Some experiments on adiabatic shear failure

2006 ◽  
Vol 134 ◽  
pp. 835-838 ◽  
Author(s):  
D. Rittel ◽  
Z. G. Wang ◽  
M. Merzer
1994 ◽  
Vol 17 (2-3) ◽  
pp. 203-214 ◽  
Author(s):  
L.W. Meyer ◽  
E. Staskewitsch ◽  
A. Burblies

2010 ◽  
Vol 58 (11) ◽  
pp. 1759-1775 ◽  
Author(s):  
M. Dolinski ◽  
D. Rittel ◽  
A. Dorogoy

2017 ◽  
Vol 708 ◽  
pp. 492-502 ◽  
Author(s):  
A.A. Tiamiyu ◽  
A.Y. Badmos ◽  
A.G. Odeshi ◽  
J.A. Szpunar

2013 ◽  
Vol 753 ◽  
pp. 72-75 ◽  
Author(s):  
Hui Zhen Wang ◽  
Xiu Rong Sun ◽  
Ping Yang ◽  
Wei Min Mao

Adiabatic shear bands (ASBs) develop generally during high strain rates. This paper investigates the transformation induced plasticity (TRIP) effect during ASBs formation at high strain rates in high manganese TRIP steels containing initial austenite and ferrite by EBSD technique. Results show that TRIP effect takes place mainly before the formation of ASBs. After ASBs formation, TRIP effect is strongly restricted by the size effect, the increase of stacking fault energy (SFE) and even inverse martensitic transformation due to the rise of temperature. The TRIP effect before ASBs formation contributes to the resistance of adiabatic shear failure. Dynamic recrystallization driven by subgrains rotation occurs within ASBs, and ultrafine grains often show strong shear textures with twin relationship owing to slip mechanism.


Author(s):  
D. Rittel ◽  
Z. G. Wang

The thermo-mechanical aspects of adiabatic shear band (ASB) formation are studied for two commercial alloys: Mg AM50 and Ti6Al4V. Tests are carried out on shear compression specimens (SCS). The evolution of the temperature in the deforming gauge section is monitored in real time, using an array of high speed infrared detectors synchronized with a Kolsky apparatus (split Hopkinson pressure bar). The evolution of the gage temperature is found to comprise 3 basic stages, in agreement with Marchand and Duffy’s simultaneous observations of mechanical data and gauge deformation patterns (1988). The onset and full formation stages of ASB are identified by combining the collected thermal and mechanical data. Full development of the ASB is identified as the point at which the measured and calculated temperature curves intersect and diverge thereon. At that stage, the homogeneous strain assumption used in calculating the maximum temperature rise is no longer valid.


2017 ◽  
Vol 20 (1) ◽  
pp. 31-42 ◽  
Author(s):  
C. Froustey ◽  
O. B. Naimark ◽  
I. A. Panteleev ◽  
D. A. Bilalov ◽  
A. N. Petrova ◽  
...  

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