4 r, Off
SMITHSONIAN MISCELLANEOUS COLLECTIONS VOLUME
143,NUMBER
5&oefclmg jf unb
A LONG-RANGE TEMPERATURE
FORECAST
By
C. G.
ABBOT
Research Associate, Smithsonian Institution
CITY OF WASHINGTON
PUBLISHED BY THE SMITHSONIAN INSTITUTION
OCTOBER
27, 1961SMITHSONIAN MISCELLANEOUS COLLECTIONS VOLUME
143,NUMBER
5&oetjling jfunb
A LONG-RANGE TEMPERATURE
FORECAST
By
C. G.
ABBOT
Research Associate, Smithsonian Institution
(Publication 4471)
CITY OF WASHINGTON
PUBLISHED BY THE SMITHSONIAN INSTITUTION
OCTOBER
27, 1961PORT CITY PRESS, INC.
BALTIMORE, MD., U. S. A.
3&oe<ng Jftmb
A LONG-RANGE TEMPERATURE FORECAST
By C
G.ABBOT
Research Associate, Smithsonian Institution
GENERAL COMMENTS
I quote the opening paragraph of
my
recent paper"A Long-Range
Forecast of United States Precipitation" x :
"A
hidden family ofharmonic
regular periods exists in weather.The
periodicmembers
of this family persist withunchanged
lengths for scores of years.By
determining their average
forms and
amplitudes for intervals of a thousand months, successful forecastsmay
bemade
for years tocome
;
or backcasts
may
bemade
forformer
yearsand compared
toformer
events.
Agreement
of such backcasts with the records warrants con- fidence in future forecasts."In the publication cited correlation coefficients ranging
between +
52and +69
percentwere found
over the interval 1950-58between
pre- dictionand
observation. Positive coefficients of correlation, as I willshow, also subsist
between
temperature forecastsand
events for thesame
interval.Examples
appear herein as figures 1, 2, 3.While
very nearlynormal weather must
obviously average closer to thenormal
values than tomy
forecasts, the case is quite different for extremes of weather.Extremes
in precipitation rangefrom
50 to200
percentaway from
the normals. It is to be able to anticipate weather of this unusual kind thatgood
forecasts are financially valuable.As an example
I give the following computations basedon
tables 10and
14 of Publication 4390:Cincinnati results from table 10
From
108 months, 1950-58, mean departures from normal,29%
from forecast,
27%
From
56 months within25%
of normal, from forecast,26%
From
52 months over25%
from normal,from forecast,
27%
From
20 months over48%
from normal, from forecast,31%
do.
SMITHSONIAN MISCELLANEOUS COLLECTIONS
VOL. I43no. 5
LONG-RANGE TEMPERATURE FORECAST — ABBOT
SMITHSONIAN MISCELLANEOUS COLLECTIONS
VOL. I43bo
c
u
bo
to
OX «?
<u C
y- «
(U O
*o S
£
a v*°H.ts
3 in O
£
00
& o
U.14-4
V
t/i I/)
O In O
<" !ri
-
C us*oM~'
•- «
<J o :^
.—•—
<
01
"8'-3
tn m
<U
1-. t/>
3 (U
rt 3
u ti
OJ rt
a, «
J3
as
ot—
I
fa
NO. 5
LONG-RANGE TEMPERATURE FORECAST — ABBOT
Fig. 4.
—
Precipitation forecast (dotted lines) and observed (solid lines) from records of 1870- 1956.SMITHSONIAN MISCELLANEOUS COLLECTIONS
VOL. I43From
27 four-month periods, 1950-58,from forecast, 26.6%
From
14 periods within25%
from normal, from forecast, 27.7%From
13 periods over25%
from normal, from forecast,23%
From
6 periods over38%
from normal, from forecast, 27.5%Cincinnati results from table 14
mean departures from normal,
25%
do.
13%
do.
38%
do.
47%
Table 1
—
Forecasts of precipitation 1950-58 and 1959-60. Departures from normal (1950-58) and percent average deviation from mean departuresGroupsofdeviationfromnormal
Station Interval
Abilene 1950-58
i959-6o Augusta 1950-58 1959-60 Bismarck 1950-58 1959-60 Cincinnati 1950-58 1959-60 Denver 1950-58 1959-60
El Paso 1950-58
1959-60 Helena 1950-58 1959-60 Independence .. 1950-58 1959-60 Madison 1950-58 1959-60 Nashville 1950-58 i959-6o Sacramento 1950-58 1959-60 Salisbury 1950-58 1959-60 Santa Fe 1950-58 1959-60
St. Paul 1950-58
1959-60
Mean
1950-58Mean/12 1950-58 A.D./27 1950-58
Mean
i959-6oMean/13 i959-6o A.D./30 i959-6o
0-25
13^25
11
±29
I2±23 io±3i
11
±24
9±24
13^24 i8±i9 I3±33 I3±35 I2±I9 I3±37 I2±2I I2±3613
±26
I3±i8 13^27 I3±37 I2±23 ii±i6
1 1
±47
I4±53 I2±24 I7±i5
1 1
±37
I7±33
1 1
±29
1 1
±32
I2±27
I I
i3±30
1 1
26-50
36±39
37±25 37±3634±38
34±3i 36±3i39±30
39±3539±34
38±38 40±43 34±55 35±3i 37±3338±30
35±36 39±32 35±2537—26
37±43 37±67 33±3i 33±i7 39±45 35±4i35±44
30±28 37±363 1-3 36
±36
3 1.2
51-75 61
±34
58±6o 58±5i66±57
56±44 64±48
6i±30
6o±3765
±32
65±73 58±40 59±49 59±42 63±37 64±2862±52 59±56
6o±36 6i±i9
6i±5777±69
62
±43
5 1.6 61
±47
5 1.6
76-100 >IO0 84±2i
8i±70
97±44
8o±i7
90±5i ii2±97 82±2I
8i±45
63±30 ioo±42
86:
7 142
8o±5i io8±55
8i±54
I35±i031.6
%
above75n8±8s
10 3-0
87±89
7 3-0
no. 5
LONG-RANGE TEMPERATURE FORECAST — ABBOT
Fig. 5.
—
Normal temperatures, sunspots few minus sunspots many.In table 1 I
compare
an analysis for 14 stations over the intervalI950_58 with an analysis for the
same
stations for the interval 1959-60.The mean
results forthetwo
intervals arealmost identical.They show
that forecasts three years after the last
month (November
1956) usedin their basis are just as
good
as earlier forecasts. Further support for this thesis will be foundby
inspection of figure 4.These
resultsshow
about asgood agreement
of forecasts with ob- served precipitation forextreme
departures as for usual departures.8 SMITHSONIAN MISCELLANEOUS COLLECTIONS
VOL. I43This
recommends my
forecasts to thosewhose
interestsdemand
fore-knowledge
ofwide
departuresfrom
the normal.A
second recom-mendation
arisesfrom
the fact,which may
be verifiedby
inspection of figures 1, 2, 10,and n
of Publication 4390, that large trends in de- parturesfrom normal
precipitation, continuing over several years,may
be tolerably forecasted. Third, as far as time has elapsed, results remain encouraging. In figure 4and
table 1 I give evidence that dur- ing the24 months
of 1959and
i960, three years afterNovember
1956,(the latest record used in the forecast) a strong correlation (about 50 percent)
between
forecastand
eventwas
observed.In preparing temperature forecasts or precipitation forecasts, as explained in
my
paper"A Long-Range
Forecast ofUnited
States Precipitation," it is necessary tocompute new monthly
normalsfrom
the published records.
These new
normals relate respectively to the yearswhen
theWolf
sunspotnumbers
are greater,and
to the yearswhen
they are less than 20.To
illustrate the need for taking account of sunspot frequency innormals of weather records,
and
toshow
interesting features of the differencebetween
stations in their relations to sunspot frequency, Igive figure 5. It
shows
the difference in percentage ofnormal
temper- aturebetween
times of sunspots lessand more
than20 Wolf numbers
for the 12
months
of the year.There
is a partial similarityamong
the graphs, but SaltLake
Cityand Los
Angeles behave rather differ- entlyfrom
the other eight. It will be noted that ranges of 2° oreven
3 F. occur forsome
cities,which
are ignored in usualmonthly
nor- malswhere
sunspot frequency is neglected.The
following datesmay
be used to separateSS > 20 and SS < 20
groups of
months:
Table 2.
—
Intervals of high and lozvsunspot numbers2
SS>20
July
NO. 5
LONG-RANGE TEMPERATURE FORECAST — ABBOT 9
In the use of tables of periods in weather for forecasting
beyond
1957, it is necessary tomake
extrapolationsfrom
the preceding tables of dates. This isdone
(of course with marginal uncertainty)by
aver- aging the intervals (given above) inmonths SS>20 and SS<20, and assuming
that future intervals will be approximately thesame
as these averages.The
uncertainty will usually not lead to important errors of forecasts, for generally the curves representingSS > 20
and SS < 20
for the periods are similar for a given periodand
differ but afew
months, or even not at all, in phases. I use for future dates:
for
SS >
20,84
months, forSS <
20, 52 months.To
avoid being misledby sudden
largejumps between
consecutivemonthly
departures, the departuresfrom
thesenew
normals aresmoothed by 3-month
consecutive means.Owing
to unpredictable lags in the phases of theharmonic
periods, it is necessary, as explained in the paper just cited, to divide the record data into special groups, de- pendingon
the time of the year, the prevalence of sunspots,and
the secularmarch
of time. This requires that220
tables should becom-
puted for the forecast of temperature at each station, just as in the precipitation forecasts of Publication 4390.This large task requires electronic computation. It
was done
for the 10 temperature stationsand
for the 32 precipitation stationsby
JonathanWexler
ofTempe,
Ariz. In order to avoidnew
procedure inprogramming
the electroniccomputer
for temperature, I directedhim
to convert recorded temperatures, published in Fahrenheit de- grees, into absolute temperatures Fahrenheitby
adding 491.7
minus
32 , or 459-7°. Departuresfrom
themonthly
normalswere
thencomputed
in percentages, aswas done
with the precipitation values.For
instance, thenormal
temperature forJune
at Detroit for years of sunspots greater than 20Wolf numbers
is 67.8 F. Subtracting 32and
adding 491.7
it
becomes
527.5° abs. F.The
observed tempera- ture of Detroit forJune
1950was
68.1° F. Similar stepsmake
it527.8 abs. F. Its ratio to
normal June
temperature is 527.8-=-527.5=
1.0006. All this rearranging
was done
with the electroniccom-
puter. In the subsequent computations
we
used the differencesfrom
1.
0000
as far as the fourth decimal place.These
differences ranged for themost
partbetween +150 and —80,
corresponding to a range of 2.3 percent of the absolute temperature, or about 11.5° F.Readers
interested in further details of themethod
are referred tomy
paper"A Long-Range
Forecast ofUnited
States Precipitation"(Publication 4390)
and
other references cited therein.Temperature
forecasts are
somewhat
less satisfactory than the precipitation fore- casts.For
while the range of percentages ofnormal
precipitation goesIO
SMITHSONIAN MISCELLANEOUS COLLECTIONS
VOL. I43from
to 1,000 or more, the entire range of absolute temperature isonly about 2.3 percent.
The
accidental fluctuations of temperature bear amuch
larger proportion to range than the accidental fluctuations of precipitation. Hence, correlation coefficientsbetween
forecastedand
observed temperature,though
always positive, are always smaller than thosebetween
forecastedand
observed precipitation.While
the 32 cities forecasted for precipitation, 1950 to 1958, all yielded positive correlation coefficients with the events rangingbetween
50and
70percent, the correlations
on
temperature for 10 cities, forecasted 1950to 1958, ran as follows: Detroit
+16
percent;Los Angeles +22
percent; Atlanta
+32
percent;and
the other 7 stations all rangedbetween +40 and +50
percent.My
forecasts of temperatureand
precipitation reston
one factand
one assumption.The
fact is that aharmonic
family of regular periods exists in solar radiationand
in weather.The
assumption is that if this family of periods is individuallyand
quantitatively determinedfrom
weather records, 1870 to 1956, themean
course of these periods willbe followedapproximatelythrough subsequent years. This assumption
may
indeed provewrong when
unusual disturbances occur in atmos- pheric conditions—
for example, the volcanoes ofKrakatoa and
Katmai
; the furiousbombing
during theworld wars
; atomicbomb
tests; the hurricane
Donna
ofSeptember
i960.But
tests such as figures 1, 2, 3, 10, 11 of Publication 4390,and
those of temperaturein this paper,
show
that generally the assumption is justified.As
yetit has not been explained
why
displacementsbetween
forecastsand
events in features of weatherby
1, 2, or 3months
occasionally are observed. If this difficulty can be overcome,much
higher coefficients of correlation will befound between
forecastsand
events. I planan
investigation of possible causes of this defect.
There
is one important differencebetween my
forecasts of precipi- tationand
of temperature.The
amplitude of the principal features in precipitation changeswas found
for all stations to be so nearly thesame
in forecastsand
events thatno
adjustmentswere made. Not
so with temperature.For
all the 10 cities the amplitudes of the features of changewere
obviously greater in the forecasts than in the events.I cannot explain
why
this is so.The
forecastswould
have been leftwoefully
wrong
unless this discrepancyhad
been corrected.To make
this correction for scale, I carefully plotted for each city the curves of forecastand
eventfrom
1950 through 1958.Then
Imeasured
as best I could the depths of obviously corresponding large depressions of thetwo
curves,and
determined their average ratio of amplitudes in forecastsand
observations for about a half dozen prin-NO. 5
LONG-RANGE TEMPERATURE FORECAST — ABBOT
IIcipal depressions.
These
ratios, in terms of event divided by forecast,were
formost
cities between 0.70and
0.75.Using
these average ratios of amplitude of features, I reduced all the forecasts to approximately thesame
scale of amplitude as the events.There
remained still another correction, but one not puzzling like that for scale.As many
have pointed out, temperatures have gradu-ally risen in parts of the United States for a great
many
years. Itwould
have been quitewrong
tomake
forecasts of temperature for 1950 through 1967 without allowing for this well-established change of level.Hence
I took the ratio of thesum
ofmonthly
departuresfrom normal
after correcting for scale, as forecastedfrom
1950 through 1959,and
divided by the correspondingsum
for the event.This gave a correction to lift the forecasts bodily
by amounts
rangingfrom
0.11 to 0.37 percent for the different cities.Expressed
in de- grees of temperature, these corrections of level rangefrom
0.5 to1.
9
F.
Having by
thesetwo
necessary corrections adjusted the forecasts to terms justly comparable with the events, Icomputed
the correlation coefficients mentioned above.RESULTS OF THE INVESTIGATION
First of all, to inspire confidence in the method, which, as I
have
said, is substantially the
same
for temperature as for precipitation, Igive in figure 4 for 14 of the 32 stations of Publication
4390
acom-
parison of forecastsand
eventson
precipitation for the 24months
of 1959and
i960. This interval is several yearsbeyond
the latest month,November
1956, used in the basis of the forecasts. Table 1, above, gives for 1959and
i960 an analysis of themonthly
values of forecastsand
events in percentage departuresfrom
thenormal monthly
pre- cipitation to befound
incolumn
B, table 9, of Publication 4390.Twelve
other precipitation stations gave almost asgood
correlation as these fourteen stations, except thatmore
cases of displacement of features by one, two, or threemonths
occurred between forecastsand
events.
Such
displacements, frequently noted inmy
former papers, are as yet impossible to forecast. This is themain
defect ofmy
fore- casts. It is true that the amplitudes of features frequently differ be-tween
forecastsand
events, but if themain
features occur zvhen pre- dicted, the moderate difference of amplitudes is not a very serious de-fect. If one could predict
when
phases of prominent featureswould
be displaced, the correlation between forecastsand
events in precipita- tionwould
risefrom
being40
to 70 percent to liebetween
70and 90
percent.
12
SMITHSONIAN MISCELLANEOUS COLLECTIONS
VOL. I43I have
computed
the correlation coefficient in precipitationbetween
forecasts
and
events, 1959 through i960,combining
the results re- ferred to in table 1 for 14 stations. Just as themean
temperatures for the decade 1950 toi960
differ generallybetween
0.5and
2.0 F.from
those of themean
values1870
to 1956, so, too, themean
values of precipitation 1950to 1961 differfrom
themean
values 1870to 1956.Before
computing
the general correlation coefficients, 1950-58and
1959-60, for the 14 stations, I have corrected these differences of levelby
lifting or lowering the forecasts bodily.These
differences rangefrom
zero to 17 percentamong
the 14 stations. This done, the general correlation coefficientbetween
forecastsand
events for the 336months
during1959 and
i960 available at the time ofcomputing from
of-ficial records resulted as
+47.0
percent.I
am
notaware
thatanyone
has ever before predicted themonthly
precipitation at 14 definite cities over 2 years of time (in
my
case1959-1960)
and
has achieved a correlation coefficient as high as+47
percent for
24
months, 3 years after the lastmonth
used in the basis of his forecast. Itseems
tome
that thismarks
an importantand
en- couraging advance in long-range forecasting.Figure
4 shows
graphically the results tabulated in table I. I call attention to cases of displacements of obviouslycommon
features in forecastsand
events that occurred,and remark
that such displace-ments must
obviouslyhave
pulleddown
the value of the correlation coefficient which, notwithstanding, reached+47
percent.These
casesare: Cincinnati, 3
months May 1959—
April i960; El Paso, 2months
aboutJune
i960; Helena, 2months
about October 1959and
2months
aboutSeptember
i960; Sacramento, 2months
aboutJanuary
i960.NUMERICAL TABULATIONS
I
was
assisted in these tabulationsby Mrs. Lena
Hilland Mrs.
Isobel
Windom. Miss M. A.
Neill assisted in reading proof.With
the electronic computer, Jonathan
Wexler
furnished3-month means
of absolute temperatures, covering the years 1870 through 1956.
We
continued
them
through 1959. Subtracting 459.7 ,we
expressedthem
in ordinary Fahrenheit degrees.
There were two
sets ofmonthly normals computed
covering 1870 through 1956:A
for the yearswhen Wolf
sunspotnumbers were
less than 20,B
for the yearswhen Wolf
sunspot
numbers
exceeded 20.The
dates included in thesetwo
cate-gories are given in table 2
and accompanying
quotationfrom
the journal "Solar Energy."Table 3 gives these
two
sets ofnormal
temperatures in both absoluteand
ordinary Fahrenheit, applying to the years 1870 through 1956.no. 5
LONG-RANGE TEMPERATURE FORECAST — ABBOT
13 Table 3.- -Normal monthly temperatures from records 1870-1956absolute and usual Fahrenheit
14
SMITHSONIAN MISCELLANEOUS COLLECTIONS
VOL. I43 Table 3—
continued Category
A
Wolf sunspot numbers
<
20Category
B
Wolf sunspot numbers
>
20NO. 5
LONG-RANGE TEMPERATURE FORECAST — ABBOT
15
were
representative, not of absolute Fahrenheit degrees of tempera-ture, but of percentages of the normals
A and B
of table 3.One
might regard
them
as flowing functions,i+X and i+Y,
times thenormal
temperaturesA and
B,where X and Y
are flowing variables,each ranging
from —80
to+150
ten-thousandths.Taking
themean 1+ X and
themean i+Y,
used as multipliers of the normalsA and
B, these normals could be transferred intonew
normals suited to the atmospheric conditions prevailing
from
1950 through 1959.By
assumption thesenew
normalswere
usable in the forecastsfrom
i960 through 1967. But, as stated above, itwas found
that neither in scale nor in level did the
new
normalsfrom X
agreewith the
new
normalsfrom Y. To make
the2
values fairlycompa-
rable with the
Obs
values, a scale correction to2 was
first determined.This
was done
as stated aboveby
plotting2 and Obs from
1950 through 1959,and
obtaining themean
ratio of amplitudes ofsome
half-dozen principal obviously
common
features of thetwo
curves.After this adjustment of scale a level correction to
2 was
computed.This
was
the ratio of thesums
of scale-corrected2
to theunchanged Obs
for the years 1950 through 1959.Applying
it, thetwo
variablesbecame
justly comparable.As
thus reconciled, thenew
finalnormal
absolute temperatureswere
tabulated,and
then theywere
reduced to ordinary Fahrenheit by subtracting 459.7 . In thisform
thenew
normals,
which
areassumed
to be suited to the atmospheric conditions 1950 through 1967, are given in table 4.Subtracting the
new
normalsfrom
thetwo
reconciledcolumns
of2 and Obs we
obtained themonthly march
ofObs from
1950 through 1959,and
that of2 from
1950 through 1967.The march 2
after i960 represents the forecast of chief interest.But
the comparativemarches
of2 and Obs
1950 through 1959 gives the evidenceon which
ajudgment
of the probable value of the forecast i960 through 1967 principally depends.For
convenient general views of the predictedmarch
of tempera-ture, I give in table 6
4-month mean
values of the forecasted de- parturesfrom normal
1950 through 1967, together with4-month means
of the observed departuresfrom normal
1950 through 1959.From
a comparison of these 10 years ajudgment may
beformed
of theworth
of the forecast after 1959.As
further evidence of the value of the forecast I give in table 7 the average discrepancybetween
forecastand
event 1950 through 1959and
the average algebraicmean
difference toshow
that the corrections for scaleand
levelcombined
closely reconciled forecastand
event.i6
SMITHSONIAN MISCELLANEOUS COLLECTIONS
VOL. I43o
b
V,
rf rf qv l>00
"to ii
d
o wco co rf tovo
O CO O In. rf tN.vq
vd
4
00 00 vd vdIn. tN. In.vo to rf co
o\ q\00 vq 00 vq in. o\vq 10 IN.
*£ co co d m cvi m vo rf06 00 in.vd co co rf
m
vo tv.tN.txvO to rf coO.
no. 5
LONG-RANGE TEMPERATURE FORECAST — ABBOT
17On
©
.si
o
O,
s
is
8e
s© a
I
8
ft, o
n km n a«\o m
oivon
-i<5 cm'
ocm n'ddwdddd
cm'° +111 ++++++
I I."g O
m
CMi8
SMITHSONIAN MISCELLANEOUS COLLECTIONS
VOL. I43o
•<
cidcidfitiiH'flMMci
° + ++++++ 111 +
00 00 00 q q t> N *>
T
*> ^^ + + + + + + + 111 +
5 {?'« 0) M M O M
n ^
to o m q\ qfi n d m h d n
I I
+ + + + +
oOio ,
q
i-;qf
,o>-<iooNo\
YoOw>-<dd'-<oiwcj'-<d6
++++ ++++++
ITf\q O}
n
>t 10 m000 *
10^
toto>-'dddddd>-<oi>-<
+ + + +
I I I+ + + + lOMtONtOONiflNWoO}
oioidddi-Ic^Mi-idi-Hi-H
+ + + +
I I I I I+ + +
U
rt60
<
C o1-1
fc
(OM'ddHtiHfiHddd
I I I
+ + + + + + +
I IO M
I I
*> w. •"! 'I" *7 M. "? <? °.
ddod>-ii-<oo)i-i II +
I++
I I Io
.,_,,,• tN N tJ-00 N
m\0 N
't^O 00 C\SS-SoddoMciwdddHJo
S
f2++
I I I I I I I I I Iq uioq n
*
^q *^ °Q to <o00 <•?ddddd>-iwddi-
|MM'
+
I I+ + + +
I I I Io
IN fo 0\ N N ^O M m N to00 M,
di-ioi-i>-iodocooo + +
I I I+ + +
I++
I
noo odO
m q|_l|*q-|,q q-|,H'dd
in. >-; vq \o|-"'oioi•-;+ + II
I I I I+ + + +
*.£ *r
^<
MO00 *
N M (O >t 10 h CO MddoHNTtifiN'oddto
I I I
+ + + +
I I+ + + + +
I+ + + +
I I+ +
rt
t>«Ja n <o 00 w "?oq 19 m q\ to in. to
o « rt _ m m w d m' co ci m >-«" d d
.**+ + + +
I I I I I I I+
1^
vototo^qqiqiio 000 n
h"3 h
d
d d to h hd
"t iri'd «° +111 + + +
I I I I Ih 10 to in O w "t N
T3
o
£ to m d d w' to oi°S ++
I I+ + +
to 10
N
10•4- -4 d
I
+
I I
.O
rt 3H*»-tOO»-< ,-H
OOO'-^HHHH
°
h ++
I I+++ + + + +
o
•«3- w \q i>oq to 10
noo
q t> to't to n' m' h to oi h d fi H M
++++++++++++
ocoTj-c\q
4
q qoq <*? "?q
|-; q*, 4">-<d>-,
°ddd
|-<>-<to>-<+++
I++++++
M <0 In. In00 to
N *
1> h Tf-O
d>n'd'-ifv
itoi-ii-iooi-<d
I
+
I I I I I I+
I+ +
tj-i-h
a
to h toto^qtoqo
wh h o to
4
10 to M m' to 6 M+
I
+++++++++
Io
kk
on
ton
q 00 to 10 q> qd •-< d d d d d m
+ + + + +
I I I I Inoo t>0
cq \q to -tvq"?"?«
d <n ni
^
^r to oi c4 to i-i dI
+
I I I I I I I I I+
no. 5
LONG-RANGE TEMPERATURE FORECAST — ABBOT
19vq is.vo in
n
h w ro - in ts cjddoHii-i'cocooirooii-ii-i
+
I 1 I IM
I I I I I0OhicO00>~iC5i-<>-(Ohi0J^O
I
+ + + + + + + +
I I Im' m « m oi i-i oi 6 h!
+ + +
I I I I III
Iot 00 00 q o» 00 m in c\ q\ r> <?
wdcSwdwi-JoidcJNro
I I
+++++++
I I IO M CO CUVO C\M 01 rn
O N t
NfiiiddoMO
oi oi w d+++++++++++
IC\ c\ in00
o m
o«
>-i 00 intoddddddoii-i'Hi'ddd
I I I I I I I I I I I
+
q 00 vq 00
d
>n h ma n
h 00d d 6 n «' to oi 6 6 hi m
I I I I
+ + +
I I I If
n vq cn m h< vq q\ r> >-> »n00>-idH<ddd>-ioiHidoii-i
I I
+ + + + + + + +
I IKNOW
0] ^t CO f<? 01 ^00 Ol-HOhHl-HO^HHOIOOOl-l
+ + +
I I+ + + + +
I ITt-qvN m oq
^
fo h in.*
t> q-' d d d d hi d h! d d oi oi
I I
++
I I I++
I I Ifs upvq vq IN. m co N h cq ro ro
(-ihhmhiO^«h-(OhhOOO
+ + + + +
I I+ + + + +
q t>
*
00 q\ 19 q\00 q "? « NdoHidoHlwH<Hic5dd
I I I I I I I I I
II
MOOHONvqininoopo
ddddn<'«j--<Tinroi-Hi-<d
+
I I I I I I I I+ +
100
c* <*? r> o in q\ »-; ^J" vq ^j-+ + + + + + + + +
I I IOn VO In. 01
m
11 m ro PO fO w rfoiHiNwdNOHidddd
+ + +
I I I+
I I+
I I(o q "p^q q* "? •>
q
*> 't ^q q^'t'dnNticifiHOHpi + + + + + + + + +
I I I 13Hjmt-^win'-jtv.^JNHii-if*}
«' n n h ci
4 4
ci«
h.' m+ + +
I+ + + + + +
I I00 q
o n
p| 10 q o vq q o vqOwi—iO'-i>-
,01>-iOOOO + + +
I+ + + + +
I>-< 1-1 -< in
m
oi h< oio «
irnohi w d w oi n ti m n fi
n
oi+
I I I I I I I I I I Iq oi tj- m oa
n
w rovqvq rovqf
,
ooo^l-lOO
MHHcioo
,-'1
+ + + + +
1++
1 1 1oi m tj-00 00 to oi cc q\ ro00 vq
dHfiddHNtofioHM
+ + +
I I I+ + + +
I Iojoq 1s.r9tv.iv.HH oq oi OvOvh.
hi' d oi c6 d d hi' d d d ni oi
I
+ + + +
I I++
I I Iq\o>
ioKKO\toiri«M3
is. odcipidHd'T'jinNHd
I
+ + + + + + + + + +
oqvqtoojinqHiinTj-fcvqin
Hi'ddoidHidoddHio + + + + +
I+
I I I I I00 q in <o in00 of1 vq q t> oi is.
HiHid'i'roi-iddHidHii-;
+ +
I I I I I+ + + + +
q\ 01 00 q io
a
^t h in q> qw
h ci ii m' d n n d d oi oi
+ + + + +
I I I+ + + + qnOHinqwO'tN'tci
>-ioirodddoi<r}oii-ii-id
+++
I+ ++++++
°°.
^
q^*
<9 o» q^t-vq rj-rt-oqd d >-i oi i-i' 6 d d d d d d
+ + +
I+
I I+ + +
I Iom
ro^ot
qoq coTj-M-q oi 00d i-i ^r t}- -rt- hi n (j h h d d
+++++++++++
Imoo c\ <*• q
n
10 iri h u? Tt f*?
MMM^MNMOdONfi
I I I I
+ + + + +
I I I5? c >? **> S.
~
>* S.C
>» 5P Q- *S £ "«
^fe S < ^ ££< $ O ^ Q 2£fn 3 < S 3,£< $ 0£ Q
20 SMITHSONIAN MISCELLANEOUS COLLECTIONS
VOL. 143o
5
feCO Ov ON m
OO
'*>-' ifOOO
ONto m oi Tt cvi oi 6 m" d
I I I I I I
+
I+
I+ +
<N 1-1
I I
t^ IO -Tf
6 (i n
ort a N
CO IN vO
'^+ + + +
O
c4
I I I I I I I
t
Oio o
I
+
IN « N
fOi-I 1-1 d
+ +
M M d m d
+ +
Iqvvq Tf q\ h vq N On00 vq vo N
O M M O TJ" IT) CO "<* N M* I-i M
I I
+ + + + + + + + + +
o
m
ujoq 00iow
co<o «*i w 1-1 oid
6N
M (J (i H M O M (i N++++++++
I+++
ow. "! r
T <-^vO "} Oi '"P ^ 10
m
oMtiMdHNMripiHd"
+ + + +
| I I I I I+ +
U
"<u- to
<
aV}
O
r^
tg
91'
c! l?9't
? h! H.
*
fOi-ii-*i,
*i-itOi-i<Ndd
I I I
+ + + + + + +
o
r>» to >-; "? **" "J •-; i-< poo
oi i-i oi d d d d m >-i oi
I I I I I
+ + + + +
vie i; to o m
^
n! O1-1 Ov O »)
- d fi m
Oi
N
O OiO
o* 1—« 1—J c5 1—
1
I I I
+ +
in00 (i nj inio «
«
in ro ^f\q i«) indo
c4r|itnroc*idi-*Mdi-'di-*
II
I I I I I+ + + 111 +
r>
o MNO'finN'<t'N'l
,NNin
>-« d
dddddddd^fidd
+ + +
III ++1111 +
o
cvj «
Nnti^HOHHHdd"
+ + ++ + + +
I I I I I I ISs
<5 Vj
in
w
ijM
<
a
11
O
1ro o\ o\ o
oi en to m"
in 10 Oi
n
inoo too d i-i d cvi 1-1
1
+
I+ + + +
r? t, d d -< >n « m d ci d d ei
°S
I I I I I I I I I I+
I.O
», en,5
•••••••-
*«*+•+ + + +
I I I I IO in
d m
O
iv,
M^qiOHMM'qqiH'fqi
ri<
di-ii-idi-'ddddi-fi-ifo
° III +I+I+I++
.<u i-ivoi-itnwio'^cjoji-irs.ov
o
£ddi-Jdddddd
i-icn'M*S
+++++++
I+
I++
l>
%£
o\ o o to q vq w Tt-tN.q rn qo«ndoirodi-idddddi-<i-i
^°
fe+ + + +
I+ + +
I+
Iqv tovq -^ vq "? n n r!" Tt c?
oi d oi w m d m m d o» en cvi
+
I+ + + + + + + + + +
00 "? «? *? w ci q vq q *?
^
^f^-^oo^oo
,-, *-, •~'oi^-^o•-,+ + + +
I I I I I I+ +
>-; 00
m nvq
00 *? co n*>9
o\m m i-i w" oi pi to to
I
+
I I I I I I I I I Ivq is
too
"* o 1900 q ojq
qtoddinintodi-itoindcvi
+ + + + + + +
I I I+ +
vq rj-vq cm rf
m
tooo 03m
n inndfiN'dddddtHH
+
I I+ + +
I+
I I+ +
°. *"i °^ ^T 9 "?°°.
^
n. is tn inOMfi'ninM'dN'Nddd
I I I I I I
+ + + +
I^2
N
•d
• V
OS
(n
n
h qn
hinmoj
q cmvooi m m oj n' pi o m* d o* <n **
+++++++ II +|
q\ w Tf w oj rt-cq n vq >-< tj- oj
ddd"NfiN«'«HMd
I I I
+ + + + + + + + +
^^in <) in
q
h <n<nts.oqwoooq
oUalinHOOHfiioNHOM
h «h
I II
+ + + + +
I+
I I I I
cni-11-imi-itNini-irs.tNcnq
i-i d oi ro i-i w in >*• in oi w
+ + +
I I+
I I I I I In n
tnvq vq Tt-r>.Ti-vqq n q M'dd<ncnddi-ii-ifni-id
+ +
I I I++
I I I I Io
qvq
tj- to inoq oj t>i-< fovq mi-iddi-iddcviroroi-idi-i
+ +
IIII + + + + + +
> d