one illustrated in Fig. 106 may prove serviceable before furnaces
required for plate work, where the doors are often only opened
for a moment at a time. This shield can be placed far enough in
front of the furnace, that it will be possible to work under it
or around it, in removing bulky work from the furnace, and yet
it will afford the furnace tender some relief from the excessive
glare that will come out the wide-opened door. To have this shield
of light weight so that it may be readily pushed aside when not
wanted, the frame may be made up of pipe and fittings, and a piece
of thin sheet steel fastened in the panel by rings about the frame.
About the most disagreeable task in a heat-treating shop is the
removal of the pots from the case-hardening furnaces; these must
be handled at a bright red heat in order that their contents may be
dumped into the quenching tank with a minimum-time contact with the
air, and before they have cooled sufficiently to require reheating.
Facing the heat before the large open doors of the majority of
these furnaces, in a man-killing task even when the weather is
moderately cool. The boxes soon become more or less distorted,
and then even the best of lifting devices will not remove a hot
pot without several minutes labor in front of the doors.
In Fig. 107 is shown a method of arranging a shield on one type of
charging and removing truck. This shield cannot afford more than
a partial protection to the body of the furnace tender, because
he must be able to see around it, and in some cases even push it
partly through the door of the furnace, but even small as it is it
may still afford some welcome protection. The great advantage in
this case of having the shield on the truck instead of stationary
in front of the furnace, is that it still affords protection as
long as the hot pot is being handled through the shop on its way
to the quenching tank.
It might be interesting to many engaged in the heat-treating or
case hardening of steel parts, to make a special note of the design
of the truck that is illustrated in connection with the shield;
the general form is shown although the actual details for the
construction of such a truck are lacking; these being simple, may be
readily worked out by anyone wishing to build one. This is considered
to be one of the quickest and easiest operated devices for the
removal of this class of work from the furnace. To be sure it may
only be used where the floor of the furnace has been built level
with the floor of the room, but many of the modern furnaces of
this class are so designed.
The pack-hardening pots are cast with legs, from two to three inches
high, to permit the circulation of the hot gases, and so heat more
quickly. Between these legs and under the body of the pot, the two
forward prongs of the truck are pushed, tilting the outer handle
to make these prongs as low as possible. The handle is then lowered
and, as it has a good leverage, the pot is easily raised from the
floor, and the truck and its load rolled out.
HEATING OF MANGANESE STEEL.--Another form of heat-treating furnace
is that which is used for the heating of manganese and other alloy
steels, which after having been brought to the proper heat are drawn
from the furnace into an immediate quenching tank. With manganese
steel in particular, the parts are so fragile and easily damaged
while hot that it is frequent practice to have a sloping platform
immediately in front of the furnace door down which the castings
may slide into a tank below the floor level. Such a furnace with
a quenching tank in front of its door is shown in Fig. 108.
These tanks are covered with plates while charging the furnace
and the cold castings are placed in a moderately cool furnace.
Since some of these steels must not be charged into a furnace where
the heat is extreme but should be brought up to their final heat
gradually, there is little discomfort during the charging process.
When quenching, however, from a temperature of 1,800° to 1,900°,
it is extremely unpleasant in front of the doors. The swinging
shield is here adapted to give protection for this work. As will
be noted it is hung a sufficient distance in front of the doors,
that it may not interfere with the castings as they come from the
furnace, and slide down into the tank.
To facilitate the work, and avoid the necessity of working with
the bars outside the edges of the shield, the slot-like hole is
cut in the center of the shield, and through this the bars or rakes
for dragging out the castings are easily inserted and manipulated.
The advantage of such a swinging shield is that it may be readily
moved from side to side, or forward and back as occasion requires.
FURNACE DATA
In order to give definite information concerning furnaces, fuels
etc., the following data is quoted from a paper by Seth A. Moulton
and W. H. Lyman before the Steel Heat Treaters Society in September,
1920.
This considers a factory producing 30,000 lb. of automobile gears
per 24 hr. The transmission gears will be of high-carbon steel and
the differential of low-carbon steel, carburized. The heat-treating
equipment required is:
1. Annealing furnaces 1,400 to 1,600°F.
2. Carburizing furnaces 1,700 to 1,800°F.
3. Hardening furnaces 1,450 to 1,550°F.
4. Drawing furnaces 350 to 950°F.
All of the forging blanks are annealed before machining, about
three-quarters of the machined gears and parts are carburized,
all the carburized gears are given a double treatment for core and
case, all gears and parts are hardened and all parts are drawn.
The possible sources of heat supply and their values are as follows:--
1. Oil 140,000 B.t.u. per gallon
2. Natural gas 1,100 B.t.u. per cubic foot
3. City gas 650 B.t.u. per cubic foot
4. Water gas 300 B.t.u. per cubic foot
5. Producer gas 170 B.t.u. per cubic foot
6. Coal 12,000 B.t.u. per pound
7. Electric current 3,412 B.t.u. per kilowatt-hour
For the heat treatment specified only comparatively low temperatures
are required. No difficulty will be experienced in attaining the
desired maximum temperature of 1,800°F. with any of the heating
medium above enumerated; but it should be noted that the producer
gas with a B.t.u. content of 170 per cubic foot and the electric
current would require _specially_ designed furnaces to obtain higher
temperatures than 1800°F.
TABLE 28.--COMPARATTVE OPERATING COSTS
Assuming
Cost of oil- and gas-fired furnaces
installed as $100.00 per square foot of hearth
Cost of coal-fired furnace installed as 150.00 per square foot of hearth
Cost of electric furnace 100 kw.
capacity installed as 90.00 per kilowatt
Cost of electric furnace 150 kw.
capacity installed as 70.00 per kilowatt
Output 3,000 lb. charge, 8 hr. heat carburizing, 2 hr. heating
only. Annual service 7,200 hr. Fixed charges including interest,
depreciation, taxes, insurance and maintenance 15 per cent. Extra
operating labor for coal-fired furnace 60 cts. per hour, one man
four furnaces.
COST OF VARIOUS TYPES OF FURNACES
-------------------------------------------------------------------------------
| Class fuel | Fuel per | Unit fuel|Installation|Efficiency| Fixed |Cost per
| | charge | cost | cost | per cent |charges| charge
-|------------|------------|----------|------------|----------|-------|--------
| 1 | 2 | 3 | 4 | 5 | 6 | 7
-|------------|------------|----------|------------|----------|-------|--------
Carburizing
-|------------|------------|----------|------------|----------|-------|--------
1|Oil | 52.0 gal. |$0.15 gal.| $2,400.00 | 12.6 | $.40 | $8.20
2|Natural gas | 4.4 M | 0.50 M | 2,400.00 | 18.8 | 0.40 | 2.60
3|City gas | 8.3 M | 0.80 M | 2,400.00 | 17.0 | 0.40 | 7.04
4|Water gas | 18.7 M | 0.40 | 2,400.00 | 16.4 | 0.40 | 7.88
5|Producer gas| 37.3 M | 0.10 M | 2,400.00 | 14.5 | 0.40 | 4.13
6|Coal |814.0 lb. | 6.00 ton | 3,600.00 | 9.4 | 0.60 | 3.98
7|Electricity |500.0 kw-hr.| 0.015 kw.| 9,000.00 | 53.0 | 1.50 | 9.00
-|------------|------------|----------|------------|----------|-------|--------
Heating
-|------------|------------|----------|------------|----------|-------|--------
1|Oil | 30.8 gal. | 0.15 gal.| 2,400.00 | 21.4 | 0.10 | 4.72
2|Natural gas | 2.61 M | 0.50 M | 2,400.00 | 32.0 | 0.10 | 1.40
3|City gas | 4.9 M | 0.80 M | 2,400.00 | 28.8 | 0.10 | 4.02
4|Water gas | 11.1 M | 0.40 M | 2,400.00 | 27.6 | 0.10 | 4.54
5|Producer gas| 22.1 M | 0.10 M | 2,400.00 | 24.6 | 0.10 | 2.31
6|Coal |348.0 lb. | 6.00 ton | 3,600.00 | 22.0 | 0.15 | 1.38
7|Electricity |329.0 kw-hr.| 0.015 kw.| 10,500.00 | 81.75 | 0.44 | 5.38
-------------------------------------------------------------------------------
This shows but two of the operations and for a single furnace.
The total costs for all operations on the 30,000 lb. of gears per
24 hr. is shown in Table 29.
TABLE 29.--COMPARATIVE ANNUAL PRODUCTION COSTS FOR 30,000 POUNDS
OUTPUT IN 24 HOURS
----------------------------------------------------------
No. | Equipment | Installation
| | cost
-----|-------------------------------------|--------------
1 | 2 | 3
| |
I | Oil | $179,000.00
II | Oil and electric | 213,000.00
III | Natural gas | 117,000.00
IV | (A) Natural gas containing furnaces | 120,000.00
V | Natural gas and electric | 181,000.00
VI | City gas | 122,000.00
VII | City gas and electric | 182,000.00
VIII| Water gas | 214,000.00
IX | Water gas and electric | 238,000.00
X | Producer gas | 246,000.00
XI | Producer gas and electric | 255,000.00
XII | Coal and electric | 194,000.00
XIII| Electric | 257,000.00
----------------------------------------------------------
---------------------------------------------------------------------
| Annual operating expenses | | Cost
No. |----------------------------------------| Total | per lb.
| Fixed | Heat | Labor | | metal,
| charges | | | | cents
-----|------------|-------------|-------------|-------------|--------
1 | 4 | 5 | 6 | 7 | 8
| | | | |
I | $26,850.00 | $156,000.00 | $105,000.00 | $287,850.00 | $3.19
II | 31,950.00 | 142,770.00 | 97,000.00 | 271,720.00 | 3.02
III | 17,550.00 | 44,250.00 | 97,000.00 | 158,800.00 | 1.78
IV | 18,000.00 | 41,000.00 | 94,000.00 | 153,000.00 | 1.70
V | 27,150.00 | 73,820.00 | 90,000.00 | 190,970.00 | 2.13
VI | 18,300.00 | 123,200.00 | 94,000.00 | 235,500.00 | 2.62
VII | 27,300.00 | 128,820.00 | 90,000.00 | 246,020.00 | 2.74
VIII| 18,600.00 | 104,000.00 | 94,000.00 | 216,600.00 | 2.41
IX | 27,450.00 | 117,420.00 | 90,000.00 | 234,870.00 | 2.62
X | 18,900.00 | 69,300.00 | 90,000.00 | 178,200.00 | 1.98
XI | 27,750.00 | 92,520.00 | 90,000.00 | 210,270.00 | 2.34
XII | 29,100.00 | 87,220.00 | 90,000.00 | 206,320.00 | 2.30
XIII| 38,550.00 | 135,000.00 | 84,000.00 | 257,550.00 | 2.86
---------------------------------------------------------------------
NOTE.--Producer plant fixed charges are included in the cost of
gas and are charged as "heat" in column 5, so they are omitted
from column 4.
CHAPTER XII
PYROMETRY AND PYROMETERS
A knowledge of the fundamental principles of pyrometry, or the
measurement of temperatures, is quite necessary for one engaged
in the heat treatment of steel. It is only by careful measurement
and control of the heating of steel that the full benefit of a
heat-treating operation is secured.
Before the advent of the thermo-couple, methods of temperature
measurement were very crude. The blacksmith depended on his eyes
to tell him when the proper temperature was reached, and of course
the "color" appeared different on light or dark days. "Cherry"
to one man was "orange" to another, and it was therefore almost
impossible to formulate any treatment which could be applied by
several men to secure the same results.
One of the early methods of measuring temperatures was the "iron
ball" method. In this method, an iron ball, to which a wire was
attached, was placed in the furnace and when it had reached the
temperature of the furnace, it was quickly removed by means of
the wire, and suspended in a can containing a known quantity of
water; the volume of water being such that the heat would not cause
it to boil. The rise in temperature of the water was measured by a
thermometer, and, knowing the heat capacity of the iron ball and
that of the water, the temperature of the ball, and therefore the
furnace, could be calculated. Usually a set of tables was prepared
to simplify the calculations. The iron ball, however, scaled, and
changed in weight with repeated use, making the determinations
less and less accurate. A copper ball was often used to decrease
this change, but even that was subject to error. This method is
still sometimes used, but for uniform results, a platinum ball,
which will not scale or change in weight, is necessary, and the
cost of this ball, together with the slowness of the method, have
rendered the practice obsolete, especially in view of modern
developments in accurate pyrometry.
PYROMETERS
Armor plate makers sometimes use the copper ball or Siemens' water
pyrometer because they can place a number of the balls or weights on
the plate in locations where it is difficult to use other pyrometers.
One of these pyrometers is shown in section in Fig. 109.
SIEMENS' WATER PYROMETER.--It consists of a cylindrical copper vessel
provided with a handle and containing a second smaller copper vessel
with double walls. An air space _a_ separates the two vessels, and
a layer of felt the two walls of the inner one, in order to retard
the exchange of temperature with the surroundings. The capacity
of the inner vessel is a little more than one pint. A mercury
thermometer _b_ is fixed close to the wall of the inner vessel,
its lower part being protected by a perforated brass tube, whilst
the upper projects above the vessel and is divided as usual on the
stem into degrees, Fahrenheit or Centigrade, as desired. At the
side of the thermometer there is a small brass scale _c_, which
slides up and down, and on which the high temperatures are marked
in the same degrees as those in which the mercury thermometer is
divided; on a level with the zero division of the brass scale a
small pointer is fixed, which traverses the scale of the thermometer.
[Illustration: FIG. 109.--Siemens' copper-ball pyrometer.]
Short cylinders _d_, of either copper, iron or platinum, are supplied
with the pyrometer, which are so adjusted that their heat capacity at
ordinary temperature is equal to one-fiftieth of that of the copper
vessel filled with one pint of water. As, however, the specific heat
of metals increases with the temperature, allowance is made on the
brass sliding scales, which are divided according to the metal used
for the pyrometer cylinder _d_. It will therefore be understood that
a different sliding scale is required for the particular kind of
metal of which a cylinder is composed. In order to obtain accurate
measurements, each sliding scale must be used only in conjunction
with its own thermometer, and in case the latter breaks a new scale
must be made and graduated for the new thermometer.
The water pyrometer is used as follows:
Exactly one pint (0.568 liter) of clean water, perfectly distilled
or rain water, is poured into the copper vessel, and the pyrometer
is left for a few minutes to allow the thermometer to attain the
temperature of the water.
The brass scale _c_ is then set with its pointer opposite the
temperature of the water as shown by the thermometer. Meanwhile
one of the metal cylinders has been exposed to the high temperature
which is to be measured, and after allowing sufficient time for
it to acquire that temperature, it is rapidly removed and dropped
into the pyrometer vessel without splashing any of the water out.
The temperature of the water will rise until, after a little while,
the mercury of the thermometer has become stationary. When this
is observed the degrees of the thermometer are read off, as well
as those on the brass scale _c_ opposite the top of the mercury.
The sum of these two values together gives the temperature of the
flue, furnace or other heated space in which the metal cylinder
had been placed. With cylinders of copper and iron, temperatures up
to 1,800°F. (1,000°C.) can be measured, but with platinum cylinders
the limit is 2,700°F. (1,500°C.).
For ordinary furnace work either copper or wrought-iron cylinders
may be used. Iron cylinders possess a higher melting point and have
less tendency to scale than those of copper, but the latter are
much less affected by the corrosive action of the furnace gases;
platinum is, of course, not subject to any of these disadvantages.
The weight to which the different metal cylinders are adjusted is
as follows:
Copper 137.0 grams
Wrought-iron 112.0 grams
Platinum 402.6 grams
In course of time the cylinders lose weight by scaling; but tables
are provided giving multipliers for the diminished weights, by
which the reading on the brass scale should be multiplied.
THE THERMO-COUPLE
With the application of the thermo-couple, the measurement of
temperatures, between, say, 700 and 2,500°F., was made more simple
and precise. The theory of the thermo-couple is simple; it is that
if two bars, rods, or wires of different metals are joined together
at their ends, when heated so that one junction is hotter than the
other, an electromotive force is set up through the metals, which
will increase with the increase of the _difference_ of temperature
between the two junctions. This electromotive force, or voltage, may
be measured, and, from a chart previously prepared, the temperature
determined. In most pyrometers, of course, the temperatures are
inscribed directly on the voltmeter, but the fact remains that
it is the voltage of a small electric current, and not heat, that
is actually measured.
There are two common types of thermo-couples, the first making use
of common, inexpensive metals, such as iron wire and nichrome wire.
This is the so-called "base metal" couple. The other is composed of
expensive metals such as platinum wire, and a wire of an alloy of
platinum with 10 per cent of rhodium or iridium. This is called
the "rare metal" couple, and because its component metals are less
affected by heat, it lasts longer, and varies less than the base
metal couple.
The cold junction of a thermo-couple may be connected by means
of copper wires to the voltmeter, although in some installations
of base metal couples, the wires forming the couple are themselves
extended to the voltmeter, making copper connections unnecessary.
From the foregoing, it may be seen that accurately to measure the
temperature of the hot end of a thermo-couple, we _must know the
temperature of the cold end_, as it is the _difference_ in the
temperatures that determines the voltmeter readings. This is absolutely
essential for precision, and its importance cannot be over-emphasized.
When pyrometers are used in daily operation, they should be checked
or calibrated two or three times a month, or even every week. Where
there are many in use, it is good practice to have a master pyrometer
of a rare metal couple, which is used only for checking up the
others. The master pyrometer, after calibrating against the melting
points of various substances, will have a calibration chart which
should be used in the checking operation.
It is customary now to send a rare metal couple to the Bureau of
Standards at Washington, where it is very carefully calibrated
for a nominal charge, and returned with the voltmeter readings
of a series of temperatures covering practically the whole range
of the couple. This couple is then used only for checking those
in daily use.
Pyrometer couples are more or less expensive, and should be cared
far when in use. The wires of the couple should be insulated from
each other by fireclay leads or tubes, and it is well to encase them
in a fireclay, porcelain, or quartz tube to keep out the furnace
gases, which in time destroy the hot junction. This tube of fireclay,
or porcelain, etc., should be protected against breakage by an
iron or nichrome tube, plugged or welded at the hot end. These
simple precautions will prolong the life of a couple and maintain
its precision longer.
Sometimes erroneous temperatures are recorded because the "cold
end" of the couple is too near the furnace and gets hot. This always
causes a temperature reading lower than the actual, and should be
guarded against. It is well to keep the cold end cool with water,
a wet cloth, or by placing it where coal air will circulate around
it. Best of all, is to have the cold junction in a box, together
with a thermometer, so that its temperature may definitely be known.
If this temperature should rise 20°F. on a hot day, a correction of
20°F. should be added to the pyrometer reading, and so on. In the
most up-to-date installations, this cold junction compensation is
taken care of automatically, a fact which indicates its importance.
Optical pyrometers are often used where it is impracticable to
use the thermo-couple, either because the temperature is so high
that it would destroy the couple, or the heat to be measured is
inaccessible to the couple of ordinary length. The temperatures of
slag or metal in furnaces or running through tap-holes or troughs
are often measured with optical pyrometers.
In one type of optical pyrometer, the observer focuses it on the
metal or slag and moves an adjustable dial or gage so as to get
an exact comparison between the color of the heat measured with
the calor of a lamp or screen in the pyrometer itself. This, of
course, requires practice, and judgment, and brings in the personal
equation. With care, however, very reliable temperature measurements
may be made. The temperatures of rails, as they leave the finishing
pass of a rolling mill, are measured in this way.
Another type of optical pyrometer is focused on the body, the
temperature of which is to be measured. The rays converge in the
telescope on metal cells, heating them, and thereby generating a
small electric current, the voltage of which is read an a calibrated
voltmeter similar to that used with the thermo-couple. The best
precision is obtained when an optical pyrometer is used each time
under similar conditions of light and the same observer.
Where it is impracticable to use either thermo-couples or optical
pyrometers, "sentinels" may be used. There are small cones or cylinders
made of salts or other substances of known melting points and covering
a wide range of temperatures.
If six of these "sentinels," melting respectively at 1,300°, 1,350°,
1,400°, 1,450°, 1,500°, and 1,550°F., were placed in a row in a
furnace, together with a piece of steel to be treated, and the
whole heated up uniformly, the sentinels would melt one by one and
the observer, by watching them through an opening in the furnace,
could tell when his furnace is at say 1,500° or between 1,500° and
1,550°, and regulate the heat accordingly.
A very accurate type of pyrometer, but one not so commonly used as
those previously described, is the resistance pyrometer. In this
type, the temperature is determined by measuring the resistance to an
electric current of a wire which is at the heat to be measured. This
wire is usually of platinum, wound around a quartz tube, the whole
being placed in the furnace. When the wire is at the temperature of
the furnace, it is connected by wires with a Wheatstone Bridge, a
delicate device for measuring electrical resistance, and an electric
current is passed through the wire. This current is balanced by
switching in resistances in the Wheatstone Bridge, until a delicate
electrical device shows that no current is flowing. The resistance
of the platinum wire at the heat to be measured is thus determined
on the "Bridge," and the temperature read off on a calibration
chart, which shows the resistance at various temperatures.
These are the common methods used to-day for measuring temperatures,
but whatever method is used, the observer should bear in mind that
the greatest precision is obtained, and hence the highest efficiency,
by keeping the apparatus in good working order, making sure that
conditions are the same each time, and calibrating or checking
against a standard at regular intervals.
THE PYROMETER AND ITS USE
In the heat treatment of steel, it has become absolutely necessary
that a measuring instrument be used which will give the operator an
exact reading of heat in furnace. There are a number of instruments
and devices manufactured for this purpose but any instrument that
will not give a direct reading without any guess work should have
no place in the heat-treating department.
A pyrometer installation is very simple and any of the leading
makers will furnish diagrams for the correct wiring and give detailed
information as to the proper care of, and how best to use their
particular instrument. There are certain general principles, however,
that must be observed by the operators and it cannot be too strongly
impressed upon them that the human factor involved is always the
deciding factor in the heat treatment of steel.
A pyrometer is merely an aid in the performance of doing good work,
and when carefully observed will help in giving a uniformity of
product and act as a check on careless operators. The operator
must bear in mind that although the reading on the pyrometer scale
gives a measure of the temperature where the junction of the two
metals is located, it will not give the temperature at the center
of work in the furnace, unless by previous tests, the heat for
penetrating a certain bulk of material has been decided on, and
the time necessary for such penetration is known.
Each analysis of plain carbon or alloy steel is a problem in itself.
Its critical temperatures will be located at slightly different
heats than for a steel which has a different proportion of alloying
elements. Furthermore, it takes time for metal to acquire the heat
of the furnace. Even the outer surface lags behind the temperature
of the furnace somewhat, and the center of the piece of steel lags
still further. It is apparent, therefore, that temperature, although
important, does not tell the whole story in heat treatment. _Time_
is also a factor.
Time at temperature is also of great importance because it takes
time, after the temperature has been reached, for the various internal
changes to take place. Hence the necessity for "soaking," when
annealing or normalizing. Therefore, a clock is as necessary to
the proper pyrometer equipment as the pyrometer itself.
For the purpose of general work where a wide range of steels or
a variable treatment is called for, it becomes necessary to have
the pyrometer calibrated constantly, and when no master instrument
is kept for this purpose the following method can be used to give
the desired results:
CALIBRATION OF PYROMETER WITH COMMON SALT
An easy and convenient method for standardization and one which
does not necessitate the use of an expensive laboratory equipment
is that based upon determining the melting point of common table
salt (sodium chloride). While theoretically salt that is chemically
pure should be used (and this is neither expensive nor difficult
to procure), commercial accuracy may be obtained by using common
table salt such as is sold by every grocer. The salt is melted in
a clean crucible of fireclay, iron or nickel, either in a furnace
or over a forge-fire, and then further heated until a temperature
of about 1,600 to 1,650°F. is attained. It is essential that this
crucible be clean because a slight admixture of a foreign substance
might noticeably change the melting point.
The thermo-couple to be calibrated is then removed from its protecting
tube and its hot end is immersed in the salt bath. When this end
has reached the temperature of the bath, the crucible is removed
from the source of heat and allowed to cool, and cooling readings
are then taken every 10 sec. on the milli-voltmeter or pyrometer. A
curve is then plotted by using time and temperature as coördinates,
and the temperature of the freezing point of salt, as indicated
by this particular thermocouple, is noted, _i.e._, at the point
where the temperature of the bath remains temporarily constant
while the salt is freezing. The length of time during which the
temperature is stationary depends on the size of the bath and the
rate of cooling, and is not a factor in the calibration. The melting
point of salt is 1,472°F., and the needed correction for the instrument
under observation can be readily applied.
It should not be understood from the above, however, that the salt-bath
calibration cannot be made without plotting a curve; in actual
practice at least a hundred tests are made without plotting any curve
to one in which it is done. The observer, if awake, may reasonably
be expected to have sufficient appreciation of the lapse of time
definitely to observe the temperature at which the falling pointer
of the instrument halts. The gradual dropping of the pointer before
freezing, unless there is a large mass of salt, takes place rapidly
enough for one to be sure that the temperature is constantly falling,
and the long period of rest during freezing is quite definite.
The procedure of detecting the solidification point of the salt
by the hesitation of the pointer without plotting any curve is
suggested because of its simplicity.
COMPLETE CALIBRATION OF PYROMETERS.--For the complete calibration
of a thermo-couple of unknown electromotive force, the new couple
may be checked against a standard instrument, placing the two bare
couples side by side in a suitable tube and taking frequent readings
over the range of temperatures desired.
If only one instrument, such as a millivoltmeter, is available,
and there is no standard couple at hand, the new couple may be
calibrated over a wide range of temperatures by the use of the following
standards:
Water, boiling point 212°F.
Tin, under charcoal, freezing point 450°F.
Lead, under charcoal, freezing point 621°F.
Zinc, under charcoal, freezing point 786°F.
Sulphur, boiling point 832°F.
Aluminum, under charcoal, freezing point 1,216°F.
Sodium chloride (salt), freezing point 1,474°F.
Potassium sulphate, freezing point 1,958°F.
A good practice is to make one pyrometer a standard; calibrate it
frequently by the melting-point-of-salt method, and each morning
check up every pyrometer in the works with the standard, making the
necessary corrections to be used for the day's work. By pursuing
this course systematically, the improved quality of the product
will much more than compensate for the extra work.
The purity of the substance affects its freezing or melting point.
The melting point of common salt is given in one widely used handbook
at 1,421°F., although chemically pure sodium chloride melts at
1,474°F. as shown above. A sufficient quantity for an extended
period should be secured. Test the melting point with a pyrometer
of known accuracy. Knowing this temperature it will be easy to
calibrate other pyrometers.
PLACING OF PYROMETERS.--When installing a pyrometer, care should be
taken that it reaches directly to the point desired to be measured,
that the cold junction is kept cold, and that the wires leading to
the recording instrument are kept in good shape. The length of
these lead wires have an effect; the longer they are, the lower
the apparent temperature.
When pyrometers placed in a number of furnaces are connected up
in series, and a multiple switch is used for control, it becomes
apparent that pyrometers could not be interchanged between furnaces
near and far from the instrument without affecting the uniformity
of product from each furnace.
Calibration can best be done without disturbing the working pyrometer,
by inserting the master instrument into each furnace separately, place
it alongside the hot junction of the working pyrometer, and compare
the reading given on the indicator connected with the multiple
switch.
Protection tubes should be replaced when cracked, as it is important
that no foreign substance is allowed to freeze in the tube, so
that the enclosed junction becomes a part of a solid mass joined
in electrical contact with the outside protecting tube. Wires over
the furnaces must be carefully inspected from time to time, as no
true reading can be had on an instrument, if insulation is burned
off and short circuits result.
If the standard calibrating instrument used contains a dry battery,
it should be examined from time to time to be sure it is in good
condition.
THE LEEDS AND NORTHRUP POTENTIOMETER SYSTEM
The potentiometer pyrometer system is both flexible and substantial
in that it is not affected by the jar and vibration of the factory
or the forge shop. Large or small couples, long or short leads
can be used without adjustment. The recording instrument may be
placed where it is most convenient, without regard to the distance
from the furnace.
ITS FUNDAMENTAL PRINCIPLE.--The potentiometer is the electrical
equivalent of the chemical balance, or balance arm scales. Measurements
are made with balance scales by varying known weights until they
equal the unknown weight. When the two are equal the scales stand
at zero, that is, in the position which they occupy when there is
no weight on either pan; the scales are then said to be balanced.
Measurements are made with the potentiometer by varying a known
electromotive force until it equals the unknown; when the two are
equal the index of the potentiometer, the galvanometer needle,
stands motionless as it is alternately connected and disconnected.
The variable known weights are units separate from the scales, but
the potentiometer provides its own variable known electromotive
force.
The potentiometer provides, first, a means of securing a known
variable electromotive force and, second, suitable electrical
connections for bringing that electromotive force to a point where
it may be balanced against the unknown electromotive force of the
couple. The two are connected with opposite polarity, or so that
the two e.m.f.s oppose one another. So long as one is stronger
than the other a current will flow through the couple; when the
two are equal no current will flow.
Figure 107 shows the wiring of the potentiometer in its simplest
form. The thermo-couple is at _H_, with its polarity as shown by
the symbols + and -. It is connected with the main circuit of the
potentiometer at the fixed point _D_ and the point _G_.
[Illustration: FIG. 110.--Simple potentiometer.]
A current from the dry cell _Ba_ is constantly flowing through the
main, or so-called potentiometer circuit, _ABCDGEF_. The section
_DGE_ of this circuit is a slide wire, uniform in resistance throughout
its length. The scale is fixed on this slide wire. The current
from the cell _Ba_ as it flows through _DGE_, undergoes a fall
in potential, setting up a difference in voltage, that is, an
electromotive force, between _D_ and _E_. There will also be
electromotive force between _D_ and all other points on the slide
wire. The polarity of this is in opposition to the polarity of the
thermo-couple which connects into the potentiometer at _D_ and
at _G_. By moving _G_ along the slide wire a point is found where
the voltage between _D_ and _G_ in the slide wire is just equal to
the voltage between _D_ and _G_ generated by the thermo-couple. A
galvanometer in the thermo-couple circuit indicates when the balance
point is reached, since at this point the galvanometer needle will
stand motionless when its circuit is opened and closed.
[Illustration: FIG. 111.--Standard cell potentiometer.]
The voltage in the slide wire will vary with the current flowing
through it from the cell _Ba_ and a means of standardizing this is
provided. _SC_, Fig. 111, is a cadmium cell whose voltage is constant.
It is connected at two points _C_ and _D_ to the potentiometer
circuit whenever the potentiometer current is to be standardized.
At this time the galvanometer is thrown in series with _SC_. The
variable rheostat _R_ is then adjusted until the current flowing
is such that as it flows through the standard resistance _CD_,
the fall in potential between _C_ and _D_ is just equal to the
voltage of the standard cell _SC_. At this time the galvanometer
will indicate a balance in the same way as when it was used with
a thermo-couple. By this operation the current in the slide wire
_DGE_ has been standardized.
[Illustration: FIG. 112.--Hand adjusted cold-end compensator.]
DEVELOPMENT OF THE WIRING SCHEME OF THE COLD-END COMPENSATOR.--The
net voltage generated by a thermo-couple depends upon the temperature
of the hot end and the temperature of the cold end. Therefore, any
method adopted for reading temperature by means of thermo-couples
must in some way provide a means of correcting for the temperature of
the cold end. The potentiometer may have either of two very simple
devices for this purpose. In one form the operator is required
to set a small index to a point on a scale corresponding to the
known cold junction temperature. In the other form an even more
simple automatic compensator is employed. The principle of each is
described in the succeeding paragraphs, in which the assumption is
made that the reader already understands the potentiometer principle
as described above.
As previously explained the voltage of the thermo-couple is measured
by balancing it against the voltage drop _DG_ in the potentiometer.
As shown in Fig. 111, the magnitude of the balancing voltage is
controlled by the position of _G_. Make _D_ movable as shown in Fig.
112 and the magnitude of the voltage _DG_ may be varied either from
the point _D_ or the point _G_. This gives a means of compensating
for cold end changes by setting the slider _D_. As the cold end
temperature rises the net voltage generated by the couple decreases,
assuming the hot end temperature to be constant. To balance this
decreased voltage the slider _D_ is moved along its scale to a new
point nearer _G_. In other words, the slider _D_ is moved along
its scale until it corresponds to the known temperature of the cold
end and then the potentiometer is balanced by moving the slider
_G_. The readings of _G_ will then be direct.
[Illustration: FIG. 113.--Another type of compensator.]
The same results will be obtained if a slide wire upon which _D_
bears is in parallel with the slide wire of _G_, as shown in Fig.
113.
AUTOMATIC COMPENSATOR.--It should be noted that the effect of moving
the contact _D_, Fig. 113, is to vary the ratio of the resistances
on the two sides of the point _D_ in the secondary slide wire. In
the recording pyrometers, an automatic compensator is employed.
This automatic compensator varies the ratio on the two sides of
the point _D_ in the following manner:
The point _D_, Fig. 114, is mechanically fixed; on one side of
_D_ is the constant resistance coil _M_, on the other the nickel
coil _N_. _N_ is placed at or near the cold end of the thermo-couple
(or couples). Nickel has a high temperature coefficient and the
electrical proportions of _M_ and _N_ are such that the resistance
change of _N_, as it varies with the temperature of the cold end,
has the same effect upon the balancing voltage between _D_ and
_G_ that the movement of the point _D_, Fig. 114, has in the
hand-operated compensator.
Instruments embodying these principles are shown in Figs. 115 to
117. The captions making their uses clear.
[Illustration: FIG. 114.--Automatic cold-end compensator.]
PLACING THE THERMO-COUPLES
The following illustrations from the Taylor Instrument Company
show different applications of the thermo-couples to furnaces of
various kinds. Figure 118 shows an oil-fired furnace with a simple
vertical installation. Figure 119 shows a method of imbedding the
thermo-couple in the floor of a furnace so as to require no space
in the heating chamber.
[Illustration: FIG. 115.--Potentiometer ready for use.]
Various methods of applying a pyrometer to common heat-treatment
furnaces are shown in Figs. 120 to 122.
[Illustration: FIG. 116.--Eight-point recording pyrometer-Carpenter
Steel Co.]
LEEDS AND NORTHRUP OPTICAL PYROMETER
The principles of this very popular method of measuring temperature
are sketched in Fig. 123.
[Illustration: FIG. 117.--Multiple-point thermocouple
recorder--Bethlehem Steel Co.]
[Illustration: FIG. 118.--Tycos pyrometer in oil-fired furnace.]
The instrument is light and portable, and can be sighted as easily
as an opera glass. The telescope, which is held in the hand, weighs
only 25 oz.; and the case containing the battery, rheostat and
milliammeter, which is slung from the shoulder, only 10 lb.
[Illustration: FIG. 119.--Thermocouple in floor of furnace.]
[Illustration: FIG. 120.--Pyrometer in gas furnace.]
A large surface to sight at is not required. So long as the image
formed by the objective is broader than the lamp filament, the
temperature can be measured accurately.
[Illustration: FIG. 121.--Tycos multiple indicating pyrometer and
recorder.]
[Illustration: FIG. 122.--Pyrometer in galvanizing tank.]
Distance does not matter, as the brightness of the image formed
by the lens is practically constant, regardless of the distance
of the instrument from the hot object.
[Illustration: FIG. 123.--Leeds & Northrup optical pyrometer.]
The manipulation is simple and rapid, consisting merely in the turning
of a knurled knob. The setting is made with great precision, due to
the rapid change in light intensity with change in temperature and
to the sensitiveness of the eye to differences of light intensity.
In the region of temperatures used for hardening steel, for example,
different observers using the instrument will agree within 3°C.
[Illustration: FIG. 124.--Too low.
FIG. 125.--Too high.
FIG. 126.--Correct.]
Only brightness, not color, of light is matched, as light of only
one color reaches the eye. Color blindness, therefore, is no hindrance
to the use of this method. The use of the instrument is shown in
Fig. 127.
OPTICAL SYSTEM AND ELECTRICAL CIRCUIT OF THE LEEDS & NORTHRUP OPTICAL
PYROMETER.--For extremely high temperature, the optical pyrometer is
largely used. This is a comparative method. By means of the rheostat
the current through the lamp is adjusted until the brightness of
the filament is just equal to the brightness of the image produced
by the lens _L_, Fig. 123, whereupon the filament blends with or
becomes indistinguishable in the background formed by the image
of the hot object. This adjustment can be made with great accuracy
and certainty, as the effect of radiation upon the eye varies some
twenty times faster than does the temperature at 1,600°F., and some
fourteen times faster at 3,400°F. When a balance has been obtained,
the observer notes the reading of the milliammeter. The temperature
corresponding to the current is then read from a calibration curve
supplied with the instrument.
[Illustration: FIG. 127.--Using the optical pyrometer.]
As the intensity of the light emitted at the higher temperatures
becomes dazzling, it is found desirable to introduce a piece of red
glass in the eye piece at _R_. This also eliminates any question
of matching colors, or of the observer's ability to distinguish
colors. It is further of value in dealing with bodies which do
not radiate light of the same composition as that emitted by a
black body, since nevertheless the intensity of radiation of any
one color from such bodies increases progressively in a definite
manner as the temperature rises. The intensity of this one color
can therefore be used as a measure of temperature for the body
in question. Figures 124 to 126 show the way it is read.
CORRECTION FOR COLD-JUNCTION ERRORS
The voltage generated by a thermo-couple of an electric pyrometer is
dependent on the difference in temperature between its hot junction,
inside the furnace, and the cold junction, or opposite end of the
thermo-couple to which the copper wires are connected. If the
temperature or this cold junction rises and falls, the indications
of the instrument will vary, although the hot junction in the furnace
may be at a constant temperature.
A cold-junction temperature of 75°F., or 25°C., is usually adopted
in commercial pyrometers, and the pointer on the pyrometer should
stand at this point on the scale when the hot junction is not heated.
If the cold-junction temperature rises about 75°F., where base metal
thermo-couples are used, the pyrometer will read approximately 1°
low for every 1° rise in temperature above 75°F. For example, if the
instrument is adjusted for a cold-junction temperature of 75°, and
the actual cold-junction temperature is 90°F., the pyrometer will
read 15° low. If, however, the cold-junction temperature falls below
75°F., the pyrometer will read high instead of low, approximately
1° for every 1° drop in temperature below 75°F.
With platinum thermo-couples, the error is approximately 1/2° for
1° change in temperature.
CORRECTION BY ZERO ADJUSTMENT.--Many pyrometers are supplied with
a zero adjuster, by means of which the pointer can be set to any
actual cold-junction temperature. If the cold junction of the
thermo-couple is in a temperature of 100°F., the pointer can be
set to this point on the scale, and the readings of the instrument
will be correct.
COMPENSATING LEADS.--By the use of compensating leads, formed of
the same material as the thermo-couple, the cold junction can be
removed from the head of the thermo-couple to a point 10, 20 or 50
ft. distant from the furnace, where the temperature is reasonably
constant. Where greater accuracy is desired, a common method is
to drive a 2-in. pipe, with a pointed closed end, some 10 to 20
ft. into the ground, as shown in Fig. 128. The compensating leads
are joined to the copper leads, and the junction forced down to
the bottom of the pipe. The cold junction is now in the ground,
beneath the building, at a depth at which the temperature is very
constant, about 70°F., throughout the year. This method will usually
control the cold-junction temperature within 5°F.
Where the greatest accuracy is desired a compensating box will
overcome cold-junction errors entirely. It consists of a case enclosing
a lamp and thermostat, which can be adjusted to maintain any desired
temperature, from 50 to 150°F. The compensating leads enter the box
and copper leads run from the compensating box to the instrument,
so that the cold junction is within the box. Figure 129 shows a
Brown compensating box.
[Illustration: FIG. 128.--Correcting cold-junction error.]
If it is desired to maintain the cold junction at 100°: the thermostat
is set at this point, and the lamp, being wired to the 110- or
220-volt lighting circuit, will light and heat the box until 100°
is reached, when the thermostat will open the circuit and the light
is extinguished. The box will now cool down to 98°, when the circuit
is again closed, the lamp lights, the box heats up, and the operation
is repeated.
[Illustration: FIG. 129.--Compensating box.]
BROWN AUTOMATIC SIGNALING PYROMETER
In large heat-treating plants it has been customary to maintain
an operator at a central pyrometer, and by colored electric lights
at the furnaces, signal whether the temperatures are correct or
not. It is common practice to locate three lights above each
furnace-red, white and green. The red light burns when the temperature
is too low, the white light when the temperature is within certain
limits--for example, 20°F. of the correct temperature--and the
green light when the temperature is too high.
[Illustration: FIG. 130.--Brown automatic signaling pyrometer.]
Instruments to operate the lights automatically have been devised and
one made by Brown is shown in Fig. 130. The same form of instrument is
used for this purpose to automatically control furnace temperatures,
and the pointer is depressed at intervals of every 10 sec. on contacts
corresponding to the red, white and green lights.
[Illustration: FIG. 131.--Automatic temperature control.]
AN AUTOMATIC TEMPERATURE CONTROL PYROMETER
Automatic temperature control instruments are similar to the Brown
indicating high resistance pyrometer with the exception that the
pointer is depressed at intervals of every 10 sec. upon contact-making
devices. No current passes through the pointer which simply depresses
the upper contact device tipped with platinum, which in turn comes
in contact with the lower contact device, platinum-tipped, and the
circuit is completed through these two contacts. The current is very
small, about 1/10 amp., as it is only necessary to operate the relay
which in turn operates the switch or valve. A small motor is used to
depress the pointer at regular intervals. The contact-making device
is adjustable throughout the scale range of the instrument, and an
index pointer indicates the point on the instrument at which the
temperature is being controlled. The space between the two contacts
on the high and low side, separated by insulating material, is
equivalent to 1 per cent of the scale range. A control of temperature
is therefore possible within 1 per cent of the total scale range.
Figure 131 shows this attached to a small furnace.
[Illustration: FIG. 132.--Portable thermocouple testing molten brass.]
PYROMETERS FOR MOLTEN METAL
Pyrometers for molten metal are connected to portable thermocouples
as in Fig. 132. Usually the pyrometer is portable, as shown in
this case, which is a Brown. Other methods of mounting for this
kind of work arc shown in Figs. 133 and 134. The bent mountings
are designed for molten metal, such as brass or copper and are
supplied with either clay, graphite or carborundum tubes. Fifteen
feet of connecting wire is usually supplied.
The angle mountings, Fig. 134, are recommended for baths such as
lead or cyanide. The horizontal arm is usually about 14 in. long,
and the whole mounting is easily taken apart making replacements
very easy. Details of the thermo-couple shown in Fig. 132 are given
in Fig. 135. This is a straight rod with a protector for the hand
of the operator. The lag in such couples is less than one minute.
These are Englehard mountings.
PROTECTORS FOR THERMO-COUPLES
Thermo-couples must be protected from the danger of mechanical
injury. For this purpose tubes of various refractory materials
are made to act as protectors. These in turn are usually protected
by outside metal tubes. Pure wrought iron is largely used for this
purpose as it scales and oxidizes very slowly. These tubes are
usually made from 2 to 4 in. shorter than the inner tubes. In lead
baths the iron tubes often have one end welded closed and are used
in connection with an angle form of mounting.
[Illustration: FIG. 133.--Bent handle thermocouple with protector.]
Where it is necessary for protecting tubes to project a considerable
distance into the furnace a tube made of nichrome is frequently used.
This is a comparatively new alloy which stands high temperatures
without bending. It is more costly than iron but also much more
durable.
When used in portable work and for high temperatures, pure nickel
tubes are sometimes used. There is also a special metal tube made
for use in cyanide. This metal withstands the intense penetrating
characteristics of cyanide. It lasts from six to ten months as
against a few days for the iron tube.
The inner tubes of refractory materials, also vary according to
the purposes for which they are to be used. They are as follows:
MARQUARDT MASS TUBES for temperatures up to 3,000°F., but they will
not stand sudden changes in temperature, such as in contact with
intermittent flames, without an extra outer covering of chamotte,
fireclay or carborundum.
[Illustration: FIG. 134.--Other styles of bent mounting.]
FUSED SILICA TUBES for continuous temperatures up to 1,800°F. and
intermittently up to 2,400°F. The expansion at various temperatures
is very small, which makes them of value for portable work. They
also resist most acids.
CHAMOTTE TUBES are useful up to 2,800°F. and are mechanically strong.
They have a small expansion and resist temperature changes well,
which makes them good as outside protectors for more fragile tubes.
They cannot be used in molten metals, or baths of any kind nor
in gases of an alkaline nature. They are used mainly to protect
a Marquardt mass or silica tube.
CARBORUNDUM TUBES are also used as outside protection to other
tubes. They stand sudden changes of temperature well and resist
all gases except chlorine, above 1,750°F. Especially useful in
protecting other tubes against molten aluminum, brass, copper and
similar metals.
CLAY TUBES are sometimes used in large annealing furnaces where they
are cemented into place, forming a sort of well for the insertion of
the thermo-couple. They are also used with portable thermo-couples
for obtaining the temperatures of molten iron and steel in ladles.
Used in this way they are naturally short-lived, but seem the best
for this purpose.
[Illustration: FIG. 135.--Straight thermocouple and guard.]
CORUNDITE TUBES are used as an outer protection for both the Marquardt
mass and the silica tubes for kilns and for glass furnaces. Graphite
tubes are also used in some cases for outer protections.
CALORIZED TUBES are wrought-iron pipe treated with aluminum vapor
which often doubles or even triples the life of the tube at high
temperature.
These tubes come in different sizes and lengths depending on the
uses for which they are intended. Heavy protecting outer tubes
may be only 1 in. in inside diameter and as much as 3 in. outside
diameter, while the inner tubes, such as the Marquardt mass and
silica tubes are usually about 3/4 in. outside and 3/8 in. inside
diameter. The length varies from 12 to 48 in. in most cases.
Special terminal heads are provided, with brass binding posts for
electrical connections, and with provisions for water cooling when
necessary.
APPENDIX
TABLE 32.--Temperature Conversion Tables.
TABLE 33.--Comparison Between Degrees Centigrade and Degrees Fahrenheit.
TABLE 34.--Weight of Round, Octagon and Square Carbon Tool Steel
per Foot.
TABLE 35.--Weight of Round Carbon Tool Steel 12 In. in Diameter
and Larger, per Foot.
TABLE 36.--Decimal Equivalents of a foot.
TEMPERATURE CONVERSION TABLES
By ALBERT SAUVEUR
--------------------------------------------------------------------------
-459.4 to 0 | 0 to 100 | 100 to 1000
-----------------|------------------------------|-------------------------
C. F. | C. F. | C. F. | C. F.| C. F.
-----------------|---------------|--------------|-----------|-------------
-273 -459.4 |-17.8 0 32 |10.0 50 122.0| 38 100 212|260 500 932
-268 -450 |-17.2 1 33.8|10.6 51 123.8| 43 110 230|266 510 950
-262 -440 |-16.7 2 35.6|11.1 52 125.6| 49 120 248|271 520 968
-257 -430 |-16.1 3 37.4|11.7 53 127.4| 54 130 266|277 530 986
-251 -420 |-15.6 4 39.2|12.2 54 129.2| 60 140 284|282 540 1004
-246 -410 |-15.0 5 41.0|12.8 55 131.0| 66 150 302|288 550 1022
-240 -400 |-14.4 6 42.8|13.3 56 132.8| 71 160 320|293 560 1040
-234 -390 |-13.9 7 44.6|13.9 57 134.6| 77 170 336|299 570 1058
-229 -380 |-13.3 8 46.4|14.4 58 136.4| 82 180 358|304 580 1076
-223 -370 |-12.8 9 48.2|15.0 59 138.2| 88 190 374|310 590 1094
-218 -360 |-12.2 10 50.0|15.6 60 140.0| 93 200 392|316 600 1112
-212 -350 |-11.7 11 51.8|16.1 61 141.8| 99 210 410|321 610 1130
-207 -340 |-11.1 12 53.6|16.7 62 143.6|100 212 413|327 620 1148
-201 -330 |-10.6 13 55.4|17.2 63 145.4|104 220 428|332 630 1166
-196 -320 |-10.0 14 57.2|17.8 64 147.2|110 230 446|338 640 1184
-190 -310 | -9.44 15 59.0|18.3 65 149.0|116 240 464|343 650 1202
-184 -300 | -8.89 16 61.8|18.9 66 150.8|121 250 482|349 660 1220
-179 -290 | -8.33 17 63.6|19.4 67 152.6|127 260 500|354 670 1238
-173 -280 | -7.78 18 65.4|20.0 68 154.4|132 270 518|360 680 1256
-169 -273 -459.4| -7.22 19 67.2|20.6 69 156.2|138 280 536|366 690 1274
-168 -270 -454 | -6.67 20 68.0|21.1 70 158.0|143 290 554|371 700 1292
-162 -260 -436 | -6.11 21 69.8|21.7 71 159.8|149 300 572|377 710 1310
-157 -250 -418 | -5.56 22 71.6|22.2 72 161.6|154 310 590|382 720 1328
-151 -240 -400 | -5.00 23 73.4|22.8 73 163.4|160 320 608|388 730 1346
-146 -230 -382 | -4.44 24 75.2|23.3 74 165.2|166 330 626|393 740 1364
-140 -220 -364 | -3.89 25 77.0|23.9 75 167.0|171 340 644|399 750 1382
-134 -210 -346 | -3.33 26 78.8|24.4 76 168.8|177 350 662|404 760 1400
-129 -200 -328 | -2.78 27 80.6|25.0 77 170.6|182 360 680|410 770 1418
-123 -190 -310 | -2.22 28 82.4|25.6 78 172.4|188 370 698|416 780 1436
-118 -180 -292 | -1.67 29 84.2|26.1 79 174.2|193 380 716|421 790 1454
-112 -170 -274 | -1.11 30 86.0|26.7 80 176.0|199 390 734|427 800 1472
-107 -160 -256 | -0.56 31 87.8|27.2 81 177.8|204 400 752|432 810 1490
-101 -150 -238 | 0 32 89.6|27.8 82 179.6|210 410 770|438 820 1508
-95.6 -140 -220 | 0.56 33 91.4|28.3 83 181.4|216 420 788|443 830 1526
-90.0 -130 -202 | 1.11 34 93.2|28.9 84 183.2|221 430 806|449 840 1544
-84.4 -120 -184 | 1.67 35 95.0|29.4 85 185.0|227 440 824|454 850 1562
-78.9 -110 -166 | 2.22 36 96.8|30.0 86 186.8|232 450 842|460 860 1580
-73.3 -100 -148 | 2.78 37 98.6|30.6 87 188.6|238 460 860|466 870 1598
-67.8 -90 -130 | 3.33 38 100.4|31.1 88 190.4|243 470 878|471 880 1616
-62.2 -80 -112 | 3.89 39 102.2|31.7 89 192.2|249 480 896|477 890 1634
-56.7 -70 -94 | 4.44 40 104.0|32.2 90 194.0|254 490 914|482 900 1652
-51.1 -60 -76 | 5.00 41 105.8|32.8 91 195.8| |488 910 1670
-45.6 -50 -58 | 5.56 42 107.6|33.3 92 197.6| |493 920 1688
-40.0 -40 -40 | 6.11 43 109.4|33.9 93 199.4| |499 930 1706
-34.4 -30 -22 | 6.67 44 111.2|34.4 94 201.2| |504 940 1724
-28.9 -20 4 | 7.22 45 113.0|35.0 95 203.0| |510 950 1742
-23.3 -10 14 | 7.78 46 114.8|35.6 96 204.8| |516 960 1760
-17.8 0 32 | 8.33 47 116.6|36.1 97 206.6| |521 970 1778
| 8.89 48 118.4|36.7 98 208.4| |527 980 1796
| 9.44 49 120.2|37.2 99 210.2| |532 990 1814
| |37.8 100 212.0| |538 1000 1832
--------------------------------------------------------------------------
----------------------------------------------------------------
1000 to 2000 | 2000 to 3000
-------------------------------|--------------------------------
C. F. | C. F. | C. F. | C. F.
--------------|----------------|----------------|---------------
538 1000 1832 | 816 1500 2732 | 1093 2000 3632 | 1371 2500 4534
543 1010 1850 | 821 1510 2750 | 1099 2010 3650 | 1377 2510 4552
549 1020 1868 | 827 1520 2768 | 1104 2020 3668 | 1382 2520 4560
554 1030 1886 | 832 1530 2786 | 1110 2030 3686 | 1388 2530 4588
560 1040 1904 | 838 1540 2804 | 1116 2040 3704 | 1393 2540 4606
566 1050 1922 | 843 1550 2822 | 1121 2050 3722 | 1399 2550 4622
571 1060 1940 | 849 1560 2840 | 1127 2060 3740 | 1404 2560 4640
577 1070 1958 | 854 1570 2858 | 1132 2070 3758 | 1410 2570 4658
582 1080 1976 | 860 1580 2876 | 1138 2080 3776 | 1416 2580 4676
588 1090 1994 | 866 1590 2894 | 1143 2090 3794 | 1421 2590 4694
593 1100 2012 | 871 1600 2912 | 1149 2100 3812 | 1427 2600 4712
599 1110 2030 | 877 1610 2930 | 1154 2110 3830 | 1432 2610 4730
604 1120 2048 | 882 1620 2948 | 1160 2120 3848 | 1438 2620 4748
610 1130 2066 | 888 1630 2966 | 1166 2130 3866 | 1443 2630 4766
616 1140 2084 | 893 1640 2984 | 1171 2140 3884 | 1449 2640 4784
621 1150 2102 | 899 1650 3002 | 1777 2150 3902 | 1454 2650 4802
627 1160 2120 | 904 1660 3020 | 1182 2160 3920 | 1460 2660 4820
632 1170 2138 | 910 1670 3038 | 1188 2170 3938 | 1466 2670 4838
638 1180 2156 | 916 1680 3056 | 1193 2180 3956 | 1471 2680 4854
643 1190 2174 | 921 1690 3074 | 1199 2190 3974 | 1477 2690 4876
649 1200 2192 | 927 1700 3092 | 1204 2200 3992 | 1482 2700 4892
654 1210 2210 | 932 1710 3110 | 1210 2210 4010 | 1488 2710 4910
660 1220 2228 | 938 1720 3128 | 1216 2220 4028 | 1493 2720 4928
666 1230 2246 | 943 1730 3146 | 1221 2230 4046 | 1499 2730 4946
671 1240 2264 | 949 1740 3164 | 1227 2240 4064 | 1504 2740 4964
677 1250 2282 | 954 1750 3182 | 1232 2250 4082 | 1510 2750 4982
682 1260 2300 | 960 1760 3200 | 1238 2260 4100 | 1516 2760 5000
688 1270 2318 | 966 1770 3218 | 1243 2270 4118 | 1521 2770 5018
693 1280 2336 | 971 1780 3236 | 1249 2280 4136 | 1527 2780 5036
699 1290 2354 | 977 1790 3254 | 1254 2290 4154 | 1532 2790 5054
704 1300 2372 | 982 1800 3272 | 1260 2300 4172 | 1538 2800 5072
710 1310 2390 | 988 1810 3290 | 1266 2310 4190 | 1543 2810 5090
716 1320 2408 | 993 1820 3308 | 1271 2320 4208 | 1549 2820 5108
721 1330 2426 | 999 1830 3326 | 1277 2330 4226 | 1554 2830 5126
727 1340 2444 | 1004 1840 3344 | 1282 2340 4244 | 1560 2840 5144
732 1350 2462 | 1010 1850 3362 | 1288 2350 4262 | 1566 2850 5162
738 1360 2480 | 1016 1860 3380 | 1293 2360 4280 | 1571 2860 5180
743 1370 2498 | 1021 1870 3398 | 1299 2370 4298 | 1577 2870 5198
749 1380 2516 | 1027 1880 3416 | 1304 2380 4316 | 1582 2880 5216
754 1390 2534 | 1032 1890 3434 | 1310 2390 4334 | 1588 2890 5234
760 1400 2552 | 1038 1900 3452 | 1316 2400 4352 | 1593 2900 5252
766 1410 2570 | 1043 1910 3470 | 1321 2410 4370 | 1599 2910 5270
771 1420 2588 | 1049 1920 3488 | 1327 2420 4388 | 1604 2920 5288
777 1430 2606 | 1054 1930 3506 | 1332 2430 4406 | 1610 2930 5306
782 1440 2624 | 1060 1940 3524 | 1338 2440 4424 | 1616 2940 5324
788 1450 2642 | 1066 1950 3542 | 1343 2450 4442 | 1621 2950 5342
793 1460 2660 | 1071 1960 3560 | 1349 2460 4460 | 1627 2960 5360
799 1470 2678 | 1077 1970 3578 | 1354 2470 4478 | 1632 2970 5378
804 1480 2696 | 1082 1980 3596 | 1360 2480 4496 | 1638 2980 5396
810 1490 2714 | 1088 1990 3614 | 1366 2490 4514 | 1643 2990 5414
| 1093 2000 3632 | | 1649 3000 5432
---------------------------------------------------------------
NOTE.--The numbers in bold face type refer to the temperature either
in degrees Centigrade or Fahrenheit which it is desired to convert
into the other scale. If converting from Fahrenheit degrees to
Centigrade degrees the equivalent temperature will be found in
the left column, while if converting from degrees Centigrade to
degrees Fahrenheit, the answer will be found in the column on the
right. These tables are a revision of those by Sauveur & Boylston,
metallurgical engineers, Cambridge, Mass. Copyright, 1920.
INTERPOLATION FACTORS
C. F. C. F.
0.56 1 1.8 | 3.33 6 10.8
1.11 2 3.6 | 3.89 7 12.6
1.67 3 5.4 | 4.44 8 14.4
2.22 4 7.2 | 5.00 9 16.2
2.78 5 9.0 | 5.56 10 18.0
Those using pyrometers will find this and the preceding conversion
table of great convenience:
TABLE 33.--COMPARISON BETWEEN DEGREES CENTIGRADE AND DEGREES FAHRENHEIT
-------------------------------------------------------------------------
Degrees | Degrees | Degrees | Degrees | Degrees | Degrees | Degrees
---------|---------|---------|---------|---------|---------|-------------
F.| C. | F.| C. | F.| C. | F.| C. | F.| C. | F.| C. | F.| C.
---|-----|---|-----|---|-----|---|-----|---|-----|---|-----|-----|-------
-40|-40.0| 3|-16.1| 46| 7.7| 89| 31.6|132| 55.5|175| 79.4| 275| 135.0
-39|-39.4| 4|-15.5| 47| 8.3| 90| 32.2|133| 56.1|176| 80.0| 300| 148.8
-38|-38.8| 5|-15.0| 48| 8.8| 91| 32.7|134| 56.6|177| 80.5| 325| 162.7
-37|-38.3| 6|-14.4| 49| 9.3| 92| 33.3|135| 57.2|178| 81.1| 350| 176.6
-36|-37.7| 7|-13.8| 50| 10.0| 93| 33.9|136| 57.7|179| 81.6| 375| 190.5
-35|-37.2| 8|-13.3| 51| 10.5| 94| 34.4|137| 58.3|180| 82.2| 400| 204.4
-34|-36.6| 9|-12.7| 52| 11.1| 95| 35.0|138| 58.8|181| 82.7| 425| 218.3
-33|-36.1| 10|-12.2| 53| 11.6| 96| 35.5|139| 59.4|182| 83.3| 450| 232.2
-32|-35.5| 11|-11.6| 54| 12.2| 97| 36.1|140| 60.0|183| 83.8| 475| 246.1
-31|-35.0| 12|-11.1| 55| 12.7| 98| 36.6|141| 60.5|184| 84.4| 500| 260.0
-30|-34.4| 13|-10.5| 56| 13.3| 99| 37.2|142| 61.1|185| 85.0| 525| 273.8
-29|-33.9| 14|-10.0| 57| 13.8|100| 37.7|143| 61.6|186| 85.5| 550| 287.7
-28|-33.3| 15| -9.3| 58| 14.4|101| 38.3|144| 62.2|187| 86.1| 575| 301.6
-27|-32.7| 16| -8.8| 59| 15.0|102| 38.8|145| 62.7|188| 86.6| 600| 315.5
-26|-32.2| 17| -8.3| 60| 15.5|103| 39.4|146| 63.3|189| 87.2| 625| 329.4
-25|-31.6| 18| -7.7| 61| 16.1|104| 40.0|147| 63.8|190| 87.7| 650| 343.3
-24|-31.1| 19| -7.2| 62| 16.6|105| 40.5|148| 64.4|191| 88.3| 675| 357.2
-23|-30.5| 20| -6.6| 63| 17.2|106| 41.1|149| 65.0|192| 88.8| 700| 371.1
-22|-30.0| 21| -6.1| 64| 17.7|107| 41.6|150| 65.5|193| 89.4| 725| 385.0
-21|-29.4| 22| -5.5| 65| 18.3|108| 42.2|151| 66.1|194| 90.0| 750| 398.8
-20|-28.8| 23| -5.0| 66| 18.8|109| 42.7|152| 66.6|195| 90.5| 775| 412.7
-19|-28.3| 24| -4.4| 67| 19.4|110| 43.3|153| 67.2|196| 91.1| 800| 426.6
-18|-27.7| 25| -3.8| 68| 20.0|111| 43.8|154| 67.7|197| 91.6| 825| 440.5
-17|-27.2| 26| -3.3| 69| 20.5|112| 44.4|155| 68.3|198| 92.2| 850| 454.4
-16|-26.6| 27| -2.7| 70| 21.1|113| 45.0|156| 68.8|199| 92.7| 875| 468.3
-15|-26.1| 28| -2.2| 71| 21.6|114| 45.5|157| 69.4|200| 93.3| 900| 482.2
-14|-25.5| 29| -1.6| 72| 22.2|115| 46.1|158| 70.0|201| 93.8| 925| 496.1
-13|-25.0| 30| -1.1| 73| 22.7|116| 46.6|159| 70.5|202| 94.4| 950| 510.0
-12|-24.4| 31| -0.5| 74| 23.3|117| 47.2|160| 71.1|203| 95.0| 975| 523.8
-11|-23.8| 32| -0.0| 75| 23.8|118| 47.7|161| 71.6|204| 95.5|1,000| 537.7
-10|-23.3| 33| +0.5| 76| 24.4|119| 48.3|162| 72.2|205| 96.1|1,100| 593.3
-9|-22.7| 34| 1.1| 77| 25.0|120| 48.8|163| 72.7|206| 96.6|1,200| 648.8
-8|-22.2| 35| 1.6| 78| 25.5|121| 49.4|164| 73.3|207| 97.2|1,300| 704.4
-7|-21.6| 36| 2.2| 79| 26.1|122| 50.0|165| 73.8|208| 97.7|1,400| 760.0
-6|-21.1| 37| 2.7| 80| 26.6|123| 50.5|166| 74.4|209| 98.3|1,500| 815.5
-5|-20.5| 38| 3.3| 81| 27.2|124| 51.1|167| 75.0|210| 98.8|1,600| 871.1
-4|-20.0| 39| 3.8| 82| 27.7|125| 51.6|168| 75.5|211| 99.4|1,700| 926.6
-3|-19.4| 40| 4.4| 83| 28.3|126| 52.2|169| 76.1|212|100.0|1,800| 982.2
-2|-18.8| 41| 5.0| 84| 28.8|127| 52.7|170| 76.6|213|100.5|1,900|1,037.7
-1|-18.3| 42| 5.5| 85| 29.4|128| 53.3|171| 77.2|214|101.1|2,000|1,093.3
0|-17.7| 43| 6.1| 86| 30.0|129| 53.8|172| 77.7|215|101.6|2,100|1,148.8
+1|-17.2| 44| 6.6| 87| 30.5|130| 54.4|173| 78.3|225|107.2|2,200|1,204.4
2|-16.6| 45| 7.2| 88| 31.1|131| 55.0|174| 78.8|250|121.1|2,300|1,260.0
-------------------------------------------------------------------------
9 x degrees C.
Degrees Fahrenheit = -------------- + 32
5
5 x (degrees F. - 32)
Degrees Centigrade = ---------------------
9
Three other useful tables are also given on the following pages.
TABLE 34.--WEIGHT OF ROUND, OCTAGON AND SQUARE CARBON TOOL STEEL PER FOOT
------------------------------------------------------------------------
Size | | | | Size | | |
in | Round |Octagon | Square | in | Round | Octagon | Square
inches | | | | inches | | |
--------|--------|--------|--------|--------|--------|---------|--------
1/16 | 0.010 | 0.011 | 0.013 | 2-1/2 | 16.79 | 17.71 | 21.37
1/8 | 0.042 | 0.044 | 0.053 | 2-5/8 | 18.51 | 19.52 | 23.56
3/16 | 0.094 | 0.099 | 0.120 | 2-3/4 | 20.31 | 21.42 | 25.86
1/4 | 0.168 | 0.177 | 0.214 | 2-7/8 | 22.20 | 23.41 | 28.27
5/16 | 0.262 | 0.277 | 0.334 | 3 | 24.17 | 25.50 | 30.78
3/8 | 0.378 | 0.398 | 0.481 | 3-1/8 | 26.23 | 27.66 | 33.40
7/16 | 0.514 | 0.542 | 0.655 | 3-1/4 | 28.37 | 29.92 | 36.12
1/2 | 0.671 | 0.708 | 0.855 | 3-3/8 | 30.59 | 32.27 | 38.95
9/16 | 0.850 | 0.896 | 1.082 | 3-1/2 | 32.90 | 34.70 | 41.89
5/8 | 1.049 | 1.107 | 1.336 | 3-5/8 | 35.29 | 37.23 | 44.94
11/16 | 1.270 | 1.339 | 1.616 | 3-3/4 | 37.77 | 39.84 | 48.09
3/4 | 1.511 | 1.594 | 1.924 | 3-7/8 | 40.33 | 42.54 | 51.35
13/16 | 1.773 | 1.870 | 2.258 | 4 | 42.97 | 45.34 | 54.72
7/8 | 2.056 | 2.169 | 2.618 | 4-1/4 | 48.51 | 51.17 | 61.77
15/16 | 2.361 | 2.490 | 3.006 | 4-1/2 | 54.39 | 57.37 | 69.25
1 | 2.686 | 2.833 | 3.420 | 4-3/4 | 60.60 | 63.92 | 77.16
1-1/8 | 3.399 | 3.585 | 4.328 | 5 | 67.15 | 70.83 | 85.50
1-1/4 | 4.197 | 4.427 | 5.344 | 5-1/4 | 74.03 | 78.08 | 94.26
1-3/8 | 5.078 | 5.356 | 6.646 | 5-1/2 | 81.25 | 85.70 | 103.45
1-1/2 | 6.044 | 6.374 | 7.695 | 5-3/4 | 88.80 | 93.67 | 113.07
1-5/8 | 7.093 | 7.481 | 9.031 | 6 | 96.69 | 101.99 | 123.12
1-3/4 | 8.226 | 8.674 | 10.474 | 7 | 131.61 | 138.82 | 167.58
1-7/8 | 9.443 | 9.960 | 12.023 | 8 | 171.90 | 181.32 | 218.88
2 | 10.744 | 11.332 | 13.680 | 9 | 217.57 | 229.48 | 277.02
2-1/8 | 12.129 | 12.793 | 15.443 | 10 | 268.60 | 283.31 | 342.00
2-1/4 | 13.598 | 14.343 | 17.314 | 11 | 325.01 | 342.80 | 413.82
2-3/8 | 15.151 | 15.981 | 19.291 | 12 | 386.79 | 407.97 | 492.48
------------------------------------------------------------------------
High-speed steel, being more dense than carbon steel, weighs from
10 to 11 per cent more than carbon steel. This should be added
to figures given in the table.
TABLE 35.--WEIGHT OF ROUND, CARBON TOOL STEEL 12 IN. IN DIAMETER
AND LARGER, PER FOOT
--------------------------------------------------------------------
Diameter, | Weight | Diameter, | Weight | Diameter, | Weight
inches | per foot | inches | per foot | inches | per foot
-----------|----------|-----------|----------|-----------|----------
12 | 386.790 | 15-7/8 | 677.527 | 19-3/4 | 1,049.010
12-1/8 | 395.518 | 16 | 687.600 | 19-7/8 | 1,061.705
12-1/4 | 404.246 | 16-1/8 | 699.017 | 20 | 1,074.400
12-3/8 | 412.974 | 16-1/4 | 710.435 | 20-1/8 | 1,088.502
12-1/2 | 421.702 | 16-3/8 | 721.852 | 20-1/4 | 1,102.605
12-5/8 | 430.430 | 16-1/2 | 733.270 | 20-3/8 | 1,116.707
12-3/4 | 439.158 | 16-5/8 | 744.687 | 20-1/2 | 1,130.810
12-7/8 | 447.886 | 16-3/4 | 756.105 | 20-5/8 | 1,144.912
13 | 456.615 | 16-7/8 | 767.522 | 20-3/4 | 1,159.015
13-1/8 | 465.343 | 17 | 778.940 | 20-7/8 | 1,173.118
13-1/4 | 474.071 | 17-1/8 | 790.358 | 21 | 1,187.220
13-3/8 | 482.799 | 17-1/4 | 801.777 | 21-1/8 | 1,201.322
13-1/2 | 491.527 | 17-3/8 | 813.195 | 21-1/4 | 1,215.425
13-5/8 | 500.255 | 17-1/2 | 824.614 | 21-3/8 | 1,229.527
13-3/4 | 508.983 | 17-5/8 | 836.030 | 21-1/2 | 1,243.630
13-7/8 | 517.711 | 17-3/4 | 847.447 | 21-5/8 | 1,257.732
14 | 526.440 | 17-7/8 | 858.863 | 21-3/4 | 1,271.835
14-1/8 | 536.512 | 18 | 870.280 | 21-7/8 | 1,285.937
14-1/4 | 546.585 | 18-1/8 | 883.105 | 22 | 1,300.040
14-3/8 | 556.657 | 18-1/4 | 895.920 | 22-1/8 | 1,315.485
14-1/2 | 566.730 | 18-3/8 | 908.740 | 22-1/4 | 1,330.930
14-5/8 | 576.802 | 18-1/2 | 921.560 | 22-3/8 | 1,346.375
14-3/4 | 586.875 | 18-5/8 | 934.380 | 22-1/2 | 1,361.820
14-7/8 | 596.947 | 18-3/4 | 947.200 | 22-5/8 | 1,377.265
15 | 607.020 | 18-7/8 | 960.020 | 22-3/4 | 1,392.710
15-1/8 | 617.092 | 19 | 972.840 | 22-7/8 | 1,408.155
15-1/4 | 627.165 | 19-1/8 | 985.035 | 23 | 1,423.600
15-3/8 | 637.237 | 19-1/4 | 998.230 | 23-1/8 | 1,454.490
15-1/2 | 647.310 | 19-3/8 |1,010.925 | 23-1/4 | 1,485.380
15-5/8 | 657.382 | 19-1/2 |1,023.620 | 23-3/8 | 1,516.270
15-3/4 | 667.455 | 19-5/8 |1,036.315 | 24 | 1,547.160
--------------------------------------------------------------------
To find the weight of discs made of carbon steel, in diameters
up to and including 12 in., without any allowance for finishing
multiply the per foot weight of round bar steel, shown herewith
by the decimal equivalent of a foot given in the following table:
TABLE 36.--DECIMAL EQUIVALENTS OF A FOOT
---------------------------------------------------------------------
In. | 0 | 1/8 | 1/4 | 3/8 | 1/2 | 5/8 | 3/4 | 7/8
-----|-------|-------|-------|-------|-------|-------|-------|-------
0 | 0.000 | 0.010 | 0.021 | 0.031 | 0.042 | 0.052 | 0.063 | 0.073
1 | 0.083 | 0.094 | 0.104 | 0.115 | 0.125 | 0.135 | 0.146 | 0.156
2 | 0.167 | 0.177 | 0.188 | 0.198 | 0.208 | 0.219 | 0.229 | 0.240
3 | 0.250 | 0.260 | 0.270 | 0.281 | 0.292 | 0.302 | 0.313 | 0.323
4 | 0.333 | 0.344 | 0.354 | 0.364 | 0.375 | 0.385 | 0.396 | 0.406
5 | 0.416 | 0.427 | 0.437 | 0.448 | 0.458 | 0.469 | 0.479 | 0.480
6 | 0.500 | 0.510 | 0.520 | 0.531 | 0.542 | 0.552 | 0.563 | 0.573
7 | 0.583 | 0.594 | 0.604 | 0.615 | 0.625 | 0.635 | 0.646 | 0.656
8 | 0.666 | 0.677 | 0.687 | 0.698 | 0.708 | 0.719 | 0.729 | 0.740
9 | 0.750 | 0.760 | 0.770 | 0.781 | 0.792 | 0.802 | 0.813 | 0.823
10 | 0.833 | 0.844 | 0.854 | 0.865 | 0.875 | 0.885 | 0.896 | 0.906
11 | 0.916 | 0.927 | 0.937 | 0.948 | 0.953 | 0.969 | 0.979 | 0.990
---------------------------------------------------------------------
EXAMPLE.--If the weight of a carbon steel disc 7 in. diameter,
1-5/8 in. thick is desired, turn to page 233, where the per foot
weight of 7 in. round is given as 131.6 lb. Multiply this by the
decimal equivalent of 1-5/8 in., or 0.135, as shown in the above
table, and the product will be the net weight of the disc.
131.61 lb. = the weight of 1 ft. of 7 in. round.
0.135 = the per foot decimal equivalent of 1-5/8 in:
------------
65805
39483
13161
------------
17.76735 lb. = weight of disc 7 in. diam. 1-5/8 in. thick without any
allowance for finishing.
AUTHORITES QUOTED
A
ADDIS, W H.
AMERICAN MACHINISTS' HANDBOOK
AMERICAN STEEL TREARERS' SOCIETY
AMERICAN GEAR MFRS. ASSO.
AUTOMATIC AND ELECTRIC FURNACES LTD.
ARNOLD, PROF. J. O.
B
BURLEIGH, R. W.
BORDEN, B.
BOKER, HERMAN & Co.
BROWN INSTRUMENT Co.
BROWN-LIPE-CHAPLIN Co.
C
CAMPBELL, H. H.
CARHART, H. A.
CLAYTON, C. Y.
CURTIS AIRPLANE Co.
E
ENGLEHARD, CHARLES
ENSAW, HOWARD
F
FIRTH-STERLING STEEL Co.
FIRTH, THOMAS & SONS
FOWLER, HENRY
G
GILBERT & BARKER
H
HAYWAHD, C. R.
HOWE, DR. H. M.
HOOVER STEEL BALL CO.
HEATHCOTE, H. L.
HARRIS, MATTHEW
HUNTER, J. V.
J
JANITZKY, E. J.
JOHNSTON, A. B.
JUTHE, K. A.
L
LATROBE STEEL CO.
LUDLUM STEEL CO.
LEEDS & NORTHRUP CO.
LYMAN, W. H.
M
MANSFIELD, C. A.
MIDVALE STEEL Co.
McKENNA, ROY C.
MOULTON, SETH A.
N
NILES, BEMENT, POND
P
PARKER, S. W.
POOLE, C. R.
R
RAWDON, H. S.
S
S. A. E. (SOCIETY AUTOMOTIVE ENGINEERS)
SAUVEUR, ALBERT
SPRINGFIELD ARMORY
SELLACK, T. G.
SMITH, A. J.
SHIRLEY, ALFRED J.
T
TAYLOR INSTRUMENT Co.
THUM, E. E.
TIEMANN, H. P.
U
U. S. BALL BEARING Co.
UNITED STEEL Co.
UNDERWOOD, CHARLES N.
V
VAN DE VENTER, JOHN H.
W
WALP, H. O.
WOOD, HAROLD F.
WHEELOCK, LOVEJOY & Co.
INDEX
A
ABC of iron and steel
Absorption of carbon, rate of
Air hardening steels
Analysis of high speed steel
Allotropic modifications
Alloy steel, annealing
properties of
Alloys and their effect
in high speed steel
in steel, value of
upon steel
Alpha iron
Annealing
care in
furnace
high-chromium steel
high speed tools
in bone
methods
proper
rifle components
rust-proof steel
steels
temperature
Arrests
Austentite
Automotive industry, application of Liberty engine materials to
temperature control
Axles, heat treatment of
B
Balls, making steel
Barium chloride process
Baths for tempering
Bessemer converter
Beta iron
Blending compounds
Blister steel
Blue brittleness
Bone, annealing in
Boxes for case hardening or carburizing
Breaking test gears
Brinell hardness
Broach hardening furnace
Brown automatic pyrometer
Burning
C
Calorized tubes
Carbon
content at various temperatures
content of case hardened work
in cast iron, ix
in tool steel
introduction of
penetration of
steel
steel forgings, Liberty engine
steel tools
steels, S. A. E.
steels, temper colors
strengthens iron
tool steel, forging
Carbonizing, _see_ Carburizing
Carborundum tubes
Carburization, preventing
Carburizing by gas
boxes
compounds
gas consumption by
local
material
nickel steel
or case hardening
pots for
Carburizing, process of
short method
sleeves
with charcoal
_See_ Case hardening
Car door type of furnace
Case, depth of
Case hardening boxes
cast iron
local
or surface carburizing
treatments for various steels
_see_ Carburizing
Cast iron, carbon in
case hardening
Cementite
Center column furnace
Centigrade table
Chamotte tubes
Chart of carbon penetration
heat treatment
shape
Chrome steel
Chrome-nickel steel
steel, forging
Chrome-vanadium steel
Chromium
steels, S. A. E.
Chromium-cobalt steel
Chromium-vanadium steel, S. A. E.
Classification of steel
Clay tubes
Cold end compensator
junction errors
shortness
worked steel
Color in tempering
Colors on carbon steels
Combination tank
Comparison of fuels
Compensating leads
Compensator for cold ends
automatic
Composition of steel
Compound, blending
separating from work
Compounds for carburizing
Connecting rods, Liberty motor
Continuous heating furnace
Converter, Bessemer
Cooling curves
Cooling quenching oil, roof system
rate of, for gear-forgings
Copper, effect of, in medium carbon steel
Copper-plating to prevent carburizing
Corrosion of high-chromium steel
of rust-proof steel
Corundite tubes
Cost of operating furnaces
Cracks in hardening, preventing
Crankshaft, Liberty motor
Critical point
Crucible or tool steel
Cutting off high speed steel
Cyanide bath for tool steel
D
Decarbonizing of outer surface
preventing
Depth of case
Detrimental elements in steel
Dies, drop forging
quenching
soft spots in
tempering round
Drawing
ends of gear teeth
Drop forging dies
Ductility
E
Effect of alloys
of different carburizing material
of size of piece
of copper in medium carbon steel
Elastic limit
Electric process of steel making
Electrode
Elements, chemical
Elongation
Endurance limit
Energizer, 81
Enlarging steel
Equipment for heat treating
Eutectoid
F
Fahrenheit temperature table
Fatigue test
Ferrite
File test
Flame shields
Flange shields for furnaces
Forging furnace
high speed tools
improper
of steel
practice, heavy
rifle barrels
Forgings, carbon steel Liberty engine
Formed tools, high speed
Fractures, examining by
Furnace, continuous heating
crucible
data
electric
Heroult
open hearth
records
Furnaces
annealing
broach hardening
car door type
center column
cost of operating
data on
forging, heavy
fuels for
gas fired
high speed steel
lead pot
manganese steel
muffle
oil fired
operating costs
screens for
tool
Furnaces, water cooled fronts
Fuels, comparison of
for furnaces
G
Gages, changes due to quenching
tempering
Gamma iron
Gas, carburizing by
consumption for carburizing
fired furnace
illuminating, for carburizing
Gear blanks, heat treatment of
forgings, rate of cooling for Liberty engine
hardening machine
steel, transmission
teeth, drawing ends of
Gears, Liberty engine
Gleason tempering machine
Grade of steel
Grain, refining
size
Graphitic carbon
Grinding high speed steel
H
Hair lines in forgings
Hardening
carbon steel for tools
cracks, preventing
dies
gears
high speed steel
high speed tools
of high-chromium steel
of rust-proof steel
room, modern
Hardness tests
Heating, effect of size
for forging
Heat, judging by color
treating departments
equipment
forgings
inspection of
Liberty motor
Heat treating, of axles
of chisels
of gears
of high speed steel
of steel
S. A. E.
Heat treatment
Heroult furnace
High-chromium steel
annealing of
corrosion of
hardening of
Highly stressed parts of Liberty engine
High speed steel, analysis of
annealing
cutting off
forging
furnace
hardening
heat treatment of
instructions for
manufacture
pack hardening
structure of
Hints for steel users
I
Illuminating gas for carburizing
Impact test
Improper forging
Influence of size on heating
Inspection of heat treatment
Internal stresses, relieving
Introduction of carbon
J
Jewelers' tools
Judging heat of steel by color
L
Latent heat
Lathe and planer tools
tools, high speed
Latrobe temper list
Lead bath
pot furnace
Leeds & Northrup potentiometer
optical pyrometer
Liberty engine, highly stressed parts of
Liberty engine materials, application to automotive industry
motor connecting rods
motor, crankshaft
motor piston pin
Local case hardening
Luting mixture
M
Machineability of steel
Machinery steel, annealing
Magnet test
Making steel in electric furnace
Manganese
steel
furnace
Manufacture of high speed steel
Marquardt mass tubes
Martensite
Medium carbon steel, effect of copper on
Metallography
Microphotographs
Microscopic examination
Milling cutters, high speed
Mixture for luting
Modern hardening room
Molten metal pyrometers
Molybdenum
Muffle furnace
N
Nickel
Nickel-chromium steel
steels, S. A. E.
Nickel, influence of, on steel
steel
affinity for carbon
steels, S. A. E.
Non-homogeneous melting
Non-shrinking steels
Normalizing
O
Oil bath for tempering
cooling on roof
fired furnace
hardening steel, forging
steels
temperature of quenching
Open hearth furnace
Operating costs of furnaces
Outer surface decarbonizer
Over-heated steel, restoring
Overheating
dies
P
Pack-hardening
high speed steel
Packing work for carburizing
Paste for hardening dies
Pearlite
Penetration of carbon
carbon, chart of
in case hardening
Phosphorus
Pickling Liberty motor forgings
Pig iron
Piston pin, Liberty motor
Placing pyrometers
Planer tools, high speed
"Points" of carbon in steel
Potentiometer, Leeds & Northrup
Pots for carburizing
Press for testing gears
Preventing carburization
cracks in hardening
Properties of alloy steels
of alloy steels, table
of steel
Protective screens for furnaces
Puddled iron
Punches and chisels, steels for
Pyrometers
calibration
copper ball
indicating
inspection
iron ball
molten metal
optical
placing
recording
Siemens
testing
water
Q
Quality and structure of high speed steel
of steel
Quenching,
after carburizing
dies in tank
obsolete method
oil, temperature of
tank
tool steel
R
Rate of absorption of carbon
Recording temperatures
Red shortness
Refining the grain
Regenerative open hearth furnace
Restoring overheated steel
Rifle barrels, forging
components, annealing
Roof system of cooling oil
Rust-proof steel
annealing of
corrosion of
hardening of
S
S. A. E. carbon steels
chromium steels
chromium-vanadium
heat treatments
nickel-chromium steels
nickel steels
screw stock
silico-manganese steel
standard steels
Salt bath for tempering
Scleroscope test
Scratch hardness
Screens for furnaces
Screw stock, S. A. E.
Sensible heat
Sentinels, melting of
Separating work from compound
Shields for furnace doors
Shore Scleroscope
Short method of carburizing
Shrinking steel
Silica tubes
Silico-manganese steels, S. A. E.
Silicon
Silversmiths' tools
Size of piece, effect of
Slags
Sleeves, carburizing
hardening and shrinking
shrinking
Solid solution
Sorbite
Specimens, test
Standard S. A. E. steels
Steel,
balls, stock for
bolts, making
composition of
deoxidation
for chisels and punches
forging of
give it a chance
heat treatment of
high speed
making
Bessemer process
crucible process
electric furnace process
open hearth
tools, carbon, in
users' hints
Structure of high speed steel
Sulphur
T
Tables, air, oil and water hardened steel
alloy steels, properties of
carbon content
carbon steels
case hardening
changes due to quenching
chromium steels
chromium-vanadium steels
colors and temperature
composition of steels
cost of furnaces
effect of size
fuels, comparison of
high-chromium steel
nickel-chromium steels
nickel steels
operating cost of furnaces
production cost of furnaces
S. A. E. steels
screw stock
silico-manganese steels
stock for balls
temperature conversion
tempering temperatures
weight of steel
Tank for quenching
dies
Taylor instruments
Temper, colors of
list, Latrobe
of steel
Temperature recorders
tables
Temperatures for tempering
Tempering colors on carbon steels
gages
high speed tools
machine, Gleason
round dies
temperatures
theory of
Tempers of carbon steel
Tensile test
Testing heat treatment
Tests of steel
Test specimens
Theory of tempering
Thermocouple
base metal
cold end
placing
protectors
rare metal
Time for hardening
Tool furnace, small
Tool or crucible steel, annealing
Tool steel, cyanide bath for
quenching
Tools, carbon in different
carbon steel
of high speed steel
sulphur in
tempers of various
transformation points
Transmission gear steel
Treatments for various steels
Troosite
Tubes, calorized
carborundum
Chamotte
clay
Marquardt mass
silica
Tungsten steel
U
Ultimate strength
Users of steel, hints for
V
Vanadium steel
W
Water annealing
cooled furnace fronts
Weight of steel bars
Working instructions for high speed steel
Wrought iron, ix
Y
Yield Point