Interface Controlled Diffusional Creep of Cu + 2.8 at.% Co Solid Solution

2012 ◽  
Vol 322 ◽  
pp. 33-39 ◽  
Author(s):  
Sergei Zhevnenko ◽  
Eugene Gershman

High-temperature creep experiments were performed on a Cu-2.8 ат.% Co solid solution. Cylindrical foils of 18 micrometers thickness were used for this purpose. Creep tests were performed in a hydrogen atmosphere in the temperature range of about from 1233 K to 1343 K and at stresses lower than 0.25 MPa. For comparison, a foil of pure copper and Cu-20 at.% Ni solid solution were investigated on high temperature creep. Measurements on the Cu foil showed classical diffusional creep behavior. The activation energy of creep was defined and turned out to be equal 203 kJ/mol, which is close to the activation energy of bulk self-diffusion of copper. There was a significant increase in activation energy for the Cu-20 at.% Ni solid solution. Its activation energy was about 273 kJ/mol. The creep behavior of Cu-Co solid solution was more complicated. There were two stages of diffusional creep at different temperatures. The extremely large activation energy (about 480 kJ/mol) was determined at relatively low temperature and a small activation energy (about 105 kJ/mol) was found at high temperatures. The creep rate of Cu-Co solid solution was lower than that of pure copper at all temperatures. In addition, the free surface tension of Cu-2.8 ат.% Co was measured at different temperatures from 1242 K to 1352 K. The surface tension increases in this temperature range from 1.6 N/m to 1.75 N/m. There were no features on the temperature dependence of the surface tension.


2018 ◽  
Vol 789 ◽  
pp. 182-186
Author(s):  
Jin Ping Pan ◽  
Shu Heng Tu ◽  
Ding Jun Chu ◽  
Xin Wei Zhu ◽  
Bin Hu ◽  
...  

A progressive increase of plant efficiency calls for new requirements of heat-resistantsteels used in the boiler and piping systems. In this paper, high-temperature creep behavior of T23and T24 steels were studied. Creep tests over a long period of time have been conducted for bothsteels at different temperatures. The creep mechanisms of the two steels have been clarified byanalyzing the minimum creep rate versus stress data. Besides, the creep rupture data from the creeptests were in good accordance with theoretical simulation on the basis of the CDM model over a longtime. Creep temperature has great effects on the rupture strength of the two steels. By creep ruptureexperiments and appropriate modelling, the high-temperature creep behavior can be well described.



1957 ◽  
Vol 24 (2) ◽  
pp. 207-213
Author(s):  
H. Laks ◽  
C. D. Wiseman ◽  
O. D. Sherby ◽  
J. E. Dorn

Abstract Experimental investigations on pure aluminum and its dilute solid-solution alloys revealed that the high-temperature creep rate ϵ̇ is related to the stress σ by ϵ̇ ∼ σn for low stresses and ϵ̇ ∼ eBσ for high stresses where n and B are constants independent of the creep strain and temperature. According to a preliminary dislocation-climb model for high-temperature creep, the activation energy for creep is that for self-diffusion, the effect of stress on the creep rate depends on the number of active Frank-Read sources, and the rate of climb depends on the structure as determined by the pattern of climbing dislocations. Many of the experimental observations on high-temperature creep can be accounted for by this model.



1994 ◽  
Vol 42 (3) ◽  
pp. 1001-1012 ◽  
Author(s):  
H. Duong ◽  
M. Beeman ◽  
J. Wolfenstine


1984 ◽  
Vol 24 (04) ◽  
pp. 408-416 ◽  
Author(s):  
Mohammad Reza Fassihi ◽  
William E. Brigham ◽  
Henry J. Ramey

Abstract A model is proposed to analyze and differentiate between crude oil/oxygen reactions at different temperatures. The results of this analysis along with correlations of apparent hydrogen/carbon (H/C) ratio and molar carbon dioxide/carbon monoxide (CO2/CO) ratio indicated three major reactions at different temperatures. Low-temperature oxidation (LTO) appears to occur between the gas and liquid phases. Middle-temperature fuel deposition reactions appear to be homogeneous. The latter was found to be the rate-determining step in clean sands. Natural cores from the reservoirs were found to have different kinetic behavior than the clean sand matrices for these reasons:metallic additives lower the activation energy of the combustion reaction and hence shift the rate-determining steps, andclay and finer sands adsorb more fuel. The proposed kinetic model was found to be applicable to the five oils tested and hence may be generalized for application to any oil. Introduction Several experiments were conducted to study the oxidation reactions of crude oil in porous media. The results of these tests were reported in Part 1 of this study (see Page 399). A kinetic model is proposed here that is useful in analyzing and differentiating between the oxidation reactions occurring in in-situ combustion. Modeling of the Reactions Appendix A presents development of a model based on Weijdema's kinetic equation. The temperature can be increased linearly with time, and, by proper graphing of the variables, a semilog straight line should result. The variable temperature runs were made to test this model. Fig. 1 shows the gases produced and the oxygen consumed as the sand mix is heated uniformly in Run 110. From the data in this graph, the relative reaction rate, was calculated and is graphed in Fig. 2. The reaction order, n, was assumed to be unity. Later on, n was obtained through the curve fit optimization. Note that the high-temperature data fall on a straight line as predicted by Weijdema's model, but at lower temperatures (increasing values of 1/T) a departure from the straight line is observed. It is clear from these data that a single-reaction model does not adequately describe the reaction kinetics observed. A straight line was drawn through the high-temperature data. From the slope of that line an activation energy, E = 135 kJ/mol, is obtained (Fig. 3a, Curve 1). It was assumed that this reaction also occurs at lower temperatures according to an extrapolation of the high-temperature data. The method used is described in Appendix B. Fig. 4a shows the original delta CO2 data for Run 110 (similar to Fig. 1). If Curve I is subtracted from this curve, Curve II (Fig, 4a) is obtained, which describes the oxidation behavior at the medium temperature range. Following the same procedure, the produced carbon oxides in the medium temperature range (Curve III, Fig. 4a) can be obtained by subtracting Curve I from the total produced carbon oxides. From Curve II of Fig. 4a, a calculation of the relative reaction rate, as a function of 1/T leads to the Curve II in Fig. 3b (open triangles). The data are not linear. However, a computation of an equivalent term for the carbon oxides formed, where, from Curve III, Fig. 4b, shows a definite straight line (Curve III, Fig. 3b). An activation energy of E = 84 kJ/g mol is calculated from the slope of this line. In this figure, although the data scatter considerably, it appears reasonable to assume that the oxygen consumption curve in the medium temperature range follows the same slope as the carbon oxides curve. Using this assumption, the oxygen consumption can be calculated and subtracted from Curve II of Fig. 4a and the remainder is represented in Curve V (Fig. 4c). When the data from Curve V, Fig. 4c are evaluated by using the Weijdema integral, and the result is graphed on Fig. 3c, a straight line (Curve V) is formed, which describes the LTO reaction. The activation energy calculated from the slope of this line is E = 93 kJ/g mol. By using the computer interactively, this same analysis was applied to other experiments. The results always fit straight lines. However, for different crude oils, the order of the reaction with respect to fuel concentration, n, was different. SPEJ P. 408^



Metals ◽  
2021 ◽  
Vol 11 (4) ◽  
pp. 581
Author(s):  
Abdulhakim A. Almajid

This study is focused on the deformation mechanism and behavior of naturally aged 7010 aluminum alloy at elevated temperatures. The specimens were naturally aged for 60 days to reach a saturated hardness state. High-temperature tensile tests for the naturally aged sample were conducted at different temperatures of 573, 623, 673, and 723 K at various strain rates ranging from 5 × 10−5 to 10−2 s−1. The dependency of stress on the strain rate showed a stress exponent, n, of ~6.5 for the low two temperatures and ~4.5 for the high two temperatures. The apparent activation energies of 290 and 165 kJ/mol are observed at the low, and high-temperature range, respectively. These values of activation energies are greater than those of solute/solvent self-diffusion. The stress exponents, n, and activation energy observed are rather high and this indicates the presence of threshold stress. This behavior occurred as a result of the dislocation interaction with the second phase particles that are existed in the alloy at the testing temperatures. The threshold stress decreases in an exponential manner as temperature increases. The true activation energy was computed by incorporating the threshold stress in the power-law relation between the stress and the strain. The magnitude of the true activation energy, Qt dropped to 234 and 102 kJ/mol at the low and high-temperature range, respectively. These values are close to that of diffusion of Zinc in Aluminum and diffusion of Magnesium in Aluminum, respectively. The Zener–Hollomon parameter for the alloy was developed as a function of effective stress. The data in each region (low and high-temperature region) coalescence in a segment line in each region.





Author(s):  
Guanfei Xiao ◽  
Jufu Jiang ◽  
Ying Wang ◽  
Yingze Liu ◽  
Ying Zhang ◽  
...  


2021 ◽  
Vol 557 ◽  
pp. 153293
Author(s):  
Apu Sarkar ◽  
Saurav Sunil ◽  
Bhupendra Kumawat ◽  
G. Bharat Reddy ◽  
Rajeev Kapoor ◽  
...  


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