Research on alternate bulge-forming process of spherical parts in near equal-thickness wall and strain field analysis

2016 ◽  
Vol 90 (5-8) ◽  
pp. 2325-2333 ◽  
Author(s):  
Yahong Xue ◽  
Shuyi Luo ◽  
Junting Luo ◽  
Qing Li
2000 ◽  
Vol 9 (1) ◽  
pp. 096369350000900 ◽  
Author(s):  
T.C. Lim ◽  
S. Ramakrishna ◽  
H.M. Shang

Previous modelling techniques in sheet forming of textile composites have focused on computational simulations due to the numerous computations involved. Recently a procedure for stretch forming analysis of plain weft-knitted fabric composites has been developed. The analytical model for the stretch forming process is now being extended for the deep drawing process in this paper. The theoretical strain field gives good approximation to the experimental results.


2013 ◽  
Vol 114 (2) ◽  
pp. 023511 ◽  
Author(s):  
R. Tanuma ◽  
D. Mori ◽  
I. Kamata ◽  
H. Tsuchida

2006 ◽  
Vol 41 (14) ◽  
pp. 4454-4465 ◽  
Author(s):  
Norbert Hueging ◽  
Martina Luysberg ◽  
Helmut Trinkaus ◽  
Karsten Tillmann ◽  
Knut Urban
Keyword(s):  

2012 ◽  
Vol 201-202 ◽  
pp. 1066-1070
Author(s):  
Zhan Li ◽  
Xue Dao Shu ◽  
Wen Fei Peng ◽  
Bao Shou Sun

The analysising of strain is the key factors to understand the forming mechanism of cross wedge rolling asymmetric shaft. due to the extrusion of dies and other external force, its interior,interactions can cause the relative position between the various parts. In order to study the deformation of workpiece at different degrees, pulling in the finite element strain field analysis, the strain of the analysis at deformation process is also a necessary precondition for forming and stress distribution. In this papre,By using Deform3D platform, the forming process of the cross wedge rolling on parity wedge asymmetric shaft is simulated. It is also to be analyzed the distribution and variation of the amount of strain in the rolling process, it shows that a cross-sectional and longitudinal section about the deformation characteristics of the strain fields, the results can achieve production of cross wedge rolling and provide important theoretical foundation to promote further cross-wedge rolling.


Strain ◽  
1983 ◽  
Vol 19 (2) ◽  
pp. 69-75 ◽  
Author(s):  
A. Peiter ◽  
W. Lode

2006 ◽  
Vol 12 (S02) ◽  
pp. 1014-1015
Author(s):  
T Bartel ◽  
C Kisielowski ◽  
P Specht

Extended abstract of a paper presented at Microscopy and Microanalysis 2006 in Chicago, Illinois, USA, July 30 – August 3, 2006


2021 ◽  
Vol 13 (12) ◽  
pp. 2298
Author(s):  
Raffaele Castaldo ◽  
Pietro Tizzani ◽  
Giuseppe Solaro

In this study, we analyze the 2009–2013 uplift phenomenon at Campi Flegrei (CF) caldera in terms of temporal and spatial variations in the stress/strain field due to the effect of an inflating source. We start by performing a 3D stationary finite element (FE) modeling of X-band COSMO-SkyMed DInSAR and GPS mean velocities to retrieve the geometry and location of the deformation source. The modeling results suggest that the best-fit source is a three-axis oblate spheroid ~3 km deep, which is mostly elongated in the NE–SW direction. Furthermore, we verify the reliability of model results by calculating the total horizontal derivative (THD) of the modeled vertical velocity component; the findings emphasize that the THD maxima overlap with the projection of source boundaries at the surface. Then, we generate a 3D time-dependent FE model, comparing the spatial and temporal distribution of the shear stress and volumetric strain with the seismic swarms beneath the caldera. We found that low values of shear stress are observed corresponding with the shallow hydrothermal system where low-magnitude earthquakes occur, whereas high values of shear stress are found at depths of about 3 km, where high-magnitude earthquakes nucleate. Finally, the volumetric strain analysis highlights that the seismicity occurs mainly at the border between compression and dilatation modeled regions, and some seismic events occur within compression regions.


2017 ◽  
Vol 160 ◽  
pp. 604-612 ◽  
Author(s):  
Zakariya Boufaida ◽  
Julien Boisse ◽  
Stéphane André ◽  
Laurent Farge

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