SYSTEMS OF WARMING Any system of warming must include, first, the combustion of fuel, which may take place in a fireplace, stove, or furnace, or a steam, or hot-water boiler; second, a system of transmission, by means of which the heat may be carried, with as little loss as possible, to the place where it is to be used for warming; and third, a system of dif fusion, which will convey the heat to the air in a room, and to its walls, floors, etc., in the most economical way.
A more even temperature may be maintained with a furnace than by the use of stoves, owing to the greater depth and size of the fire, which allows it to be more easily controlled.
When a building is placed in an exposed location, there is often difficulty in warming rooms on the north and west sides, or on that side toward the prevailing winds. This may be overcome to some ex tent by a proper location of the furnace and by the use of extra large pipes for conveying the hot air to those rooms requiring special at tention.
One of the principal advantages of direct steam is the ability to heat all rooms alike, regardless of their location or of the action of winds.
When compared with hot-water heating, it has still another desirable feature—which is its freedom from damage by the freezing of .water in the radiators when closed, which is likely to happen in unused rooms during very cold weather in the case of the former system.
On the other hand, the sizes of the radiators must be proportioned for warming the rooms in the coldest weather, and unfortunately there is no satisfactory method of regulating the amount of heat in mild weather, except by shutting off or turning on steam in the radia ators at more or less frequent intervals as may be required, unless one Of the expensive systems of automatic control is employed. In large rooms, a certain amount of regulation can be secured by dividing the radiation into two or more parts, so that different combinations may be used under varying conditions of outside temperature. If two radiators are used, their surface should be proportioned, when convenient, in the ratio of 1 to 2, in which case one-third, two-thirds, or the whole power of the radiation can be used as desired.