Table I.—Properties of Air
| Temperature of the air | Weight of vapor per cubic foot of saturated air | Weight of cubic foot of saturated air |
| Fahrenheit | Grains | Grains |
| 10° | 1.11 | 589.4 |
| 11 | 1.15 | 588.1 |
| 12 | 1.19 | 586.8 |
| 13 | 1.24 | 585.5 |
| 14 | 1.28 | 584.2 |
| 15 | 1.32 | 582.9 |
| 16 | 1.37 | 581.6 |
| 17 | 1.41 | 580.3 |
| 18 | 1.47 | 579.1 |
| 19 | 1.52 | 577.8 |
| 20 | 1.58 | 576.5 |
| 21 | 1.63 | 575.3 |
| 22 | 1.69 | 574.0 |
| 23 | 1.75 | 572.7 |
| 24 | 1.81 | 571.5 |
| 25 | 1.87 | 570.2 |
| 26 | 1.93 | 569.0 |
| 27 | 2.00 | 567.7 |
| 28 | 2.07 | 566.5 |
| 29 | 2.14 | 565.3 |
| 30 | 2.21 | 564.1 |
| 31 | 2.29 | 562.8 |
| 32 | 2.37 | 561.6 |
| 33 | 2.45 | 566.4 |
| 34 | 2.53 | 559.2 |
| 35 | 2.62 | 558.0 |
| 36 | 2.71 | 556.8 |
| 37 | 2.80 | 555.6 |
| 38 | 2.89 | 554.4 |
| 39 | 2.99 | 553.2 |
| 40 | 3.09 | 552.0 |
| 41 | 3.19 | 550.8 |
| 42 | 3.30 | 549.6 |
| 43 | 3.41 | 548.4 |
| 44 | 3.52 | 547.2 |
| 45 | 3.64 | 546.1 |
| 46 | 3.76 | 544.9 |
| 47 | 3.88 | 543.7 |
| 48 | 4.01 | 541.3 |
| 49 | 4.14 | 542.5 |
| 50 | 4.28 | 540.2 |
| 51 | 4.42 | 539.0 |
| 52 | 4.56 | 537.9 |
| 53 | 4.71 | 536.7 |
| 54 | 4.86 | 535.5 |
| 55 | 5.02 | 534.4 |
| 56 | 5.18 | 533.2 |
| 57 | 5.34 | 532.1 |
| 58 | 5.51 | 534.9 |
| 59 | 5.69 | 529.8 |
| 60 | 5.87 | 528.6 |
| 61 | 6.06 | 527.0 |
| 62 | 6.25 | 526.3 |
| 63 | 5.45 | 525.2 |
| 64 | 6.65 | 524.0 |
| 65 | 6.87 | 522.0 |
| 66 | 7.08 | 521.7 |
| 67 | 7.30 | 520.0 |
| 68 | 7.53 | 519.4 |
| 69 | 7.76 | 518.3 |
| 70 | 8.00 | 517.2 |
The evaporation of moisture is always accompanied with the loss of heat required to produce such change of condition. This is known as the heat of vaporization and represents a definite amount of heat that is used up whenever water is changed into vapor. No matter what its temperature may be—whether hot or cold—when water is vaporized, a definite amount of heat is required to change the water into vapor.
Water may be evaporated at any temperature; even ice evaporates. A common instance of the latter is that of wet clothes which “freeze dry” in winter weather when hung on the clothes line. The rate at which evaporation takes place depends on the dryness of the surrounding air and the rapidity of its motion. In dry windy weather evaporation is most rapid.
As before stated, whenever water evaporates—at no matter what temperature—a definite quantity of heat is necessary to change the water into vapor. The exact amount of heat required to produce this change varies somewhat with the temperature and atmospheric pressure but it always represents a large loss of heat. At the boiling point of water (212°F.) the heat of vaporization is 970 B.t.u. for each pound of water evaporated, but at a lower temperature it is greater than that amount. At the temperature of the body (98.6°) the heat necessary to evaporate a pound of moisture from its surface is 1045 B.t.u.
It is the absorption of heat due to evaporation that cools the air of a sprinkled street. The more rapid the evaporation the more pronounced is the decline of temperature in the immediate vicinity. The same effect is produced when moisture is evaporated from the surface of the body. The acceleration of evaporation caused by a breeze or the blast of air from an electric fan is that which produces the chilling sensation to the body. During winter weather the effect of the cold wind is rendered more severe by evaporation of moisture from the body. In health, the body being in a slightly moist condition, the evaporation which goes on from its surface is what keeps it cool in warm weather, but if on account of excessive dryness of the surrounding air the evaporation is very rapid, a sensation of cold is the result.
Not only does excessively dry air produce the sensation of chilliness but the loss of heat from the body due to sudden or long exposure effects the general health and is conducive to chills that are followed by fever. In health the temperature of the body is constant and normally 98.6°F.; any condition that reduces that temperature tends toward a lowering of vitality and the consequent inability to withstand the attack of disease. In a very dry atmosphere the skin, instead of being slightly moist, is kept dry, the result of which is the irritation that produces chaps and roughness of the surface.
Reports of the U. S. Weather Department show that the relative humidity of Death Valley, which is the driest and hottest known country, during the driest period of the year—between May and September—averages 15.5 per cent. saturation. In winter, many buildings, particularly offices and school buildings are not far from that atmospheric condition, constantly. Under the usual conditions of house heating, there is an almost absolute lack of means to give moisture to the air. Almost without exception steam-heating plants and hot-water heating plants in office buildings and dwellings are without any provision for changing the atmospheric humidity.
In school buildings that are not kept under a more desirable condition of temperature and humidity, the general health is impaired and the behavior of the pupils very markedly influenced. The tension of a school-room full of fidgety nervous children can be very promptly and greatly reduced by the introduction of water vapor into the air to 50 per cent. saturation.
All modern school buildings, auditoriums, etc., are provided—aside from the heating plants—with means of ventilating in which the entering air is washed and humidified to the desired degree, before being sent into the rooms.