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236 r<strong>org</strong>ing- Stamping - Heat Treating<br />
July, 1925<br />
T e s t s o n S t e e l a t E l e v a t e d T e m p e r a t u r e s<br />
Short-Time Static Experimental Results for High-Strength Steel<br />
Are Compared with Long-Time Static Results on the<br />
T H E use of metals at elevated temperatures has<br />
become an important question to builders and<br />
users of steam generating machinery and internal<br />
combustion engines. Certain parts of such machinery<br />
are subjected to elevated temperatures, and these temperatures<br />
have steadily increased in recent years with<br />
the improvement in size and efficiency of such equipment<br />
until, at the present time, metal under considerable<br />
stress is subjected to temperatures which keep<br />
them constantly at from 600 to 900 deg. F Certain<br />
metal parts used at elevated temperatures, such as<br />
steam piping, valves, boilers, and turbine cases, are<br />
subjected in general to static stresses only. Other<br />
metal parts, such as turbine wheels, turbine blades,<br />
piston rods, and cylinders of internal combustion engines,<br />
are subjected to reversed stresses which may<br />
be repeated many times.<br />
The metals in general use at elevated temperatures<br />
are almost all ferrous, and consist in the main<br />
of wrought steel, cast steel and cast iron. It is gradually<br />
becoming known that certain ferrous alloys are<br />
capable of withstanding stress at high temperatures<br />
better than others. Such metals are usually high in<br />
tungsten, nickel, chromium, or some satisfactory combination<br />
of these alloys. Fig. 1 gives a general idea<br />
of the relative values of steels containing these alloys<br />
when tensile strength at elevated temperatures is considered.<br />
These data are from annealed steels and cast<br />
iron, and are largely drawn from results by Harper<br />
and MacPherrant. The results of tests on steels at<br />
elevated temperatures show that in general the static<br />
properties other than strength are affected by temperature<br />
in the following manner: the higher the<br />
strength for any particular steel, the lower the percentages<br />
of reduction of area and elongation and the<br />
higher the hardness factors.<br />
In obtaining strength data at elevated temperatures<br />
for use in actual design, care must be exercised<br />
to approach as nearly as possible the conditions under<br />
which the metal is to be used. The method usually<br />
adopted in testing metals at ordinary temperatures<br />
has been to make a test which lasts less than 10 minutes,<br />
and expect this to represent the strength and<br />
ductility factors to which the metal will conform<br />
when subjected to stress for months, or even years.<br />
For wrought and cast ferrous metals at ordinary<br />
atmospheric temperatures, this assumption may be<br />
made without serious error, but at elevated temperatures<br />
an error of from 30 to 50 per cent depending on<br />
the temperature used may result when this procedureis<br />
followed. Static testing at elevated temperatures.<br />
therefore, is not so simple, nor can it be as expedi<br />
*A paper presented at the twenty-eighth annual meeting<br />
of the American Society for Testing Materials, held at Atlantic<br />
City, N. J.. June. 1925.<br />
tSpecial Research Assistant Professor of Engineering Materials.<br />
University of Illinois.<br />
{Bulletin Xo. 141. Allis-Chalmers Manufacturing Comnany,<br />
1922.<br />
Same Steel Under Similar Conditions<br />
By T. McLEAN JASPERf<br />
tiously carried out as at ordinary atmospheric temperatures.<br />
At ordinary atmospheric temperatures steel is a<br />
crystallin substance which, within its elastic range<br />
under static load, acts as an isotropic, elastic substance.<br />
Under elevated temperatures, however, this<br />
general state of affairs no longer exists, and as the<br />
temperature is increased the metal gradually loses certain<br />
of its elastic properties and at the same time<br />
assumes a state approaching that of a plastic amorphous<br />
material. As this condition is approached, the<br />
steel tends to continually increase its stretch or strain<br />
without an accompanying increase of load, and the<br />
result is that long-time tensile strength varies from<br />
the short-time tensile strength in an increasing percenage<br />
as the temperature is increased. The effect of<br />
this is well illustrated in Fig. 2, which shows the<br />
variation of the static properties of a quenched metal<br />
and indicates the values of the tensile strength at"<br />
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FIG. 1—Curves showing the effect of certain ingredients on<br />
the tensile strength of various annealed steels and cast iron<br />
at elevated temperatures.<br />
elevated temperatures under ordinary test conditions<br />
and under long-time test conditions. In the shorttime<br />
test the material was continuously loaded to its<br />
tensile strength within a period of about five minutes<br />
after it was raised to the correct temperature. The<br />
values of the tensile strengths in this case are shown<br />
by the upper tensile strength curve. In the long-time<br />
test, the specimen was tested to its proportional limit<br />
fairly rapidly and then increments of load were added<br />
only when strain or stretch had become zero, or<br />
almost so. for each increment of load. In this manner,<br />
the time necessary to break a long-time test specimen<br />
varied from 12 to 72 hours, depending on the<br />
material and on the temperature at which it was being<br />
tested. The values of the long-time tensile strengths<br />
are shown by the lower portion of the tensile strength<br />
curve. It will be noticed that, as the values of the<br />
temperature of specimens are increased, the ductilityvalues<br />
are also increased and the strength values are