Diffusion-kinetic modeling of the electron radiolysis of water at elevated temperatures

1993 ◽  
Vol 97 (13) ◽  
pp. 3291-3297 ◽  
Author(s):  
Jay A. LaVerne ◽  
Simon M. Pimblott
Fuel ◽  
2016 ◽  
Vol 184 ◽  
pp. 836-845 ◽  
Author(s):  
Qianqian Li ◽  
Weijie Zhang ◽  
Wu Jin ◽  
Yongliang Xie ◽  
Zuohua Huang

2005 ◽  
Vol 38 (9) ◽  
pp. 701-710 ◽  
Author(s):  
Maurice S. Onyango ◽  
Yoshihiro Kojima ◽  
Dalibor Kuchar ◽  
Simon O. Osembo ◽  
Hitoki Matsuda

2007 ◽  
Vol 55 (9) ◽  
pp. 3408-3413 ◽  
Author(s):  
Nirupama A. Vaidya ◽  
Kevin Mathias ◽  
Baraem Ismail ◽  
Kirby D. Hayes ◽  
Carlos M. Corvalan

1997 ◽  
Vol 101 (8) ◽  
pp. 1628-1634 ◽  
Author(s):  
Jay A. LaVerne ◽  
Simon M. Pimblott ◽  
Laszlo Wojnarovits

Author(s):  
N. M. P. Low ◽  
L. E. Brosselard

There has been considerable interest over the past several years in materials capable of converting infrared radiation to visible light by means of sequential excitation in two or more steps. Several rare-earth trifluorides (LaF3, YF3, GdF3, and LuF3) containing a small amount of other trivalent rare-earth ions (Yb3+ and Er3+, or Ho3+, or Tm3+) have been found to exhibit such phenomenon. The methods of preparation of these rare-earth fluorides in the crystalline solid form generally involve a co-precipitation process and a subsequent solid state reaction at elevated temperatures. This investigation was undertaken to examine the morphological features of both the precipitated and the thermally treated fluoride powders by both transmission and scanning electron microscopy.Rare-earth oxides of stoichiometric composition were dissolved in nitric acid and the mixed rare-earth fluoride was then coprecipitated out as fine granules by the addition of excess hydrofluoric acid. The precipitated rare-earth fluorides were washed with water, separated from the aqueous solution, and oven-dried.


Author(s):  
J. L. Brimhall ◽  
H. E. Kissinger ◽  
B. Mastel

Some information on the size and density of voids that develop in several high purity metals and alloys during irradiation with neutrons at elevated temperatures has been reported as a function of irradiation parameters. An area of particular interest is the nucleation and early growth stage of voids. It is the purpose of this paper to describe the microstructure in high purity nickel after irradiation to a very low but constant neutron exposure at three different temperatures.Annealed specimens of 99-997% pure nickel in the form of foils 75μ thick were irradiated in a capsule to a total fluence of 2.2 × 1019 n/cm2 (E > 1.0 MeV). The capsule consisted of three temperature zones maintained by heaters and monitored by thermocouples at 350, 400, and 450°C, respectively. The temperature was automatically dropped to 60°C while the reactor was down.


Author(s):  
Robert C. Rau ◽  
Robert L. Ladd

Recent studies have shown the presence of voids in several face-centered cubic metals after neutron irradiation at elevated temperatures. These voids were found when the irradiation temperature was above 0.3 Tm where Tm is the absolute melting point, and were ascribed to the agglomeration of lattice vacancies resulting from fast neutron generated displacement cascades. The present paper reports the existence of similar voids in the body-centered cubic metals tungsten and molybdenum.


Author(s):  
Ernest L. Hall ◽  
J. B. Vander Sande

The present paper describes research on the mechanical properties and related dislocation structure of CdTe, a II-VI semiconductor compound with a wide range of uses in electrical and optical devices. At room temperature CdTe exhibits little plasticity and at the same time relatively low strength and hardness. The mechanical behavior of CdTe was examined at elevated temperatures with the goal of understanding plastic flow in this material and eventually improving the room temperature properties. Several samples of single crystal CdTe of identical size and crystallographic orientation were deformed in compression at 300°C to various levels of total strain. A resolved shear stress vs. compressive glide strain curve (Figure la) was derived from the results of the tests and the knowledge of the sample orientation.


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