Hot Water Heating]

And the inventor saw the tired, worn look of the housewife, removed the

stove to the cellar and installed tin pipes from this central heater

to the various rooms, and then waited for applause and purchasers. It

seemed so simple, but it did not solve the problem entirely, for when

the wind blew from the north into the windows, it pressed out the warm

air from the exposed rooms, forced it down the pipes up through which

it was supposed to come, and then rushed it up the flues on the south

or warm side of the house, overheating this part and leaving the cold

rooms of the house unheated. The drum of the furnace over which the air

passed to receive its warmth from the burning coal would leak every

time fresh fuel was added, for the odor of coal-gas became very evident

throughout the house. Moreover, the heat was very dry and unpleasant,

so that water-jars had to be set about to moisten the air.

Then came the inventor again with a new device, a steam-boiler, pipes

to distribute the steam, and radiators to give off the heat in the

steam to the room. Here at last was a method of heating which would

supply warmth in the cold parts of the house, even under the windows,

through which the chilliest air penetrated. But the sizes of the

radiators were calculated to heat the house to 70 degrees when it was

zero outside, although the average winter day was much warmer than

this. In this way the occupants of the house were cooked with an excess

of heat during moderate weather, for there was no way to regulate the

amount of heat given off from the radiator; it either was filled with

steam, giving off its maximum quantity of heat, or else it was empty

and cold.

To meet this difficulty presented by the steam-heated radiator,

the hot-water system was developed. Instead of distributing heat

with the medium of steam which under low pressure was fixed at one

temperature, heat was circulated by hot water from the central boiler.

The temperature of this water could be regulated for mild weather by

lowering the fire. However, since the hottest water was cooler than

steam, it required larger radiators and more piping, so that the

initial cost of a hot-water plant was more than that of a steam system.

[Illustration: Simplified diagram of Vapor-vacuum system]

In order to overcome the disadvantages of the inflexible

steam-radiator, inventors finally developed the so-called

“vapor-vacuum” system of steam-heating. In this equipment the air was

driven from the entire length of pipes and from the radiators by the

pressure of the rising steam from the boiler, and forced through a

special ejector which closed when the steam came in contact with it,

preventing the return of air into the interior. Thus when the pipes and

radiators were filled with steam (there being no air left), no pressure

was set up to resist the circulation of the water vapor, and when the

hot steam condensed in a radiator to a thimbleful of water, more steam

was drawn in to take its place, for no air could enter the pipes. In

this way the quantity of steam delivered to the radiators could be

regulated by a special valve with a varying number of ports, and by

turning the valve to a certain position enough steam would be permitted

to enter the radiator to keep it half full, or by shifting the valve

to another point enough steam would enter to fill the radiator to

three-quarters of its capacity. In fact, the requisite amount of steam

could be admitted to the radiator to balance the speed of condensation

and retain whatever level of steam in it was desirable. Thus the steam

system became at once a flexible system of heating, and could meet the

changing requirements of the weather.

[Illustration: Hot water radiator heated by steam]

A further development of the hot-water system then came about. In this

device the radiators were made to contain water, but the heat was

circulated through the pipes by means of steam. This steam was poured

over the surface of the water in the radiator and transferred its heat

to it. According to the quantity of steam poured over the water, the

latter could be heated to various temperatures. Of course the water in

the radiator was the medium for distributing the heat outward from the

radiator itself.

Still another improvement was made upon the hot-water system by

introducing the principle of the closed expansion tank. In the ordinary

system the water is allowed to expand at the top through an expansion

tank, so that the actual pressure on the water of the system is

atmospheric. Under this pressure the temperature of the water cannot be

raised to more than 212 degrees Fahrenheit, for beyond this it boils

and changes to steam. However, in the closed-tank system a so-called

heat-generator is added on the line leading to the expansion tank,

which, by means of a column of mercury, is capable of adding 10 pounds

more pressure than the atmosphere to the water in the system, and thus

raising the boiling-point to about 240 degrees. This generator is so

designed, however, that, although it adds this greater pressure to

the water, yet the natural expansion of the water in the system is

permitted through it in case of emergency. By permitting the raising of

the temperature of the water, the size of radiators can be cut down 50

per cent, which, of course, reduces the quantity of water needed and

permits a quicker heating of the system when the fire is started. Thus

a saving of fuel is accomplished and the disadvantage of the ordinary

hot-water system is eliminated; namely, the long time required to get

hot water in the radiators after the fire is started in the morning

from its banked condition of the previous night.

[Illustration: Pipeless Furnace]

However, the genius of the inventor was not at rest on the problem of

warm-air heating, for he discovered that he could abolish the flues,

which he once thought were essential, and use but one register and one

flue. This is called the pipeless furnace. A register is employed

which has an outer and inner section. The outer section permits the

cold air from the house to pass down through it and over the drum of

the furnace. The inner section of the register permits this hot air to

escape upward and through the house by natural distribution. Thus the

hot air rises from, and the cool air settles back into, the furnace

without utilizing flues. The circulation of this system was found to

be superior to the older method as ordinarily installed, and very much

cheaper to install. In fact, it is the cheapest of all systems of

heating. It is especially adapted to the small, low-cost house.

[Illustration: Hot Water Heating—Boiler in Dining-Room]

To reduce the cost of hot-water heating and make it also available for

this class of small house, the manufacturers produced another type of

water heating-plant. In this device the water-heater was installed

in one of the rooms of the house, like a stove, but the exterior was

designed to serve as a hot-water radiator for the room in which it was

placed. From this heater pipes were taken off to distribute heat to

other radiators, located in adjoining rooms. The principle remains the

same as the former system; the only difference lies in the reduction of

cost by eliminating the boiler from the cellar and utilizing it to heat

the room in which it was placed.

Other attempts to improve the mechanics of heating have been more along

the line of perfecting the operation of valves or the utilization of

other fuels than coal. Gas-radiators have been tried, but they are so

expensive to operate in most parts of the country that they are not

always suited to the needs of the small house. Electric heaters, too,

are not within the pocketbook of the average person owning the small

house. Fuel oil-burners also have been devised to take the place of the

coal-grate. Wherever oil is cheap enough to permit their use they are

great labor-savers, since they eliminate all the shovelling of coal and

handling of ashes. These will be discussed later.

Briefly, then, the available systems for the heating of the small house

are:

_Hot-air.—a._ Furnace with flues.

_b._ Furnace without flues.

_Steam.—a._ Ordinary gravity system.

One-pipe.

Two-pipe.

_b._ Vapor-vacuum system.

_Hot-water.—a._ Ordinary open-tank system.

One-pipe.

Two-pipe.

_b._ Closed-tank system.

_c._ Special open-tank system with boiler used

as radiator.

_d._ Patent system using water in radiators but

steam for circulation.

_Methods Employed in Calculating the Required Size of Heater_

The basis of calculating the required size of any one of the systems

previously mentioned is to assume that a certain temperature of heat

is to be maintained when the weather is zero, and then by means of the

laws of heat transmission estimate the quantity of heat lost per hour

from the house. The amount of heat lost per hour is, of course, the

quantity which the heating system must supply. Knowing this, a system

is installed which is capable of supplying this heat loss.

In such devices as the warm-air furnace the required size can be

computed directly to meet the heat loss, but where radiators are used

the required sizes of these must first be determined to offset the

losses from the rooms in which they are installed, and then the size of

the heater must be estimated to supply sufficient heat to the radiators

and to make up for the losses of heat through the distributing-pipes.

The usual temperature to which the small house is heated when it is

zero outside is 70 degrees Fahrenheit. It is then assumed that a

certain quantity of heat is lost through the walls of the house by

radiation and convection and conduction, and another quantity lost by

the leakage of warm air out through the window-cracks. (The quantity of

heat is measured in British thermal units, called B. T. U.’s.)

To understand the manner by which heat is lost through the exterior

walls, it is necessary to know the meaning of radiation, convection,

and conduction.

By standing before an open fire the heat given off by radiation can be

observed by shutting it off with a piece of paper held between the face

and the fire. This is the transmission of the heat through the ether,

and is similar to the transmission of light, since this heat will pass

through glass, like light.

Convection of heat is illustrated by heating air in one place and

transferring that air to another place, where it will give up its heat

to surrounding bodies.

Conduction of heat is illustrated by heating the end of an iron rod and

noticing that the heat will eventually be transmitted along the length

of it to the other end.

The heat within a house escapes from the interior to the colder

atmosphere of the exterior through the walls, by radiation through the

glass windows and the substance of the walls, by the convection action

of the warm air of the interior giving up its heat to the interior

face of the wall and the cold air of the exterior extracting this heat

from the exterior face and carrying it off, and also by the action of

conduction of the materials of which the wall is composed.

The quantity of heat lost is measured by the number of B. T. U.’s lost

through one square foot of the wall each hour. As the window-glass

loses heat through it more quickly than the wall, it is necessary to

calculate this separately. The process, then, for estimating the heat

loss from a room is as follows:

1. Estimate the number of square feet of exposed wall surface

in the room, including windows.

2. Subtract from the above the area of the windows to find the

net wall area.

3. Multiply this net wall area by the number of B. T. U.’s

which the wall loses per square foot of surface for each hour.

These factors are given in the following table:

Zero outside and 70 degrees

inside—Number of B. T. U.’s

TYPE OF WALL lost for each square foot of

wall surface each hour

Brick wall, furred and plastered:

8" thick 21.0

12" thick 17.5

Frame wall, sheathed, clapboarded,

and plastered 21.7 (with building-paper use

20.3)

Hollow-tile wall and concrete and stone have factors about the same as

for the furred brick wall.

[Illustration: SIDE ELEVATION]

4. Add to this the number of B. T. U.’s lost per

hour through the windows. This is determined by

multiplying the area of the windows by the heat

loss in B. T. U.’s per hour for each square foot of

window, which is 78.8 for single windows, and where

storm-windows are added it is 31.5 B. T. U.’s.

5. This total sum is the number of B. T. U.’s lost

through walls and windows for each hour.

6. To this must be added the heat lost by leakage

through the window-cracks. This is secured by

measuring the length of window-cracks on the

side which has the greatest length of crack and

multiplying this by 168, or the number of B. T. U.’s

lost each hour for each linear foot of window-crack.

For very tight windows reduce above to 84.

7. The total of all the above gives the number of

B. T. U.’s lost each hour from the room when the

outside temperature is zero and the inside is 70

degrees Fahrenheit.

Knowing the quantity of heat lost per hour, a radiator must be

installed which will supply this amount per hour. As the average

steam-radiator supplies about 250 B. T. U.’s per hour from each square

foot of its surface, the number of square feet required for a radiator

to be installed in the room can be found by dividing 250 into the

number of B. T. U.’s which were found to be lost from the room each

hour.

A hot-water radiator gives off about 150 B. T. U.’s per hour for

each square foot of surface, so that the radiator is generally about

one-third larger than the steam-radiator.

Knowing the required number of feet of radiation for the radiator, the

proper size can be selected from the manufacturer’s catalogue.

By lumping the total number of square feet of radiation for all the

radiators throughout the house together and adding 35 per cent to this

to make up for loss through pipes and under-rating of boilers, the size

of the boiler can be selected from the catalogue to fit this need.

To estimate the size of a warm-air furnace, the total quantity of heat

lost from all the rooms of the house should be calculated in the same

way, and then 25 per cent added to allow for cold attics and exposure.

This quantity should then be multiplied by 2.4 and divided by 8,000

to find the number of pounds of coal which will be required to be

burned per hour. By dividing this amount by 5, the grate area of the

required furnace can be found, and the correct size selected from the

manufacturer’s catalogue.

The Construction of the Small House A Simple and Useful Source of Information of the Methods of Building Small American Homes, for Anyone Planning to Build · 第 63 / 98 题