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126<br />

grade" temperature scale, and is the standard for<br />

scientific work.<br />

Certain properties of matter such as the expansion<br />

of gases change with temperature according to known<br />

laws. From these laws the absolute zero of temperature<br />

has been found to correspond to minus 2/3 deg.<br />

C, that is, 273 C. deg. below the temperature of melting<br />

ice.<br />

Before the Centigrade scale was established, another<br />

arbitrary but less scientific temperature scale<br />

had come into extensive use, in English speaking<br />

countries. This was the Fahrenheit scale, and is still<br />

the one in popular use in the United States. We<br />

therefore may speak of temperature in either of these<br />

scales, and it is fortunately easy to change from one<br />

to another.<br />

The melting point of ice corresponds to 32 degrees<br />

on the Fahrenheit scale, and the boiling point of water<br />

to 212 degrees. We may lay off the two scales side<br />

by side as shown in Fig. 71. The figure, might in<br />

fact, represent two ordinary mercurial thermometers,<br />

one graduated in Centigrade, the other in Fahrenheit<br />

Since a temperature of 32 deg. F. corresponds to 0<br />

deg. C, and 212 deg. F corresponds to 100 deg. C, it<br />

follows that 100 divisions on the Centigrade scale are<br />

equivalent to 212 — 32 or 180 divisions on the Fahrenheit<br />

scale. One degree Fahrenheit, therefore, equals<br />

100<br />

or 5/9 of a degree Centigrade, and we may change<br />

180<br />

from one scale to the other by the following simple<br />

formula:<br />

Fahrenheit to Centigrade: Substract 32 deg. and<br />

multiply by 5/9.<br />

Centigrade to Fahrenheit: Multiply by 9/5 and add<br />

32 deg.<br />

Examples:<br />

100° F 1292° F.<br />

—32 —32<br />

68 X 5/9 = 37.7°C.<br />

1000° C. X 9/5 = 1800<br />

32<br />

F<strong>org</strong>ing- Stamping - Heat Tieating<br />

1260 X 5/9 = 700° C.<br />

-20° C. X 9/5 = -36<br />

32<br />

183:2° f - 4°F-<br />

It is important to know how to make this conversion,<br />

but where many conversions are to be made<br />

it saves time to have a conversion table in which<br />

corresponding temperatures in the two scales are<br />

given in parallel columns. Many such tables have<br />

been published. A convenient one for use in connection<br />

with heat treating operations is given in<br />

Fig. 72. This table gives equivalent Fahrenheit and<br />

Centigrade temperatures at intervals of 5 degrees<br />

Centigrade (9 deg. F.) over a range which covers<br />

all ordinary metallurgical work. The columns have<br />

been arranged for easy reading and the Fahrenheit<br />

and Centigrade figures distinguished by different<br />

tvpe. For many purposes it is satisfactory to know<br />

the temperature to the nearest 5 deg. C. (that is,<br />

within plus or minus 2y deg. C). For somewhat<br />

greater accuracy, intermediate temperatures may be<br />

figured closely enough by taking 2 deg. F. as the<br />

equivalent of 1 deg. C, counting from the nearest even<br />

5 deg. C. For example :<br />

537° C. = 995 plus 4 = 999° F<br />

539° C. = 1004 minus 2 = 1002° F.<br />

This may be done mentally.<br />

April, 1925<br />

For complete accuracy, intermediate temperatures<br />

may readily be interpolated on the basis that 5 deg.<br />

C. = 9 deg. F. Thus, to change 537 deg. C. to Fahrenheit<br />

:<br />

535° C =995° F.<br />

2° C. X 9/5 = 3.6<br />

Or, 1000° F. to Centigrade<br />

Answer 998.6° F.<br />

995° F.<br />

5 X 5/9<br />

= 535° C.<br />

= 2.8<br />

Answer 537.8° C.<br />

PART 2.<br />

METHODS OF MEASURING TEMPERATURE<br />

Gas Thermometer.<br />

If the temperature of a certain quantity of a pure gas<br />

is raised, and it is meanwhile kept at constant volume, the<br />

pressure will increase in proportion to the absolute temperature.<br />

p v = K T<br />

Where p = pressure<br />

v = volume<br />

T = absolute temperature<br />

K = a constant, depending upon the<br />

nature of the gas<br />

The absolute temperature T is equal to the Centrigrade<br />

temperature plus 273 degrees.<br />

By confining a gas in a container of known volume,<br />

heating it and measuring the pressure, the temperature<br />

scale may be extended as high as the material of the container,<br />

and other limitations of the apparatus, will permit.<br />

In this way, temperatures up to about 1500 deg. (J. have<br />

been established with considerable accuracy. Such an apparatus<br />

is called a "gas thermometer" or "gas pyrometer".<br />

It is fragile and tedious to operate, and is used only as a<br />

laboratory tool to standardize other and more convenient<br />

means of temperature measurement.<br />

Melting, Freezing, Boiling Point.<br />

By the aid of a gas pyrometer the melting or boiling<br />

temperatures of certain materials, such as pure metals or<br />

salts, may be found, and these may then be used as standards<br />

of temperature in calibrating pyrometers of various<br />

types. This will be discussed further under "Calibration"<br />

Expansion.<br />

The commonest type of temperature measuring instrument<br />

is the familiar mercurial thermometer. This consists<br />

of a glass bulb containing mercury, connected to a<br />

stem in which there is a fine capillary tube. The mercury<br />

in the bulb expands when heated, forcing a column<br />

of mercury up into the tube. The amount of mercury in<br />

the tube varies directly with the temperature, and a scale<br />

on the tube may therefore be marked off in degrees C<br />

or F. Thermometers of this type have been developed for<br />

commercial use up to about 550 deg. C, which is the

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