SMITHSONIAN. MISCELLANEOUS COLLECTIONS
VOLUME
114
(WHOLE VOLUME)
SMITHSONIAN
METEOROLOGICAL TABLES
SIXTH REVISED EDITION
Prepared by
ROBERT
Meteorologist, U. S.
J.
LIST
Weather Bureau
SMITHSONIAN INSTITUTION PRESS
CITY OF WASHINGTON
Smithsonian Publication 4014
Sixth revised edition published 1949
Fourth reprint issued 1968
NOV
1
6 2000
n
PREFACE
The
two
and con-
rapid development of .the science of meteorology during the past
made necessary a complete
decades has
revision of both the scope
tents of the Smithsonian Meteorological Tables.
A. Wetmore, Secretary of
the Smithsonian Institution, which has been publishing these tables since
1852, and F.
A
need.
this
sisting of
W.
Weather Bureau, recognized
Weather Bureau meteorologists, con-
Reichelderfer, Chief of the
steering committee of
H. Wexler, Chairman, R. A. Allen,
R. N. Culnan, R. D. Fletcher,
J.
J.
E. Caskey,
Jr.,
P. F. Clapp,
R. Fulks, C. Harmantas, L. P. Harrison,
McGuire, J. Namias, and H. W. Norton, was formed to
make recommendations concerning the new revision and to serve in an
advisory capacity. Funds for the preparation of the manuscript were transferred by the Weather Bureau to the Smithsonian Institution, and under the
W.
C. Jacobs, J. K.
supervision of L. B. Aldrich, Director of the Astrophysical Observatory,
work on
the
new manuscript was
started.
It is a
pleasure to acknowledge
both the administrative cooperation and scientific information received from
Mr. Aldrich.
In preparing this volume, every effort has been made to obtain the latest
and most authoritative data available, and to follow as far as possible the
most recent recommendations of the International Meteorological Organization. Suggestions were also solicited from the various branches of the armed
forces concerned with meteorological problems, from the several universities
having meteorology departments, and from other interested individuals and
organizations. Explanations, sources of data, methods of computation, and
pertinent references accompany all tables. No material on meteorological
codes and symbols, descriptions of meteorological stations, or climatological
data have been included in this revision.
It
would be impossible
to
acknowledge
all
received in the preparation of this volume.
the cooperation and assistance
A
particularly large debt of
owed to L. P. Harrison, Chief of the Technical Investigations
Section of the Weather Bureau, who has unhesitatingly given so much of
his time and attention to this project, and without whose mature judgment
it would have been impossible to complete this work in its present form.
gratitude
is
Grateful acknowledgments are also due to
Towne
all
J.
Scientific School of the University of
A. Goff and
S.
Gratch of the
Pennsylvania for contributing
the material for tables 84-92 and for furnishing the computations for
table 72
;
to S. Fritz of the
the section on radiation
;
to
Weather Bureau for his assistance in preparing
W. D. Lambert and J. A. Duerksen of the Coast
and Geodetic Survey for information concerning gravity and other geodetic
PREFACE
iv
problems
;
to E.
W. Woolard
of the Nautical
Almanac
Office of the
Naval
Observatory for astronomical and related data; and to the many experts
consulted at the National Bureau of Standards. Computations for several of
the longer tables were made by the Machine Tabulation Unit of the Weather
Bureau. Special data or computations for individual tables were furnished
by R. Gunn, I. F. Hand, W. E. Howell, L. D. Kaplan, J. B. Leighly, T. H.
MacDonald, and R. B. Montgomery, all of which have added greatly to the
value of this volume. Permission to reproduce copyrighted material has been
Company, Inc., the McGraw-Hill
and the Reinhold Publishing Cor-
kindly granted by the American Air Filter
Book Company,
Inc., Prentice-Hall, Inc.,
is acknowledged at its point of insertion in the text.
due Mrs. G. B. Morgan for her invaluable assistance in performing many of the computations and in typing the manuscript.
Robert J. List
Washington, D. C.
poration
;
such material
all
Thanks are
also
September
30, 1949.
NOTE TO FIRST REPRINT
Opportunity has been taken in
this
few errors that have been
reprint to correct the
discovered in these tables since the original printing.
Editor.
February 1958
NOTE TO SECOND REPRINT
This reprint corrects three or four errors discovered
in
these tables
since the
first
reprinting.
Editor.
March 1963
NOTE TO THIRD REPRINT
This reprint
is
without change in the text, since no errors have been brought to our
attention since the second reprinting.
Editor.
April 1966
CONTENTS
Page
Preface
iii
Introduction
1
Conversion of units of length and mass
1
Standard gravity for reducing barometric observations
3
Calorie
4
Section
CONVERSION TABLES
I.
Table
9
1.
Conversion factors
2.
Approximate absolute, centigrade, Fahrenheit, and Reaumur tem-
3.
Fahrenheit to centigrade
perature scales
17
.
.
.
20
,,
4.
Centigrade to Fahrenheit
25
5.
Differences Fahrenheit to differences centigrade
6.
Differences centigrade to differences Fahrenheit
29
29
7.
Centigrade degrees per kilometer to Fahrenheit degrees per 1000
8.
Fahrenheit degrees per 1000 feet to centigrade degrees per kilo-
9.
Inches of mercury to millibars
31
10.
Millibars to inches of mercury
38
11.
Millimeters of mercury to millibars
51
12.
Millibars to millimeters of
mercury
59
13.
Inches to millimeters
14.
Millimeters to inches
79
15.
Feet to meters
16.
Meters to feet
92
94
30
feet
meter
30
72
17.
Statute miles to kilometers
18.
Kilometers to statute miles
96
98
19.
Nautical miles to statute miles
100
20.
Statute miles to nautical miles
100
21.
Nautical miles to kilometers
101
22.
Kilometers to nautical miles
101
23.
Days
24.
Time
25.
Hours, minutes, and seconds to decimals of a day
Decimals of a day to hours, minutes, and seconds
Minutes and seconds to decimals of an hour
26.
27.
to decimals of a year
and angle
to arc
102
106
v
106
107
107
smithsonian meteorological tables
vj
Page
Table
28.
29.
Grains to
31.
Grams
32.
Miles per hour
34.
35.
108
109
grams
30.
33.
108
Avoirdupois pounds and ounces to kilograms
Kilograms to avoirdupois pounds and ounces
109
to grains
to knots,
meters per second, feet per second, kilo-
1 10
meters per hour, feet per minute
Meters per second to miles per hour, feet per second, kilometers per
112
hour, knots, feet per minute
Kilometers per hour to knots, miles per hour, meters per second,
113
feet per second
Knots to miles per hour, meters per second,
meters per hour, feet per minute
Section
II.
feet per second, kilo-
115
WIND AND DYNAMICAL TABLES
119
36.
Beaufort wind scale
37.
Geostrophic wind,
38.
Geostrophic wind, constant pressure surface
39.
Geostrophic wind, constant level surface:
constant
pressure
100 geopotential
surface:
120
meter contours
:
200 geopotential foot
122
contours
air density
1
kg. m.~ 3
isobars,
124
,
126
40.
Gradient wind
41.
Coriolis parameter
42.
Inertial
43.
Rossby's long-wave formula
and
130
latitudinal variation
motion
Section
44.
Three millibar
III.
130
131
BAROMETRIC AND HYPSOMETRIC TABLES
Capillary correction for mercurial barometers
45-46.
135
Reduction of the mercury column to standard temperature (explanation)
136
45.
Reduction of the mercury column to standard temperature, English
46.
Reduction of the mercury column to standard temperature, metric
47.
Corrections to reduce barometric readings to standard gravity
48.
Determination of height by the barometer and reduction of pressure
units
139
units
164
to fixed levels
Section IV.
49-51.
203
GEOPOTENTIAL AND AEROLOGICAL TABLES
Relation between geopotential and geometric height
tion)
200
(explana-
217
CONTENTS
Vll
Page
Table
49.
Factors for computing the relation between geopotential and geo-
50.
Geometric meters to geopotential meters
51.
Geopotential meters to geometric meters
52.
Geopotential computations
219
metric height
53-56.
220
222
224
Thickness and mean adjusted virtual temperature of strata be241
tween standard isobaric surfaces (explanation)
53.
Thickness
in geopotential
meters of strata between standard isobaric
surfaces as a function of
54.
Thickness
Mean
56.
Mean
virtual temperature.
.
mean adjusted
virtual temperature.
.
254
adjusted virtual temperature between standard isobaric sur-
255
faces as a function of thickness in geopotential feet
Relation between pressure change and geopotential change (ex-
256
planation)
57.
Change
58.
Change
59.
Change
60.
Change
61.
Change
62.
Change
in height (geopotential meters) corresponding to
change
1
millibar
257
in pressure
in height
change
(geopotential feet) corresponding to
millibar
1
258
in pressure
in height (geopotential feet)
corresponding to a change in
pressure of one-tenth of an inch of mercury
in pressure (millibars)
259
corresponding to a change
in
height
260
of 10 geopotential meters
in pressure (millibars)
corresponding to a change in height
261
of 10 geopotential feet
in pressure (inches of
mercury) corresponding
to a
change
262
in height of 10 geopotential feet
Section V.
STANDARD ATMOSPHERE AND ALTIMETRY TABLES
63.
NACA
64.
ICAN
65.
Altimeter setting computation factors
66.
NACA
67.
Correction of altimeter readings for
265
268
269
273
standard atmosphere, lower atmosphere
standard atmosphere
standard atmosphere altitude-pressure table
mean temperature
of the air
column
68.
NACA
274
standard atmosphere, tentative properties of the upper at-
mosphere
69.
248
adjusted virtual temperature between standard isobaric sur-
faces as a function of thickness in geopotential meters
57-62.
242
of strata between standard isobaric
in geopotential feet
surfaces as a function of
55.
mean adjusted
Density-altitude diagram
280
285
SMITHSONIAN METEOROLOGICAL TABLES
v JiJ
Section VI.
Table
70. Thermodynamic
THERMODYNAMIC TABLES
Density of air
72.
Virtual temperature increment of saturated air
73.
Saturation mixing ratio over water
Saturation mixing ratio over ice
75.
Potential temperature
76.
78.
Two-sevenths power of pressure
Two-sevenths power of ( 1000/p)
Temperature and pressure along saturation pseudoadiabats
79.
Pseudoadiabatic lapse rate
:
80.
Pseudoadiabatic lapse rate
:
81.
82.
Rate of condensation in ascending moist air
Precipitable water in a saturated pseudoadiabatic atmosphere
83.
Lifting condensation level data
77.
84-92.
289
290
295
302
306
308
constants
71.
74.
p
r ™~
314
316
318
323
324
325
327
328
Water stage
Ice stage
Thermodynamic properties
331
of moist air (explanation)
84.
Compressibility factor of moist air
332
85.
86.
Enthalpy residual of moist air
Entropy residual of moist air
87.
Mixing entropy of moist
88.
Isobaric specific heat residual of moist air
334
336
338
339
89.
90.
The
The
91.
Properties of water vapor
341
92.
Properties of condensed water, latent and specific heats
343
coefficient /„
340
coefficient ft
341
Section VII.
93.
air
HYGROMETRIC AND PSYCHROMETRIC TABLES
Definitions and specifications of water vapor in the atmosphere.
94-97.
94.
Saturation vapor pressure over water, metric units
95.
Saturation vapor pressure over water, English units
96.
Saturation vapor pressure over
ice,
metric units
97.
Saturation vapor pressure over
ice,
English units
98-99.
98.
.
.
.
Reduction of psychrometric data (explanation)
Reduction
psychrometric observations
347
350
351
354
360
362
Saturation vapor pressure tables (explanation)
365
368
Reduction of psychrometric observations Fahrenheit temperatures.
369
100. Ratio of the saturation vapor pressure over water to that over ice at
of
99.
:
Centigrade temperatures
.
.
the
same temperature
370
102.
Ratio of the saturation vapor pressure over ice to that over water at
the same temperature
370
Dew point conversion chart
371
103.
Variation of saturation vapor pressure over water with temperature.
101.
372
.
contents
ix
Page
Table
372
104.
Variation of saturation vapor pressure over ice with temperature
105.
Saturation vapor pressure over water of salinity
106.
Equilibrium supersaturation over solution droplets
374
107.
Relative humidity over saturated salt solutions
380
108-109.
Density of pure water vapor
at saturation
.
.
35%
373
(explanation)
381
108.
Density of pure water vapor at saturation over water
382
109.
Density of pure water vapor at saturation over
384
ice
TABLES OF MISCELLANEOUS PHYSICAL PROPERTIES OF
AIR AND AIR-BORNE PARTICLES
Section VIII.
up
389
to about 25 kilometers
110.
Composition of dry
111.
Index
112.
Velocity of sound in air
113.
Viscosity and thermal conductivity of air and diffusivity of water
114.
Terminal velocity of
115.
Size and characteristics of air-borne solids
397
116.
Sizes of atmospheric particles
398
117.
Evaporation of freely falling water drops
398
vapor in
389
390
394
air
fall for distilled
water droplets
in stagnant air.
403
Density of water
Thermal
120. Thermal
121. Thermal
122. Thermal
119.
conductivity of water
conductivity and thermal diffusivity of ice
snow
and density of soils and rocks.
conductivity and thermal diffusivity of
conductivity, specific heat,
123.
Latent heat of melting of sea
124.
Specific heat of sea water
ice
125.
Specific heat of sea ice
126.
Melting point
127.
Depth of water corresponding
in sea
water
to the weight of
snow or
Quantity of rainfall corresponding to given depths
Section X.
129.
407
407
RADIATION AND VISIBILITY TABLES
Blackbody radiation
130-131.
403
404
404
405
405
406
406
406
rain col-
lected in gages of various diameters
128.
396
TABLES OF MISCELLANEOUS PROPERTIES OF WATER
SUBSTANCE AND SOILS
Section IX.
118.
air
of refraction of air
Solar radiation outside the atmosphere (explanation)
411
414
130.
Intensity of solar radiation outside the atmosphere
415
131.
Energy
416
distribution of solar radiation outside the atmosphere
.
smithsonian meteorological tables
x
Page
Table
132-134.
Total solar radiation at the top of the atmosphere (explana-
417
tion)
132.
133.
Total daily solar radiation at
418
the top of the atmosphere
Total annual and seasonal solar radiation
at the top of the at-
418
mosphere
134. Chart of the total daily solar radiation at the top of the atmosphere. 419
135-136. Total direct solar radiation reaching the ground with various
420
atmospheric transmission coefficients (explanation)
135.
Total daily direct solar radiation reaching the ground with various
136.
Total annual and seasonal direct solar radiation reaching the ground
137.
Optical air mass corresponding to different zenith distances of the
138.
Absorption of radiation by water vapor, 10-25/x
139.
Absorption of radiation by water vapor,
140.
Transmission of solar radiation by water vapor,
141.
142.
Absorption of radiation by carbon dioxide
Absorption of radiation by ozone
143.
Absorption coefficients of oxygen
144.
Transmission of radiation through pure, dry
145.
Scattering of solar radiation by water vapor
146.
Transmission of solar radiation by the atmosphere, 5.5-22/*
Transmission of solar radiation through moist air
421
atmospheric transmission coefficients
422
with various atmospheric transmission coefficients
422
sun
147.
423
425
1.3-9/u.
425
427
0. 7-2.2/*
428
430
431
air
432
433
436
438
148.
Spectral distribution of solar radiation at sea level
149.
Total solar and sky radiation on a horizontal surface during cloud-
150.
Relation between the vertical component of direct solar radiation
151.
Relation between average sunshine and solar radiation on a hori-
152.
154.
Transmission of solar radiation through clouds (overcast)
Relation between illumination and total radiation
Albedo of various surfaces
155.
Reflectivity of a water surface
156.
Absorption of radiation by pure liquid water
Absorption of radiation by sea water
438
less conditions
and
total solar
and sky radiation on a horizontal surface
439
zontal surface
153.
157.
440
158.
Scattering area coefficients for water drops in air
159.
Relative spectral luminosity for the
levels
160.
Horizontal
•.
visibility
human
441
442
442
:
444
445
446
446
eye at various luminance
448
452
CONTENTS
rr
Table
Section
XI
XL GEODETIC AND ASTRONOMICAL TABLES
-,-,
Page
Geodetic and astronomical constants
481
Length of one degree of the meridian
163. Length of one degree of the parallel
164. Distribution of water and land in various
482
483
484
485
486
488
491
493
495
497
161.
162.
map
latitude belts
165.
Scale variation for standard
166.
Radius of curvature on a polar stereographic projection
167-168.
projections
Acceleration of gravity (explanation)
167.
Acceleration of gravity at sea level
168.
Relative acceleration of gravity at sea level
Ephemeris of the sun
170. Solar altitude and azimuth
171-174. Duration of daylight, civil
169.
twilight,
and astronomical twilight
(explanation)
171.
506
507
Duration of daylight
172.
Duration of
173.
Duration of astronomical twilight
Daylight and twilight for southern latitudes
Index
174.
civil twilight
513
U>&
lwA-"
517
520
521
'
:
INTRODUCTION
CONVERSION OF UNITS OF LENGTH AND MASS
United States usage.
— No
to be used in the conversion
general agreement yet exists on the factors
between the metric and the English systems of
In the United States, an Act of Congress of July 28, 1866 (14 Stat.
339; 15 U.S.C. 204) established the metric system as lawful throughout the
United States and ordered the units of weights and measures in common
use to be defined in terms of this system. A schedule annexed to this Act
units.
established 39.3700 inches as the equivalent of the meter
and 2.2046 pounds
(avoirdupois) as the equivalent of the kilogram. In 1893 T. C. Mendenhall,
Superintendent of Standard Weights and Measures, issued an order
*
stating
would regard the International Prototype Meter and Kilogram 2
as the fundamental standards and affirmed the equivalents of the Act of 1866.
In actual practice, the National Bureau of Standards still uses the length
that his office
ratio
annexed to
this Act,
which yields
1
=
inch
2.540005 centimeters.
How-
Bureau of Standards has adopted
the results of a comparison of the British Imperial Standard Pound and the
International Prototype Kilogram made in 1883, 1 pound = 453.5924277
grams, rather than the ratio annexed to the Act of 1866, which yields 1
pound = 453.597+ grams.
ever, in the case of the pound, the National
British usage.
mass are
—In
Great Britain, the English standards of length and
by the Imperial Standard Yard and the Imperial
legally defined
Standard Pound, respectively, and the relation of the English to the metric
units are experimentally determined
now
legally sanctioned in
1
1
Recent comparisons.
1
inch
pound
=
=
3
direct comparison.
The conversions
2.539998 centimeters
453.59234 grams
—According
Imperial
1
by
Great Britain are:
Yard
meter
1
inch
_
~
=
to the
most recent comparisons
3600000
3937014
>
4
which yields
2.539996 centimeters
U. S. Coast and Geodetic Survey, Bull. 26, 1893.
Prepared by the International Bureau of Weights and Measures, Sevres, France.
This bureau was established by the International Metric Convention, 1875, and is supported by the contributions of many nations, including the United States.
8
For a discussion of the problems involved, see Darwin, C, et al., Proc. Roy. Soc.
London, ser. A, vol. 186, p. 175, 1946.
4 Nat. Bur. Stand., private communication,
July 1949.
1
2
1
;
SMITHSONIAN METEOROLOGICAL TABLES
2
in the conversion:
In the case of the pound, this comparison resulted
1
pound
=
453.59234 grams
have
Industrial usage.— In recent years improved industrial techniques
Englishvarious
the
by
used
relationships
made it desirable to standardize the
The conversion
speaking countries.
1
inch
=
2.54 centimeters has been sug-
gested as the best compromise, with the practical advantage of
facilitating
mechanical conversion between the two systems by means, for example, of a
127-tooth gear wheel on a lathe or measuring instrument. The above relation-
American and British industrial use for several
5
years and has been adopted by both the American Standards Association
6
and the British Standards Institution.
Even less practical difference exists between the various definitions of the
pound, but the conversion 1 pound = 453.5923 grams has been urged, since
ship has been the standard for
this figure is divisible
At
this writing a
by 7000, the number of grains
bill
to legalize these
pound.
in a
two conversions has been prepared
for introduction in Congress and the British are expected to legally sanction
them by an Order
in Council
has already adopted the
Accordingly,
in this
upon enactment of the
new conversion
bill
into law.
Australia
factors.
conversions between the English and metric systems
all
volume are based on the relationships:
1
1
Nautical mile.
inch
=
2.54 centimeters
pound = 453.5923 grams
— Originally
and
practically for uses at sea, the nautical
mile was considered to be the length of
1
minute of arc on the earth's surface
for the given latitude and in the given azimuth on a representative spheroid.
more
precise definition
is
desirable
and
in the tables issued
by the U.
of Standard Weights and Measures, September 1898, the nautical mile
defined as a minute of arc of a great circle on a sphere
that of the Clarke spheroid of 1866.
mile by the
National Bureau of
The
value
Standards
7
now
is
Clarke's ratio of the foot to the meter this length
6080.20
is
feet,
8
given for the nautical
6080.27
feet, the
Using
value
8
given in Bowditch
adoption of the
is
whose surface equals
1853.248 meters.
is
A
S. Office
using the ratio annexed to the Act of 1866 this length
the value given in previous editions of these tables. The
new
ratio of the foot to the
American Standards Association Report B
meter (1 foot
48.1,
=
0.3048 meter)
"Inch-Millimeter Conversion
for
Industrial Use," 1933.
6
British Standards Institution Report B. S. 350, "Conversion
Factors
7
U.
8
Navy Hydrographic
and Tables,"
1944.
M
Nat. Bur. Stand. Misc. Publ.
121, 1936.
Bowditch, N., American Practical Navigator, 1938 rev.
S.
Office,
Washington, 1939.
On
ed., pp. 20 and 327.
U. S.
page 144 the factor 6080.20 is given.
INTRODUCTION
results in the following definition of the
U.
6
S. nautical mile,
which
used
is
throughout this volume:
U.
1
S. nautical
mile
=
1853.248 meters
=
6080.21 feet
Other definitions of the nautical mile are in use. The British Admiralty
6080 feet (exactly) the international
defines the nautical mile as being
nautical mile
;
defined as being 1852 meters (exactly). 1111
is
STANDARD GRAVITY FOR REDUCING BAROMETRIC OBSERVATIONS
common
Prior to the introduction of the millibar as the
unit of pressure in
was customary to express barometric pressures in terms of
the height of a column of mercury reduced to standard conditions of tempera-
meteorology,
it
ture and gravity.
gravity adopted
To
Conventionally, the standard value for the acceleration of
was
that at latitude 45°
and sea
level.
9
reduce units of pressure expressed in terms of the height of a mercury
column to standard gravity,
it is
only necessary to
know
the ratio of the local
In general, this ratio
acceleration of gravity to the standard value.
de-
is
terminable with more precision than the absolute value of the acceleration of
gravity at a given place.
However,
absolute units (e.g., millibars),
if
pressures are to be converted to
necessary to
it is
know
the standard acceleration
of gravity.
At
meetings of the International Committee on Weights and
the 1891
made
in
10
announced the results of an investigation
1888 which yielded an acceleration of gravity at latitude 45° and
Measures, Defforges and Lubanski
sea level of 980.665 cm. sec." 2 This value has been used extensively since that
time by physicists and others as an arbitrary standard value of gravity,
though
it
has long been
known
that
it
gravity at latitude 45° and sea level. 11
that the best value
is
The most
near 980.616 cm.
Most meteorological
al-
does not represent the absolute value of
sec."
2
recent determinations indicate
(see Table 167).
services, including the
U.
S.
Weather Bureau,
first
reduce barometer readings in terms of inches or millimeters of mercury to
gravity at latitude 45° and sea level (g 45 o) by means of a correction depending
,
on the
ratio of local gravity to
lute units.
Strictly speaking,
g i5
it is
,
(see Table 47) and then convert to abso-
therefore necessary to use the best estimate
of the value of gravity at latitude 45°
and sea
level in converting the inch or
millimeter of mercury to millibars. This procedure
was adopted by the
national Meteorological Organization in 1939 (Resolution 25, Berlin).
ever, for
many
Inter-
How-
physical applications (e.g., the definition of the International
Temperature Scale, 1948, see footnote, page 17) one atmosphere is defined as
1013.250 mb. This pressure corresponds to the pressure exerted by a column
International Meteorological Tables, Paris, 1890.
10
Defforges and Lubanski, Com. Int. des Poids
11
Dryden, H.
lla Effective
L.,
July
et
Mes., Ann.
Nat. Bur. Stand. Journ. Res., vol. 29,
1,
1954,
I, p.
135, Paris, 1892.
p. 303, 1942.
the international nautical mile
Department of Defense and the Department of Commerce.
was adopted bv the L.
S.
SMITHSONIAN METEOROLOGICAL TABLES
4
of
3
to
mercury 760 mm. high, having a density of 13.5951 gm. cm.' and subject
2
a gravitational attraction of 980.665 cm. sec."
millimeter
distinction is therefore necessary between the standard inch or
-2
"45°"
of
millimeter
or
inch
and the
of mercury based on 980.665 cm. sec.
A
mercury based on 980.616 cm. sec." (see Table 1). Owing to the action of
adopting the conthe International Committee on Weights and Measures, in
2
ventional standard value 980.665 cm. sec.," it is advisable to employ this datum
2
for
Accordingly, with a view to maintaining conon which the International Temperature Scale of 1948
barometric readings.
all
sistency with the basis
established, the tables presented herein for conversions of inches or millimeters of mercury to millibars, and vice versa, are based on the conventional
2
standard acceleration of gravity (980.665 cm. sec." ).
is
If
it is
desired to convert "45°" inches or millimeters of mercury to milli1 1 must be decreased by 0.005 percent.
bars, the tabular values in Tables 9 and
Conversely,
if
millibars are to be converted to
of mercury, the tabular values in Tables 10
"45°" inches or millimeters
and 12 must be increased by
0.005 percent.
CALORIE
15° gram-calorie.
—The small- or gram-calorie
12
was
originally defined as
the quantity of heat necessary to raise the temperature of
1
degree centigrade.
It
temperature over which the water was heated and
many such
calories,
it
depending on the range. The
to 15.5°
gram of water
became possible
C, has
until recently
to define
15° gram-calorie (cal.i 5 ),
the quantity of heat necessary to raise the temperature of
from 14.5° C.
1
was found necessary to specify the exact range of
1
gram
been one of the most
of water
common
units of heat used in scientific work.
International
Steam Tables
calorie.
—Modern laboratory procedures for
the determination of amounts of heat usually involve electrical apparatus and
it
has been found advantageous to define the calorie in terms of electrical
equivalents.
Tables
18
Therefore
in
1929 the First International Conference on Steam
defined the International
equivalent to 1/860
xlO 3 mean
international kilowatt-hour
=
nition has also been adopted
Steam Tables
calorie
(ITcal.) as being
international kilowatt-hours,
where
1
mean
1.00019 absolute kilowatt-hours. 14
This defiby the International Meteorological Organiza-
12
The
13
Mech. Eng.,
14
In the United States, the National Bureau of Standards uses the relation 1 inter1.000170 absolute joules, where the "international joule" is the inter-
large- or kilogram-calorie
national joule
(Kcal.) has not been used in this volume.
vol. 52, p. 120, 1930.
=
national joule as maintained in this country, and not the
mean
international joule.
definition yields the relation:
1
ITcal.
=
4.18674 absolute joules
=
4.18605 international joules.
This
:
INTRODUCTION
tion.
15
The
gram-calorie
relation of the International
is
5
Steam Tables
15°
calorie to the
16
1
ITcal.
Meteorological practice.
=
1.00032
cal. 15
— From the relationship above,
it is
evident that
for most ordinary meteorological purposes the difference between the
calorie
and the 15°
calorie
is
negligible.
However,
it is still
the 15° calorie in radiation and associated fields of meteorology, while the
calorie has
become the standard for use
in
thermodynamic
calculations.
dual usage has been adopted in general throughout this volume.
instances the type of calorie
such that the difference
15 Int.
is
is
unspecified
;
IT
This
In some
here the nature of the data
is
immaterial.
Meteorol. Org. Twelfth Conference of Directors, Resolution 164, Washington,
1947.
16
IT
customary to use
See Birge, R.
T.,
Rev. Mod. Phys.,
vol.
13, p. 233,
1941.
(#b\
JL
Section
I
CONVERSION TABLES
~1
%h\
Table
1
CONVERSION FACTORS
1
Organization of Table
A. Length
K. Energy, work
Mass
F.
D. Time
I.
Pressure
L. Power
M. Energy per unit area
N. Power per unit area
E. Velocity; speed
J.
Force
O. Illumination, brightness,
G. Density, specific volume
Area
Volume
B.
C.
H. Viscosity
etc.
A. Length:
1
Angstrom unit (A.)
= 10"V
1
= 25.4 mm.
= 2.54 cm.
= 10-»cm.
=
1
micron
10- 10
=
=
m.
1
(ft)
= 10
in.
A.
KT* cm.
1
= 10" cm.
= 10^ m.
= 0.039370079
1
1-
ft.
in.
centimeter (cm.)
1
= lO" m.
= 0.39370079
= 0.032808399
ft.
in.
1
ft.
ft.
1
ft.
statute mile
(stat.
mi.)
= 5280
= 0.868391 naut. mi.
= 1609.344 m.
= 1.609344 km.
ft.
in.
kilometer (km.)
= 10 cm.
= l(fm.
= 3280.8399
= 0.621371
mi.
= 0.539593 naut. mi.
B
1
ft.
ft.
stat.
degree of latitude* (°lat.)
= 111137 m.
= 111.137 km.
= 69.057
mi.
= 59.969 ss 60 naut.
U. S. nautical mile (naut. mi.) t
= 6080.21
= 1.151555
= 1853.248 m.
= 1.853248 km.
stat.
1
rod (rd.)
= 16.5
= 5.0292 m.
meter (m.)
10* cm.
=
= 3.2808399
= 39.370079
1
fathom (fath.)
=6
= 1.8288 m.
8
1
yard (yd.)
36 in.
=
=3
= 91.44 cm.
= 0.9144 m.
(mm.)
millimeter
foot (ft.)
= 12
= 30.48 cm.
= 0.3048 m.
4
1
1
inch (in.)
1
British Admiralty nautical mile
1
International nautical mile
= 6080
stat.
mi.
mi.
ft.
= 1852 m.
= 6076.1
= 1.150779
ft.
stat.
mi.
B. Area:
1
square millimeter (mm.*)
= 0.001550003
*
1
square inch
Average value, 1/90 of meridian quadrant.
t
See Introduction,
1
1 in.
1 lb.
=
=
2.54 cm.
453.5923
in bold-face type.
(continued)
g.
3
p. 2.
See Introduction for discussion of the basic conversion factors adopted.
conversions are based on the factors:
SMITHSONIAN METEOROLOGICAL TABLES
(in. )
= 6.4516 cm.
8
in.
Fundamental conversion factors are
2
All
metric-English unit
Table
10
1
(continued)
CONVERSION FACTORS
B. Area: (continued)
1
square centimeter (cm.')
= 10' ram.
= 0.1550003
1
square foot
1
s
in.'
8
4
1
in.'
square meter (m.')
= 10 cm.
= 1550.003
= 1076391
(ft.')
= 144
= 929.0304 cm.
= 0.09290304 m.'
1
1
)
=9
= 8361.2736 cm.'
= 0.83612736 m.'
ft.'
in.'
8
ft.
(km.')
square kilometer
2
square yard (yd.
= 10 cm.'
= 10" m.'
= 1.076391 X 10
= 247.1054 acre
= 0.3861022
10
1
acre
= 43560
= 4840 yd.'
= 4046.8564 m.'
ft.'
7
ft.'
stat. mi.'
1
square statute mile
(stat. mi.
= 2.78784 X 10
= 640 acres
= 2.58999 km.
2
)
7
ft.'
3
C.
Volume:
1
cubic centimeter
(cm.
= 0.999972 ml.
= 0.0610237
= 0.0338140 U.
8
1
)
cubic inch (in.
in.*
1
cubic meter (m.
= cm.
= 999.972
= 35.3147
= 264.172
10"
= 219.97
1
milliliter
8
)
S.
fl.
oz.
or stere (s.)
1
8
ft.
Brit. gal.
1 fluid
its
8
fl.
fl.
oz.
oz.
fl.
oz.)
fl.
oz.)
8
in.
density.)
8
1
8
U.
quart, liquid,
in.
fl.
S.
oz.
fl.
(U. S.
S.
= 57.75
= 32 U. S.
= 946.353 cm.
= 0.946326
8
8
fl.
oz.
8
1.
fl.
1
gallon,
U.
S.
(U. S. gab)
= 231 in.3
= 128 U. S.
= 133.23 Brit.
= 0.83267 Brit.
= 3785.41 cm.
= 3.78531
fl.
8
1.
(continued)
SMITHSONIAN METEOROLOGICAL TABLES
oz.
8
maximum
= 1000.028 cm.
= 61.0255
= 33.815 U. S. oz.
= 1.05672 U. S. qt.
= 0.264179 U. S. gal.
= 35.196 Brit. oz.
fl.
fluid ounce, British (Brit.
= 1.7339
= 28.413 cm.
= 28.412 ml.
= 0.96076 U.
volume
kilogram of water
in.
gal.
8
8
temperature of
qt.
ounce, U. S. (U. S.
= 1.80469
= 29.5735 cm.
= 29.5727 ml.
= 1.0408 Brit.
1
1
8
in.
(1 liter is defined as the
at
oz.
1.
(ml.)
(1.)
occupied by
fl.
8
S. gal.
8
liter
S.
8
(ft. )
in.
in.
)
= 1728
= 29.9221 U. S.
= 7.48052 U. S.
= 28316.8 cm.
= 28.3161
1.
= 1.000028 cm.
= 0.0610255
= 0.033815 U. S.
= 0.035196 Brit.
1
cubic foot
8
U.
8
= 0.554113 U.
= 16.3871 cm.
= 16.3866 ml.
oz.
fl.
oz.
gal.
qt.)
Table
(continued)
1
11
CONVERSION FACTORS
C. Volume: (continued)
1
gallon, British (Brit, gal.)
(Im-
perial gallon)
(1
British gallon
defined as
is
the volume occupied by 10 pounds
of water at 62° F.)
= 160 Brit. oz.
= 277.42
= 1.2010 U. S. gal.
= 153.72 U. S. oz.
= 4546.1 cm.
= 4.5460
fl.
in.»
fl.
3
1.
D. Time:
1
mean
solar second (sec, s.)
= 1.002738
1
mean
1
mean
sidereal seconds
solar minute (min., m.)
= 60
(mean
sec.
solar)
solar hour (hr., h.)
= 3600 sec. (mean solar)
= 60 min. (mean solar)
1
mean
solar day (da., d.)
= 86400 sec. (mean solar)
= 1440 min. (mean solar)
= 24 hr. (mean solar)
= 24 hours 3 minutes 56.555
1
tropical
(mean
solar,
seconds of
mean
sidereal time
ordinary) year (yr.)
= 31.5569 X 10* sec. (mean solar)
= 525949 min. (mean solar)
= 8765.81 hr. (mean solar)
= 365.2422 da. (mean solar)
= 366.2422 sidereal days
1
sidereal second
1
sidereal
= 0.997270 sec.
(mean
solar)
day
= 86164.1
= 23 hr.
(mean
sec.
solar)
56 min. 4.091 sec. (mean solar)
Velocity; speed:
1
meter per second (m.
sec."
= 3.6 km. hr."
= 1.94254 knots
= 2.23694 mi. hr."
= 3.28084 sec."
= 196.850 min."
= 0.77742
day
1
,
mps)
1
-1
1
1
1
1
ft.
1
1
ft.
°lat.
1
1
1
ft.
kilometer per hour
1
1
(km.
ft.
hr.
-1
°lat.
,
kph)
= 0.277778
= 0.539593
= 0.621371
= 0.911344
= 0.21595
1
m.
sec."
-1
,
1
ft.
-1
1
mi. hr."
sec.
1
°lat.
mile per hour (mi. hr.
= 0.868391 knot
= 1.46667 sec."
= 0.44704 m.
= 1.609344 km. hr.= 88 min."
= 0.34754 Mat. day"
1
knot
ft.
knot
= naut. mi. hr.
= 1.15155 mi. hr."
= 1.68895 sec."
= 0.514791 m. sec."
= 1.85325 km. hr."
= 101.337 min."
= 0.40021 s* 0.4
1
sec."
day"
1
1
1
ft.
1
(continued)
SMITHSONIAN METEOROLOGICAL TABLES
day"
mph)
Table
12
1
(continued)
CONVERSION FACTORS
E. Velocity; speed: (continued)
1
degree of latitude per day (°lat.
1
foot per second
)
= 1.2863 m. sec."
= 4.6307 km. hr."
= 2.4987 =* 2.5 knots
= 2.8774 mi. hr.
1
1
1
1
ft.
1
1
1
foot per minute
min.
(ft.
-1
,
= 0.00986808 knot
= 0.0113636 mi. hr."
= 0.00508 m. sec."
= 0.018288 km. hr."
1
1
F. Mass:
1
gram
1
(g.)
grain (gr.)
= 0.0647989 g.
= 0.00228571 oz.
= 15.4324 gr.
= 0.0352740 oz.
= 0.002204623
lb.
1
1
ounce avoirdupois (oz.)
= 437.5 gr.
= 28.3495 g.
kilogram (kg.)
= 10
= 35.2740 oz.
= 2.204623
s
g.
1
pound avoirdupois
= 7000 gr.
= 16 oz.
= 453.5923
= 0.4535923
lb.
1
metric ton, tonne
(t.)
= 10 kg.
= 2204.623
= 1.10231 short tons
= 0.9842107 long ton
s
(lb.)
g.
lb.
1
kg.
short ton
= 2000
= 0.892857 long
= 907.1846 kg.
= 0.9071846
lb.
ton
t.
1
long ton
= 2240
= 1.12 short tons
= 1016.047 kg.
= 1.016047
lb.
t.
G. Density,
1
specific
volume:
3
g. cm."*
1
= 62.4280
=
m."*
lb. ft."
= 0.0160185
3
lb. ft."
1
1
cm. 8
t.
1
3
ft.
lb."
g.
ft.
3
3
S
1
lb."
H. Viscosity
1
poise
= g. cm."
= 0.002089
1
1
1
sec."
lb.
(wt.)
sec.
3
ft."
(continued)
SMITHSONIAN METEOROLOGICAL TABLES
lb.
(wt.) sec.
= 478.8
1
cm.
1
= 62.4280 cm.
g." 1
= 0.0160185
\ fps)
sec.
(ft.
= 0.592085 knot
= 0.681818 mi. hr."
= 60 min."
= 0.3048 m. sec."
= 1.09728 km. hr."
1
day"
3
ft."
poises
„
g
-1
1
fpm)
Table
1
(continued)
13
CONVERSION FACTORS
I.
Pressure:
N ot e. — The
pressure units one standard inch of mercury, one standard millimeter
and one standard atmosphere are denned in terms of the conventional
2
standard value of gravity 980.665 cm. sec." which was adopted by the InternaThese units have been proposed for
Measures.
tional Committee on Weights and
general meteorological use. The pressure units one 45° inch of mercury, one 45°
millimeter of mercury, and one 45° atmosphere are defined in terms of the best
2
value of gravity at 45° latitude and sea level, 980.616 cm. sec." See introduction,
of mercury,
,
page
3.
centimeter
dyne per square
1
(dyne cm." )
1 barye
10"8 mb.
10^ bar.
1
1
standard inch of mercury
= 0.491154
= 33.8639 mb.
= 0.0345316 kg. cm."
= 25.4013 mm. Hg. (45°)
=
=
=
lb. in."
= 10 dynes cm."
= 0.00101972 kg. cm."
= 0.750099 mm. Hg. (45°)
= 0.750062 mm. Hg. (stand-
= 25.4 mm. Hg.
3
3
2
1
45°
in.
in.
= 0.0145038
lb.
lb.
in."
2
6
1
dynes cm.
s
mb.
a
barye
,
in.
in.
Hg. (45°)
Hg. (stand-
ard)
= 1.333224 mb.
= 0.001359504 kg. cm."
= 0.03937205 Hg. (45°)
= 0.03937008 Hg.( stand2
in.
in.
ard)
2
lb.
2
ard)
1
standard atmosphere
= 1013.250 mb.
= 1.03323 kg. cm."
= 760 mm. Hg. (standard)
Hg. (stand= 29.9213
2
in.
in."
(mm.
45° millimeter of mercury
ard)
= 14.6960
= 760.038 mm. Hg. (45°)
= 29.9228
Hg. (45°)
= 1.000050 45° atmosphere
lb.
Hg. (45°))
= 0.999950 mm.
Hg.( stand-
in.
ard)
= 1.333157 mb.
= 0.00135944 kg. cm."
= 0.03937008 Hg. (45°)
= 0.0393681 Hg. (stand2
in.
in.
ard)
= 0.0193358
2
(lb. in."
= 68.9476 mb.
= 0.0703069 kg. cm."
= 51.7175 mm. Hg. (45°)
= 51.7149 mm. Hg. (stand-
(mm. Hg. (standard))
= 1.000050 mm. Hg. (45°)
1
pound per square inch
= 2.03612
= 2.03602
-2
standard millimeter of mercury
= 0.0193368
2
psi)
bar (b.)
= 10
= 10
= 10
in."
ard)
1
= 10 mb.
1
Hg.
2
Hg. (45°)
Hg. (stand-
(cb.)
centibar
(in.
= 0.491130
= 33.8622 mb.
= 0.0345298 kg. cm."
= 25.4 mm. Hg. (45°)
= 25.3987 mm. Hg. (stand-
ard)
1
(standard)
inch of mercury
(45°))
ard)
= 0.0295315
= 0.0295300
2
2
millibar (mb.)
1
(in.
Hg. (standard))
lb. in."
2
{continued)
SMITHSONIAN METEOROLOGICAL TABLES
in."
2