scholarly journals Effect of FeF$sub 2$ addition on mass transfer in a Hastelloy N: LiF-- BeF$sub 2$--UF$sub 4$ thermal convection loop system

1972 ◽  
Author(s):  
J. W. Koger
Author(s):  
V.V. Shekhovtsov ◽  
◽  
YU.A. Abzaev ◽  
O.G. Volokitin ◽  
A.A. Klopotov ◽  
...  

The paper presents the results of numerical modeling of development melting zone hollow spherical microparticle α-Al2O3. The object of the study was part circular sector, which represents the shell of hollow particle, which is formed under action plasma flow. Numerically describe the unsteady convective heat and mass transfer in shell hollow particle, we used the system Navier-Stokes equations in Boussinesq approximation, which describes the weak convection medium. Due to the high coefficient of porosity (P = 0.56) initial agglomerated particle with the α-Al2O3 structure, the inner region at the stage of heating Tp ≥ Tmelt is in the conditions heat exchange with the incoming heat flux, as result of which the temperature center coincided with the temperature particle surface. Result of overheating of the condensed phase, liquid layer of fused grains is formed in the inner and outer regions microparticle. In this case, the melting front is directed towards center shell. Result of numerical modeling, it has been established that convective heat and mass transfer is observed in melting zones (liquid phase), vector field of which covers almost the entire region of the liquid phase. It was found that thermal convection in the external liquid phase is characterized by velocities that are more than 2 times higher than the displacement velocity in the inner region of the particle. It is shown that there is no displacement of the material inside the convection region, thereby inhomogeneous heating occurs in the molten layer of the particle, which significantly affects the speed of movement of the melting front.


CORROSION ◽  
1965 ◽  
Vol 21 (2) ◽  
pp. 57-61 ◽  
Author(s):  
JAMES Y. N. WANG

Abstract Mass transfer of nickel to the hot leg (454 C, 850 F) of a mercury thermal convection loop in which titanium samples were exposed has been observed. This involved dissolution of nickel in mercury at 320 C (608 F), its transfer to the surface of the sample in the hot leg, and subsequent interdiffusion of nickel and titanium. Microprobe study of surface layers on the titanium sample indicated stratification of nickel. Outer layer contained two materials with compositions closely approximating those of TiNi and TiNi3, and an inner layer a material with nickel content close to the reported solubility limit for nickel in β-Ti, even though the reaction was conducted below α-β transformation temperature. Effects of other metallic additives are also discussed.


2011 ◽  
Vol 417 (1-3) ◽  
pp. 1200-1204 ◽  
Author(s):  
Masatoshi Kondo ◽  
Takeo Muroga ◽  
Takuya Nagasaka ◽  
Qi Xu ◽  
Valentyn Tsisar ◽  
...  

2017 ◽  
Author(s):  
V. V. Kuneevsky ◽  
V. B. Osnos ◽  
Yu. V. Vankov ◽  
V. M. Larionov ◽  
E. R. Saifullin

2017 ◽  
Author(s):  
V. V. Kuneevsky ◽  
V. B. Osnos ◽  
Yu. V. Vankov ◽  
V. M. Larionov ◽  
E. R. Saifullin

2021 ◽  
Author(s):  
Stephen Raiman ◽  
J Matthew Kurley ◽  
Dino Sulejmanovic ◽  
Adam Willoughby ◽  
Scott Nelson ◽  
...  

Type 316H stainless steel samples were exposed to flowing FLiNaK salt for 1000h in a thermal convection loop with a maximum temperature of 650°C and a minimum of 540°C. Samples in the hottest part of the loop lost mass, with a maximum mass loss of 1.8 mg/cm2, while samples in the coldest parts of the loop gained mass. Analysis of the samples that gained mass showed an iron-rich layer on the sample surfaces, suggesting that iron, not chromium, accounted for the majority of the mass transfer in the loop. Analysis of the salt showed major increases in the Cr, Fe, and Mn content of the salt during exposure. The loop was modeled using the TRANSFORM code. Modeled values matched the experimental temperature measurements showing that TRANSFORM is capable of accurately simulating the conditions in the loop.


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