanographer
Bureau of Commercial Fisheries Biological Laboratory
Honolulu, Hawaii 96812
ABSTRACT
Meteorological data were summarized and large-scale heat exchange proc-
esses computed, in 5° square units of the area lat. 0° to 35° N., long. 130° to 170°
W., for each month. The results complement time-sequence oceanographic
observations of the Trade Wind Zone Oceanography Pilot Study in the area lat.
10° to 26° N., long. 148° to 157° W., February 1964 to June 1965. The source and
processing of meteorological data, and the computation of the radiation from sun
and sky, the effective back radiation, the heat of evaporation, and the conduction
of sensible heat are described. The results are consistent with monthly heat
exchange processes computed from long-term mean meteorological properties
in the North Pacific. Despite inadequacies in the distribution and quality of
data, the meteorological data summaries and the derived heat exchange proc-
esses are adequate for interseason and interyear comparisons of large-scale,
sea-air interactions.
INTRODUCTION
This report contains monthly summaries of
sea-level meteorological observations and de-
rived heat exchange processes at the sea sur-
face in the area bounded by lat. 0° and 35°N. and
long. 130° and 170° W., July 1963 through June
1965. The meteorological data complement the
TWZO (Trade Wind Zone Oceanography) Pilot
Study oceanographic data that were published in
the first six reports of this series (Charnell,
Au, and Seckel, 1967a-f).
The TWZO Pilot Study is designed to further
an understanding of the mechanisms that change
the distribution of sea-water properties and wa-
ter masses in the North Pacific trade wind zone
(Seckel, 1968). The meteorological processes
are an essential part of these mechanisms.
The oceanographic field work took place from
February 1964 through June 1965 in the area
from lat. 10° to 26° N. and long. 148° to 157° W.
Oceanographic stations in a fixed grid were oc-
cupied at monthly intervals.
Meteorological processes at the sea surface
are intimately related to the behavior of the
trade wind system. The area of interest, there-
fore, encompasses the region of strongest trade
winds, which is located between the North I'a-
cific high and the equatorial low pressure re-
gions. Figure 1 shows the areas of the TWZO
oceanographic and meteorological observations.
Because the results reported here begin in July
1963, they antecede and cover the oceanographic
study period.
Meteorological data summaries and the de-
rived heat exchange processes are presented in
two tables, which show the information for every
month of the 2-year study period. Table A con-
tains mean values per 5° square of the air tem-
perature, the difference between water and air
120" E. 130°
140° 150° 160° 170° 180° 170°
160° 150°
130° 120° 110° W 100°
METEOROLOGICAL
STUDY REGION
TWZO REGION
^M^ "^^^ ^N 0 R t H PACIFIC "\ \
y0^y: EQUATORIAL WATER j)
I 10°
120° E 130° 140° 150° 160° 170° 180° 170°
150° 140° 130° 120°
1 10° W. 100°
Figure 1. — The oceanographic and meteorological observational regions for the Trade Wind Zone
Oceanography Pilot Study.
temperature, the difference between the satura-
tion vapor pressure of water and air vapor pres-
sure, the vapor pressure of the air, the cloud
cover, the sea level atmospheric pressure, the
wind speed, and the zonal and meridional com-
ponents of the wind velocity. Table B contains
interpolated values for the center of each 5°
square of the sea-water temperature, the air
temperature, the vapor pressure of the air, the
cloud cover, and the wind speed. Tabulated
alongside these meteorological properties are
the derived heat exchange processes: the radia-
tion from sun and sky, the back radiation, the
heat of evaporation, the conduction of sensible
heat, and the net heat exchange across the sea
surface. Interpolated meteorological proper-
ties and their derived heat exchange processes
are presented in geographic format to facilitate
contouring.
The magnetic tape containing the data that
were used for the summaries and for the de-
rived heat exchange processes computed for
each weather record is kept on file to permit a
more detailed analysis than is presented here.
The sources of data, the methods of process-
ing, and the computation of heat exchange proc-
esses, as well as an evaluation of the results,
are presented below.
SOURCES OF DATA
About 80,000 sets of meteorological observa-
tions were used in the preparation of this report.
Their principal source was the surface marine
observations Card Deck No. 128 of the National
Weather Records Center. To those data were
added the meteorological observations recorded
onboard the BCF (Bureau of Commercial Fish-
eries) research vessels Townsend Cromwell and
Charles H. Gilbert which were not already a
part of the surface marine deck.
Meteorological data in latitudes of the central
North Pacific south of Hawaii are scarce. It is
therefore valuable to add to the surface marine
observations those made on Johnston Island (lat.
16°45' N., long. 169°30' W.) and on Christmas
Island (lat. 1°51' N., long. 157°23' W.). Because
both islands are atolls, the early morning mete-
orological conditions would approximate those
over the adjacent ocean.
Johnston Island sea level observations were
obtained from the National Weather Records
Center, Card Deck No. 144. To these data were
added the sea surface temperatures measured
weekly at Johnston Island for BCF, Honolulu.
At Christmas Island, meteorological observa-
tions are made three times dally and the sea
surface temperature ismeasured dailyfor BCF.
The sea surface temperatures and the 1800
G.m.t. synoptic meteorological observations
from the two islands (0800 local time, Christ-
mas Island, and 0700 local time, Johnston Is-
land) have been combined with the surface ma-
rine data.
At the time of the initial sorting, derived prop-
erties and heat exchange processes were also
computed. Thus the data tape referred to in the
introduction contains in chronological order by
day and by 1° square the sea surface tempera-
ture, the dry and wet bulb air temperatures,
the sea level atmospheric pressure, the cloud
cover, the sea-air vapor pressure difference,
the vapor pressure of the air, the wind speed
and direction, the zonal and meridional com-
ponents of the wind velocity, the radiation from
sun and sky, the effective back radiation, the
heat of evaporation, and the conduction of sensi-
ble heat.
I planned originally to summarize the mete-
orological data for periods of, possibly, 5 days
and then, by summation, obtain values for the
monthly sea-air interaction processes. The
spatial and temporal distribution of marine sur-
face observations, however, proved inadequate
to permit this procedure; I had to use the tradi-
tional climatic approach.
PROCESSING OF DATA
The meteorological data were initially sorted
chronologically by day and by 1° square units of
area. When more than one set of observations
occurred in a 1° square per day, the meteoro-
logical properties, including the wind speeds and
the zonal and meridional components of the wind
velocity, were averaged. In consequence only
one set of meteorological observations can occur
per day in any 1° square.
Quality control over the large number of data
proved to be a major task. In the initial sorting
process, "flagging" values that fell outside the
climatic limits proved unsuccessful. This pro-
cedure had been used in the preparation of the
Indian Ocean meteorological atlas (Ramage,
Miller, and Jefferies, in press). Too many ob-
servations that were consistent with surrounding
data fell outside the climatic limits during the
2 years of this study. An initial listing of the
data was therefore inspected without computer
aid. Only obviously erroneous values, deter-
mined by comparison with values in the same
geographic region and within a few days, were
eliminated.
Of the original marine surface and island
decks, I sorted only those meteorological data
that enter into the computation of large-scale,
sea-air interactions: the dry and wet bulb air
temperatures; the sea-air temperature differ-
ence; the sea-level atmospheric pressure; the
speed and direction of wind; and the total cloud
cover.
The meteorological properties were, there-
fore, summarized by 5° square units of area and
by months and are presented in table A. The
summaries for each property contain the mean
value, the highest and lowest values observed,
the standard deviation if there were more than
four observations, and the number of observa-
tions. In addition, the summary also includes
the mean location of observations.
Smoothed charts of the sea surface temper-
ature, the air temperature, the vapor pressure
of the air, the cloud cover, and the wind speed
were obtained by contouring the summarized
data plotted at the mean location of the obser-
vations. This procedure had been used in the
preparation of the Indian Ocean meteorological
atlas (Ramage et al., in press). In turn, the
smoothed charts were used to obtain interpo-
lated values at the center of each 5° square, and
to compute the radiation from sun and sky, the
effective back radiation, the heat of evapora-
tion, the conduction of sensible heat, and the net
heat exchange across the sea surface. Table B
presents both the interpolated values and the
derived heat exchange processes.
When table B is used in combination with ta-
ble A, it is possible to judge the reliability of
the results in any area and month covered by
this report.
HEAT EXCHANGE COMPUTATIONS
Sea-air interaction processes cannot, in gen-
eral, be measured directly except for the radi-
ative energy exchange. Radiation measurements
over the oceans, however, are scarce. Quanti-
tative evaluation of these processes, therefore,
depends on computations in which empirically
derived formulas are used. These formulas
were reviewed by Laevastu (1960) and the more
general subject of large-scale, sea-air inter-
actions has been discussed in detail by Malkus
(1962). The empirical formulas are still the
subject of intensive research and may change.
Should changes be made, the derived results of
this paper can be adjusted, since the original
meteorological properties are also given.
Two criteria are important in the computation
of the heat exchange processes presented in ta-
ble B. First, the results must satisfy the needs
of the TWZO investigation, in which relative
changes from month to month and season to sea-
son are of primary interest. Secondly, there
must be a basis for comparison with the results
in the North Pacific such as were obtained by
Wyrtlci (1966).
The net heat gain or loss to the sea water
as a result of the exchange processes at the sea
surface is of interest to the oceanographer and
is expressed in the budget equation
Q(N)= Q(S)- Q(B)- Q(E)- Q(C).
The net heat exchange across the sea surface,
Q(N), is positive when the sea water gains heat.
The terms on the right side of the equation are:
Q(S), the radiation from sun and sky; Q(B), the
effective back radiation; Q(E), the heat of evap-
oration; and Q(C), the conduction of sensible
heat.
The following formulas have been used to
compute the heat exchange processes in table B:
Q(S) = 0.98 Q^ (1 - 0.30C - 0.38C^)
Q(B) = 1.14 (10)-^ (273.16 + T,^)'' (0.39 - 0.05/e^)
(1- 0.6C^) + 4.58 (10)"'^ (273.16 + T„)^
(T„-Ta)
Q(E)= 3767 C (0,98e„-eg)W
Q(C)= 4(T^-Ta)W.
The heat exchange components are expressed in
cal. cm7^day~' and the symbols are:
C , the cloudiness in tenths of sky cov-
ered;
Cg , the vapor pressure of the air in
millibars;
e^, , the saturation vapor pressure over
pure water at the sea-water temper-
ature, in millibars;
T(j , the temperature of the air in degrees
Celsius;
T^ , the temperature of the water in de-
grees Celsius;
W
'D '
the wind speed in meters per second;
the radiation from sun and cloudless
sky in calories per square centi-
meter per day;
the nondimensional drag coefficient.
The values of e^ and e„ were computed from
formulas given by List (1951: p. 366) and Mur-
ray (1967). The methods of computing Qo and
Crj are given below in the discussion for each
formula. In the computation of Q(B), Q(E),
(e), and Q(C), the sea surface temperature
based on surface marine observations was re-
duced by 0.7° C. (Saur, 1963).
Although different workers agree about the
meteorological properties that affect the heat
exchange processes, the coefficients used in the
empirical formulas vary. To allow compari-
sons of the results in this paper with those of
other workers, each of the heat exchange proc-
esses and the choice of coefficient used here
are discussed below.
Q(S), Radiation from Sun and Sky
Departures from the formulas used by Wyrtki
(1966), Roden (1959), and Laevastu (1960, 1965)
are based on direct pyranometer measurements
of radiation from sun and sky during the cruises
of the TWZO Pilot Study. It was possible to
integrate the analog traces for clear sky and
solid overcast conditions by means of a polar
planimeter. The clear sky direct and diffuse
radiation values for a transmission coefficient
of 0.6 given in the Smithsonian tables (List,
1951: tables 132 and 136), when multiplied by
1.03, corresponded to the measured values.
These results agree with the values given by
Bolsenga (1964). The albedo factor, 0.95, when
multiplied by 1.03 gives the coefficient, 0.98,
used in the equation.
To facilitate the calculation of Q„ by compu-
ter, the harmonic analysis of the clear sky di-
rect and diffuse radiation values of the Smith-
sonian tables gives
Qo - ^o'^ A| cose + B| sine +A2 cos 2e + Bj sin2e
2TT
where & = -y-(t - 21), t is the time in days begin-
ning with January 1, T the number of days in a
year, and the A's and B's are coefficients in the
harmonic series. Table 1 lists the coefficients
for lat. 0°, 10°, 20°, 30°, and 40° N. Coefficients
applicable for the computation of Q^ at inter-
mediate latitudes were obtained by linear inter-
polation.
Expressions that have been used in the Pacific
area for the cloud correction of the clear sky
radiation range from linear to cubic functions
of cloudiness: Tabata (1958) used the Angstrom
factor (1 - 0.71C). Roden (1959) used the Budyko
factor (1 - kC) where k ranges from 0.65 at the
Equator to 0,68 at lat. 35° N. Johnson, Flittner,
and Cline (1965) and Wyrtki (1966) used the quad-
ratic Beriland factor (1 - aC - 0.38C^). (John-
son et al. listed for the coefficient "a" the val-
ues 0.38, 0.40, 0.39, 0.37, 0.35, 0.36, 0.38, cor-
responding to lat. 0°, 5°, 10°, 15°, 20°, 25°, 30°,
and 35° N., respectively, and Wyrtki used "a" =
0.38.) Finally, Laevastu (1960, 1965) suggested
the use of a cubic cloud factor (1 — 0.6c').
In this paper I use the Beriland expression.
Qualitatively, the pyranometer records of the
TWZO cruises indicate that a linear decrease
of Q(S) with Increasing cloudiness is too rapid
and a cubic decrease is initially too slow. The
coefficient "a" = 0.3 has been chosen for the
Beriland expression and is based on pyranom-
eter records for 21 days of solid overcast which
gave an average cloud factor of 0.32. This fac-
tor compares with others for solid overcast as
follows: Tabata 0.29, Roden 0.32 to 0.35, Wyrt-
ki 0.24, Johnson etal. 0.22 to 0.27, and Laevastu
0.4.
Table 1 .--Coefficients in the harmonic series for
the computation of Q at lat. 0°, 10°, 20°, 30°,
and 40° N. °
Lati-
tude
Ao
Al
Bi
As
Bs
north
0°
595.83
18.55
-4.97
-15.42
25.26
10°
589.42
-46.84
30.16
-17.08
28.15
20°
555.42
-112.46
66.72
-14.58
26.70
30°
507.50
-169.24
100.21
-10.83
20.21
40°
447.50
-218.56
126.76
-2.50
8.66
Q(B), Effective Back Radiation
The seasonal and spatial variations in effec-
tive back radiation are relatively small com-
pared with those of the radiation received from
sun and sky. Wyrtki (1966) calculated a range
of 60 to 200 cal. cm:2 day-i for the North Pacific;
Tabata (1958) reported 85 to 130 cal. cmr^day"'
off the British Columbia coast; Roden (1959)
calculated 84 to 138 cal. cmr^day"' for the re-
gion off California and Baja California; and Sec-
kel (1962) estimated 115 to 150 cal. cmT^day"'
for the Hawaiian region.
During the TWZO cruises, the net long wave
radiation was measured by means of a Suoml-
Kuhn net radiometer (Charnell, 1967). These
measurements indicate a range of 58 to 173 cal.
cmr^ day"'.
Roden (1959), Johnson et al. (1965), and Wyrtki
(1966) used the Beriland expression for the com-
putation of the effective back radiation in which
the coefficient to correct for cloudiness ranges
from 0.5 at the Equator to 0.65 at lat. 35° N.
Charnell (1967) computed this coefficient for
solid overcast conditions to be, on the average,
0.6. In this report I have used the Beriland ex-
pression for Q(B) with cloud coefficient 0.6 and
have neglected the variation with latitude.
Q(E), the Heat of Evaporation
Together with the radiation from sun and sky,
the heat used for evaporation is the most impor-
tant term affecting the net heat exchange across
the sea surface. In the expressions used by all
of the workers cited above, the evaporation de-
pends on the difference between the saturation
vapor pressure over sea water at the sea sur-
face temperature and the actual vapor pressure
of the air above the sea surface (in this paper
termed sea-air vapor pressure difference'), the
wind speed, and a coefficient. The evaporation
coefficient is affected by the wind speed and the
stability of the air above the sea surface. The
height above the sea surface at which psychro-
metric and wind measurements are made can
also be important in the computation of evapor-
ation, depending on the vertical gradients of hu-
midity and wind speed near the height of mea-
surement. Laevastu (1960) and Malkus (1962)
have discussed the unresolved uncertainties
concerning the choice of the coefficient.
The evaporation coefficient computed from
the expression discussed by Malkus (1962) de-
pends on the drag coefficient and varies with
the wind speed from 3 (winds below 4 m. sec."' )
to 9 (winds above 12 m. sec."'). Most workers
use a constant coefficient for the computation
of climatic averages of the evaporation. Wyrtki
(1966) used a coefficient of 6 obtained from the
Malkus formula, which corresponds to a wind
speed of 8 m. sec."' at 10 m. height. Tabata
Subsequently in this paper the difference be-
tween the saturation vapor pressure over sea
water at the sea surface temperature and the
actual vapor pressure of the air above the sea
surface is referred to as the sea-air vapor pres-
sure difference.
(1958) and Johnson et al. (1965) used 4.7 for
wind measurements at 20 m. height. The coef-
ficient of Laevastu (1960) varies with wind speed
but at 10 m. sec."' the evaporation would be
about the same as that computed by Wyrtki. Be-
low this wind speed, values would be higher and
above this speed they would be lower than Wyrt-
ki's values. For a wind speed of 8 m. sec."'
measured at 10 m. above sea level, Roden's
(1959) coefficient is also 6.
In this paper the formula suggested by Malkus
has been used. In the trade wind zone it Is rea-
sonable to assume neutral stability at the usual
height of marine wind measurements. The un-
certainties in this height are therefore not crit-
ical, and the drag coefficient for neutral stabil-
ity (Malkus, 1962: fig. 6, p. 110) can be used.
Inspection of the wind summaries in table A and
the smoothed values in table B show that the spa-
tial and temporal variations in the wind speed
generally lie in the range of 4 to 12 m. sec.~'
Within this range the nondimensional drag coef-
ficient changes rapidly. In the calculations of
this paper the variable nature of the coefficient
has therefore been taken into account.
The equation
C -
D
arctan (W - 8)
1.96
+ 1.6
10
-3
approximates the curve for the drag coefficient,
CjD, as a function of wind speed, W (inm. sec."'),
under conditions of neutral stability given by
Malkus, and facilitates the computation of the
evaporation.
In the evaporation equation of this paper the
saturation vapor pressure over pure water has
been multiplied by 0.98 to account for the salt
effect (Miyake, 1952). Also the computer pro-
gram was written so that for negative sea-air
vapor pressure differences, the computed heat
of evaporation would be 0, This part of the com-
puter program does not affect the results of ta-
ble B since monthly mean values of the sea-air
vapor pressure difference are always positive
(see table A). The program, however, affects
results based on evaporation rates computed for
each set of meteorological observations.
Since fog is rarely reported except, possibly,
in the northern region of the area considered in
this paper (McDonald, 1938), minimum sea-air
vapor pressure differences that are negative in
table A are probably due to erroneous observa-
tions. The computer program, therefore, re-
duces the error if evaporation rates of individ-
ual sets of observations are summed. Where a
negative sea-air temperature difference may
actually have occurred, the computer program
reflects the belief that the heat of condensation
gained by the ocean is small (Roden, 1959).
Q(C), Conduction of Sensible Heat
The exchange of sensible heat across the sea
surface is the smallest term in the net heat ex-
change across the sea surface. It is generally
computed from the ratio of Q(C) to Q(E), the
Bowen ratio, and depends upon the temperature
difference between water and air and the wind
speed. Wyrtki (1966) used the form suggested
by Malkus (1962) with a conduction factor of
3.86. Johnson et al. (1965) used a factor of 3
and Roden (1959), 3.96. Laevastu's (1965) fac-
tor again varies with the wind speed but at 10 m.
sec."' it is essentially the same as that used by
Wyrtki or Roden. When the sea-air tempera-
ture difference is negative, Laevastu used the
same form as other workers with a factor of 3.
Here a factor of 4 is used and no change is
made when the sea-air temperature difference
becomes negative.
EVALUATION OF RESULTS
Uncertainties in the estimation of large-scale,
sea-air interaction processes calculated in this
paper are due to (1) inadequacies in the distri-
bution and quality of the data, (2) the methods of
processing which must be used because of inad-
equate spatial and temporal distribution of ob-
servations, and (3) uncertainties in the empiri-
cal formulas. The empirical formulas which
are the subject of intensive research, and their
uncertainties have been thoroughly treated in
the literature cited here, and elsewhere. The
evaluation is, therefore, concerned with the data
inadequacies, effects of these inadequacies on
the heat exchange results, and the effects on the
results of the processing methods which must
be used because of data inadequacies. Finally,
comparisons with other results in the North Pa-
cific and interseason and interyear compari-
sons are made.
Inadequacies in the Distribution
and Quality of Data
Table A shows that south of lat. 15° N. the
number of observations per month is small and
that some 5° squares have no observations. For
these latitudes the results presented in table B
must therefore be regarded with caution, except
at lat. 2° N., long. 157° W. where daily observa-
tions from Christmas Island have been used.
North of lat. 15° N. sampling is more ade-
quate, particularly from Hawaii northward, in
the latitudes that contain the shipping lanes
from North America to the Far East and to
Hawaii. Reliable results in table B are those
from lat. 17° N., long. 167° W., an area which
contains the daily Johnston Island observations,
and from lat. 32° N., long. 142° W., which, in
addition to a large number of observations from
merchant vessels, contains those from the U.S.
Coast Guard Weather Station November.
Of the interpolated meteorological properties
in table B, the cloudiness and the wind speed
are most subject to error due to insufficient
observations. The cloud cover may materially
change during timespans of less than an hour
and from day to day. A large number of obser-
vations is therefore necessary to provide a
measure of the monthly cloudiness. Only in the
latitudes north of Hawaii are the observations,
on average, more frequent than once per day.
In the trade wind zone, similar wind speeds
and directions have a greater persistence than
the amount of cloud cover but may show rela-
tively large variations in timespans of a few
days. South of lat. 15° N. the interpolated winds
and cloudiness of table B are heavily biased by
the values obtained from a few monthly obser-
vations which, although they may be correctly
measured, do not necessarily reflect the month-
ly mean value.
Despite the sparse data south of lat. 15° N.,
interpolated results of the smoothed charts are
presented in table B. As a consequence large
evaporation rates of more than 700 cal. cmr^
day"' may appear as, for example, in the east-
ern portion of the region at lat. 2° N. during
September and October 1963. These evapora-
tion rates are due to relatively few observations
with wind speeds of more than 10 m. sec."' (see
table A), The choice in the preparation of table
B was either to leave the area in question blank
ortopresent values based on the limited obser-
vations. The latter course was chosen since it
draws attention to the high winds which may
occur in this area and cause high evaporation
rates.
Inadequacies in the quality of marine meteor-
ological observations are well known. Visual
inspection of the data used in this report again
served to draw attention to the primary causes
which reduce the quality of data. Because the
quality can be so easily improved, the causes
for the inadequacies and their effect on the heat
exchange results are reviewed. Errors in the
marine surface data are not so much due to in-
correct reading of instruments and recording of
observations as to improper placement and cali-
bration of the instruments, improper techniques
of measurement, and errors in data reduction
at sea.
To illustrate--high values for the wet and dry
bulb air temperatures indicate that the instru-
ments were placed in a warm location aboard
ship or that the psychrometric measurements
were not made in air freshly flowing off the sea.
It was previously stated that negative values in
the minimum sea-air vapor pressure differ-
ences of table A are probably due to erroneous
observations. Improper techniques in the psy-
chrometric measurement are believed to be the
primary cause. If the dry and wet bulb temper-
atures are not noted when the minimum wet bulb
temperature is reached, an overestimate of the
vapor pressure of the air results. Consequent-
ly, the sea-air vapor pressure difference will
be too low and may be negative.
In an analysis of sea surface temperatures
taken aboard merchant ships, Saur (1963) found
that deviations from mean values were large
and that the "injection temperatures," which
are often used in marine weather observations,
are measured in enginerooms and tend to be too
high. The large temperature deviations, in
terms of use in oceanography or meteorology,
may be due to improper placement and calibra-
tion of engineroom thermometers. Saur sug-
gested a correction of -0.7° C. for average sea-
water temperatures obtained from the marine
surface meteorological observations.
Errors in air and water temperatures affect
primarily the sea-air vapor pressure differ-
ence and so the heat of evaporation. Overesti-
mating the sea-water temperature by 0.7° C.
would mean an overestimate of the saturation
vapor pressure of water by 0.8 mb. at 15° C.
and 1.6 mb.at 28° C. Errors of similar magni-
tude occur in the vapor pressure of the air ow-
ing to wrong psychrometric measurements. The
sea-air vapor pressure differences of table A
are generally below 10 mb. and often below Smb.
The possible error in the heat of evaporation
may therefore be relatively large.
Visual inspection of data also indicated that
erroneous data reduction is the probable cause
for wrong wind speeds and directions. For ex-
ample, in areas with a large number of obser-
vations showing an easterly wind, an observa-
tion with a westerly wind may appear. A re-
versal in wind direction can easily occur in the
vector addition of the measured apparent wind
and the speed and direction of the ship. Incor-
rect vector addition also results in wrong wind
speeds and directions which are not as readily
detected as a 180° error in wind direction.
Effects of Data Inadequacies
on the Heat Exchange Results
The effects of data inadequacies in the trade
wind zone on the estimates of heat exchange
processes are best illustrated by examples.
Most critical are uncertainties in the cloudi-
ness, since it affects the primary process in
the net heat exchange across the sea surface,
the heat of radiation from sun and sky.
The cloudiness (table B) shows remarkable
consistency both in spatial and temporal distri-
bution. This consistency may, however, be
misleading. The average obtained from only a
few cloud observations per month that range
from clear sky to solid overcast quickly con-
verges to a value representing a semiovercast
condition. With at least daily observations,
however, the monthly average may shift to a
higher or lower value.
If an error of 0.1 is assumed for the cloudi-
ness, the cloud factor would be in error from
about 5 percent for low values in cloudiness to
over 20 percent for high values in cloudiness.
For example, at lat. 7° N., long. 142° W., July
1963, table B shows that C - 0.9 and Q(S) - 247
cal. cm7^day~'. An error of 0,1 in cloudiness
would change the heat of radiation from sun and
sky about 50 cal. cm7^day~'. A similar error
at lat. 22° N., long. 157° W., July 1963 with C =
0.4 and Q(S) - 529 cal. cmT^day"' would produce
a change of 30 to 40 cal. cmT^day"' in the heat
of radiation from sun and sky.
The error in the monthly cloud estimate may
be larger than O.I, and other factors, such as
the type and thickness of clouds, that have not
been considered here may introduce errors of
similar magnitude.
Values for the effective back radiation of ta-
ble B show that they fall within the limits of ob-
servation during the TWZO cruises (Charnell,
1967) and are small compared with the magni-
tude of the radiation from sun and sky. The ef-
fect of variations in effective back radiation on
the net heat exchange is also smaller than that
of variations in the radiation from sun and sky.
Again, cloudiness enters into the effective
back radiation, since the long wave radiation
from the sky reduces the magnitude of the long
wave radiation which escapes into space from
the sea surface. An error of 0.1 in the cloudi-
ness introduces a relative error in the cloud
factor that ranges from 1 percent for low val-
ues of cloudiness to about 20 percent for high
values of cloudiness. In terms of the results
listed in table B, to use an extreme example,
the effective back radiation at lat. 7° N., long.
142° W., July 1963, for a solid overcast would
be 52 cal. cmT^ day"' instead of 65 cal. cmT^
day"' for 0.9 cloudiness.
In low latitudes the thickness of the humid,
tropical air layer may be as important as the
cloudiness. Charnell (1967) reported that the
variations of long wave radiation measured
during clear sky conditions were of the same
magnitude as the differences between clear sky
and overcast conditions. He pointed out that
radiosonde data indicate variations of thickness
of the tropical air mass of the order of 1,000 m.
within a few days. Such variations in the thick-
ness of the humid air layer may have an effect
on the long wave radiation similar to that of a
varying cloud cover. Although the factor con-
taining the vapor pressure in the effective back
radiation equation partially accounts for the hu-
mid air mass effect, in low latitudes the effect
of variations in the thickness of the humid air
mass should also be considered.
The conduction of sensible heat is a small
quantity as compared with the other heat ex-
change processes. Uncertainties in this term
due to the shortcomings of the meteorological
observations have a negligible effect on the esti-
mate of net heat exchange across the sea sur-
face.
Since the heat of evaporation is a large quan-
tity, errors in this process due to data uncer-
tainties may seriously affect the net heat ex-
change results. The heat of evaporation depends
on the sea-air vapor pressure difference and
the nonlinear function of the wind speed when a
variable drag coefficient is used. The effect on
the former due to erroneous sea-water temper-
ature or psychrometric measurements has al-
ready been considered. The latter is affected
by the manner of processing the meteorological
data.
Effects of Processing Techniques
on the Heat Exchange Results
Ideally, if interest lies in the total of a heat
exchange process for an area such as a 5° square
about the Hawaiian Islands, for a month, an area
integral should first be obtained for each day (or
more frequently) and then be summed for the
month. If interest is concerned with a process
at a single location, values should be obtained
for each day (or more frequently) at that loca-
tion and then be summed for the month. With
some exceptions, the spatial and temporal dis-
tribution of meteorological data has been inad-
equate to follow these processing procedures.
It has therefore been necessary in the past as
well as here, to estimate monthly mean values
of the required meteorological properties for
relatively large areas and then to compute the
exchange processes.
This procedure involves the question of how
large is the difference between the mean of the
product and the product of mean values, since
all the empirical heat exchange expressions are
products of independently varying properties.
Malkus (1962) discussed this problem and cited
examples where the conduction of sensible heat
and the heat of evaporation were computed by
the two methods. The use of mean meteorolog-
ical properties resulted in an underestimate of
about 7 percent.
Table 2 lists for the three locations where
daily observations are available--lat. 2° N.,
long. 157° W. (Christmas Island), lat. 16° N.,
long. 169° W. (Johnston Island), and lat. 30° N.,
long. 140° W. (Ocean Weather Station Novem-
ber)— for each month, the exchange processes
as based on the values computed daily (subscripts
1), and those computed from mean monthly
meteorological properties (subscripts 2). In
general, for each of the sample locations, Q(S|)
is smaller than Q(S2), Q(B|) is smaller than
Q(B2), Q(E|) is larger than Q(E2), andQ(C|)is
about the same as QiCg). In consequence of
these differences, Q(N|) would be smaller than
Q(N2) due to Q(S|) and Q(E|) but larger due to
Q(B|) and Q(C|). At Christmas Island the dif-
ferences in the exchange processes are small
both in absolute and in relative terms. At John-
ston Island and Ocean Weather Station Novem-
ber, the differences (in the exchange processes)
are about the same as at Christmas Island ex-
cept for the heat of evaporation, which is signif-
icantly larger both in absolute and in relative
terms. The month-to-month variation in the
difference between Q(E,) and Q(E2) can also be
relatively large. Values of Q(C|) - Q(C2) are
unimportant. The differences in each of the ex-
change processes due to the manner of compu-
tation are reflected in the 2-year mean values
which are also tabulated.
It is evident from the tabulation that at John-
ston Island and at Ocean Weather Station No-
vember the relatively large values of Q(E|) -
Q(E2) have a pronounced effect on the differ-
ences between Q(N,) and Q(N2). An important
cause for the relatively large differences in the
heat of evaporation is the use of a variable drag
coefficient.
Consider the portion of the evaporation equa-
tion which depends on the wind speed, the heat
of evaporation per unit difference in sea-air
vapor pressure.
G(W) = 3.77
arctan (W - 8)
cal. cm
1.96
■2 day-'
+ 1.6 W
mb.'
It is apparent from figure 2, where G(W) is
plotted as a function of wind speed, that the
evaporation factor changes most rapidly be-
tween 6 and 10 m. sec."' Below and above these
speeds the change is about linear. Wind speeds
in the trade wind zone generally fall within the
range where .the change of G(W) is nonlinear.
One would therefore not expect the wind factor,
G(W), of the mean wind to be the same as the
mean wind factor, G(W). For example, in Feb-
G(w) = 3.77 [^^ecM::81+ 1.6] w,^
WIND SPEED (M. SEC."')
Figure 2. — The heat of evaporation per unit dif-
ference in sea-air vapor pressure as a function
of the wind speed.
Table 2. --Heat exchange processes for each month, cal. cm. day", July 1963 to June 1965, at Christmas
Island, lat. 2° N., long. 157° W. ; Johnston Island, lat. 16° N., long. 169° W. ; and Ocean Weather
Station November, lat. 30° N., long. 140° W. Subscripts 1, exchange processes computed daily; sub-
scripts 2, exchange processes comouted from mean monthly meteorological pronertles
Year Month QCS^) Q(Sj) QCBj) Q(Bj) Q(Ei) QCE^) Q(Ci) Q(C2) Q(Ni) QCNs)
Christmas Island
Gal, cm. 'day ^
1963 July
1963 Aug.
1963 Sept.
1963 Oct.
1963 Nov.
1963 Dec.
1964 Jan.
1964 Feb.
1964 Mar.
1964 Apr.
1964 May
1964 June
1964 July
1964 Aug.
1964 Sept.
1964 Oct.
1964 Nov.
1964 Dec.
1965 Jan.
1965 Feb.
1965 Mar.
1965 Apr.
1965 May
1965 June
409
408
452
408
382
369
357
400
378
397
387
412
417
441
436
455
431
426
430
468
442
438
392
372
2-year average 413
421
424
471
42 7
395
380
368
417
397
407
401
430
434
460
463
478
452
444
457
494
472
460
413
392
432
88
84
84
77
80
78
74
80
68
72
78
84
84
85
72
72
63
74
93
89
90
82
84
81
78
85
74
74
82
92
91
93
81
78
69
81
83
69
81
83
147
89
124
81
70
50
89
101
88
116
73
54
50
38
56
67
81
83
106
88
102
78
69
44
83
101
95
105
72
53
47
39
55
76
-2
-6
-15
-16
-9
-10
-10
-8
-9
-19
-22
-19
-30
-33
-34
-42
-22
-29
-22
-19
-13
-14
-7
-18
-3
-4
-13
-15
-9
-10
-8
-7
-10
-20
-21
-19
-30
-33
-32
-41
-22
-25
-20
-17
-13
-13
-5
-17
250
248
299
201
221
176
212
258
273
254
229
259
271
331
335
330
302
254
261
264
258
311
254
232
207
220
270
289
270
239
264
295
349
355
348
318
261
278
Johnston Island
1963
July
382
399
73
76
141
123
-18
-18
174
218
1963
Aug.
378
403
72
80
145
131
-13
-14
172
206
1963
Sept.
420
434
93
94
178
153
-2
-1
136
188
1963
Oct.
2 92
306
69
73
169
142
-6
-7
80
98
1963
Nov.
321
329
95
100
210
168
5
6
6
55
1963
Dec.
264
278
102
111
317
249
24
26
-191
-108
1964
Jan.
305
312
101
106
398
390
0
1
-216
-185
1964
Feb.
310
323
94
103
367
347
7
9
-191
-136
1964
Mar.
387
402
107
115
233
192
12
15
35
80
1964
Apr.
343
360
81
86
164
134
2
2
62
138
1964
May
444
472
98
106
148
128
4
4
190
234
1964
June
403
421
93
98
203
174
0
0
114
149
1964
July
469
483
103
108
231
194
-5
-5
151
186
1964
Aug.
347
371
82
90
232
204
3
4
19
73
1964
Sept.
315
347
82
90
166
147
10
11
87
99
1964
Oct.
389
416
107
116
201
185
15
16
41
99
1964
Nov.
332
353
113
117
203
166
17
21
50
49
1964
Dec.
320
333
118
126
174
143
17
22
-4
42
1965
Jan.
292
306
126
134
229
166
28
29
-56
-23
1965
Feb.
356
386
136
149
565
538
43
40
-357
-341
1965
Mar.
434
450
132
137
256
184
16
15
62
114
1965
Apr.
461
491
118
123
174
159
-3
-2
178
211
1965
May
442
462
100
109
182
143
0
1
144
209
1965
June
451
473
103
110
381
387
6
5
-50
-29
2-year average 369
388
100
107
236
206
27
68
10
Table 2. — Heat exchange processes for each month, cal. cm.~^day~^, July 1963 to June 1965, at Christmas
Island, lat. 2° N. , long. 157° W. ; Johnston Island, lat. 16° N. , long. 169° W. ; and Ocean Weather
Station November, lat. 30° N. , long. 140° W. Subscripts 1, exchange processes computed daily; sub-
scripts 2, exchange processes computed from mean monthly meteorological properties — Continued
Year
Month
Q(Si)
Q(S2)
Q(Bi)
Q(B2)
Q(Ei)
Q(E2)
Q(Ci)
QCCz)
Q(Ni)
Q(N2)
Cal. cm. "^ day
-I
Ocean Weather
Station November
1963
July
354
364
92
96
122
94
-2
-4
141
178
1963
Aug.
387
408
104
110
94
81
-2
-3
191
220
1963
Sept.
387
398
117
120
140
112
1
2
128
164
1963
Oct.
304
314
132
136
177
137
20
18
-26
23
1963
Nov.
191
198
118
122
135
124
20
19
-82
-67
1963
Dec.
177
182
105
110
100
85
-5
-2
-23
-11
1964
Jan.
167
169
108
112
190
132
11
11
-143
-86
1964
Feb.
230
234
122
126
266
192
22
23
-180
-107
1964
Mar.
230
235
98
102
248
207
13
16
-130
-90
1964
Apr.
239
243
91
93
221
183
21
22
-95
-55
1964
May
333
344
115
120
188
150
30
30
-1
44
1964
June
345
360
96
101
114
94
7
6
128
159
1964
July
338
348
91
94
110
94
0
0
136
160
1964
Aug.
395
409
112
116
114
94
6
6
162
193
1964
Sept.
315
328
107
111
190
163
3
3
14
51
1964
Oct.
284
296
113
117
155
106
1
3
13
71
1964
Nov.
202
209
116
120
227
152
11
10
-153
-73
1964
Dec.
173
177
98
102
66
64
-14
-9
22
20
1965
Jan.
182
185
100
105
133
91
-6
-5
-44
-6
1965
Feb.
195
204
92
96
252
213
2
0
-151
-105
1965
Mar.
258
267
103
106
205
128
10
9
-61
24
1965
Apr.
316
326
100
104
161
134
-3
-2
57
90
1965
May
306
329
97
106
165
122
12
14
36
87
1965
June
407
421
115
120
157
118
8
8
125
175
2-year avera
ge 280
290
106
110
164
128
7
7
3
44
ruary 1964, at lat. 30° N., long. 140° W., Q(E|) =
266 cal. cmT^day"' and QCEg) - 192 cal. cmr^
day"'. The evaporation computed from mean
monthly meteorological properties was 28 per-
cent below that computed daily. The mean wind
speed for this month was 6.4 m. secT' giving
G(6.4) = 26 cal. cm7^ day"'mb.~' The average
daily value of G(W) was 38.3 cal. cm7^ day~'mbr'
Here G(6,4) was 32 percent below G(W). Be-
cause of the nonlinearity of G(W), a changing
frequency distribution of wind speeds from
month to month would contribute to the chang-
ing differences between Q(E|) and Q(E2) in the
above listing for the three locations.
The differences between Q(E|) and Q(E2) at
Christmas Island are small because winds are
generally below 6 m. sec."', so that they fall in
the approximately linear portionof G(W) (fig. 2).
The discussion concerning the effect of tem-
poral changes in wind speed on the mean value
of G(W) applies also to spatial changes in wind
speed. It can be shown, however, that the effect
of wind gradients of the magnitude occurring in
the trade wind zone on the area mean of G(W) is
small.
The dependence of the computed heat of evap-
oration on the method of processing can be dem-
onstrated further for the 5° square lat. 25° to
29° N., long. 140° to 144° W., where the number
of observations were 164 to 225 per month.
Three methods of computations were used: (1)
the heat of evaporation was computed for each
set of meteorological data and the daily mean
value of the heat of evaporation was then used
to obtain the monthly average, which is desig-
nated Q(E); (2) mean daily meteorological prop-
erties for the 5° square were used to compute
the daily heat of evaporation from which the
monthly means were then obtained--these values
are equivalent to those in the above listing of
the three locations which were designated Q(E|);
(3) from the daily mean values for the 5° square
the monthly mean meteorological properties
were computed which, in turn, were used to ob-
II
tain the monthly heat of evaporation--these val-
ues are equivalent to QiEg) of the above listing.
The results of the three methods of computation
are presented in figure 3.
In method 1, if for each day the meteorologi-
cal observations were uniformly distributed in
the 5° square, Q(E) would represent the mean
monthly evaporation for the area. In methods 2
and 3, Q(E|) and Q(E2) represent the results for
the mean location of observations. Since the
heat exchange processes in table B are based
on the interpolated, mean meteorological prop-
erties, they, too, represent values at the loca-
tions listed rather than for the 5° square.
For the 24 months, the differences between
Q(E) and Q(E|) range from 2 to 32 cal. cm."^
day"' and average 17 cal. cmT^ day"'. The dif-
ferences between Q(E|) and Q(E2) range from
-56 to 69 cal. cmT^ day"' and average 35 cal.
cmT^day"'. The average difference between
Q(E) and Q(E|) is less than 7 percent, about as
reported by Malkus (1962), and reflects the ef-
fects of variability in the data. The differences
between Q(E|) and QCEg) are about the same as
those for the computations at Johnston Island
and Weather Station November, listed above.
Figures shows that in all months QiEj) is the
lowest value except for December 1964, when it
was 10 cal. cmr^day"' above Q(E|), and Feb-
ruary 1965, when it was 56 cal. cmr^day"' above
Q(E|). The large deviation in Q(E|) - QCEg)
during February 1965 from the common occur-
rence illustrates that fluctuations in the evap-
oration are not only due to the variable wind
factor, G(W), but also due to changes in the sea-
air vapor pressure difference. Daily values
showed that meteorological conditions departed
from those commonly observed in this 5°
square. During February 1965, a relatively
high frequency of winds above 10 m. sec."' cor-
responded with low values of the sea-air vapor
pressure difference. The winds below 10 m.
sec."' corresponded with higher sea-air vapor
pressure differences. In consequence, the mean
monthly meteorological properties yielded a
higher evaporation rate than the mean daily
evaporation rates. The departure in meteoro-
logical conditions for this month is apparent
from the data summaries in table A (lat. 25°-
29° N., long. 140°-144° W.). Relatively strong
southeasterly winds with a lower sea-air vapor
pressure difference contrasted with northeast-
300
a
1963
1964
1965
Figure 3. — Monthly heat of evaporation, cal. cm. day , lat.
25° to 29° N., long. 140° to 144° W. , July 1963 to June
1965, Q(E), mean heat of evaporation based on computations
made for each set of meteorological observations, Q(Ei),
mean heat of evaporation based on daily mean meteorological
properties, and QCEa), mean heat of evaporation based on
monthly mean meteorological properties.
12
erly or easterly winds of lower speed and with
a higher sea-air vapor pressure difference as,
for example, during February 1964.
A relative difference in the heat of evapora-
tion, possibly 20 percent, due to the difference
in processing methods can cause a much larger
relative error in the net heat exchange, whose
absolute value ranges from 0 to 200 cal. cmr^
day-'. This effect is apparent in figure 4, where
the net heat exchange across the sea surface
has been plotted by using the three methods of
computation described for the heat of evapora-
tion, in the area lat. 25° to 29° N., long. 140° to
144° W. The 2-year average of Q(N|) is -32 cal.
cmT^day"' and that of Q(N2) is 7 cal. cm.'^day"'.
In the trade wind zone such differences in the
ocean heat budget are significant.
Comparison with Other Results
in the North Pacific
It remains to compare the results of table B
with other heat exchange values for the North
Pacific. Most suitable for comparison are the
monthly charts of the heat of evaporation and
the net heat exchange across the sea surface
prepared by Wyrtki (1966). His charts are based
on 1947 to 1960 averages of marine surface
meteorological data. He calculated the heat ex-
change processes with the same empirical for-
mulas as were used here except for minor dif-
ferences in the coefficients and for his use of
constant drag coefficient in the evaporation
equation. The comparison, therefore, primarily
shows the differences between the monthly ex-
change processes of individual years and those
200
-300
_ I 1 1 1 1 1 1 1 1
1 1
1 1 I 1
1 1 I 1 1 1 1 1 _
_
i
n
;• ':
fl
0(N,)
•/!•:
OCNj)
/'«=
f '1 ll
■1 ':
'/ '^
~
~ •It I 1 '■
'/ I;
: „ ~
/ v-
/.
J
|\
/
j
/ 1/
f\ l>^'
/ 1 :.
1 Ir
TTT
1 \ •''/ \^
s
1 1 1
1 ^
1'
11'
/ I--
1
a'
4 1^
\ V ■•
•' //
/
' ■' W 1
••■■//
/7
1
y \\ /
w \xii\
U V -
\ \ //
1 1
\ \' /
1/
\ V /
V
1111
1
1 1 1 1
1 1 1 1 1 1 1
1963
SONDIJ FMAMJ
0 N D I ,
F M A M
1964
I96S
Figure 4. — Monthly net heat exchange across the sea surface
(cal. cm. "^day"'^) lat. 25° to 29° N. , long. 140° to 144° W. ,
July 1963 to June 1963. Q(N), mean net heat exchange based
on computations made for each set of meteorological obser-
vations, Q(Ni), mean net heat exchange based on daily mean
meteorological properties, and Q(N2), mean net heat exchange
based on monthly mean meteorological properties.
13
based on long-term mean meteorological data.
Differences resulting from the use of a constant
instead of a variable drag coefficient in the
evaporation equation also become apparent.
Results from two locations were chosen for
comparisons: (1) lat. 17° N., long. 152° W., in
the trade wind region. (2) lat. 2°N., long. 157°
W., in the equatorial region. The heat of evap-
oration and the net heat exchange across the
sea surface from the trade wind region are
shown in figure 5 and those from the equatorial
region are shown in figure 6.
In the trade wind zone (fig. 5), the large fluc-
tuations in Q(E), which change from year to
year, make it difficult to discern a seasonal
trend. A seasonal trend in the variation of Q(N),
however, is not obscured even though the effects
of the large fluctuations of Q(E) are apparent.
The relatively large amplitude in the seasonal
cycle of Q(S) must, therefore, be a dominant
factor in the net heat exchange across the sea
surface at lat. 17° N.
In view of the large variability in the heat of
evaporation, the month-to-month trend of Wyrt-
ki's Q(E) values is not expected to correspond
with those during either of the 2 years from
1963 to 1965. As was true for the results of
table B, Wyrtki's 0(E) fluctuations do not ob-
scure the seasonal trend of Q(N).
Comparison of Q(E) and Q(N) averages shows
good agreement. The 1963 to 1965 average Q(E)
is about 260 cal. cmr^day-' and Wyrtki's annual
average 0(E) is about 270 cal. cmT^day"'. Sim-
ilar mean values of Q(N) are about 30 cal.
cmT^ day"' and 50 cal. cmT^day"', respectively.
In the equatorial example (fig. 6), fluctua-
tions in Q(E) during 1963 to 1965 are less pro-
nounced than in the trade wind zone and a sea-
sonal trend is apparent; evaporation is high
during summer and autumn and low during win-
ter and spring. Year-to-year changes inQ(N),
however, are larger than expected from the dif-
ferences in Q(E), particularly from November
to February. In the equatorial region the ampli-
tude of the seasonal variations in the clear sky
radiation, Qq, is relatively small so that year-
to-year differences in cloudiness must play an
important role in the net heat exchange across
the sea surface. This variability in Q(S) also
obscures the seasonal trend of the heat of evap-
oration in 0(N).
N D J F
MONTHS
1 1 1 1
1 -
/i Q{N)
r:rrt(r\ /iir.7 nrti
200
SECKEL (1964-65) -
r-1
:
\ 1 ^
1 \ ■ '
1 > ■
1 \
100
0
-
\ V
= \ V
1 rk \/
p \ 1
-
> \-
A/ lA :
-
\ \
1 \
; y
-100
-
\ \
\ \
f. \
-
\
-200
_
V
-
1 1 1 1 . 1
N 0 J F
MONTHS
M A M J
Figure 5. — The heat of evaporation, Q(E), and the net heat exchange across
the sea surface, Q(N), at lat. 17° N. , long. 152° W. , July 1963 to June
1965 (from table B) , and interpolated values from climatic charts by
Wyrtki (1966).
lA
The seasonal trend in Wyrtkl's Q(E) values
is consistent with those during 1963 to 1965.
Again, in view of the variability in Q(N) near
the Equator during 1963 to 1965, the trend of
Wyrtki's month-to-month values of Q(N) is not
expected to be similar to either of the 2 years.
In contrast to the good agreement in average
values of Q(E) and Q(N) in the trade wind zone,
those in the equatorial region differ consider-
ably. The 1963 to 1965 average Q(E) is about
100 cal. cmT^day"', whereas Wyrtki's annual
average Q(E) is about 200 cal. cmT^ day"'. Sim-
ilar mean values of Q(N) are about 240 cal.
cm7^day"'and 160 cal. cm7^ day"' , respectively.
The difference in Q(E) is primarily due to the
use of different drag coefficients in the evapor-
ation equation. The average wind speed at lat.
2" N., long. 157° W., July 1963 to June 1965
(table B) was 4.7 m. seer' for which the drag
coefficient is 0.96 x 10"'. Wyrtkl used a con-
stant drag coefficient, Cp = 1.55 x 10"'. Thus,
the difference in drag coefficients accounts for
the major portion of the difference in the evap-
oration rates and therefore also In the differ-
ence of the net heat exchange across the sea
surface.
Within the limitation discussed above, the re-
sults for the two sample areas show that the
heat exchange processes computed here are
consistent with those based on long-term aver-
age data presented by Wyrtki.
Interseason and Interyear Comparisons
In a previous section it was shown that the
manner of processing affects mainly the heat of
evaporation and, therefore, also the results for
the net heat exchange across the sea surface.
Figures 3 and 4 show that, regardless of the
manner of computation, the month-to-month
trends in the heat of evaporation and the net heat
exchange across the sea surface are similar.
Here, then, the importance of absolute magni-
tudes in interseason and interyear comparisons
is examined.
Results for the area, lat. 25° to 29° N., long.
140° to 144° W., which were previously used,
are also used to compute the differences be-
tween principal extremum values of Q(E|) and
Q(E2)--see figure 3--and Q(N|) and QCNg) (fig.
4). These differences, listed in table 3, show
that the trends of change (increasing or de-
creasing) are the same whether the exchange
processes are based on daily or mean monthly
meteorological properties. The magnitudes of
change are also similar but agreement tends
to be better in spring and summer than during
autumn and winter.
400
T — I — I — I — I — I — \ — r
Q(E)
SECKELI 1963-64)
SECKEL (1964-65)
WYRTKI
1 1 1 I 1 1 1
Till!
-
Q(N)
-
\ \ /
/ ' v
-
/ \ r
' '•^■••■' :
-
■■■■■■.■ ■: :
\ 1
"
-
V
-
-
1 1 t 1 1 1
S 0 N D
MONTHS
ASONDJFMAMJ
MONTHS
Figure 6. — The heat of evaporation, Q(E), and the net heat exchange
across the sea surface, Q(N), at lat. 2° N. , long. 157° W. , July
1963 to June 1965 (from table B) , and interpolated values from
climatic charts by Wyrtki (1966).
Table 3. — Differences in extremum values of Q(Ei),
Q(E2). Q(Ni), and Q(N2), lat. 25° to 29° N., long.
140° to 144° W.
Time period
QCEi-)
Q(E2)
Cal. cm."^day-'
Cal. cm.~^day"'
Sept. -Nov. 1963
95
62
Nov. -Dec. 1963
-3
-19
Dec. 1963-Feb. 1964
129
163
Feb. -June 1964
-183
-191
June-July 1964
17
24
July-Aug. 1964
-49
-40
Aug. -Sept. 1964
148
121
Sept. -Oct. 1964
-98
-63
Oct. -Nov. 1964
100
67
Nov. -Dec. 1964
-203
-138
Dec. 1964-Feb. 1965
207
253
Feb. 1965-Apr. 1965
-119
-205
Q(Ni)
Q(N2)
Cal. cm.-^day"'
Cal. cm.~^day"'
Aug. 1963-Feb. 1964
-380
-385
Feb. -Aug. 1964
420
414
Aug. -Sept. 1964
-246
-220
Sept. -Oct. 1964
92
54
Oct. -Nov. 1964
-218
-182
Nov. -Dec. 1964
246
173
Dec. 1964-Jan. 1965
-205
-246
Feb. -Apr. 1965
191
282
Table 4. Interyear
comparisons of 4
-month averages
of Q(E ) and QCE^),
to 144* W.
lat. 25° to 29°
N., long. 140°
Time period
Q(Ei)
QCEa)
Cal. cm."^day"'
Cal. cm."^day"'
Aug. -Nov. 1963 averag
e 200
158
Aug. -Nov. 1964 averag
e 237
196
Interyear difference
37
38
Jan. -Apr. 1964 averag
e 321
287
Jan. -Apr. 1965 averag
e 254
257
Interyear difference
-67
-30
Table 5. --Interyear comparisons of 3-month averages
of Q(Nj) and QCN^), lat. 25° to 29° N., long. 140°
to 144° W.
Time
period
Q(N,
)
Q(Na)
Cal
cm.'
^day-'
Cal. cra.'^day"'
July-Sept
1963 average
98
136
July-Sept
1964 average
67
113
Interyear
difference
-31
-23
Jan. -May.
1964 average
-183
-139
J an. -Mar .
1965 average
-111
-123
Interyear
difference
•72
16
For month-to-month differences of Q(E|) and
Q(E2) the averages of the absolute magnitudes
are 96 cal. cmT^ day"' and 84 cal. cmr^day"',
respectively, and for Q(N|) and Q(^2) ^^ °^^-
cmT^day~'and 64 cal. cmT^day"', respectively.
For interyear comparisons of similar sea-
sons figure 3 shows that the maximum evapo-
ration period was longer during the first part
of 1964 than during the first part of 1965 and
that the differences were marked in the summer
and autumn evaporation of 1963 and 1964. Table
4 shows 4-month averages of Q(E|) and QCEg) at
lat. 25° to 29° N., long. 140° to 144° W., for Au-
gust to November and January to April.
Figure 4 shows that values of the net heat ex-
change across the sea surface are highest dur-
ing late summer and early autumn and lowest
during winter. For interyear comparisons, 3-
month averages of Q(N,) and QCNg) (lat. 25° to
29° N., long. 140° to 144° W.) are listed in table
5.
The trend of change is the same, but inter-
year differences based on results computed
daily are larger than differences based on re-
sults computed from monthly mean meteoro-
logical properties. When the interyear differ-
ences are compared, it should be remembered
that those for Q(E) are not expected to be the
same as those for Q(N) since in the latter the
interyear differences of Q(S) and Q(B) are also
involved.
Generalizing the results of these compari-
sons, a tendency exists to underestimate the
interyear differences of the heat of evapora-
tion and of the net heat exchange across the sea
surface presented in table B. The underesti-
mates will be largest in areas and at times of
greatest variability in the meteorological prop-
erties that affect the heat exchange processes.
The use of table B for interyear comparisons
is illustrated below for three sample areas,
each of which lies in a different climatic zone.
The trade wind zone extends over the largest
portion of the region under consideration here.
This region, however, also extends into two
other climatic zones. The northern portion of
the region lies near the North Pacific pressure
ridge and generally has low wind speeds but,
during the winter, may come under the influ-
ence of the Northwest Pacific atmospheric cir-
culation. The southern portion of the region
lies in the equatorial zone.
Consider first the northern zone. The abso-
lute magnitude of interyear differences of Q(E)
and Q(N) at lat. 32° N., long. 167° W. in table B
16
from April to November are relatively low and
average 28cal. cmT^day"' and 56 cal. cmT^day"',
respectively. From December to March these
interyear differences, however, are an order of
magnitude larger (table 6).
Consider next lat. 17° N., long. 152° W. (table
B) in the trade wind zone, where the variations
of Q(E) are large and where the most pronounced
interyear differences occur during January to
April (fig. 5). Table 7 lists average values of
Q(E) and Q(N) for the 4 months January to April.
Finally, in the equatorial zone, lat. 2° N.,
long. 157° W. (table B, fig. 6), interyear dif-
ferences are primarily reflected by the net heat
exchange across the sea surface. From No-
vember 1964 to May 1965, Q(N) was larger than
during the same months 1 year earlier. Table
8 lists average values of Q(E) and Q(N) for the
4 months November to February, the period of
largest interyear difference in Q(N).
The illustrations based on the results of ta-
ble B show that interyear differences of Q(E)
and Q(N) during the 2-year period under con-
sideration were larger than the variations to be
expected from the data uncertainties discussed
earlier in this paper. Furthermore, the inter-
year differences in the northern zone and in the
trade wind zone are probably underestimated.
The interyear differences in the northern
zone and in the trade wind zone are also con-
sistent with the monthly mean sea-level pres-
Table 6. --Interyear differences of Q(E) and Q(N),
lat. 32° N., long. 167° W. (from table B)
Time period
Q(E)
Q(N)
Cal.
cm."
= day-'
Cal
cm." day ^
Dec. 1963
568
-638
Dec. 196A
351
-354
Interyear difference
-217
284
Jan. -Mar. 1964 average
lOA
49
Jan. -Mar. 1965 average
273
-206
Interyear difference
169
-255
Table 7. --Interyear differences of Q(E) and Q(N) ,
lat. 17° N., long. 152° W. (from table B)
Time
period
Q(E)
Q(N)
Cal.
cm.~ day"
Cal.
cm. ^day '
Jan. -Apr.
1964 average
441
-44
Jan. -Apr .
1965 average
134
100
Interyear
difference
-307
144
sure distributions (Northern Hemisphere charts
of mean sea-level atmospheric pressure. Ex-
tended Forecast Division, National Meteoro-
logical Center, Environmental Science Ser-
vices Administration). During the winter and
spring of 1964, the trade winds were well de-
veloped and contributed to the large evapora-
tion rates in the trade wind zone. During the
winter of 1965 the trade winds were weak and
the northern zone came under the influence of
the Northwest Pacific circulation. In conse-
quence evaporation rates were high in the
northern zone but low in the trade wind zone.
Table 8. --Interyear differences of Q(E) and Q(N),
lat. 2° N., long. 157° W. (from table B)
Time period
Q(E)
Q(N)
Cal.
cm.-^
day"'
Cal.
cm. ^day"'
Nov. 1963 to Feb. 1964
average
112
195
Nov. 1964 to Feb. 1965
93
274
average
Interyear difference
-19
79
CONCLUSION
Despite the limitations of the marine surface
meteorological data, meaningful measures of
the month-to-month and year-to-year changes
in the large-scale heat exchange processes have
been obtained for a large portion of the North
Pacific trade wind region. The results pre-
sented in table B, therefore, satisfy the needs
of the TWZO investigation.
Beyond this application, the need for monthly
measures of large-scale, sea-air interaction
processes in the trade wind zone will continue
and increase; the experience gained in the prep-
aration of this paper may be of help in future
work. Some suggestions to facilitate the calcu-
lations and improve the results are therefore
made.
The mechanics of processing large quantities
of meteorological and oceanographic observa-
tions for the computation of sea-air interaction
processes are still in the developmental stages.
In the work reported here, quality control pro-
cedures involved laborious visual inspection of
original data. Obvious errors that were initially
overlooked could usually be corrected during
the preparation of the smoothed charts. By us-
ing the statistics of table A, it is now possible
17
to impose limits so that for a second pass of
the data through the computer , programs can be
written to reject erroneous data.
A more sophisticated use of computers to
summarize oceanographic and meteorological
data was suggested by Frye (1968), who report-
ed a regression analysis of sea-surface-tem-
perature patterns for the North Pacific Ocean.
For limited areas of the ocean, such as the
trade wind region, it may in the future be pos-
sible to develop suitable models so that the dis-
tribution of properties can be expressed as
functions of latitude, longitude, and time.
In the previous section the effect of short-
comings in the distribution and quality of data
on the heat exchange values was illustrated. A
most difficult distribution to estimate from iso-
lated ships' observations is the cloudiness.
This property affects the most important term
in the heat budget, the radiation from sun and
sky. In this area of uncertainty greatest im-
provement may come from satellite observa-
tions of the cloud cover. It may also be possi-
ble to compute the effective back radiation from
direct satellite measurements.
The mainstay of data for the computations of
large-scale, sea-air interactions will, neverthe-
less, remain the synoptic observations made by
ships at sea. It was shown that the inability to
compute the heat of evaporation daily may lead
to relatively large underestimates of this im-
portant process. In a large portion of the trade
wind zone, observations are sufficiently frequent
to permit daily computation of the heat of evap-
oration. In critical areas of the low latitudes,
however (see table A), the sampling frequency
should be increased; this may be accomplished
by an effort to enlist in the synoptic weather
observations program the cooperation of all
ships which travel through these areas.
Since ships' observations will continue to pro-
vide the largest number of data for the compu-
tation of sea-air interaction processes, an ef-
fort should be made to improve the quality of
data. Most important are the sea surface tem-
perature, psychrometric, and wind measure-
ments. These observations can be materially
improved by the calibration of instruments,
particularly those for the measurement of the
sea surface temperature. The observations can
also be improved by proper location of instru-
ments and by instruction of observers in proper
techniques of measurement.
ACKNOWLEDGMENT
Colin S. Ramage, University of Hawaii, made
suggestions during the preparation of this paper
and Colin S. Ramage and Saul Price, Environ-
mental Science Services Administration, re-
viewed the manuscript.
LITERATURE CITED
BOLSENGA, S. J.
1964. Daily sums of global radiation for cloud-
less skies. U.S. Army Mater. Command,
Cold Regions Res. and Eng. Lab., Han-
over, N. H., Res. Rep. 160, iv + 124 pp.
CHARNELL, ROBERT L.
1967. Long-wave radiation near the Hawaiian
Islands. J. Geophys. Res. 72: 489-495.
CHARNELL, ROBERT L., DAVID W. K. AU, and
GUNTER R. SECKEL.
1967a. The Trade Wind Zone Oceanography
Pilot Study. Part I: Townsend Cromwell
cruises 1, 2, and 3, February to April
1964. U.S. Fish Wildl. Serv., Spec. Sci.
Rep. Fish. 552, v + 75 pp.
1967b. The Trade Wind Zone Oceanography
Pilot Study. Part II: Townsend Cromwell
cruises 4, 5, and 6, May to July 1964.
U.S. Fish Wildl. Serv., Spec. Sci. Rep.
Fish. 553, v + 78 pp.
1967c. The Trade Wind Zone Oceanography
Pilot Study. Part III: Townsend Cromwell
cruises 8, 9, and 10, September to No-
vember 1964. U.S. Fish Wildl. Serv.,
Spec. Sci. Rep. Fish. 554, v + 78 pp.
1967d. The Trade Wind Zone Oceanography
Pilot Study. Part IV: Townsend Cromwell
cruises 11, 12, and 13, December 1964 to
February 1965. U.S. Fish Wildl. Serv.,
Spec. Sci. Rep. Fish. 555, v + 78 pp.
1967e. The Trade Wind Zone Oceanography
Pilot Study. Part V: Townsend Cromwell
cruises 14 and 15, March and April 1965.
U.S. Fish Wildl. Serv., Spec. Sci. Rep.
Fish. 556, iv + 54 pp.
1967f. The Trade Wind Zone Oceanography
Pilot Study. Part VI: Townsend Cromwell
cruises 16, 17, and 21, May and June 1965
and January 1966. U.S. Fish Wildl. Serv.,
Spec. Sci. Rep. Fish. 557, iv + 59 pp.
18
FRYE, H. W.
1968. Regression analysis of sea-surface-
temperature patterns for the North Pa-
cific Ocean. Naval Undersea Warfare
Center, San Diego, Calif., NUWC TP 30,
28 pp.
JOHNSON, JAMES H., GLENN A. FLITTNER,
and MARVIN W. CLINE.
1965. Automatic data processing program for,
marine synoptic radio weather reports.
U.S. Fish Wildl. Serv., Spec. Sci. Rep.
Fish. 503, iv+ 74 pp.
LAEVASTU, T.
1960. Factors affecting the temperature of
the surface layer of the sea. Commentat.
Physico-Math. Soc. Sci. Fennica, 25, 136
pp.
1965. Synoptic scale heat exchange and its
relations to weather. Fleet Numerical
Weather Facility, Monterey, Calif., Tech.
Note 7, 16 pp.
LIST, ROBERT J.
1951. Smithsonian meteorological tables. 6th
rev. ed. Smithsonian Miscel. Collect. 114,
527 pp.
Mcdonald, willard f.
1938. Atlas of climatic charts of the oceans.
Dep. Agr. Weather Bur., Washington,
D.C., W.B. 1247, vi + 65 pp.
MALKUS, JOANNE S.
1962. Large-scale interactions. In M.N. Hill
(editor), The sea, ideas and observations
on progress in the study of the seas, vol.
1, pp. 88-294, Interscience Publishers,
New York.
MIYAKE, YASUO.
1952. A table of the saturated vapour pres-
sure of sea water. Oceanogr. Mag. 4:
95-118.
MURRAY, F. W.
1967. On the computation of saturation vapor
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RAMAGE, C, S., F. R. MILLER, and C. JEF-
FERIES.
In press. International Indian Ocean Expedi-
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surface climate of 1963 and 1964. East-
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1959. On the heat and salt balance of the Cal-
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1963. A study of the quality of sea water tem-
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417-425.
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1962. Atlas of the oceanographlc climate of
the Hawaiian Islands region. U.S. Fish
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1968. A time-sequence oceanographlc inves-
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8 pp., 72 figs.
MS*1949
19
APPENDIX TABLE A
Observed meteorological properties, lat. 0° to 35° N., long. 130° to 170° W. ,
summarized by 5° square units of area and by months, July 1963 to June 1965
List of notations
T(A) Air temperature, degrees Celsius.
T(W) Sea surface temperature, degrees Celsius.
E(W) Saturation vapor pressure over pure water at sea surface temperature, millibars.
E(A) Vapor pressure of air, millibars.
C Cloudiness, proportion of sky covered.
P Atmospheric pressure, millibars minus 1,000.
W Wind speed, meters per second.
W(X) East-west component of wind velocity, meters per second; wind from the east is negative.
W(Y) North-south component of wind velocity, meters per second; wind from the north is negative.
Example
Sample column for July 1963, lat. 30° to 35° N., long. 170° to 165° W.
Mean location of observations: 30 + A = 3A° N. lat., 165 + 2 = 167° W. long.
Mean value of observations.
Highest value.
Lowest value.
Standard deviation.
Number of observations.
This example applies to the tabulations of all properties except that in the columns for W(X) and
W(Y) the number of observations is not repeated from the column for W.
170
li
T(A)
4
2
23.
5
27.
5
18.
0
2.
0
28
20
lO
I
o
3
if)
3
O
<
o
'^
--mom ■rcOo'^ «m*Df^^ Oo*^**^ ■OOO'^ tr\ r^f^ -Q OVOfM mo-*"*000'>4
i/>
om(M-.o o-ttf>.-(? ,*i,Nh»iNO o*r-ff''^o> o-.ooCT' f^J«r-p^^(^ ^A'^JO(MC^o*a)'^(r^■*f^J'.^
f.^ ff\imi<n f^ r^ m tilt
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APPENDIX TABLE B
Interpolated values of meteorological properties and heat exchange processes, lat.
0° to 35° N. , long. 130° to 170° W. , at the center of 5° square units of area for
each month, July 1963 to June 1965, presented in geographic format with decimal
point at center of the 5° square
List of notations
T(W) Sea surface temperature, degrees Celsius.
T(A) Air temperature, degrees Celsius.
E(A) Vapor pressure of air, millibars.
C Cloudiness, proportion of sky covered.
W Wind speed, meters per second.
Q(S) Radiation from sun and sky, calories per square centimeter per day, positive if water gains
heat.
Q(B) Effective back radiation, calories per square centimeter per day, positive if water loses
heat.
Q(E) Heat of evaporation, calories per square centimeter per day, positive if water loses heat.
Q(C) Conduction of sensible heat, calories per square centimeter per day, positive if water loses
heat.
Q(N) Net heat exchange across the sea surface, calories per square centimeter per day, positive
if water gains heat.
105
JULY 1963
LONGITUDE WEST
TIM)
167
162
157
152
147
142
137
132
32
23.0
22.4
21.7
21.1
20.7
20.3
19.5
18.8
I
1-
1
27
22
23.8
25.2
23.7
24.7
23.2
24.5
22.7
24.0
22.3
23.3
21.4
22.7
20.5
22.0
19.7
21.7
UJ
O
3
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17
12
7
25.7
26.5
28.0
25.0
26.5
28.0
25.3
26.3
27.3
24.5
25.7
27.0
23.9
26.2
28.0
24.2
26.5
27.7
24.2
26.3
27.5
23.8
26.0
27.5
2
27.7
27.8
27.9
27.9
27.7
27.5
27.7
27.0
TIA)
167
162
157
152
147
142
137
132
32
23.7
22.7
21.7
21.0
20.7
20.0
19.5
19.0
I
O
7'
27
22
2*. 7
25.5
24.0
25.2
23.2
24.7
22.5
24.0
22.2
23.5
21.5
23.2
20.6
22.4
19.9
21.2
i\
17
26.5
26.2
25.5
24.9
24.4
24.1
24.0
23.1
3
1-
12
7
26.7
27.0
26.5
27.0
26,0
26.7
25.7
26.5
25.8
26.8
25.7
27.0
25.2
26.3
25.5
25.8
2
27.8
27.7
27.7
26.9
26.7
26.5
26.5
26.3
EU)
167
162
157
152
147
142
137
132
32
23.3
21.6
20.5
19.4
18.6
18.8
17.8
16.8
I
27
22
25.0
26.2
24.2
25.8
22.8
24.3
22.1
23.5
21.0
23.1
19.7
23.1
18.8
22.2
17.3
20.4
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1-
17
12
7
27.2
29.0
26.2
26.7
28.6
30.0
25.9
27.9
29.0
24.9
27.4
28.6
24.3
27.0
29.5
24.2
28.0
30.0
24.5
28.6
30.0
23.4
27.1
28.2
2
29.3
29.8
28.8
26.7
27.0
27.5
27.6
27.5
c
167
162
157
152
147
142
137
132
32
0.6
0.6
0.6
0.6
0.7
0.8
0.8
0.8
I
I-
27
0.6
0.5
0.5
0.7
0.7
0.8
0.8
0.8
fe
z
22
0.5
0.5
0. 4
0.6
0.6
0.6
0.8
0.9
UJ
17
0.6
0.6
0.5
0.5
0.5
0.6
0.8
0.8
3
1-
12
7
0.5
0.*
0.5
0.6
0.6
0.8
0.7
0.9
0.6
1.0
0.6
0.9
0.8
0.8
0.5
0.5
2
0.2
0.3
0-5
0.6
0.6
0.5
0.4
0.3
M
167
162
157
152
147
142
137
132
32
6.7
6.3
6.0
6.0
6.0
6.0
6.3
6.4
I
27
7.7
6.6
6.7
7.0
7.5
7.0
6.0
7.0
22
7.5
7.5
7.7
8.1
7.7
6.6
6.2
8.0
UJ
n
17
7.1
7.5
8.0
8.0
7.8
7.0
7.0
7.0
3
-I
12
7
7.8
B.e
9.2
9.5
9.0
8.0
8.2
6.4
7.4
4.7
7.1
4. 1
6.6
4.0
6.4
4.0
2
8.3
7.0
4.0
4.0
4.2
5.1
5.3
5.3
LONGITUDE WEST
Q.SI
167
162
157
152
147
142
137
132
32
451.
451.
451.
451.
399.
341.
341.
341.
^
27
22
447.
488.
494.
488.
494.
529.
395.
441.
395.
441.
338.
441.
338.
334.
338.
273.
UJ
B
1-
17
12
7
430.
460.
478.
430.
460.
399.
475.
416.
302.
475.
368.
247.
475.
416.
187.
430.
416.
247.
326.
315.
302.
326.
460.
441.
2
514.
487.
420.
380.
380.
420.
4 56.
487.
aiei
167
162
157
152
147
142
137
132
2
32
27
22
95.
87.
100.
105.
106.
99.
111.
114.
115.
116.
99.
104.
106.
101.
102.
95.
89.
97.
93.
90.
78.
93.
93.
79.
UJ
Q
3
1-
17
12
7
83.
93.
119.
79.
97.
99.
103.
95.
77.
103.
83.
65.
103.
99.
60.
103.
101.
65.
81.
84.
82.
90.
108.
121.
^
108.
106.
100.
110.
109.
115.
123.
121.
giEi
167
162
157
152
147
142
137
132
32
121.
126.
116.
120.
125.
107.
113.
117.
I
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a.
o
z
27
22
164.
201.
126.
181.
145.
246.
157.
290.
208.
208.
167.
110.
114.
92.
165.
243.
3
1-
17
12
7
170.
217.
570.
168.
378.
530.
27 5.
382.
317.
253.
261.
155.
210.
234.
127.
171.
195.
92.
162.
137.
84.
174.
153.
109.
2
389.
216.
112.
141.
139.
158.
173.
146.
QIC)
167
162
157
152
147
142
137
132
32
-19.
-8.
1.
3.
1.
8.
1.
-6.
I
1-
27
22
-28.
-9.
-8.
-15.
1.
-7.
6.
1.
3.
-7.
-3.
-14.
-3.
-10.
-6.
16.
UJ
o
3
1-
17
-23.
-36.
-7.
-13.
-16.
3.
6.
20.
12
7
-7.
35.
1.
38.
11.
20.
1.
13.
12.
23.
23.
12.
29.
20.
13.
27.
2
-4.
3.
4.
16.
17.
21.
26.
15.
giNi
167
162
157
152
147
142
137
132
32
255.
229.
224.
213.
168.
133.
135.
137.
I
1-
27
224.
272.
235.
134.
84.
86.
138.
38.
22
17
196.
201.
224.
220.
175.
10 5.
48.
133.
138.
178.
248.
154.
174.
77.
-67.
42.
12
7
157.
-247.
-16.
-268.
-73.
-112.
23.
3.
71.
-23.
98.
78.
65.
117.
186.
IBS.
2
21.
163.
204.
113.
116.
127.
134.
205.
106
AUGUST 1963
LONGITUDE WEST
T(HI
167
162
157
152
147
142
137
132
32
24.1
23,7
23.1
22.6
21.9
21.4
20.8
19.8
X
27
25.3
25.3
25.0
24.2
23.1
22.1
21.1
20.5
22
26.2
26.1
25. 7
24.6
23.7
23.3
22.6
21.3
n
17
25.2
26.6
26. 2
25.3
24.4
23.9
23.8
23.7
t-
12
7
2 7.3
27.8
27.2
27.7
26.8
27.7
26.3
27.4
25.7
27. 1
26.3
27. 2
26.6
27.4
25.7
27.2
2
26. t
28.3
27.5
27.5
27.5
27.5
27.5
27.5
TMI
167
162
157
152
147
142
137
132
32
23.6
23.2
23.0
22.4
21.8
21. 5
21.0
21.0
I
i
27
22
25.3
26.3
25.0
25.9
24.1
25.1
22.9
24.3
22.9
23.7
22.3
23.4
21.4
22.8
21.0
21.8
1-
17
26.8
26.6
26.2
25.0
24.7
24.5
24.0
23.6
12
7
27.9
27.2
27.5
26.7
27.1
26.2
26.2
26.1
26.0
27.0
26.8
27.0
26.9
27.0
25.8
27.0
2
27.7
27.5
27.5
27.0
27.0
27.0
27.0
27.0
EUl
167
162
157
152
147
142
137
132
32
23.9
24.0
23.8
21.9
20.7
20.2
19.3
18.7
i
27
25.3
25.1
23.4
21.7
20.8
19.8
18.9
18.0
22
26.7
26.1
24.9
23.5
23.0
22.2
20.7
20.1
17
29.1
28.1
26.3
25.4
25.0
25.1
25.0
24.0
12
7
2 9.3
29.5
2 8. 7
28.9
28.5
29.0
29.1
28.9
29.0
30.0
29.0
30. 5
30.1
29.8
29.0
30.0
2
28.7
28.5
29.1
29.5
29.7
28.9
28.5
28.3
C
167
162
157
152
147
142
137
132
32
0.6
0.7
0.7
0.7
0.7
0.7
0.6
0.6
I
g
27
22
0.4
0.6
0.5
0.5
0.5
3.5
0.6
0.5
0.6
0.6
0.6
0. 6
0.7
0. 7
0.7
0.9
UJ
Q
17
0.6
0.5
0.6
0.5
0.6
0.7
0.8
0.8
12
7
0.5
0.7
e.6
0.8
0.7
0.7
0.6
0.8
0.6
0. e
0.6
0.8
0.7
0.7
0.7
0.7
2
0.5
0.4
0.5
0.9
0.9
0.9
0.8
0.8
M
167
162
157
152
147
142
137
132
32
5.8
7.2
7.3
5.8
5.3
4.8
5.0
5.3
I
5.2
5.7
6.0
6.6
7.0
7.2
7.2
7.3
6.4
7.3
6.0
7.5
6.2
7.9
6.0
5.9
6.3
6.8
7.2
7.6
8.0
8.0
7.3
6.8
5.8
5.5
6.5
5.8
7. 1
5.1
7.9
6.0
8.0
5.3
7.0
3.4
6.1
5.8
6.2
5.8
2
*. 5
5.1
4.5
3.7
3.8
6.0
7.5
7.5
LONGITUDE WEST
SIS)
167
162
157
152
147
142
137
132
32
419.
370.
370.
370.
370.
370.
419.
419.
X
27
510.
425.
470.
42 5.
425.
425.
3 76.
376.
^
22
42 9.
474.
474.
474.
429.
429.
379.
265.
'H
17
427.
472.
427.
472.
42 7.
377.
323.
323.
12
466.
421.
372.
421.
421.
421.
372.
372.
7
354.
312.
364.
312.
312.
312.
364.
364.
2
441.
479.
441.
247.
247.
247.
302.
302.
giBi
157
162
157
152
147
142
137
132
32
109.
98.
9 3.
99.
101.
100.
112.
1D2.
X
27
114.
103.
125.
125.
115.
112.
102.
102.
o
z
22
94.
108.
117.
117.
105.
105.
99.
68.
17
80.
99.
97.
in.
95.
81.
75.
81.
t-
12
88.
86.
77.
89.
83.
81.
72.
77.
-I
7
87.
83.
99.
86.
68.
58.
83.
79.
2
108.
116.
96.
54.
63.
55.
78.
78.
Q(E)
167
162
157
152
147
142
137
132
32
123.
161.
139.
HI.
99.
83.
87.
77.
X
z
27
121.
153.
242.
269.
181.
147.
139.
132.
22
144.
196.
255.
242.
203.
225.
2 85.
108.
UJ
Q
17
108.
178.
240.
250.
239.
192.
138.
140.
3
12
139.
179.
198.
205.
152.
144.
97.
83.
Ht
-I
7
147.
167.
178.
161.
101.
57.
133.
119.
2
147.
171.
110.
83.
83.
166.
2 88.
296.
QIC)
157
162
157
152
147
142
137
132
32
12.
15.
3.
5.
3.
-2.
-4.
-26.
X
27
1.
8,
25.
38.
6.
-5.
-8.
-12.
22
-3.
6.
IB.
9.
1.
-3.
-7.
-12.
S
17
-15.
1.
1.
10.
-10.
-20.
-5.
3.
H
12
-14.
-8.
-9.
4.
-10.
-14.
-8.
-3.
!5
-I
7
14.
23.
37.
31.
3.
3.
10.
5.
2
13.
17.
1.
8.
8.
12.
15.
15.
giNi
167
162
157
152
147
142
137
132
32
175.
98.
136.
156.
158.
191.
225.
266.
X
27
275.
162.
77.
-9.
124.
171.
143.
155.
IE
O
z
22
194.
165.
8 5.
106.
120.
101.
3.
102.
3
17
255.
195.
90.
102.
103.
125.
117.
99.
H
''
253.
165.
106.
125.
186.
211.
211.
215.
§
7
118.
39.
50.
33.
140.
184.
139.
161.
2
174.
175.
235.
93.
93.
4.
-80.
-88.
107
SEPTEMBER 1963
LONGITUDE WEST
TU)
167
162
157
152
147
142
137
132
J2
2*. 3
24.2
23.8
23.4
22.9
22.4
22.0
21.4
Z
1-
p:
27
25.7
25.3
25.2
24.5
23.9
23.1
22.5
22.2
z
22
26.3
25.7
25.7
25.3
24.7
24.1
23.0
22.8
1*{
17
26.7
26.3
26.4
26.3
25.7
25.0
24.7
24.7
3
1-
12
27.9
27.1
27.3
27.0
27.1
27.0
26.6
26.5
K
-I
7
29.5
29.1
28.2
27.5
27.5
27.4
27.4
27.3
2
28.5
28.2
27.7
27.4
27.2
27.0
27.1
27.2
T(At
167
162
157
152
147
142
137
132
32
24.5
24.0
23.5
23.1
22.5
22.0
21.6
21.2
I
27
25.9
25.2
24.7
24.3
23.8
22.9
22.4
22.3
^
22
26.3
26.0
25.3
24.9
24.5
24.0
23.2
23.4
iH
17
26.6
26.4
26.2
25.7
25.0
24.8
24.7
24.3
3
1-
12
26.5
26.3
26.3
26.5
27.0
26.7
26.7
26.8
Ht
<
7
26.9
27.1
26.8
26.8
27.0
27.0
26.0
26.0
2
27.4
27.8
28. 0
27.0
27.0
26.6
26.0
26.0
E(AI
167
162
157
152
147
142
137
132
32
25.2
24.2
22.6
22.2
21.3
20.4
19.7
19.6
I
27
25.9
25.7
23.9
24.5
22.8
22.0
21.6
21.0
22
27.3
26.4
25.3
24.5
24.4
24.3
23.5
23.2
1-
17
28.1
27.2
26.6
26.2
26.4
26.3
25.1
24.3
12
29.1
27.9
28.1
29.1
29.4
28.6
28.0
26.6
hr
_l
7
29.4
29.3
29.0
29.2
29.6
29.7
28.8
28.7
2
28.6
28.4
28.3
28.6
28.1
27.3
26.8
26.8
C
167
162
157
152
147
142
137
132
32
0.5
0.5
0.6
0.5
0.5
0.6
0.5
0.5
I
1—
27
0.5
0.4
0.5
0.5
0.5
0.5
0.5
0.5
a:
y
22
0.4
0.5
0.5
0.5
0.5
0.5
0.4
0.6
1-
17
0.5
0.5
0.6
0.6
0.5
0.4
0.4
0.6
12
0.6
0.6
0.6
0.5
0.4
0.3
0.4
0.5
1-
_l
7
0.8
0.8
0.7
0.5
0.5
0.7
0.8
0.9
2
0.5
0.5
0.5
0.5
0.5
0.6
0.6
0.8
H
167
162
157
152
147
142
137
132
32
5.5
5.7
5.7
5.9
6.2
6.2
6.0
5.6
I
27
5.8
6.5
6.0
4.9
5.2
5.5
5.6
5.2
a:
o
z
22
6.3
6.7
7.2
6.3
5.4
5.9
7.8
7.4
s
17
6.8
7. 2
6.7
6.3
5.8
4.9
5.3
5.7
12
6.8
6.7
6.0
4.8
4.7
3.8
4.0
5.3
1-
_l
7
4.7
4.7
4.3
3.6
3.7
5.3
5.8
5.6
2
4.5
4.3
4.0
4.5
4.5
4.9
10.3
10.2
32
27
22
17
12
7
2
a(B)
32
27
22
17
12
7
2
QIEI
32
27
22
17
12
7
2
0«C)
32
27
22
17
12
7
2
32
27
22
17
12
7
2
LONGITUDE WEST
157
152
147 142
397.
418.
473.
448.
413.
314.
458.
397.
453.
436.
448.
413.
314.
458.
359.
418.
436.
405.
413.
367.
458.
397.
418.
436.
405.
456.
459.
458.
397.
418.
436.
448.
495.
459.
458.
359.
418.
436.
486.
529.
367.
414.
397.
418.
473.
486.
495.
314.
414.
397.
418.
394.
405.
456.
257.
314.
152
104.
103.
108.
100.
107.
104.
113.
112.
114.
100.
100.
102.
96.
105.
110.
119.
113.
98.
104.
99.
96.
120.
112.
115.
105.
102.
104.
103.
124.
116.
112.
112.
102.
101.
102.
118.
119.
111.
112.
112.
8 3.
99.
129.
119.
116.
114.
104.
88.
110.
126.
lie.
96.
107.
100.
75.
91.
137
132
95.
144.
159.
184.
229.
185.
152.
117.
159.
171.
216.
208.
171.
138.
137.
176.
241.
204.
175.
129.
113.
137.
100.
181.
187.
101.
84.
115.
150.
120.
123.
133.
97.
82.
116.
152.
118.
117.
84.
84.
119.
136.
146.
108.
178.
106.
86.
155.
710.
114.
100.
148.
134.
144.
145.
718.
152
147
142
132
-5.
-5.
1.
3.
38.
49.
20.
5.
3.
-8.
-3.
22.
38.
7.
7.
12.
12.
6.
24.
2 4.
-5.
10.
15.
10.
10.
10.
3.
5.
17.
2.
10.
5.
3.
4.
5.
9.
8.
10.
3.
-7.
1.
-2.
33.
45.
5.
-3.
-18.
10.
-7.
29.
49.
157
132
204.
176.
206.
161.
40.
-24.
173.
163.
178.
174.
135.
82.
10.
209.
106.
HI.
71.
97.
110.
116.
255.
133.
202.
130.
99.
244.
260.
233.
113.
179.
196.
187.
295.
269.
236.
80.
176.
206.
286.
329.
157.
172.
113.
188.
186.
266.
308.
39.
■451.
153.
202.
169.
155.
220.
108
OCTOBER 1963
LONGITUDE WEST
TUt
167
162
157
152
147
142
137
132
32
24.0
23.5
22.7
22.1
21.6
21.0
20.6
20.2
I
27
25.7
25.3
24.5
23.9
23.3
22.7
22.2
21.7
i
22
26.2
25.7
25.4
24.8
24.4
24.0
23.3
22.7
!H
17
26.7
26.*
26. 3
25.7
25.7
25.5
25.0
24.7 j
3
l-
12
27.6
27.2
26.8
26.9
27.2
27.3
27.0
26.1
_1
7
29.0
28.6
28.0
27.4
27.5
27.5
27.4
27.3
2
28.7
27.7
27.1
27.2
27.3
27.3
27.4
27.4
TIAI
167
162
157
152
147
142
137
132
32
23.2
22.6
21.9
20.9
20.7
20.0
19.7
19.5
I
o
27
25.3
25.0
24.3
23.5
22.9
22.0
21.5
21.0
22
26.1
25.7
25.3
24.5
24.0
23.7
23.3
23.0
IH
17
26.8
26.9
26.1
25.6
25.3
25.2
24.9
24.5
3
(-
12
27.6
26.8
26.5
25.3
26.0
26.0
26.0
25.0
5
7
27.9
27.3
27.3
27.2
27.0
27.0
27.0
27.0
2
28.0
28.0
28.0
28.1
27.2
27.0
27.0
27.0
E(AI
167
162
157
152
147
142
137
132
32
24.0
22.2
20. 1
18.9
18.2
17.5
17.2
17.0
f
27
25.3
24.6
23.6
22.1
20.6
19.4
19.0
18.9
1
22
26.2
25.5
24.7
23.5
22.9
22.2
21.5
21.0
UJ
O
17
28.1
28.0
25.5
25.3
25.9
25. 1
24.0
23.2
3
1-
12
29.1
29.6
28.9
28.8
29.1
29.2
28.6
26.5
_1
7
32.0
30.5
29.1
28.6
28.3
28.3
28.4
29.0
2
31.0
29.4
28.3
27.3
26.8
26.7
26.8
27.0
c
157
162
157
152
147
142
137
132
32
0.7
0.6
0.6
0.6
0.5
0.6
0.6
0.6
f
27
0.5
0.5
0.5
0.5
0.5
0.5
0.5
0.6
22
0.5
0.5
0.5
0.5
0.5
0.5
0.6
0.7
s
17
0.6
0.6
0.5
0.5
0.6
0.5
0.6
0.7
ili
12
0.8
0.8
0.7
0.7
0.6
0.6
0.6
0.5
^
7
1.0
0.8
0.7
0.6
0.6
0.6
0.8
0.5
2
0.7
0.7
0.6
0.4
0.4
0.5
0.7
0.8
H
167
162
157
152
147
142
137
132
32
7.3
7.2
6.5
6.6
6.7
6.5
6.5
6.0
X
27
6.1
5.6
5.8
6.3
6.2
5.4
5.2
5.4
22
7.2
6.6
7.0
6.8
6.6
6.1
4.9
5.8
g
17
7.2
7.4
7.9
7.7
7.0
6.8
7.4
7.5
H
12
6.5
7.1
7.2
7.6
6.9
7.2
7.3
6.2
5
7
5.7
5.8
4.7
7.2
8.4
9.3
9.6
8.0
2
5.9
5.1
4.8
7.2
9.2
10.6
11.5
11.4
LONGITUDE WEST
QISI
157
162
157 152 147 142
137
132
32
252.
285.
285. 285. 285. 2BS.
285.
285.
X
g
Z
27
22
346.
375.
346.
375.
346. 346. 345. 345.
375. 375. 375. 375.
346.
340.
313.
300.
17
12
7
35 3.
290.
187.
363.
290.
302.
401. 401. 363. 401.
339. 339. 383. 383.
352. 399. 399. 399.
363.
383.
302.
321.
424.
440.
2
363.
353.
410. 492. 492. 454.
363.
311.
a(Bi
167
162
157 152 147 142
137
132
32
102.
119.
124. 132. 131. 134.
133.
131.
I
27
22
113.
106.
114.
107.
115. 123. 128. 135.
111. 117. 120. 121.
136.
110.
126.
97.
UJ
o
3
1-
17
12
7
90.
70.
55.
85.
73.
83.
107. 109. 102. 112.
83. 88. 103. 104.
89. 93. 98. 98.
105.
102.
77.
98.
105.
100.
2
84.
75.
80. 98. 112. 109.
92.
SO.
OIEI
167
152
157 152 147 142
137
132
32
186.
211.
187. 199. 203. 185.
177.
146.
I
I-
Z
27
22
170.
243.
148.
191.
145. 177. 184. 154.
225. 212. 196. 170.
138.
116.
132.
134.
UJ
a
3
H
-I
17
12
7
213.
191.
157.
212.
189.
175.
324. 298. 205. 204.
192. 239. 191. 217.
134. 245. 435. 556.
260.
225.
564.
281.
164.
317.
2
173.
131.
118. 275. 622. 784.
878.
849.
QIC)
167
162
157 152 147 142
137
132
32
24.
26.
21. 32. 24. 26.
24.
17.
I
1-
i
27
22
10.
3.
7.
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3. 9. 11. 8.
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-7.
3
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17
12
7
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1.
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12.
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7. 4. 12. 9.
9. 19. 33. 38.
14. 5. 17. 19.
3.
29.
16.
6.
3.
10.
2
17.
-7.
-18. -26. 4. 13.
19.
19.
aiNi
167
162
157 152 147 142
137
132
32
-50.
-71.
-48. -79. -74. -61.
-50.
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I
i
27
22
53.
23.
77.
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37. 38. 49. 77.
57.
114.
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1-
17
12
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29.
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152.
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7
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14.
116. 56. -153. -275.
-355.
14.
2
89.
164.
230. 146. -247. -452.
-626.
-638.
109
NOVEMBER 1963
LONGITUDE WEST
TtHI
167
162
157
152
147
142
137
132
32
20.9
20.9
20.5
19.9
19.5
18.9
18.8
18.8
f
27
23.9
23.7
23.3
22.7
22.1
21.8
21.6
21.2
O
z
22
25.3
25.1
24.9
24.4
23.9
23.6
23.3
22.7
lU
n
17
26.3
26.3
26.2
26.0
25.9
25.2
24.8
24.5
3
1-
12
26.8
26.8
26.8
26.9
26.8
26.3
26.3
27.1
7
28.2
28.3
27.9
28.3
28.6
27.5
27.1
27.4
2
28.1
27.5
27.5
28.4
27.7
26.9
26.8
26.7
TIAI
167
162
157
152
147
142
137
132
32
20.0
20.0
19.2
19.2
19.0
17.8
18.0
18.0
I
27
22.7
22.2
22.0
21.7
21.6
21.3
21.0
20.1
22
25.0
24.7
24.3
23.8
23.3
23.0
22.7
22.2
LU
n
17
26.0
26.2
25.6
25.3
24.7
24.4
24.2
24.1
3
1-
12
27.0
26.5
26.4
27.0
26.9
26.7
26.8
26.3
5
_i
7
27.8
27.0
27.0
27.0
27.0
27.0
26.3
26.0
2
28.0
27.7
27.8
27.7
27.4
26.8
26.0
26.0
E(«l
167
162
157
152
147
142
137
132
18.6
17.7
17.7
17.8
17.3
16.0
16.3
16.1
i
21.9
20.3
20.5
21.0
19.5
19.1
18.8
18.2
25.2
23.8
23.2
22.8
22.6
22.8
22.3
22.2
UJ
26.3
26.1
25.3
25.4
25.3
25.1
24.9
23.9
3
1-
27.2
27.6
28.3
29.2
29.1
29.2
28.4
27.4
5
28.9
29.2
2 8.6
29.0
30.1
30.1
30.0
29.0
28.3
28.3
28.1
28.8
28.8
28.3
27.7
27.7
c
167
162
157
152
147
142
137
132
32
0.7
0.7
0.7
0.7
0.7
0.7
0.7
0.7
f
27
0.7
0.6
0.6
0.7
0.6
0.7
0.7
0.7
22
0.6
0.6
0.4
0.5
0.5
0.6
0.6
0.6
UJ
B
17
0.5
0.5
0.5
0.4
0.5
0.5
0.6
0.7
12
0.5
C.7
0.6
0.7
0.7
0.6
0.6
0.7
7
0.6
0.8
0.8
0.8
0.8
0.9
1.0
l.O
2
0.4
0.5
0.6
0.7
0.7
0.6
0.6
0.6
M
167
162
157
152
147
142
137
132
32
9.3
7.7
7.7
7.4
7.6
7.8
7.2
6.8
I
1-
27
8.3
7.1
6.7
6.7
6.7
6.2
5.7
6.4
22
6.8
6.6
7.0
6.7
6.5
6.4
6.6
7.2
g
17
6.6
7.3
8.3
8.1
6.3
6.5
6.7
7.3
(-
12
7.5
7.3
7.2
7.2
6.2
4.7
5.7
6.6
^
7
6.1
7.5
4.1
5. 1
4.9
4. 7
6.4
5.9
2
3.3
3.8
3.5
4.2
4.5
4.8
5.9
6.5
LONGITUDE WEST
Q<S)
167
162
157
152 147 142
137
132
32
189.
189.
189.
189. 189. 189.
189.
189.
I
Z
27
22
219.
281.
248.
281.
248.
337.
219. 248. 219.
311. 311. 281.
219.
281.
219.
281.
UJ
a
17
345.
345.
345.
375. 345. 345.
313.
276.
3
-J
12
7
379.
369.
303.
279.
259.
279.
30 3. 30 3. 343.
279. 279. 228.
343.
173.
303.
173.
2
471.
434.
39 3.
347. 347. 393.
393.
393.
0(B)
167
162
157
152 147 142
137
132
32
116.
120.
124.
115. 114. 125.
120.
121.
I
t-
g
Z
27
22
113.
103.
133.
109.
129.
130.
112. 122. 111.
123. 123. 113.
113.
114.
121.
113.
UJ
o
1-
-J
17
12
7
109.
100.
95.
107.
88.
87.
116.
7 6.
83.
123. 123. 118.
78. 78. 82.
87. 88. 62.
107.
84.
54.
98.
95.
63.
2
107.
97.
88.
91. 85. 92.
103.
101.
OIE)
167
162
157
152 147 142
137
132
32
408.
275.
250.
184. 198. 238.
170.
153.
I
27
22
392.
190.
277.
206.
216.
243.
173. 188. 161.
205. 174. 151.
141.
159.
170.
166.
1-
17
12
7
201.
283.
207.
264.
246.
328.
44 0.
213.
118.
380. 190. 170.
189. 135. 73.
162. 146. 99.
166.
111.
135.
221.
215.
155.
2
118.
101.
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135. 122. 111.
156.
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aic)
167
162
157
152 147 142
137
132
32
34.
28.
40.
21. 16. 34.
23.
22.
i
27
22
40.
9.
43.
11.
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17.
27. 14. 13.
16. 16. 16.
14.
16.
28.
15.
UJ
a
1-
17
12
7
8.
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10.
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9.
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15.
23. 30. 21.
-3. -3. -8.
27. 32. 10.
16.
-12.
21.
12.
21.
33.
2
2.
-4.
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12. 6. 2.
19.
19.
a(Ni
167
162
157
152 147 142
137
132
32
-369.
-234.
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I
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27
22
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1-
12
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40. 94. 196.
4. 14. 57.
160.
-37.
-29.
-78.
2
243.
240.
214.
110. 135. 187.
115.
95.
10
DECEMBER 1963
LONGITUDE WEST
T(M1
167
162
157
152
147
142
137
132
32
17.9
18.1
18.0
18.0
18.5
18.5
18.6
18.0
X
27
21.7
21.8
22.0
21.9
21.5
21.1
20.7
20.0
22
24.2
24.3
24.3
24.0
23.3
22.8
22.1
21.6
UJ
17
25.3
25.2
25.3
25. 1
24.2
23.9
23.6
23.1
1
_J
12
7
25.7
27.1
25.9
27.2
26.2
27.0
26.1
25.8
25.9
2T.0
25.6
28.0
25.4
26.8
25.3
25.7
2
27.3
27.2
27.1
27.3
27.8
28.1
27.6
27.6
1(41
167
162
157
152
147
142
137
132
32
15.7
16.0
17.1
18.0
18.9
18.6
18.1
17.5
I
g
27
22
20.1
22.7
20.3
23.0
20.7
23.3
21.1
23.2
21.3
22.7
20.7
22.3
19.9
21.7
19.1
20.7
g
17
2*. 5
24.8
25.2
24.5
24.2
23.7
23.4
23.0
3
-I
12
7
26.0
27.7
26.3
28.0
25.7
27.0
2 5.4
25.9
25.3
26.0
25.5
26.0
25.8
26.0
25.5
26.0
2
28. C
28.0
27.3
26.7
25.4
26.1
26.0
26.0
E(A)
167
162
157
152
147
1*2
137
132
32
13.6
13.5
16.0
17.3
17.7
17.7
16.8
15.7
I
27
22
17.8
19.8
IB.O
21.0
19.7
22.7
20.2
22.5
20. C
21. 1
18.5
19. 3
17.5
18. a
17.0
20.5
H^
17
23.5
24.4
25.4
25.2
24.4
23.8
23.0
21.5
3
I-
12
7
26.2
28.6
28.3
3C.1
28.2
28.7
26.7
27.5
26.5
27.7
27.0
29.4
2B.3
30.0
28.2
28.4
2
28.5
28.6
28.8
28.7
29.1
29.3
28.3
27.5
C
167
162
157
152
147
14 2
137
132
32
0.5
0.6
0.7
0.7
0.7
0.7
0.7
0.7
I
H
g
Z
27
22
0.7
0.5
0.6
0.4
0.6
0.4
C.7
0.5
0.7
0. 5
0.5
0.5
0.7
0.5
0.7
C.6
iH
17
0.5
0.5
0.5
0.4
0.4
0.4
0.5
0.6
3
12
7
0.5
0.6
0.5
0.8
0. 7
0.8
0.8
0.8
0.8
0.8
0.6
0.9
0.5
0.8
0.7
0.8
2
0.6
0.6
0.6
0.7
0.7
0.7
0.7
0.7
H
167
162
157
152
147
142
137
132
32
10.5
10.3
10.1
9.5
9.1
7.5
6.5
6.2
I
i
27
22
8.3
5.8
7.7
5.3
8. 1
5.2
8.0
5.1
7.7
6.6
6.7
6.4
5.9
6.7
5.7
6.4
^
17
6.3
5.8
5.4
4.9
5.9
6.3
7.2
7.2
3
_l
12
7
6.7
7.0
7.8
8.1
7.4
8.2
7.5
8.5
8.3
9.2
7.7
9.5
7.0
9.2
7.5
7.9
2
5.3
5.1
5.4
7.9
8.7
9.1
6.7
8.5
LONGITUDE WEST
0(S)
167
152
157
152 147 142
137
132
32
181.
181.
16C.
150. 160. 150.
160.
160.
X
27
191.
216.
216.
191. 191. 216.
191.
191.
z
22
277.
301.
301.
277. 277. 277.
277.
251.
UJ
17
316.
316.
316.
343. 343. 343.
316.
286.
3
12
354.
354.
263.
242. 242. 320.
3 54.
283.
1-
_1
7
351.
2 55.
255.
256. 256. 217.
255.
255.
2
381.
3ai.
381.
336. 336. 336.
3 36.
336.
giBi
167
152
157
152 147 142
137
132
32
158.
157.
121.
105. 101. 104.
115.
118.
X
o
z
27
129.
139.
130.
111. 106. 123.
119.
121.
22
145.
145.
135.
125. 128. 134.
133.
122.
UJ
Q
1-
17
124.
115.
10 8.
120. 116. 121.
115.
HI.
12
101.
92.
87.
84. 62. 95.
91.
78.
^
7
82.
57.
70.
64. 65. 83.
77.
80.
2
82.
80.
87.
88. 98. 105.
102.
105.
e<E)
167
162
157
152 147 142
137
X32
32
568.
583.
350.
221. 221. 123.
114.
112.
X
27
418.
320.
313.
268. 223. 173.
147.
128.
q;
z
22
218.
172.
135.
162. 193. 207.
208.
125.
s
17
205.
156.
125.
107. 119. 134.
169.
212.
12
177.
195.
190.
248. 335. 218.
111.
131.
7
207.
255.
328.
408. 514. 575.
322.
274.
2
139.
126.
128.
317. 471. 553.
495.
511.
QIC)
167
152
157
152 147 142
137
132
32
92.
86.
36.
1. -15. -3.
13.
13.
I
27
53.
46.
42.
26. 10. 11.
19.
21.
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22
35.
28.
21.
20. 15. 13.
11.
23.
3
17
20.
10.
3.
10. 1. 5.
6.
3.
1-
12
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-13.
15.
21. 20. 4.
-12.
-6.
7
-17.
-25.
1.
31. 37. 76.
30.
22.
2
-15.
-17.
-5.
19. 49. 73.
56.
54.
QCNI
167
162
157
152 147 142
137
132
32
-538.
-547.
-348.
-156. -148. -64.
-82.
-83.
I
27
-410.
-290.
-27 1.
-215. -148. -92.
-95.
-80.
22
-122.
-46.
10.
-31. -50. -77.
-75.
-20.
n
17
-35.
35.
81.
106. 108. 63.
5.
-41.
3
1-
12
85.
79.
-10.
-111. -197. 4.
154.
81.
_l
7
79.
-30.
-134.
-258. -371. -517.
-163.
-110.
2
176.
192.
171.
-86. -262. -394.
-317.
-335.
in
JANUARY 1964
LONGITUDE WEST
TIUI
167
162
157
152
147
142
137
132
32
15.9
15.9
16.3
17.0
17.4
17.0
17.0
16.7
I
Z
27
20.1
20.3
20.5
20.6
20.7
20.0
19.6
18.8
22
23.3
23.2
23.2
22.8
22.2
21.3
20.7
20.5
a
IT
24.7
24.6
24.4
24,0
23.2
22.6
22.2
22.0
_)
t-
12
7
25.6
26.7
25.9
27.1
25.7
26.7
25.4
26.3
25.1
26.3
24.2
26.3
24.2
26. 3
24.4
26.2
2
27.2
27.3
27.1
26.9
26.5
26.8
27.2
27.5
TIA)
167
162
157
152
147
142
137
132
32
16.8
16.7
17.0
16.8
16.6
16.7
16.3
16.0
I
27
22
20.1
23.0
20.2
23.0
20.6
22.9
20.4
22.5
20.0
22.1
19.3
21.4
18.8
20.7
18.0
20.3
n
17
24.5
24.5
24.3
23.7
22.2
22.8
22.3
21.9
13
1-
12
7
25.6
26.6
25.7
26.3
25.3
25.8
25.3
25.5
24.3
25.2
24.2
25.6
24.7
25.9
25.0
26.0
2
27.0
27.0
27.0
26.0
26.0
26.0
26.0
25.5
EIAI
167
162
157
152
147
142
137
132
32
15.8
15.9
16.1
16.2
15.9
15.3
14.6
14.1
I
1-
g
7
27
22
18.2
22.0
19.3
22.1
19.9
21.9
19.6
21.1
18.4
20.1
17. 1
18.7
15.7
17.8
14.9
17.7
n
17
24.5
24.4
23.5
22.0
21.7
21.1
20.7
20.6
3
_l
12
7
25.7
28.2
26.3
28.9
26.2
27.7
25.2
27.3
25.7
28.1
25.0
28.1
25.2
28.4
26.0
28.6
2
28.8
30.4
29.1
29.0
28.2
27.5
27.5
28.3
C
167
162
157
152
147
142
137
132
32
0.7
0.6
0.7
0.7
0.7
0.8
0.8
0.7
I
27
22
0.6
0.5
0.5
0.4
0.5
0.5
0.6
0.6
0.6
0.6
0.7
0.7
0.7
0.8
0.7
0.8
UJ
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17
12
7
0.5
0.4
0.6
0.5
0.5
0.8
0.4
0.4
0.8
0.5
0.5
0.8
0.6
0.8
0.8
0.7
0.7
0.7
0.7
0.8
0.6
0.8
0.7
0.7
2
0.7
0.7
0.7
0.7
0.6
0.4
0.4
0.6
W
167
162
157
152
147
142
137
132
32
8.6
e.o
7.3
7.4
7.8
8.2
7.0
6.6
I
27
7.6
6.8
6.9
7.7
7.7
7.0
7.4
6.7
O
22
7.9
7.9
8.3
8.3
8.8
9.5
8.7
7.8
UJ
§
1-
17
12
8.5
9.2
8.2
8.8
7.3
8.9
7.6
9.0
8.4
9.2
8.9
9.5
9.5
9. 1
8.8
8.5
^,
7
8.6
10.3
10.2
9.0
8.9
7.8
8.0
8.9
2
7.3
6.5
5.1
6. 1
7. 1
7.5
6.5
5.5
LONGITUDE WEST
acsi
167
162
157 152 147 142
137
132
32
174.
197.
174. 174. 174. 149.
149.
174.
I
z
27
22
231.
294.
256.
319.
255. 231. 231. 205.
294. 256. 256. 235.
205.
201.
205.
201.
UJ
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17
12
7
330.
397.
360.
330.
356.
273.
358. 330. 299. 264.
397. 365. 251. 293.
273. 273. 273. 319.
2 64.
251.
360.
226.
293.
319.
2
343.
343.
343. 343. 388. 465.
465.
388.
gc8i
167
162
157 152 147 142
137
132
32
98.
111.
100. 111. 117. 101.
108.
124.
z
27
22
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127.
120. 116. 126. 118.
121. 114. 115. 105.
124.
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125.
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12
7
112.
113.
92.
111.
107.
80.
121. 122. 121. 97.
115. 109. 86. 89.
84. 83. 85. 90.
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89.
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83.
2
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167
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157 152 147 142
137
132
32
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408. 447. 393. 346.
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132
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5.
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2
21.
115.
147. 92. 89. 52.
99.
69.
112
FEBRUARY 1964
LONGITUDE WEST
T(M»
167
162
157
152
147
142
137
132
32
16.4
17.0
17.0
16.8
17.0
16.7
16.3
15.8
I
27
20.3
20.4
20.5
20.5
20.0
19.2
18.6
17.9
1
22
22.8
22.9
22.5
22.3
22.0
20.8
20.1
19.6
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17
24.1
24.2
23.5
22.9
22.8
22.3
21.8
21.2
3
1-
-1
12
7
2<..9
26.3
24.8
25.1
24.3
25.4
23.8
25.3
24.1
25.4
24.3
25.5
24.2
25.5
24.0
25.4
2
27.2
26.7
26.5
26.5
26.5
26.5
26.5
26.5
T(AI
167
162
157
152
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142
137
132
32
16. S
16.9
17.0
16.8
16.7
15.8
15.3
15.0
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O
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27
22
20.8
22.8
20.7
22.7
20.4
22.3
20.0
22.0
19.3
21.2
18.5
20.5
17.8
19.8
15.7
18.8
UJ
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1-
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17
12
7
24.2
25.2
26.2
24.2
24.9
25.7
23.6
24.6
26.2
22.7
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25.7
22.1
24.3
25.5
21.9
24.0
25.0
21.7
23.8
24.4
21.4
23.3
25.0
2
28.0
26.8
26.7
26.3
26.0
25.3
25.0
26.0
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167
162
157
152
147
142
137
132
32
16.7
16.0
16.6
15.7
14.5
13.5
12.8
12.3
I
27
22
20.0
21.8
19.3
20.9
18.3
19.7
17.7
19.0
15.4
19.0
15.8
19.0
15.0
18.9
14.0
17.8
g
3
K
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17
12
7
23.4
26.0
29.1
22.8
26.1
28.8
21.8
25.0
26.9
21.3
23.9
27.2
20.8
24.1
25.1
20.7
22.9
25.3
20.4
24.2
26.2
20.0
23.7
25.9
2
29.6
28.5
27.9
28.3
27.5
27.0
27.0
27.8
C
167
162
157
152
147
142
137
132
32
0.7
0.8
0.6
0.6
0.6
0.8
0.8
0.8
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7
27
22
0.5
0.4
0.4
0.4
0.6
0.4
0.6
0.5
0.5
0.5
0.7
0.6
0. 7
0.8
0.9
0.8
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12
7
0.6
0.7
0.7
0.4
0.5
0.6
0.4
0.4
0.4
0.4
0.5
0.6
0.7
0.6
0.7
0.7
0.5
0.8
0. 7
0.7
0.9
0.9
0.5
0.8
2
0.7
0.6
0.5
0.5
0.5
0.5
0.7
0.8
w
167
162
157
152
147
142
137
132
32
7.9
6.9
6.5
6.8
6.9
7.5
7.1
7.5
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27
22
6.7
6.8
6.6
7.3
7.1
8.2
7.5
8.4
7.5
8.3
7.7
9.1
8.0
10.8
8.3
8.5
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12
7
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9.5
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7.8
8.7
7.5
7.7
8.2
7.7
8.2
7.1
2
7.4
6.2
5.0
6.0
6.2
7.6
8.0
4.6
LONGITUDE WEST
QIS)
157
152
157 152 147 142
137
132
32
228.
195.
258. 258. 258. 195.
195.
195.
X
1-
27
22
319.
381.
345.
381.
289. 289. 289. 255.
381. 351. 351. 318.
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178.
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12
7
345.
325.
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413.
408.
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413. 413. 305. 305.
443. 408. 369. 359.
468. 390. 345. 295.
305.
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213.
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2
361.
408.
451. 451. 451. 408.
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157
162
157 152 147 142
137
132
32
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119. 122. 130. 113.
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22
115.
125.
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131.
119. 126. 133. 121.
136. 132. 137. 119.
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7
103.
83.
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123.
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157 152 147 142
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175. 229. 251. 253.
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281. 382. 400. 303.
197. 232. 386. 419.
210.
228.
304.
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167
152
157 152 147 142
137
132
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157 152 147 142
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176.
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2
104.
179.
249. 214. 173. -18. -
-126.
121.
113
MARCH 1964
LONGITUDE WEST
T(W)
167
162
157
152
147
142
137
132
32
16.0
16. 3
16.8
16.9
16.8
16.7
16.1
15.0
I
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27
22
20.7
23.1
20.6
22.3
20.4
22.3
20.3
22.0
19.8
21.5
19.0
21.0
18.2
19.9
17.2
19.4
UJ
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17
23.6
23.5
23.4
22.8
22.5
22.3
22.0
21.7
12
2*. a
24.8
24.5
24.6
24.3
23.7
23.4
23.2
7
26. <.
26. 0
25.4
25.4
25.3
25.3
25.3
25.0
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26.8
26.4
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26.0
26.5
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167
162
157
152
147
142
137
132
32
16.2
16.4
16.8
17.0
15.7
15.7
15.4
14.4
I
27
22
20.0
23.1
20.1
22.7
20.3
22.3
19.5
21.7
19.3
21.3
18.4
20.5
17.7
19.7
16.8
19.5
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17
24.0
24.3
23.7
23.0
22.7
22.1
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2 0.9
12
25.2
25.0
24.7
25.1
25.0
24.7
24.2
23.0
7
27.0
26.3
26.2
25.8
26.0
26.0
25.7
25.2
2
27.0
26.8
26.6
26.0
25.8
25.7
25.5
25.0
EIAI
167
162
157
152
147
142
137
132
32
lA.l
14.8
15.9
15.7
15.0
14.0
13.3
12.8
I
27
16.7
19.0
19.5
17.8
17. C
15.4
14.3
13.7
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22
22.1
21.3
21.3
20.0
19.1
17.9
16.5
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23.8
23.3
23.3
23.1
22.0
21.9
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12
25.8
25.8
26.4
25.4
25.3
25.5
24.0
22.5
7
28.2
28.0
29.2
28.5
2 7.7
28. 1
26.0
26.5
2
29.8
30.0
29.5
29.6
28.7
28.3
27.7
27.5
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167
162
157
152
147
142
137
132
32
0.6
0.7
0.7
0.7
0.7
0.7
0.7
0.8
X
27
0.7
0.6
0.6
0.7
0.7
0.8
0.7
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22
0.6
0.5
0.5
0.7
0.7
0.7
0.6
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17
0.6
0.5
0.5
0.6
0.6
0.6
0.7
0.8
t-
12
0.4
0.5
0.6
0.6
0.7
0.7
0.7
0.6
7
0.6
0.5
0.7
0.9
0.8
0.9
0.7
0.6
2
0.5
0.5
0.6
0.7
0.7
0.6
0.6
0.5
H
167
162
157
152
147
142
137
132
32
7.1
7.3
7.5
7.7
7.5
7.1
7.3
7.5
I
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27
8.0
7.7
8.3
8.4
8.4
8.2
7.9
6.9
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7.3
7.2
8.2
8.5
9.3
9.3
9.0
5.5
a
17
6.7
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6.6
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9.4
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8.9
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12
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7.2
7.5
9.0
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7.8
7.6
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7
5.9
8.4
7.8
9.2
9.3
9. 5
8.6
7.7
2
6.3
6.0
5.0
6.0
6.7
7.1
9.0
9.5
LONGITUDE WEST
QISI
167
162
157
152 147 142
137
132
32
328.
290.
290.
290. 290. 290.
2 90.
248.
I
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27
22
311.
373.
352.
412.
352.
412.
311. 311. 256.
330. 330. 330.
311.
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311.
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17
390.
431.
431.
390. 390. 390.
345.
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12
7
485.
414.
447.
458.
40 5.
366.
405. 358. 358.
256. 313. 256.
358.
366.
405.
414.
2
465.
465.
421.
372. 372. 421.
421.
421.
Q(B)
157
162
157
152 147 142
137
132
32
125.
112.
109.
109. 114. 127.
126.
110.
I
H
27
22
113.
103.
121.
114.
114.
119.
117. 116. 107.
106. 107. 114.
123.
127.
123.
116.
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17
97.
103.
109.
101. 105. 110.
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102.
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1-
12
7
107.
83.
102.
95.
92.
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114
APRIL 1964
LONGITUDE WEST
TIHI
167
162
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152
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137
132
32
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LONGITUDE WEST
0(S)
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32
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115
MAY 1964
LONGITUDE WEST
T(MI
167
162
157
152
147
142
137
132
32
18.8
18,9
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LONGITUDE WEST
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157
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147
142
137
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147
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157
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132
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JUNE r964
LONGITUDE WEST
T«MI
167
162
157
152
147
142
137
132
J2
20.0
20.3
20.2
19.6
18.4
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27
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26.6
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26.3
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26.8
26.6
27.3
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T«A»
167
162
157
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147
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137
132
32
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167
162
157
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147
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137
132
32
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20.3
18.0
20.5
1-
17
12
7
27.8
28.6
27.9
26.6
27.7
29.2
25.6
26.8
28.5
25.1
25.9
28.3
23.4
27.1
27.7
22.4
25.7
27.7
22.2
26.9
28.0
22.0
25.8
27.3
2
27.4
27.8
27.4
28.5
28.2
26.7
26.3
25.2
C
167
162
157
152
147
142
137
132
32
0.6
0.6
0.7
0.7
0.7
0.8
0.8
0.9
X
27
22
0.6
0.5
0.5
0.5
0.6
0.5
0.5
0.6
0.7
0.6
0.8
0.6
0.8
0.7
0.7
0.8
UJ
n
17
0.6
0.5
0.5
0.5
0.4
0.5
0.7
0.7
3
I-
-1
12
7
0.5
0.6
0.6
0.8
0.6
0.9
0.5
0.9
0.6
0.8
0.7
0.8
0.7
0.6
0.7
0.8
2
0.3
0.6
0.5
0.5
0.7
0.5
0.5
0.4
M
167
162
157
152
147
142
137
132
32
6.5
6.3
6.0
5.5
6.2
6.5
6.5
6.3
X
27
22
6.6
6.7
6.6
7.2
6.6
7.3
6.5
7.3
6.9
7.3
6.6
6.5
6.2
7.3
5.6
6.3
17
6.8
7.7
8.2
6.5
7.2
6.8
7.4
6.8
12
7
6.8
6.5
9.2
6.8
8.3
6.9
8.3
6.7
8.2
6.0
7.2
4.9
7.2
4.0
6.8
5.2
2
5.6
5.3
4.7
7. I
6.0
6.7
7.2
6.7
LONGITUDE WEST
QISI
167
162
157 152
147 142
137
132
32
457.
457.
404. 404.
404. 346.
346.
283.
I
27
451.
499.
451. 499.
399. 341.
341.
399.
1
22
489.
489.
489. 443.
443. 443.
391.
335.
I-
17
12
7
430.
458.
396.
475.
415.
300.
475. 475.
415. 458.
245. 245.
516. 475.
415. 365.
300. 300.
3 80.
366.
396.
380.
366.
300.
2
482.
376.
416. 416.
333. 416.
416.
451.
Qial
167
162
157 152
147 142
137
132
32
92.
89.
78. 84.
96. 81.
67.
78.
I
i
27
22
91.
101.
100.
108.
92. 106.
113. 105.
94. 93.
105. 110.
94.
113.
99.
90.
17
12
7
75.
8B.
93.
99.
89.
72.
100. 106.
88. 96.
65. 63.
lis. 114.
94. 88.
74. 70.
96.
84.
89.
97.
84.
75.
2
110.
86.
95. 107.
90. 110.
108.
103.
QIE)
167
162
157 152
147 142
137
132
32
30.
35.
24. 41.
95. 64.
76.
79.
1
27
22
75.
152.
85.
203.
80. 113.
215. 210.
131. 139.
199. 144.
115.
188.
69.
103.
s
§
_l
17
12
7
75.
146.
212.
211.
386.
182.
257. 130.
284. 282.
185. 167.
182. 177.
247. 201.
155. 104.
210.
151.
77.
149.
150.
131.
2
151.
132.
113. 232.
144. 158.
213.
157.
QIC)
167
162
157 152
147 142
137
132
32
-29.
-33.
-31. -27.
-28. -24.
-16.
-5.
I
1-
g
Z
27
22
-16.
-6.
-19.
-19. -21.
3. 1.
-17. 3.
-9. -3.
3.
29.
-12.
8.
UJ
8
1-
17
12
7
-33.
-19.
1.
-10.
-8.
6.
-17. -3.
-17. -24.
14. 8.
-3. -6.
4. 1.
3. -4.
-3.
1.
-4.
1.
-9.
3.
2
-5.
-11.
-10. 20.
17. 16.
9.
-24.
0(N)
167
162
157 152
147 142
137
132
32
355.
367.
334. 307.
241. 224.
199.
132.
I
1-
27
301.
333.
299. 301.
191. 107.
130.
242.
O
22
242.
179.
159. 127.
148. 193.
61.
135.
UJ
o
3
1-
17
12
314.
244.
175.
-53.
125. 243.
60. 104.
220. 191.
70. 77.
79.
122.
134.
142.
i
7
92.
41.
-19. 7.
58. 131.
2 35.
92.
2
226.
170.
218. 56.
32. 122.
86.
216.
117
JULY 1964
LONGITUDE WEST
T(HI
147
162
157
152
147
142
137
132
32
23.9
23.6
23.2
22.3
21. 1
20.3
19.4
18.3
I
O
27
22
2».7
25.3
2<..3
25.2
24.1
24.7
22.8
24.1
22.0
23.4
21.3
22.6
20.5
21 .7
19.7
21.1
llJ
Q
17
25.6
26.0
25.3
25.0
24.7
24.6
24. 3
23.9
3
I-
12
7
25.9
26.7
25.9
27. 5
25.8
26.7
25.8
27.2
26.1
26.3
26.3
26.3
26.4
27.1
26.6
27.4
2
26.3
26.5
26.3
26.3
24.6
24.2
25.2
25.6
T<A)
167
162
157
152
147
142
137
132
32
24.6
24.0
23.2
22.3
21.0
20.3
19.6
18.7
I
O
7"
27
22
25.2
25.6
24.6
25.4
23.9
24.7
23.0
23.9
22.1
23.3
21.3
22.4
20.4
21.6
19.5
20.8
liJ
Q
17
26.3
26.1
25.4
24.8
24.7
24.5
24.3
23.9
_)
1-
_i
12
7
26.5
26. B
26.3
26.7
26.2
26.5
26 .1
26.3
25.7
26.1
25.7
25.3
26.0
26.5
25.9
26.5
2
26.8
26.6
26.4
26.2
25.6
25.2
25.0
25.0
EIAI
167
162
157
152
147
142
137
132
32
20.4
23.7
22.7
21.8
19.8
18.9
18.0
17.3
I
27
22
24.8
25.6
24.1
24.7
23.0
23.8
21.7
23.4
20.8
22.7
19.6
21.6
18.9
21. 1
17.9
20.5
IH
17
26.9
26.4
25.8
25.8
24.2
23.5
23.4
23.4
12
7
28.1
28.3
29.1
28.7
27.9
28.1
26.8
27.5
25.9
27.4
26.2
27.5
26.2
27.0
26.5
28.1
2
27.5
27.1
26.4
26.5
26.4
25.8
24.8
23.0
c
167
162
157
152
147
142
137
132
32
0.5
0.5
0.6
0.6
0.7
0.8
0.8
0.8
I
1-
27
22
0.5
0.5
0.5
0.5
0.5
0.5
0.6
0.6
0.7
0.7
0.7
0.7
0.6
0.9
0.9
0.9
^
17
0.5
0.5
0.5
0.5
0.5
0.6
0.7
0.9
_l
12
7
0.5
0.5
0.7
0.7
0.7
0.9
0.5
0.7
0.6
0.6
0.6
0.8
0.6
0.6
0.7
0.6
2
0.5
0.5
0.5
0.4
0.3
0.3
0.4
0.4
M
167
162
15 7
152
147
142
137
132
32
5.8
6.5
6.6
6.0
5.7
5.5
5.2
5.7
I
1
27
22
6.7
7.6
7.2
B.3
7.1
8.5
7.6
7.9
6.9
7.3
6.7
7.8
6.9
8.7
7.0
9.4
1-
17
12
6.6
5.8
7.5
9.2
8.0
8.3
7.1
6.7
7.0
5.7
5.7
5.2
6.3
4.0
7.3
5.1
-I
7
6.8
7.2
4.8
5.4
5.3
5.4
4.3
3.7
2
7.5
6.3
4.6
6.3
4.5
4.5
4.7
4.3
LONGITUDE WEST
a<si
167
162
157
152
147
142
137
132
32
499.
499.
451.
451.
399.
341.
341.
341.
I
27
494.
494.
49 4.
447.
395.
395.
338.
277.
(C
o
22
488.
488.
488.
441.
390.
390.
273.
273.
LlJ
n
17
475.
475.
475.
475.
475.
430.
380.
266.
?
12
460.
368.
368.
460.
416.
416.
416.
368.
H
-I
7
441.
353.
247.
353.
399.
302.
399.
399.
2
42 0.
420.
420.
456.
487.
487.
456.
456.
Q(BI
167
162
157
152
147
142
137
132
32
100.
106.
106.
108.
103.
91.
90.
89.
f
27
102.
107.
117.
106.
99.
103.
92.
80.
CE
Z
22
103.
107.
112.
1C7.
97.
100.
73.
76.
a
?
17
93.
103.
104.
108.
HI.
106.
94.
68.
12
90.
73.
77.
99.
103.
10 5.
102.
96.
1-
:i
7
125.
91.
62.
96.
96.
85.
103.
103.
2
94.
101.
103.
112.
102.
104.
119.
132.
QIE)
167
162
157
152
147
142
137
132
32
104.
131.
144.
108.
103.
92.
78.
72.
I
27
163.
194.
211.
222.
157.
150.
145.
146.
22
242.
368.
394.
278.
195.
233.
2 72.
297.
y
17
147.
252.
280.
172.
199.
148.
162.
201.
_)
1-
12
104.
259.
255.
165.
157.
140.
105.
142.
y-.
^
7
304.
248.
108.
158.
120.
121.
124.
9B.
2
233.
174.
117.
179.
63.
61.
112.
139.
OIC)
167
162
157
152
147
142
137
132
32
-17.
-11.
1.
1.
3.
1.
-5.
-10.
z
27
-14.
-9.
6.
-7.
-3.
1.
3.
6.
22
-10.
-7.
1.
7.
3.
7.
4.
12.
s
17
-19.
-3.
-4.
6.
1.
3.
1.
1.
1-
12
-14.
-15.
-14.
-8.
10.
13.
7.
15.
I-;
^
7
52.
23.
4.
20.
5.
22.
11.
14.
2
-15.
-3.
-2.
3.
-18.
-18.
4.
11.
aiNi
167
162
157
152
147
142
137
132
32
311.
273.
202.
236.
191.
159-
178.
191.
I
27
243.
203.
161.
126.
144.
142.
98.
45.
22
153.
20.
-20.
50.
95.
51.
-77.
-113.
UJ
o
17
255.
124.
95.
190.
165.
174.
124.
-4.
1-
12
280.
51.
50.
205.
147.
159.
202.
116.
1
7
-40.
-11.
73.
80.
179.
74.
162.
184.
2
109.
149.
202.
162.
341.
341.
222.
175.
118
AUGUST 1964
LONGITUDE WEST
TIM)
167
162
157
152
147
142
137
132
32
24.8
24.6
24.2
23.5
22.7
21.8
21.2
20.3
I
27
22
25.2
25.5
24.7
25.4
24.5
25.3
24.3
24.7
23.5
24.0
22.8
23.4
21.8
22.5
21.2
21.7
^
17
26.2
25.8
25.4
24.8
24.7
24.4
24.3
24.2
1
12
7
26.5
26.7
26.3
26.8
25.9
27.0
26.1
26.4
26.3
26.3
26.3
26.2
26.3
26.2
26.3
26.0
2
26.8
27.3
25.9
25.9
25.6
25.3
24,9
24.7
T(AI
167
162
157
152
147
142
137
132
32
24.8
24.8
23.7
22.9
22.3
21.8
21.2
20.5
7
27
25.4
24.8
24.4
24.0
23.4
22.9
22.0
21.2
22
26.0
25.5
25.0
24.6
24.2
23.7
23.2
21.8
JH
17
26.3
26.1
25.5
25.3
25.1
25.2
24.8
24.5
3
1-
12
7
26.6
27.0
26.2
26.8
26.2
26.7
26.3
25.5
26.3
26.3
26.2
26.1
26.1
26.0
25.9
25.4
2
26.8
26.7
26. S
26.3
26.1
25.9
25.0
24.0
EIAI
167
162
157
152
147
142
137
132
32
24.5
23.9
23.1
22.1
21.1
20.5
19.8
18.6
I
27
22
25.4
26.1
24.9
25.2
24.2
24.3
23.0
23.4
21.9
22.6
20.9
21.6
19.8
20.8
19.2
20.5
a
17
27.3
26.7
26.2
25.3
24.7
24. 1
24.0
23.9
_)
1-
12
7
27.7
27.7
28.2
29.0
28.3
30.1
27.7
28.3
27.2
27.4
27.9
27.3
29.0
27.7
29.1
27.8
2
27.3
27.5
26.2
25.8
25.0
25.5
27.1
26.9
C
167
162
157
152
147
142
137
132
32
0.5
0.4
0.5
0.6
0.6
0.7
0.7
0.8
I
z
27
22
0.5
0.5
0.6
0.5
0.5
0.5
0.5
0.5
0.5
0.5
0.6
0.6
0.7
0.8
0.7
0.8
1-
-1
17
12
7
0.6
0.5
0.6
0.6
0.6
0.7
0.5
0.7
0.8
0.4
0.7
0.7
0.5
0.6
0.6
0.6
0.6
0.6
0.8
0.7
0.8
0.8
0.8
0.9
2
0.5
0.5
0.5
0.6
0.3
0.6
0.5
0.4
H
167
162
157
152
147
142
137
132
32
5.9
5.4
5.5
6.2
5.8
6.0
5.2
4.7
I
1-
1-
• 27
22
17
12
7
6.9
7.5
7.1
6.6
6.2
6.8
7.5
6.9
5.5
4.6
7.1
7.2
6.8
6.4
5.7
6.4
7.3
7.3
6.5
6.7
5.7
6.7
7.3
7.4
7.0
4.8
6.9
6.5
6.2
5.3
4.6
5.8
7.0
5.2
5.8
4.6
5.7
6.8
5.5
6.0
2
6.3
5.9
6.0
8.3
9.0
9.2
8.0
7.5
LONGITUDE WEST
gisi
167
152
157
152
147
142
137
132
32
463.
502.
463.
419.
419,
370,
370,
317.
I
27
22
470.
474.
425.
474.
470.
474.
470.
474.
470.
474.
425,
429.
376,
324.
376.
324.
UJ
o
3
17
12
7
427.
466.
412.
427.
421.
364.
472.
37 2.
312.
512.
372.
364.
472.
421.
412.
427,
421,
412,
323,
372.
312.
323.
319.
255.
2
441.
441.
441.
399.
512.
399.
441,
479.
0IBI
167
162
157
152
147
142
137
132
I
3.
27
110.
104.
116.
99.
120.
112.
115.
119.
115.
119,
101.
110.
102,
101.
89.
104.
^
22
99.
107.
115.
115.
114,
106.
79.
87.
UJ
§
1-
17
12
7
92.
99.
89.
91.
92.
79.
103.
77.
70.
107.
80.
80.
104.
94.
93.
93.
9 3.
95.
75.
81.
75.
77.
74.
67.
2
102.
109.
97.
93.
115.
91.
99.
115.
0(EI
167
162
157
152
147
142
137
132
32
141.
129.
134.
155.
132.
120.
93.
80.
T
27
22
184.
227.
166.
254.
19 5.
249.
177.
252.
141.
190.
109.
202.
95.
132.
90.
107.
3
t-
17
12
7
198.
173.
164.
179.
110.
91.
165.
117.
105.
191.
147.
156.
206.
234.
194.
158.
139.
118.
183.
87.
126.
169.
92.
121.
2
184.
184.
154.
380.
487.
433.
182.
139.
QIC)
157
162
157
152
147
142
137
132
32
1.
-5.
11.
15.
10.
1.
1.
-4.
I
27
22
-6.
-15.
-3.
-3.
3.
9.
8.
3.
3.
-6.
-2.
-9.
-4.
-17.
1.
-3.
UJ
n
17
-3.
-9.
-3.
-15.
-12.
-21.
-14.
-9.
3
1-
12
7
-3.
-8.
3.
1.
-8.
7.
-6.
-3.
1.
1.
3.
3.
5.
5.
9.
15.
2
1.
15.
-15.
-14.
-18.
-22.
-4.
21.
QINI
157
162
157
152
147
142
137
132
32
212.
252.
198.
134.
162.
150.
175.
152.
I
1-
27
188.
155.
160.
166.
208.
208.
184.
181.
Z
22
17
154.
140.
117.
156.
101.
207.
104.
229.
175.
175.
129.
198.
130.
80.
134.
86.
3
12
7
197.
167.
218.
193.
187.
129.
152.
132.
93.
124.
187.
197.
200.
107.
145.
52.
2
155.
134.
205.
-61.
-72,
-103.
165.
204.
119
SEPTEMBER 1964
LONGITUDE WEST
TIUI
167
162
157
152
147
142
137
132
32
2*. 9
24.5
24.2
23.4
22.4
21.6
20.6
19.5
I
1-
27
22
25.3
26.0
24.8
25.8
24.4
25.3
24.0
24.6
23.1
23.8
22. 1
23.0
21.3
21.9
20.7
21.8
o
IT
26.6
26.2
25.7
25.2
24.8
24.6
24.3
24.2
§
12
7
26.7
27.3
26.5
26.8
26.3
26.4
26.1
26.3
26.1
26.0
26.2
25.9
26.3
26.3
26.3
26.2
2
26.3
25.9
25.9
25.7
25.7
25.7
25.7
25.7
TIAl
167
162
157
152
147
142
137
132
32
24.3
24.2
24.0
23.3
22.3
21.3
20.3
19.2
I
1-
(r
o
z
27
22
24.8
26.0
24.7
25.4
24.4
25.1
24.1
24.6
23.1
24.1
22.3
23.1
21.4
22.6
20.5
22.0
g
17
26.3
26.2
26.0
25.3
24.8
24.5
24.2
24.3
3
_1
12
7
26.7
27.0
26.7
26.8
26.7
26.6
26.1
26.4
26.2
26.2
25.7
25.9
25.4
25.7
25.3
25.3
2
26.1
26.2
26.6
26.1
25.3
25.0
25.0
25.2
EIAI
167
162
157
152
147
142
137
132
32
24.5
24.0
22.9
21.3
19.9
18.9
17.7
16.6
X
Z
27
22
24.0
25.8
24.9
25.6
24.2
24.6
22.1
23.5
21.0
23.1
19.6
21.9
18.3
20.1
17.2
18.8
1-
-I
17
12
7
27.2
29.1
29.2
26.9
28.9
28.8
25.9
28.2
28.0
25.6
27.9
28.0
25.9
28.6
27.8
24.9
27.1
27.4
23.6
26.9
27.1
22.6
27.1
27.2
2
27.0
26.1
25.5
26.0
26.1
26.0
25.7
26.1
c
167
162
157
152
147
142
137
132
32
0.5
0.5
0.4
0.4
0.6
0.7
0.7
0.8
X
l-
(£
O
z
27
22
0.5
0.4
0.6
0.5
0.6
0.6
0.5
0.6
0.6
0.6
0.7
0.6
0.7
0.7
0.7
0.7
IH
17
0.6
0.6
0.5
0.5
0.7
0.7
0.5
0.7
I-
_i
12
7
0.9
0.7
0.6
0.7
0.5
0.9
0.5
0.7
0.7
0.6
0.7
0.6
0.5
0.6
0.7
0.8
2
0.6
0.5
0.5
0.3
0.5
0.7
0.7
0.8
u
167
162
157
152
147
142
137
132
32
5.5
5.3
4.8
5.2
5.6
5.8
6.4
6.9
X
o
z
27
22
6.0
7. 1
6.1
7.2
6.0
8.0
6.6
7.8
7.3
8.0
6.8
7.1
6.5
6.7
6.6
5.8
lu
n
17
5.6
6.8
7.4
7.9
8.8
8.3
5.6
6.7
3
I-
-J
12
7
4.6
4.7
6.0
6.3
6.2
6.0
6.2
5.4
S.2
6.3
8.0
5.5
3.5
6.0
5.4
5.7
2
4.5
4.7
5.5
7.0
6.1
7.0
8.5
8.5
LONGITUDE WEST
0(SI
167
162
157
152
147
142
137
132
32
397.
397.
431.
431.
359.
318.
318.
272.
I
27
22
418.
473.
378.
436.
378.
394.
418.
394.
378.
394.
334.
394.
3 34.
349.
334.
349.
-J
17
12
7
405.
255.
367.
405.
413.
367.
448.
456.
257.
405.
456.
367.
358.
365.
416.
358.
365.
415.
448.
4 56.
416.
358.
365.
314.
2
414.
458.
458.
531.
45 8.
366.
366.
314.
a(B)
167
162
157
152
147
142
137
132
32
117.
115.
125.
129.
116.
109.
112.
100.
27
119.
101.
102.
117.
112.
102.
106.
113.
22
113.
112.
104.
105.
101.
107.
94.
104.
3
1-
17
12
7
98.
58.
83.
95.
86.
80.
102.
93.
57.
97.
99.
81.
87.
79.
89.
91.
91.
93.
114.
114.
101.
95.
97.
85.
2
97.
102.
98.
112.
110.
96.
97.
82.
g(E)
167
162
157
152
147
142
137
132
32
131.
120.
116.
132.
141.
142.
159.
172.
X
o
z
27
2i
178.
235.
139.
237.
135.
338.
211.
300.
238.
280.
191.
185.
176.
162.
187.
151.
3
1-
17
12
147.
86.
190.
118.
239.
132.
268.
130.
308.
239.
295.
301.
131.
80.
200.
129.
7
107.
146.
134.
111.
131.
110.
151.
133.
2
105.
112.
146.
202.
151.
202.
392.
369.
QIC)
167
162
157
152
147
142
137
132
32
14.
7.
4.
3.
3.
7.
8.
9.
X
27
22
12.
1.
3.
12.
1.
7.
-3.
1.
1.
-10.
-6.
-3.
-3.
-19.
6.
-5.
UJ
n
17
7.
1.
-9.
-4.
1.
4.
3.
-3.
-I
12
7
1.
6.
-5.
1.
-10.
-5.
1.
-3.
-4.
-5.
16.
1.
13.
15.
22.
21.
2
4.
-6.
-18.
-12.
10.
20.
24.
17.
OIN)
167
162
157
152
147
142
137
132
32
136.
156.
186.
168.
101.
59.
39.
-9.
X
27
22
109.
125.
135.
75.
141.
-55.
93.
-12.
29.
24.
47.
106.
55.
112.
29.
99.
IH
17
154.
120.
117.
44.
-38.
-33.
201.
65.
3
1-
12
7
112.
171.
215.
141.
242.
71.
228.
178.
52.
202.
-43.
212.
250.
149.
117.
76.
2
209.
251.
233.
229.
188.
49. -
147. -
155.
120
OCTOBER 1964
LONGITUDE WEST
TIHI
167
162
157
152
147
142
137
132
22.T
22.3
21.9
21. S
21.0
20.6
19.8
19.0
X
2*.)
26.2
23.7
23.3
22.8
21.9
20.9
20.3
25,3
25.0
24.7
24.3
23.8
23.3
22.6
21.8
g
26.2
26.0
25.6
25.4
25.0
24.6
24.7
24.4
3
26.6
26.4
26.3
26.2
25.9
26.0
26.3
26.1
5
27.6
26.6
26.0
26.2
26.2
26.2
26.3
26.3
26.6
26.3
25.7
25.3
24.9
25.0
25.2
25.3
T(»t
167
162
157
152
147
142
137
132
32
21. e
21.3
20.8
20.4
19.9
19.9
19.8
19.0
I
27
23. S
23.0
22.7
22.3
22.1
21.7
20.8
20.2
Z
22
25.0
24.7
24.1
23.7
23.3
23.3
22.4
21.2
UJ
o
17
25.8
25.9
25.3
25.0
24.6
24.4
24.5
23.7
_)
1-
12
26.7
26.2
26.0
26.0
25.7
25.8
25.7
25.3
5
_l
7
26.5
26.3
26.2
26.1
26.0
26.0
25.8
25.4
2
26.5
26.5
26.5
25.7
25.0
24.3
24.0
24.0
EiA)
167
162
157
152
147
142
137
132
32
20.1
19.4
18.7
17.9
17.8
18.2
18.3
17.6
I
27
22.1
21.3
20.1
20.0
19.5
19.3
18.9
18.1
p
22
24.4
23.7
22.7
22.3
21.6
20.1
19.0
19.4
UJ
17
26.4
26.0
26.1
24.7
24.6
23.0
24.2
23.5
g
12
28.2
28.0
28.1
27.0
26.5
26.5
27.0
26.3
S
7
28.0
29.0
28.2
28. 1
27.3
26.3
25.3
25.0
2
26.7
26.2
25.7
26.0
26.1
25.0
23.7
23.5
c
167
163~
157
152
147
142
137
132
32
0.6
0.6
0.7
0.7
0.6
0.6
0.6
0.7
X
27
0.6
0.5
0.5
0.6
0.6
0.5
0.6
0.6
ir
i
22
0.6
0.6
0.5
0.6
0.5
0.5
0.6
0.6
iH
17
0.6
0.6
0.6
0.6
0.5
0.5
0.6
0.6
3
t-
12
0.6
0.6
0.7
0.6
0.6
0.6
0.6
0.6
7
Q.8
0.8
0.8
0.5
0.5
0.5
0.7
O.S
2
0.5
0.4
0.5
0.5
0.4
0.3
0.3
0-7
H
167
162
157
152
147
142
137
132
32
7.3
7.4
7.7
7.8
7.6
7.7
6.7
6.0
I
27
8.9
8.1
7.7
7.3
6.8
6.3
5.7
5.5
CC
22
9.0
8.3
7.7
7.7
8.2
7.7
6.8
6.3
o
17
7.7
7.8
6.9
8.2
8.6
6.7
7.1
6.6
I-
12
6.7
7.1
6.3
6.4
6.7
6.1
5.3
5.8
-J
7
3.6
5.3
5.4
5.5
5.0
3.6
5.3
4.7
2
5.3
6.0
6.4
6.4
5.3
4.9
6.1
4.5
LONGITUDE WEST
HI SI
167
162
157 152 147 142
137
132
32
285.
285.
252. 252. 285. 285.
285.
252.
J.
27
313.
346.
346. 313. 313. 346.
313.
313.
z
22
340.
340.
375. 340. 375. 375.
340.
340.
1-
-J
17
12
7
363.
383.
302.
363.
383.
302.
363. 363. 401. 401.
339. 383. 383. 383.
302. 440. 440. 440.
363.
383.
352.
363.
383.
440.
2
454.
492.
454. 454. 492. 526.
526.
363.
g(8i
167
162
157 152 147 142
137
132
I
32
27
125.
115.
128.
136.
120. 122. 134. 127.
138. 128. 125. 128.
117.
117.
107.
120.
Z
22
106.
108.
124. 116. 126. 125.
121.
123.
t-
17
12
7
101.
89.
84.
99.
94.
73.
100. 106. 115. 118.
85. 97. 98. 98.
68. 99. 104. 107.
105.
102.
97.
113.
106.
121.
2
105.
110.
97. 100. 109. 129.
141.
111.
QIEI
167
162
157 152 147 142
137
132
I
32
27
246.
508.
258.
418.
297. 319. 265. 235.
363. 285. 228. 164.
124.
116.
93.
108.
o
z
22
489.
402.
328. 315. 384. 334.
233.
158.
UJ
Q
3
K
-1
17
12
7
292.
170.
103.
306.
188.
101.
186. 373. 392. 210.
138. 166. 179. 155.
96. 108. 110. 88.
207.
128.
161.
179.
152.
144.
2
146.
172.
174. 147. 94. 107.
186.
130.
OIC)
167
162
157 152 147 142
137
132
32
27.
30.
34. 34. 34. 22.
1.
1.
I
1-
27
22
18.
11.
39.
10.
31. 29. 19. 5.
19. 19. 17. 1.
3.
6.
3.
15.
3
1-
-I
17
12
7
13.
-3.
14.
4.
6.
7.
9. 13. 14. 6.
8. 6. 6. 5.
-5. 3. 4. 3.
6.
13.
11.
19.
19.
17.
2
3.
-5.
-21. -11. -3. 14.
29.
24.
QtNl
167
162
157 152 147 142
137
132
32
-114.
-132.
-200. -224. -148. -100.
43.
53.
I
1-
q:
iH
27
22
17
-329.
-267.
-44.
-248.
-181.
-46.
-187. -130. -60. 48.
-96. -110. -151. -85.
68. -130. -120. 68.
78.
-21.
46.
83.
44.
52.
3
1-
12
7
128.
102.
96.
122.
108. 116. 101. 125.
143. 231. 223. 243.
141.
84.
106.
159.
2
201.
216.
204. 218. 292. 276.
170.
99.
121
NOVEMBER 1964
LONGITUDE WEST
TIH)
167
162
157
152
147
142
137
132
32
20.3
19.8
19.3
19.7
19.3
18.7
18.3
17.7
I
o
z
27
22
22.6
24.3
22.3
2<..3
22. 3
23.8
22.0
23.4
21.3
23.1
20.5
22.5
19 .8
22.0
19.5
21.5
UJ
Q
17
25. •!
25.4
24.9
24.4
24.3
24.2
23.7
23.1
3
1-
12
7
26. 3
27.3
26.2
27.0
25.7
26.5
25.3
26.2
25.2
25.3
25.2
24.8
25.2
25. 7
25.0
26.3
2
26.2
26.0
25.5
25.3
24.7
24.6
24.9
25.3
r(Ai
167
162
157
152
147
142
137
132
32
19.8
19.0
18.3
18.3
18.6
17.9
17.5
17.0
I
27
22
22.2
24.1
21.5
24.0
21.4
23.7
21.3
23.1
20.8
22.7
20.0
22.3
19.3
22.0
19.0
21.3
g
17
25.3
25.3
25.3
24.4
24.3
23.9
23.0
22.8
1-
12
7
26.3
27.0
26.1
26.7
25.6
26.2
25. 1
25.5
25.2
24.3
25.0
24.6
24. 7
25.0
24.8
25.2
2
26.2
26.0
26.1
25.6
25.1
24.3
24.0
25.0
E(AI
167
162
157
152
147
142
137
132
32
17.8
17.0
16.9
16.9
16.9
16.4
15.6
15.1
I
1-
(E
O
Z
27
22
20.3
23.0
20.0
23.4
20.4
23.1
20.3
22.8
19.9
22.6
17.9
20.9
16.8
20. 1
16.0
19.2
17
12
7
26.1
26.8
27.5
25.6
27.6
28.1
25.2
26.9
27.6
25.1
27.2
27.2
25.0
27.4
26.2
24.2
27. 5
26.6
23.0
27.9
27. 3
22.4
28.0
27.2
2
27.3
26.1
25.9
24.8
23.7
24.7
25.1
24.7
C
167
162
157
152
147
142
137
132
32
0.7
0.7
0.7
0.8
0.8
0.7
0.7
0.7
I
9
27
22
0. 7
0.5
0.6
0.5
0. 7
0.6
0.7
0.6
0.8
0.7
0.8
0.7
0.7
0.7
0.7
0.9
S^
17
0.5
C.5
0.5
0.6
0.6
0.7
0.7
0.7
3
12
0.5
0.5
0.6
0. B
0. 7
0.8
0.7
0.5
-J
7
0.3
0.7
0.7
0.7
0.8
0.9
0.8
0.6
2
0.2
0.4
0.4
0.3
0.4
0.5
0.6
0.6
H
167
162
157
152
147
142
137
132
32
10.0
9.2
7.8
7.5
8.8
8.2
7.6
7.3
I
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27
22
10.3
7.8
9. 2
8.9
8. 5
B.6
8.3
8.7
8.3
7.8
7.3
6.9
6.3
5.9
6.5
6.5
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17
7.2
7.8
9.0
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6.6
6.2
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12
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7.3
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7
a. 5
8.4
7.5
6.0
5.7
6.2
7.3
8.2
2
7.3
6.4
4. 7
7.0
6.5
8.1
6.8
7.8
LONGITUDE WEST
QIS)
167
162
157 152
147
142
137
132
32
189.
189.
1B9. 162.
162.
189.
189.
189.
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22
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311.
248.
311.
219. 219.
281. 231.
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188.
248.
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174.
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17
345.
345.
345. 313.
313.
276.
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276.
3
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12
379.
379.
343. 259.
303.
259.
303.
379.
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7
473.
326.
326. 326.
279.
228.
2 79.
369.
2
531.
471.
471. 50 3.
471.
434.
3 93.
393.
got
167
162
157 152
147
142
137
132
32
U4.
119.
123. 112.
104.
120.
122.
122.
X
1-
27
107.
124.
112. no.
95.
100.
116.
119.
z
22
117.
117.
106. 109.
100.
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79.
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17
106.
108.
102. 99.
99.
95.
103.
100.
3
1-
12
103.
101.
95. 75.
83.
74.
87.
99.
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7
117.
86.
87. 93.
88.
64.
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107.
2
116.
112.
1C5. 116.
115.
112.
no.
105.
QIEI
167
162
157 152
147
142
137
132
32
452.
400.
253. 216.
325.
249.
202.
169.
I
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27
559.
454.
353. 307.
270.
204.
149.
168.
Z
22
299.
422.
341. 339.
225.
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133.
160.
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17
194.
273.
384. 352.
133.
134.
221.
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1-
12
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42 5. 3 06.
143.
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120.
85.
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7
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244. 144.
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103. 216.
183.
2 83.
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167
162
157 152
147
142
137
132
32
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7
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9INI
167
162
157 152
147
142
137
132
32
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12
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52.
58.
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2
201.
179.
275. 179.
184.
29.
88.
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122
DECEMBER 1964
LONGITUDE WEST
riHi
167
162
157
152
147
142
137
132
32
18.0
18.5
18.5
18.7
18. S
17.9
17.6
16.7
I
27
21.0
21.2
21.2
21.2
20.9
20.2
19.6
18.9
o
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22
23.6
23.7
23.4
23.0
22.3
21.8
21.1
20.7
UJ
n
17
24.8
24.9
24.7
24.4
23.9
23.2
22.8
22.7
3
1-
12
25.6
25.5
25.4
25.0
25.0
24.5
24.4
24.1
5
-I
7
26.3
26.4
26.1
25.6
25.4
25.4
25.5
25.5
2
2S. 1
25.1
25.3
25.5
25.3
25. 1
24.5
24.1
T(AI
167
162
157
152
147
142
137
132
32
17.0
17.0
18.0
18.2
18.5
18.4
18.0
17.2
I
27
20.3
21.0
21.4
21.3
21.1
20.4
19.8
18.8
7
22
23.3
23.6
23.5
23.0
22.7
22.1
21.4
20.6
^
17
24.8
25. 2
2 5. 1
24.5
24.0
23.6
22.8
22.0
J3
1-
12
26.3
25.8
25.5
25.3
25.1
24.6
24.2
24.0
7
27.0
26.4
25.8
25.6
25.3
25.3
25.2
24.6
2
26.7
26.5
26.3
25.7
25.0
24.5
24.3
24.0
E(A)
167
162
157
152
147
142
137
132
32
15.8
16.0
17.4
17.6
18.0
18.4
17.7
16.8
I
27
18.3
20.2
21.0
20. 7
20.3
19.7
18.7
17.5
22
22.7
23.3
23.7
22.9
21.9
21.1
19.9
18.2
S
17
25.2
25.8
25.6
25.1
23.8
22.9
21.9
20.6
3
(-
12
28.1
27.6
27.2
25.8
26.0
26.0
24.7
24.0
-I
7
28.5
28.5
28.5
28.5
28.3
27.8
27.2
26.3
2
27.7
27.7
26.5
26.0
25.9
25.9
25.0
26.1
C
167
162
157
152
147
142
137
132
32
0.7
0.7
0.8
0.7
0.7
0.7
0.7
0.8
I
1-
27
0.7
0.6
0.6
0.6
0.6
0.5
C. 7
0.7
22
0.5
0.5
0.5
0.5
0.6
0.5
0.7
0.8
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17
0.5
0.4
0.4
C.6
0.7
0.5
C.7
0.6
3
12
0.5
0.5
0.5
0.5
0.6
0.7
0.7
0.5
7
0.5
0.6
0.7
0.3
0.8
0.8
0.7
0.7
2
0.5
0.4
0.5
0.5
0.6
0.6
0.6
0.5
W
167
162
157
152
147
142
137
132
32
9.8
9.6
9.2
8.4
7.9
8.1
7.0
5.3
F
27
9.2
8.7
8.0
6.7
6.6
6.7
6. 3
5.7
a.
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22
8.2
6.3
7.7
7.5
7.2
5.9
7.4
7.0
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17
6.7
7.5
8.0
8. 3
8. 1
8.0
7.7
8.3
1-
12
7.4
7.8
3.2
7.8
8.3
7.5
7.7
8.2
§
7
7.5
6. 1
6.8
7. 5
6.8
5.9
8.8
6.7
2
6.6
6.4
4.5
6.9
7.2
8.3
7.7
6.7
LONGITUDE WEST
QISI
167
162
157
152 147
14 2
137
132
32
160.
160.
137.
160. 160.
160.
160.
137.
I
27
191.
216.
216.
216. 216.
216.
191.
191.
Z
22
277.
277.
277.
277. 251.
277.
222.
190.
UJ
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17
316.
343.
343.
286. 253.
285.
253.
286.
1-
12
354.
354.
354.
354. 320.
283.
283.
320.
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7
388.
351.
311.
266. 266.
256.
311.
311.
2
420.
456.
420.
420. 381.
381.
381.
381.
9(8)
167
162
157
152 147
142
137
132
32
123.
129.
99.
112. 105.
97.
100.
87.
X
27
115.
114.
107.
109. 109.
110.
101.
108.
z
22
119.
114.
110.
113. 102.
115.
98.
95.
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17
107.
108.
107.
97. 91.
101.
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3
1-
12
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89.
88,
95.
89.
99.
84.
101. 95.
70. 71.
85.
73.
93.
87.
103.
97.
2
79.
87.
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103. 101.
103.
99.
95.
Q(E 1
157
162
157
152 147
142
137
132
32
351.
373.
247.
201. 133.
86.
64.
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27
431.
261.
178.
114. 109.
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22
308.
297.
190.
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171.
182.
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157.
195.
236.
256. 256.
240.
224.
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231. 275.
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308.
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2
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183. 195.
292.
182.
95.
QIC)
167
162
157
152 147
142
137
132
32
39.
58.
19.
17. 1.
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27
25.
7.
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157
162
157
152 147
142
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132
32
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27
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128.
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54. 88.
58.
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26.
2
2 86.
313.
257.
141. 77.
-31.
90.
187.
123
JANUARY 1965
LONGITUDE WEST
Tl Wl
157
162
157
152
147
142
137
132
32
16.0
16.8
17.0
17.7
17.9
17.7
17.0
16.0
I
27
20.3
21.0
21.3
21.0
20.4
19.9
19.1
18.0
22
23.2
23.0
23.2
22.7
22.0
21.3
21.2
21.0
SH
17
24.4
24.5
24.3
23.6
23.0
22. 7
22.3
22.3
3
12
25.7
25.4
24.9
24.7
24.6
25.3
24.6
24.4
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7
26.9
26. 3
26.3
26.3
2 6.3
25.0
25.3
25.2
2
27. C
26.3
25.7
26.6
27.1
25.9
25.7
25.5
TIAl
167
162
157
152
147
142
137
132
32
15.0
15.8
16.7
17.0
17.5
17.7
17.0
15.4
I
1-
27
19.2
19.3
20.4
20.2
20.2
19.6
18.8
17.9
22
21.7
21.7
22.3
22.3
22.2
21.5
21.0
19.9
UJ
Q
17
23.8
24.3
24.3
24.2
23.5
23.2
22.3
21.5
3
1-
12
25.2
25.1
25.1
24.6
24.0
24.0
24.0
22.8
7
26.3
25.9
26.2
25.9
25.4
25.0
24.5
24.8
2
26.6
26.6
26.6
26.2
25.6
24.3
24.0
24.6
E(AI
167
162
157
152
147
142
137
132
32
13. C
14.0
15.6
16.0
17.0
16.9
15.9
14.3
I
27
16.9
18.0
19.2
19.2
19.3
16.3
15.8
15.8
22
19.5
20.5
21.3
21.5
21.1
19.9
18.7
15.9
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17
23.3
23.8
23.9
23.3
21.9
20.9
20.2
19.2
3
I-
12
27.1
25.5
25.4
25.1
23.2
23.0
24.0
22.0
7
27.2
27.2
26.7
26. 6
25.3
25.7
25.5
26.2
2
26.7
27.0
27.8
28.2
27.2
26.2
26.0
27.5
C
167
162
157
152
147
142
137
132
32
0.7
0.6
0.7
0.7
0.6
0.7
0.7
0.7
I
27
0.6
0.6
0.6
0.5
0.5
0.7
0.6
0.5
22
0.5
0. 6
0.6
0.6
0.6
0.5
0.4
0.6
a
17
0.5
0.5
0.6
0.6
0.5
0.6
0.7
0.6
ji;
12
0.3
0.7
0.6
0.5
0.4
0.5
0.5
0.4
7
0.6
0.7
0.6
0.6
0.4
0.5
0. 6
0.6
2
0.3
0.5
0.5
0.6
0.4
0.6
0.8
o.e
H
167
162
157
152
147
142
137
132
32
8.5
8.2
8.8
8.2
7.7
8.4
7.6
6.3
I
9
27
7.9
9.0
8.4
8.5
8.3
7.2
5.7
5.8
22
7.2
7.9
7.6
7.8
7.1
6.2
7.3
7.3
17
5.8
6.6
6.5
5.8
6.3
6.1
8.3
8.4
K
12
9.3
8.5
7.2
7.7
7. 1
7.7
8.3
9.2
_l
7
7.7
7.4
5.7
6.3
7.8
8.2
6.7
7.0
2
5.6
6.0
4.7
6.4
7.5
8.2
6.6
7.5
LONGITUDE WEST
a(S)
167
152
157
152
147 142
137
132
32
174.
197.
174.
174.
197. 174.
174.
174.
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27
22
231.
294.
231.
266.
231.
266.
231.
266.
231. 205.
265. 294.
231.
319.
231.
266.
1-
17
12
7
330.
424.
360.
299.
293.
319.
299.
331.
360.
299.
331.
360.
330. 299.
397. 331.
432. 396.
264.
366.
350.
299.
3 97.
360.
2
497.
428.
42 3.
388.
465. 338.
293.
293.
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167
162
157
152
147 142
137
132
1
32
27
130.
136.
145.
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140.
129.
114.
126.
121.
118.
125.
114.
123. 107.
116. 109.
107. 120.
110.
125.
138.
121.
125.
137.
3
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17
12
7
121.
119.
102.
106.
92.
89.
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97.
100.
101.
111. 106.
129. 123.
123. 119.
102.
119.
108.
127.
146.
101.
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121.
99.
88.
96.
128. 116.
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a(E)
167
162
157
152
147 142
137
132
O
z
32
27
22
2 84.
297.
285.
250.
433.
325.
219.
320.
265.
203.
305.
240.
131. 158.
229. 153.
158. 122.
125.
1C6.
212.
90.
99.
265.
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t
17
12
143.
381.
176.
364.
158.
186.
155.
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143. 148.
234. 363.
339.
345.
408.
564.
5
7
318.
234.
148.
176.
319. 381.
175.
155.
2
174.
153.
77.
155.
306. 344.
177.
173.
QIC)
167
162
157
152
147 142
137
132
32
34.
33.
11.
23.
13. 1.
1.
15.
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27
22
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43.
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17. 40.
28. 33.
20.
22.
59.
12.
2
9.
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11.
45. 52.
45.
27.
QINI
167
162
157
152
147 142
137
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32
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119. -
55.
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373.
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193.
185.
281.
127.
-15. -126.
-26.
10.
124
FEBRUARY 1965
LONGITUDE WEST
TIMI
167
162
157
152
147
142
137
132
32
15.*
IS. 7
16.0
16.7
17.5
17.2
16.5
15.4
1
27
22
19.3
21.7
19.5
21.8
19.6
22.0
19.6
22.0
19.8
21.5
19.5
21.3
18.7
20.5
17.8
19.6
^
17
24.0
23.7
23.3
22.7
22.5
22.2
22.4
21.7
^
§
12
7
25.3
26.3
25.2
25.8
24.0
25.3
23.7
25.3
24.2
25.3
24.4
25.3
24.1
25.3
23.6
25.3
2
26.6
26.3
25.6
26.0
25.9
25.6
25.6
26.0
TIAI
167
162
157
152
147
142
137
132
32
14.2
14.7
15.3
16.0
16.7
16.7
16.5
15.0
I
27
22
18.4
21.1
18.0
20.7
18.3
20.7
18.7
20.7
19.0
20.8
19.0
20.8
18.4
20.2
17.0
19.0
1-
!
17
12
7
22.9
24.8
26.2
23.1
24.5
25.9
23.1
24.0
25.5
22.6
24.3
25.5
22.2
24.2
25.5
22.1
23.7
25.3
22.0
23.5
25.3
21.6
23.5
25.9
2
26.6
26.6
26.6
25.9
25.5
25.3
25.8
24.2
E(A)
167
162
157
152
147
142
137
132
32
13.0
12.3
13.6
14.9
15.9
15.6
14.8
13.5
I
Z
27
22
15.1
17.3
15.5
17.0
16.4
17.5
17.7
19.0
18.1
19.5
17.4
19.2
16.2
18.2
14.8
16.7
a
3
K
§
17
12
7
19.9
24. C
26.9
20.0
23.9
26.4
20.8
24.1
26.1
21.3
24.8
26.4
21.4
24.5
27.1
22.1
23.4
27.5
21.6
24.0
27.3
20.5
24.0
27.2
2
28.3
27.0
26.5
27.1
27.6
28.1
28.1
27.7
C
167
162
157
152
147
142
137
132
32
0.7
0.7
0.7
0.8
0.9
0.8
0.8
0.8
I
27
22
0.6
0.5
0.7
0.5
0.7
0.5
0.7
0.6
0.7
0.7
0.8
0.8
0.8
0.8
0.8
0.7
1
-I
17
12
7
0.5
0.5
0.6
0.4
0.4
0.6
0.4
0.6
0.6
0.7
0.6
0.7
0.6
0.7
0.8
0.8
0.8
0.8
0.7
0.7
0.8
0.7
0.6
0.7
2
0.7
0.5
0.5
0.6
0.6
0.6
0.5
0.7
M
167
162
157
152
147
142
137
132
32
9.0
7.7
8.3
9.7
11. 1
9.2
8.3
7.5
I
27
22
6.8
6.8
7.8
7.5
7.8
7.8
8.9
8.5
10.2
7.7
9.4
a. 7
8.0
8.3
7.5
6.9
1-
17
12
7
8.2
9.0
9.1
7. 8
8.7
10. 0
7.0
9.1
8.4
7.2
8.0
8.1
6.0
9.4
8.2
6.8
8.3
7.6
7.0
6.9
7.3
8.5
8.6
6.6
2
8.0
5.8
5.2
7.7
7.5
6.0
4.9
4.2
LONGITUDE WEST
QIS)
167
162
157
152
147
142
137
132
32
228.
228.
228.
195.
160.
19S.
19S.
195.
Z
1-
27
289.
255.
255.
255.
255.
218.
218.
218.
o:
z
22
351.
351.
351.
318.
281.
241.
241.
281.
1*1
17
381.
413.
413.
305.
345.
261.
305.
305.
s
K
12
408.
443.
369.
369.
326.
279.
326.
369.
1-
_l
7
390.
390.
390.
345.
295.
295.
295.
345.
2
361.
451.
451.
408.
408.
408.
451.
361.
aiBi
167
162
157
152
147
142
137
132
32
131.
132.
124.
106.
90.
103.
99.
106.
I
l-
27
139.
132.
127.
117.
115.
100.
100.
109.
i
22
141.
149.
149.
133.
112.
97.
97.
118.
IjJ
17
140.
141.
132.
100.
113.
85.
102.
102.
3
1-
12
119.
128.
102.
92.
91.
91.
99.
103.
(-
3
7
96.
96.
94.
83.
71.
72.
73.
.6.
2
81.
99.
91.
95.
97.
93.
95.
105.
01 E)
167
162
157
152
147
142
137
132
32
282.
219.
231.
291.
347.
258.
197.
141.
I
27
202.
296.
263.
308.
381.
356.
238.
200.
o:
o
z
22
241.
34t>.
371.
407.
237.
353.
298.
173.
UJ
Q
17
491.
385.
229.
196.
125.
122.
157.
291.
s
1-
12
516.
471.
357.
189.
376.
359.
166.
277.
K
_I
7
461.
502.
313.
262.
237.
166.
153.
122.
2
281.
145.
109.
246.
199.
96.
72.
78.
OICI
167
162
157
152
147
142
137
132
32
43.
31.
24.
27.
36.
19.
1.
12.
I
27
25.
47.
41.
32.
33.
19.
10.
24.
q;
^
22
17.
34.
41.
44.
22.
18.
10.
17.
III
17
36.
19.
6.
3.
8.
3.
12.
4.
Q
12
18.
25.
1.
-20.
1.
24.
17.
4.
H
4
_l
7
4.
-4.
-7.
-7.
-7.
1.
1.
-16.
2
1.
-7.
-21.
4.
12.
8.
-4.
30.
a(Ni
157
162
157
152
147
142
137
132
32
-229. ■
-154.
-152. -
-230. -
-313. -
■185. -
-102.
-64.
I
27
-78. -
■221. -
-176. -
-204. -
■274. -
■257. -
131. -
116.
Q
22
-48. ■
-178.
-210. ■
-257.
-91. -
227. -
164.
-27.
z
Ul
17
-287. ■
-132.
46.
6.
100.
51.
34.
-92.
o
H
12
-245.
-182.
-91.
108. -
142. -
194.
45.
-14.
t-
3
7
-171.
-2 03.
-10.
6.
-6.
58.
70.
163.
2
-3.
215.
273.
64.
101.
212.
2 89.
149.
125
MARCH 1965
LONGITUDE WEST
TIWI
167
162
157
152
147
142
137
132
32
16.3
16.2
1«. 0
16.5
17.2
16.9
15.9
14.8
I
Z
27
22
19.0
22.1
19.0
22.1
19.2
22.0
19.4
21.4
19.6
21.3
19.1
21.1
18. 3
20.5
17.5
20.0
IH
17
24.0
23.7
23.3
22.7
22.5
22.0
21.6
21.2
1
-I
12
7
26.5
27.4
25.7
26.7
23.9
25.2
23.6
24.7
24.2
25.3
23.3
25.2
22.6
25.1
22.5
25.1
2
27.3
26.6
25.9
25.5
25.7
25.7
25.7
25.7
T(AI
167
162
157
152
147
142
137
132
32
16.1
16.0
15.5
16.3
17.3
16.7
15. B
14.4
I
27
22
18.6
21.6
18.5
21.2
la.o
21.4
18.7
21.2
19.3
21.2
19.0
20.6
18.0
20.0
17.0
19.0
^
17
23.3
23.3
23.3
23.0
22.7
22.5
22.0
21.0
3
1-
12
7
25.1
25.8
24.9
26. 1
24.5
26.7
24.6
26.0
24.4
25.4
23.8
25.3
24.1
25.6
23.6
26.0
2
26.8
27.0
27.0
26.6
26.3
26.3
26.5
26.5
EIA)
167
162
157
152
147
142
137
132
32
14.0
13.9
14.1
15.7
16.2
14.9
13.5
12.0
I
1-
27
22
16.1
18. 6
16.1
18. 5
15.1
18.8
17.0
19. 0
17.7
20.1
17.0
20.2
16.2
18.1
14.6
17.2
17
12
7
21.0
23.6
25.7
21.2
23.7
2 5. 9
21.4
24.0
27.3
20.9
24.4
28.3
21.4
24.9
2 8.1
21.5
24.5
27.9
19. 8
23.5
27.7
18.7
23.1
27.6
2
29.1
29.5
29.7
29.7
29.1
29.0
29. I
29.2
C
167
162
157
152
147
142
137
132
32
0.8
0.8
0.7
0.8
0.8
0.7
0.7
0.7
I
27
22
0.7
0.5
0.8
0.5
0.6
0.5
0.6
0.6
0.7
0.7
0.7
0.8
0.7
0.7
0.7
0.7
iH
17
0.4
0.4
0.5
0.6
0.5
0.6
0.7
0.8
3
I-
12
7
0.6
0.6
0.3
0.3
0.4
D.2
0.4
0.5
D.5
0.6
0.6
0.7
0.7
0.7
0.6
0.6
2
0.5
0.5
0.5
0.5
0.5
0.5
0.6
0.6
M
167
16 2
157
152
147
142
137
132
32
8.6
9.2
10.0
7.9
7.5
6.6
7.4
6.6
I
g
27
22
7.5
6.8
7.7
6.2
7.7
6.2
7.5
6.6
7.8
7.0
7.6
7.1
7.2
7.1
6.5
5.9
IH
17
5.6
5.8
5.6
5.6
6.2
6.3
6.3
7.2
3
1-
.J
12
7
5.6
6.2
5.8
8.0
6.7
9.6
7.0
8.7
8.2
9. 4
7.6
9.4
7.8
9. 7
8.5
10.3
2
4.9
6.0
5.2
6.8
7.4
6.9
7.1
7.7
LONGITUDE WEST
QtSI
167
162
157
152
147
142
137
132
32
248.
248.
290.
248.
248.
290.
290.
290.
X
1-
g
z
27
22
311.
412.
266.
412.
352.
412.
352.
373.
311.
330.
311.
282.
311.
330.
311.
330.
1-
17
12
7
468.
405.
414.
458.
518.
531.
431.
485.
561.
390.
485.
458.
431.
447.
414.
390.
405.
366.
345.
358.
356.
295.
405.
414.
2
465.
465.
465.
465.
465.
465.
421.
421.
a(Bi
167
162
157
152
147
142
137
132
32
103.
103.
120.
98.
94.
lis.
118.
125.
I
27
117.
103.
143.
129.
111.
110.
114.
121.
o
z
22
134.
140.
135.
119.
102.
94.
113.
121.
B
1-
-I
17
12
7
139.
124.
120.
134.
137.
127.
120.
110.
94.
108.
103.
80.
H6.
105.
88.
102.
93.
80.
98.
74.
76.
95.
90.
BO.
2
102.
89.
78.
78.
87.
67.
77.
76.
QIEI
167
162
157
152
147
142
137
132
32
253.
295.
304.
125.
117.
111.
156.
125.
CE
O
z
27
2Z
210.
215.
229.
187.
283.
176.
196.
166.
205.
150.
188.
142.
151.
182.
135.
131.
17
12
7
1B3.
218.
249.
167.
193.
407.
140.
145.
277.
130.
132.
138.
132.
247.
259.
112.
143.
260.
140.
149.
275.
204.
213.
309.
^
115.
109.
59.
68.
121.
103.
107.
134.
Q(CI
167
162
157
152
147
142
137
132
32
7.
8.
20.
7.
-3.
6.
3.
11.
I
O
z
27
22
12.
14.
16.
23.
37.
15.
21.
6.
10.
3.
4.
15.
9.
15.
13.
24.
_1
17
17.
10.
1.
-7.
-5.
-13.
-10.
6.
12
7
32.
40.
19.
20.
-16.
-58.
-28.
-45.
-7.
-4.
-16.
-4.
-47.
-20.
-38.
-37.
2
10.
-10.
-23.
-30.
-18.
-17.
-23.
-25.
aiNi
167
162
157
152
147
142
137
132
32
-116.
-158.
-155.
19.
41.
59.
13.
29.
I
27
22
-28.
49.
-83.
62.
-HI.
86.
5.
82.
-15.
75.
9.
32.
38.
21.
42.
55.
g
17
129.
157.
171.
160.
189.
189.
118.
-10.
(-
12
31.
170.
246.
279.
103.
185.
182.
140.
5
7
6.
-22.
247.
2 86.
72.
31.
36.
63.
2
239.
278.
352.
350.
276.
292.
260.
235.
126
APRIL 1965
LONGITUDE WEST
TIKI
167
162
157
152
147
142
137
132
32
IS. 2
16.0
16. <i
16.9
17.0
16.8
16. 1
15.1
I
O
Z
27
22
19.5
22.2
19.0
22.3
19.6
22.3
19.9
22.3
19.9
21.9
19.2
21.0
18.4
20.2
17.4
18.9
UJ
17
23.8
2*. 2
24.3
23.5
23.3
22.8
22.0
21.7
12
7
25.3
26.2
25.0
26.2
24.6
25.5
24.4
25.4
24.4
25.9
24.5
26.3
24.3
26.7
23.7
27.3
2
26.5
26.5
26.5
26.5
26.5
26.5
26.5
26.5
T(»)
167
162
157
152
1*7
142
137
132
32
16.1
16.0
16.5
16.5
16.3
16.1
15.7
15.0
I
1-
27
IV. 1
19.1
19.8
19.8
19.6
19.1
18.5
17.1
7
22
21.5
21.7
22.5
22. 1
21.9
21.3
20.3
19.5
1-
17
12
7
23.7
27. 1
26.7
2<..0
25. <.
26.3
24.3
25.0
26.2
23.6
25.2
26.3
23.3
25.0
26.3
23.0
24.9
25.8
22.0
24.0
25.3
21.2
22.5
25. 1
2
27.2
27.0
27.4
27.1
26.7
26.3
25.9
25.4
E(AI
167
162
157
152
147
142
137
132
32
15.0
11.9
15.0
14.7
14.7
14.3
13.6
13.2
I
O
z
27
22
17.9
20.1
18.3
20.9
18.9
21.6
17.0
20. 6
17.4
20.3
17.0
20.0
15.8
18.2
14.6
15.8
UJ
s
1-
17
12
7
23.0
27.5
30.2
2<..0
28.0
29.0
24.1
27.1
27.9
23.3
25.0
29.9
22.6
25.0
29.7
20.8
24.7
28.2
19.9
23.3
27.6
19.6
21.9
27.3
2
29.6
30.5
30.8
32.1
30.6
29.1
28.5
28.5
c
167
162
157
152
147
142
137
132
32
0.7
0.7
0.8
0.8
0.7
0.7
0.7
0.7
X
9
27
22
0.7
0.6
0.7
0.6
0.7
0.6
0.6
0.6
0.7
0.6
0.7
0.7
0.7
0.6
0.7
0.5
tH
17
0.5
O.*
0.6
0.6
0.6
0.7
0.8
0.8
1-
12
0.3
0.4
0.7
0.5
0.4
0.6
0.6
0.5
5
7
0.3
0.5
0.8
0.5
0.3
0.5
0. 7
0.8
2
0.3
0.6
0.6
0.5
0.4
0.4
0.5
0.6
u
167
162
157
1S2
147
142
137
132
32
7.7
7.2
7.3
6.7
7.6
6.9
7.3
7.5
o
27
22
8.5
7.4
8.4
7.0
8.4
7.3
8.2
7.5
7.3
7.2
6.5
6.6
6.9
6.6
7.2
6.5
a
?
17
12
6.3
9.0
6.6
8. 8
6.8
8.0
6.9
7.2
8.3
3.3
7.4
8. I
7.3
8.2
7.2
9.2
§
7
8.2
8.5
6.2
7.4
8.3
7.7
7.8
6.8
2
6.7
6.0
4.0
6.2
6.4
6.0
5.7
5.5
LONGITUDE WEST
Ql SI
167
16 2
157
152
147
142
137
132
32
350.
350.
300.
300.
350.
350.
350.
350.
I
O
z
27
22
361.
418.
361.
418.
361.
418.
409.
418.
361.
418.
361.
369.
361.
418.
361.
461.
-J
17
12
7
466.
543.
539.
506.
508.
465.
422.
375.
318.
422.
468.
465.
422.
508.
539.
373.
424.
465.
3 19.
424.
372.
319.
468.
318.
2
531.
414.
414.
458.
497.
497.
458.
414.
9(8)
167
162
157
152
147
142
137
132
32
113.
112.
97.
104.
122.
123.
121.
118.
I
g
27
111.
122.
103.
118.
101.
106.
120.
114.
112.
113.
110.
98.
111.
117.
118.
129.
1-
_1
17
12
7
115.
88.
95.
120.
98.
94.
102.
78.
63.
103.
98.
80.
106.
107.
97.
99.
95.
104.
90.
109.
101.
96.
133.
102.
2
95.
77.
71.
77.
93.
103.
104.
103.
QUI
167
162
157
152
147
142
137
132
32
129.
100.
117.
120.
173.
136.
154.
140.
I
Z
27
254.
184.
196.
256.
191.
130.
151.
160.
22
227.
174.
170.
223.
186.
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139.
151.
O
1-
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17
12
7
150.
2 79.
165.
156.
197.
255.
168.
155.
101.
155.
169.
70.
298.
271.
167.
237.
274.
225.
213.
340.
2 97.
199.
484.
244.
2
124.
81.
44.
46.
87.
113.
118.
112.
QIC)
167
162
157
152
147
142
137
132
32
4.
1.
-3.
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22.
20.
12.
3.
I
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27
11
14.
21.
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9.
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7
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-12.
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5.
14.
24.
a(Ni
167
162
157
152
147
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137
132
32
106.
139.
90.
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27
22
17
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48.
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78.
109.
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72.
148.
152.
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74.
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289.
121.
-70.
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2
332.
270.
315.
351.
323.
275.
222.
175.
127
MAY 1965
LONGITUDE WEST
TIHt
167
162
157
152
147
142
137
132
32
16.8
17.0
17.6
17.8
18.0
17.7
17.2
15.7
O
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27
22
20.6
23.3
20.6
23.7
21.0
24.0
21.2
23.1
21.0
22.4
20.0
21.7
19.3
21.0
17.9
20.2
s
17
25.2
25.2
25.1
24.1
24.0
23.5
22.5
21.7
1-
12
7
26.0
27.2
26.0
27.3
25.8
27.3
25.4
27.1
25.3
26.7
25.3
26.6
25.2 .
26.8
24.1
27.4
2
' 2 8.1
27.7
27.4
27.1
26.8
26.6
26.6
26.7
TIAl
167
162
157
152
147
142
137
132
32
16.5
17.0
ia.3
18.3
18.5
17.8
16.8
15.5
I
27
20.2
20.7
21.1
21.4
20.8
19.9
19.1
17.4
22
23.1
23.7
23.8
23.0
22.5
22. 1
21.4
19.4
n
17
25.3
26.2
25.2
23.7
23.6
23.0
22.0
21.5
1
12
7
26.0
26.6
26.0
26.7
26.1
26.6
25.3
26.4
25.0
26.3
25.3
26.2
25.1
26.1
24.8
26.5
2
27.6
27.4
27.7
27.2
26.8
26.7
26.6
26.5
E(AI
167
162
157
152
147
142
137
132
32
15.1
16.0
17.5
17.9
17.1
15.6
14.6
13.5
O
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27
22
18.5
23.6
19. 3
24.0
20.2
23.8
21.0
22.3
19.0
21.3
17.3
20.0
16.2
19.1
14.9
16.6
iH
17
27.1
28.9
25.0
23.0
22.9
22.0
20.7
19.4
3
12
7
29.2
30.2
27.8
30.0
27.2
29.4
26.7
29.4
26.0
29.5
25.0
29.7
25.9
30.1
26.1
30.1
2
30.5
30.8
31.0
29.5
29.3
29.2
29.9
31.1
C
167
162
157
152
147
142
137
132
32
0.8
0.7
0.7
0.6
0.6
0.6
0.7
0.9
I
g
27
0.7
0.7
0.6
0.6
0.6
0.7
0.8
0.8
22
0.6
0.6
0.6
0.7
0.7
0.7
0.8
O.B
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17
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0.6
0.6
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0.7
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1-
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12
7
0.7
0.9
0.5
0.7
0.5
0.7
0.5
0.7
0.7
0.9
0.8
0.9
0.7
0.6
0.7
0.8
2
0.4
0.5
0.6
0.6
0.7
0.7
0.6
0.8
H
167
162
157
152
147
142
137
132
32
6.7
7.1
6.7
6.4
6.5
5.9
5.6
5.7
I
27
22
6.7
6.5
7.3
6.4
6.6
6.9
7.2
7.6
7.2
7.6
7.1
7.6
6. 5
7.4
6.8
8.1
8
1-
17
12
5.6
7.1
6.3
8.0
7.3
7.5
8.0
6.7
7.8
8.8
8.1
8.1
8.4
9.2
8.3
8.6
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7
7.1
6.9
6.7
7.5
8.0
7.8
8.2
8.2
2
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4.2
3.8
5.6
5.8
5.8
6.2
6.2
LONGITUDE WEST
OIS)
167
162
157 152 147
142
137
132
32
332.
388.
388. 439. 439.
439.
388.
272.
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27
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2
471.
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393. 393. 348.
348.
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QCBI
167
162
157 152 147
14 2
137
132
32
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109.
97. 110. 113.
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119.
87.
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1
27
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162
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JUNE 1965
LONGITUDE WEST
T(M)
lfc7
162
157
152
147
142
137
132
32
20.0
20.8
21.0
20.9
20.4
19.7
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27
22
23.*
24.8
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24.6
23.4
24.3
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18.7
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1-
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17
12
7
25.5
25.9
27.6
25.4
25.9
27.4
25.0
25.5
26.9
23.8
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26.9
23.0
24.9
27.0
22.2
24.6
26.6
22.0
23.9
27.2
21.5
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26.3
2
28.1
28.1
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157
162
157
152
147
142
137
132
32
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22
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25.5
23.9
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18.0
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1-
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12
7
26.1
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26.2
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26.3
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26.2
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24.7
26.2
22.8
24.6
26.2
22.1
24.6
26.2
21.6
22.7
26.3
2
26.9
26.8
27.0
27.0
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EIAI
167
162
157
152
147
142
137
132
32
20.1
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27
22
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3
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12
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167
162
157
152
147
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137
132
32
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0.7
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27
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0.7
0.8
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M
167
162
157
152
147
142
137
132
32
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7.3
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17
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7.1
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7.1
6.3
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♦ .5
4.8
4.1
4.1
5.2
5.3
6.6
4.5
LONGITUDE WEST
Q(SI
167
162
157
152 147
142
137
132
32
404.
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41 Nl
167
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157
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129
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