Methods Of Ascertaining The Exact Boiling Temperature
The normal boiling temperature of water all nations have tacitly agreed to fix under a normal barometric pressure of 29·922 inches of mercury, having the temperature of melting ice, in the latitude of 45°, and at the sea-level. If the atmospheric pressure at the time or place of graduating a thermometer does not equal this, the boiling temperature will be higher or lower according as the pressure is greater or less. Hence a reading must be taken from a reliable barometer, which must also be corrected for errors and temperature, and reduced for latitude, in order to compare the actual atmospheric pressure at the time with the assumed normal pressure. Tables of vapour tension, as they are termed, have been computed from accurate experimental investigations and theory,—giving the temperatures of the vapour of water for all probable pressures; Regnault’s, the most recent, is considered the most accurate; and his investigations are based upon the standard pressure given above, and are for the same latitude. His Table, therefore, will give the temperature on the thermometric scale corresponding to the pressure.
The Commissioners appointed by the British Government to construct standard weights and measures, decided that the normal boiling-point, 212°, on the thermometer should represent the temperature of steam generated under an atmospheric pressure equal in inches of mercury, at the temperature of freezing water, to 29·922 + (cos. 2 latitude × ·0766) + (·00000179 × height in feet above the sea-level). Hence, at London, lat. 51°30´ N., we deduce 29·905 as the barometric pressure representing the normal boiling point of water,—the trifling correction due to height being neglected. If then, in the latitude of London, the barometric pressure, at the time of fixing the boiling point, be not 29·905 inches, that point will be higher or lower, according to the difference of the pressure from the normal. Near the sea-level about 0·59 inch of such difference is equivalent to 1° Fahrenheit in the boiling point.
Suppose, then, the atmospheric pressure at London to be 30·785 inches, the following calculation gives the corresponding boiling temperature for Fahrenheit’s scale:—
Observed
pressure
30·785
Normal
"
29·905
Difference
·880
As 0·59 is to 0·88, so is 1° to 1°·5.
That is, the water boils at 1°·5 above its normal temperature; so that, in this case, the normal temperature to be placed on the scale, viz. 212°, must be 1°·5 lower than the mark made on the tube at the height at which the mercury stood under the influence of the boiling water.
The temperature of the vapour of boiling water may be found, at any time and place, as follows:—Multiply the atmospheric pressure by the factor due to the latitude, given in the annexed Table V., and with the result seek the temperature in Table VI.
Table V.
Table VI.
Latitude.
Factor.
Temperature
of Vapour.
Tension.
Temperature
of Vapour.
Tension.
Degrees.
Degrees.
Inches.
Degrees.
Inches.
0
0·99735
179
14·934
197
22·036
5
0·99739
180
15·271
198
22·501
10
0·99751
181
15·614
199
22·974
15
0·99770
182
15·963
200
23·456
20
0·99797
183
16·318
201
23·946
25
0·99830
184
16·680
202
24·445
30
0·99868
185
17·049
203
24·952
35
0·99910
186
17·425
204
25·468
40
0·99954
187
17·808
205
25·993
45
1·00000
188
18·197
206
26·527
50
1·00046
189
18·594
207
27·070
55
1·00090
190
18·998
208
27·623
60
1·00132
191
19·409
209
28·185
65
1·00170
192
19·828
210
28·756
70
1·00203
193
20·254
211
29·335
75
1·00230
194
20·688
212
29·922
80
1·00249
195
21·129
213
30·515
196
21·578
214
31·115
How to use the Tables.—When the temperature is known to decimals of a degree, take out the tension for the degree, and multiply the difference between it and the next tension by the decimals of the temperature, and add the product to the tension, for the degree.
Required the tension corresponding to 197°·84.
°
197
=
22·036
·465 × ·84
=
·391
198
=
22·501
197°
=
22·036
Difference
·465
197·84
=
22·427
When the tension is given, take the difference between it and the next less tension in the Table, and divide this difference by the difference between the next less and next greater tensions. The quotient will be the decimals to add to the degree opposite the next less tension.
Thus, for 23·214 inches, required the temperature.
Given
23·214
Next
greater
23·456
22·974
Next
less
22·974
·240
Difference
·482
And
·240
=
·5
·482
Temperature opposite next less
199·0
Temperature required
199·5
A similar method of interpolation in taking out numerical quantities is applicable to almost all tables; and should be practised with all those given in this work.
Example.—Thus, in Liverpool, lat. 53° 30´ N., the barometer reading 29·876 inches, its attached thermometer 55°, and the correction of the instrument being + ·015 (including index error, capillarity and capacity), what temperature should be assigned for the boiling point marked on the thermometer?