The Influence of Nitrogen and Certain Other Elements on the Creep-Rupture Properties of Wholly Austenitic Type 304 Steel

1967 ◽  
Vol 89 (3) ◽  
pp. 517-524 ◽  
Author(s):  
P. D. Goodell ◽  
T. M. Cullen ◽  
J. W. Freeman

Experimental heats of Type 304 steel, compositionally balanced to be wholly austenitic and thus simulate the material used to produce seamless superheater tubing, were prepared to determine the influence of selected elements on the creep-rupture properties of this steel and thereby assess their possible contribution to the improvement in the elevated temperature properties which has been noted over the past years. Nitrogen is shown to increase the rupture strength at 1200 deg F of the wholly austenitic laboratory heats to a pronounced extent. Furthermore, almost the full effect of nitrogen was obtained after heat-treating at temperatures as low as 1750 deg F. Rupture strengths also increased with increasing carbon content although heat-treatment above 1750 deg F was necessary to obtain the maximum strengthening effect from the higher levels of this element. Nitrogen was a somewhat more effective strengthener than carbon, the rupture strengths correlating with (%C) + 1.25 × (%N). Small amounts of titanium, aluminum, boron, copper, and molybdenum had no or at most only minor effects on the properties. More than 0.1 percent manganese was necessary for good rupture properties but otherwise had little effect at levels up to at least 1.5 percent. Published data for commercial heats fitted the correlation developed from the laboratory heats. The generally higher level of the rupture strength data for Type 304 austenitic steel published since the early 1950’s appears to be closely related to higher levels of nitrogen. The data indicate that it is extremely important to control nitrogen content to obtain expected creep-rupture properties at 1200 deg F.

1966 ◽  
Vol 88 (4) ◽  
pp. 755-761
Author(s):  
C. L. Dotson ◽  
C. K. Donoho

The creep-rupture properties of tensile specimens made from 1 1/4 Cr-1/2 Mo centrifugally cast alloy steel pipe, conforming to ASTM A426-CP11, were evaluated at 1000, 1100, and 1200 F. At 1000 F, the pipe was evaluated in two normalized-and-tempered conditions, and at 1100 and 1200 F, in one normalized-and-tempered condition. Specimens were loaded to produce rupture in time ranging from less than 100 to about 2000 hr for determination of the minimum creep rate and the creep-rupture strength, and at lower loads to obtain additional minimum creep rate data. The rupture strength and minimum creep rate of the centrifugally cast pipe were compared to similar properties for the alloy in statically cast and wrought forms. Stresses required to produce a minimum creep rate of 10−5 percent/hr and rupture in 100,000 hr were compared to allowable design stresses specified by the ASME Boiler and Pressure Vessel Code and American Standards Association Specifications B31.1, Pressure Piping, and B31.3, Petroleum Refinery Piping. In both heat-treated conditions evaluated, the minimum creep rate of the pipe compared favorably with published data for the alloy in noncentrifugally cast forms and with the allowable stresses set by the ASME and ASA codes.


1975 ◽  
Vol 97 (3) ◽  
pp. 234-244 ◽  
Author(s):  
T. Wada ◽  
D. L. Sponseller

A laboratory heat of an improved boiler steel containing 0.13 percent C, 1.36 percent Mn, 0.27 percent Mo, 0.03 percent Cb, and 0.010 percent N was prepared; creep-rupture properties, resistance to temper embrittlement and resistance to hydrogen attack were investigated. The rupture strength was much higher than that of carbon steel and columbium-treated carbon steel, but was somewhat lower than that of two European carbon-0.3 percent Mo boiler steels. Creep-rupture ductility was high. The experimental steel exhibited high toughness, especially in the normalized and stress-relieved condition. No temper embrittlement was induced by step-cooling normalized or normalized and stress-relieved material. Good resistance to hydrogen attack was revealed by tests in a hydrogen autoclave at a pressure of 1000 psi (6.9 N/mm2); the steel retained the original Charpy impact toughness after exposures up to 5000 hr at 900 deg F (480 deg C) and 500 hr at 1000 deg F (540 deg C). No blistering or fissuring were observed.


Alloy Digest ◽  
1991 ◽  
Vol 40 (4) ◽  

Abstract ALLVAC 90 is a nickel-base alloy containing cobalt to provide improved tensile and creep-rupture properties up to 1600 F (871 C) and chromium for oxidation and corrosion resistance. Titanium and aluminum confer precipitation characteristics. This datasheet provides information on composition, physical properties, and elasticity. It also includes information on corrosion resistance as well as forming, heat treating, machining, and joining. Filing Code: Ni-393. Producer or source: Allvac Inc..


1967 ◽  
Vol 89 (3) ◽  
pp. 465-478 ◽  
Author(s):  
J. A. VanEcho ◽  
D. B. Roach ◽  
A. M. Hall

The short-time tensile properties of the A CI Type HK-40 cast heat-resistant alloy and AISI Type 310 wrought stainless steel were investigated from room temperature to 2000 F. The creep-rupture properties of the HK-40 alloy were studied in the range of 1400 to 2000 F for times long enough to permit extrapolation to 100,000 hr. In addition, the creep-rupture properties of Type 310 were investigated at 1800 to 2000 F, and observations were made of the microstructural changes that occurred in the two materials during creep exposure. The Type 310 material tended to have a higher yield strength and ultimate tensile strength at moderate temperatures than the HK-40; however, from 1200 to 2000 F, the HK-40 was the stronger. The Type 310 was more ductile at all temperatures. The HK-40 displayed about twice the rupture strength of the Type 310 at each test temperature. On the basis of comparable minimum creep rates, the HK-40 showed five to six times the strength of the Type 310 at the same temperature. During exposure at the lower temperatures, chromium carbides precipitated in finely dispersed form in the matrix of the HK-40; isolated islands of sigma phase also tended to form. At high temperatures, the primary eutectic carbides in the HK-40 alloy tended to spheroidize; and both materials absorbed nitrogen from the atmosphere, needles of chromium nitride forming in the matrix.


2020 ◽  
Vol 39 (1) ◽  
pp. 178-188
Author(s):  
Lakshmiprasad Maddi ◽  
Atul Ramesh Ballal ◽  
Dilip Ramkrishna Peshwe ◽  
M. D. Mathew

AbstractP92 steel is used as a piping material in ultra super critical power plants that can be operated at steam temperatures up to 650°C. The changes in the martensitic microstructure of P92 steel must be evaluated thoroughly before it is put into actual service. In this study, indigenously developed P92 steel was used. The steel was subjected to normalizing and tempering heat treatments in the range of 1,040–1,060°C and 740–780°C. The changes in the microstructure were evaluated and creep-rupture properties were studied at test temperatures of 600 and 650°C. Although normalizing temperatures influenced the microstructure and creep strength marginally, the change in tempering temperatures led to significant changes. The creep rupture strength at 600°C was influenced largely by the changes in the dislocation substructure, while the precipitation of Laves phases was a significant observation made for 650°C test temperature. Proposed mechanisms for the microstructural evolution and its consequences on the rupture life are discussed in this study.


1985 ◽  
Vol 107 (4) ◽  
pp. 421-429 ◽  
Author(s):  
R. L. Huddleston

An improved strength model is developed for predicting creep rupture under multiaxial stress states. The new model incorporates three independent stress parameters and distinguishes between life under tensile versus compressive stress states. Assessments of the new model based on experimental biaxial creep-rupture data for type 304 stainless steel tested at 593°C show the new model to be significantly more accurate than the classical criteria of von Mises, Tresca, or Rankine.


1983 ◽  
Vol 69 (14) ◽  
pp. 1668-1675 ◽  
Author(s):  
Norio SHINYA ◽  
Junro KYONO ◽  
Hideo TANAKA ◽  
Masaharu MURATA ◽  
Shin YOKOI

1975 ◽  
Vol 97 (4) ◽  
pp. 243-251 ◽  
Author(s):  
V. K. Sikka ◽  
H. E. McCoy ◽  
M. K. Booker ◽  
C. R. Brinkman

A wide variation in creep-rupture and long-term creep properties of 20 heats of type 304 and seven heats of type 316 stainless steel was observed. The observed variation in 1000-hr creep-rupture strength, SRt, has been related to the corresponding ultimate tensile strength variation, Sur, by a relationship of the form: SRt=αexp(βSur), where α and β are material constants. This relationship between creep-rupture strength and ultimate tensile strength was further extended for minimum-expected 105-hr creep-rupture strength data reported in the literature. The heat-to-heat variation in ultimate tensile strength for both types 304 and 316 stailness steel was explained in terms of carbon plus nitrogen content and grain intercept, d, by a relationship of the form Sur = A(C + N)−1/2 + B, where A and B are constants for a given temperature. The time to onset of third-stage creep for various heats of type 304 and 316 stainless steel was related to time to rupture by relationships that are independent of test temperature, for test times reaching 22,622 hr.


Author(s):  
B. Z. Margolin ◽  
A. G. Gulenko ◽  
A. A. Buchatsky

The paper presents the physical and mechanical model that allows predicting fracture of materials subjected to neutron irradiation under creep. The model is based on the equations of void nucleation and growth on grain boundaries that were proposed earlier. The equations are developed for the case of neutron irradiation of a material. The constitutive equations describing viscoplastic deformation of a material with regard to void evolution are formulated. The criterion of microplastic collapse of a unit cell is used as a fracture criterion. The creep-rupture strength and ductility of austenitic materials in the initial and irradiated conditions with different neutron flux levels are predicted on the basis of the model. The calculated results are compared with the available experimental data.


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