Stainless‐steel elastic constants at low temperatures

1981 ◽  
Vol 52 (3) ◽  
pp. 1587-1589 ◽  
Author(s):  
H. M. Ledbetter
1967 ◽  
Vol 45 (23) ◽  
pp. 2913-2919 ◽  
Author(s):  
Russell Sutton ◽  
W. E. Harris

The variables important to the development of pyrolysis gas chromatography as a means of identification of liquids and gases were studied by placing a pyrolysis tube at the inlet of a gas chromatographic column. The pyrolysis conditions can be controlled to limit the formation of methane and to yield the maximum quantities of other products for identification of the parent compounds. Conditions that reduce methane formation are the absence of air, low temperatures, a long residence time, and the use of quartz rather than stainless-steel pyrolysis tubes. There is a limited range of pyrolysis temperatures that permits the formation and observation of all products in a pyrogram.


The thermal conductivity between 0.4 and 4.2 K and in magnetic fields up to 50 kOe of KMgF 3 doped with Ni 2+ has been measured. The results are analysed to give values of the average spin-lattice coupling constants ( x Sl ) for the Ni 2+ ion. These are in agreement with values calculated using the magneto-elastic constants (GX1 and 6r44) derived from acoustic paramagnetic resonance (a.p.r.) experiments. Below IK the thermal resistivity as a function of magnetic field shows a number of anomalies, for which possible causes are discussed; it is concluded that they result from phonon interactions with exchange-coupled pairs of Ni 2+ ions. Such pairs are also observed in a.p.r. experiments.


1970 ◽  
Vol 41 (10) ◽  
pp. 4010-4014 ◽  
Author(s):  
M. Ghafelehbashi ◽  
K. M. Koliwad

1978 ◽  
Vol 15 (2) ◽  
pp. 706-709 ◽  
Author(s):  
C. J. Altstetter ◽  
R. Behrisch ◽  
B. M. U. Scherzer

1971 ◽  
Vol 3 (6) ◽  
pp. 741-743
Author(s):  
A. P. Nazarenko ◽  
V. G. Komarenko

CORROSION ◽  
1965 ◽  
Vol 21 (2) ◽  
pp. 53-56 ◽  
Author(s):  
M. B. WHITEMAN ◽  
A. R. TROIANO

Abstract Type 310 stainless steel in thin sections was embrittled by hydrogen. The temperature and strain rate dependence of this embrittlement was almost analogous to that well-established for hydrogenated body-centered cubic (b.c.c.) metals, differing only in that at low temperatures and relatively high strain rates complete recovery in ductility was not achieved. The activation energy for recovery in ductility, determined by aging at several temperatures, was 10,900 cal/mole.


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