Terminal solid solubility determinations in the H–Ti system

2015 ◽  
Vol 40 (47) ◽  
pp. 16928-16937 ◽  
Author(s):  
P. Vizcaíno ◽  
I.A. Lopez Vergara ◽  
A.D. Banchik ◽  
J.P. Abriata
Author(s):  
Heidi M. Nordin ◽  
Vicky Hilton ◽  
Andrew W. Buyers ◽  
Christopher E. Coleman ◽  
Glenn A. McRae

2018 ◽  
Vol 510 ◽  
pp. 277-281 ◽  
Author(s):  
Peter Kaufholz ◽  
Maik Stuke ◽  
Felix Boldt ◽  
Marc Péridis

1996 ◽  
Vol 228 (2) ◽  
pp. 227-237 ◽  
Author(s):  
Z.L. Pan ◽  
I.G. Ritchie ◽  
M.P. Puls

Author(s):  
Sanjay Kumar ◽  
Manju Taxak ◽  
N. Krishnamurthy ◽  
A.K. Suri ◽  
G.P. Tiwari

2005 ◽  
Vol 297-300 ◽  
pp. 1685-1690
Author(s):  
Young Suk Kim ◽  
Kyung Soo Im ◽  
Yong Moo Cheong

The hydrogen concentration limit and critical temperatures for a delayed hydride cracking (DHC) in zirconium alloys have been reanalyzed using Kim’s DHC model that a driving force for DHC is not the stress gradient but the supersaturated hydrogen concentration or ∆C arising from a hysteresis of the terminal solid solubility on a heating and on a cooling. The DHC initiation occurs generally at the temperatures corresponding to the terminal solid solubility for precipititation (TSSP), demonstrating that the supercooling from the terminal solid solubility for dissolution (TSSD) is required to initiate the DHC. The DHC arrest temperatures correspond to the temperatures where the ∆C is reduced to zero. Therefore, we conclude that the ∆C is the driving force for the DHC and that the Kim’s DHC model is feasible.


Sign in / Sign up

Export Citation Format

Share Document