shock modeling
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2019 ◽  
Vol 64 (8) ◽  
pp. 859-868
Author(s):  
E. V. Petrova ◽  
V. I. Grokhovsky ◽  
T. Kohout ◽  
R. F. Muftakhetdinova ◽  
G. G. Yakovlev

The shock experiment with Chelyabinsk LL5 light lithology material was performed as a spherical geometry shock. The material experienced shock and thermal metamorphism from the initial S3–4 up to complete melt stage. Temperature and pressure realized were estimated above 2000°С and 90 GPa. Textural shock effects were studied by the means of optical and electron microscopy. By the only experimental impact, all the range of the shock pressures and temperatures was realized. Four zones were revealed from the petrographic analysis: 1 – melt zone, 2 – melted silicates zone, 3 – black ring zone, 4 – weakly shocked initial material. Several features of the material texture were noted: displacement of the metal and troilite phases from the central melt zone; mixed lithology zone formation (light-colored chondrules within the silicate melt); dark-colored lithology ring formation; generation of radial-oriented shock veins. Thus, at the experimental fragment, four texture zones were formed. These zones correspond to the different lithology types of the Chelyabinsk LL5 meteorite, which could be found in different fragments of the meteoritic shower from UrFU collection. The results obtained prove that the shock wave loading experiment could be used for space shock modeling. Therefore, the processes of the small bodies of the Solar system could be experimentally modeled at the laboratory conditions.


2017 ◽  
Vol 836 (1) ◽  
pp. 76 ◽  
Author(s):  
P. N. Appleton ◽  
P. Guillard ◽  
A. Togi ◽  
K. Alatalo ◽  
F. Boulanger ◽  
...  
Keyword(s):  

2014 ◽  
Author(s):  
Jim Gilliat ◽  
Derek Bale ◽  
Rajani Prakash Satti ◽  
Crystal Li ◽  
Jesse James Howard

2013 ◽  
Vol 196 ◽  
pp. 51-61
Author(s):  
Andrzej Grządziela ◽  
Bogdan Szturomski

Ship shock tests have been conducted for shock qualification of hull integrity and proper operation systems and subsystems. The ship shock trial identifies design and construction and it also validates shock hardening criteria. The main problem is that ship shock trials are costly. Numerical modeling and simulation, using FEM, may provide information to look into the details of fluid model, dynamic characteristics of ship hull and its internal component. The ship shock modeling and simulation has been performed and the predicted results were compared with ship shock test data made into sea trials. The preliminary studies of shock analysis approach are presented and the important parameters are discussed


2012 ◽  
Vol 117 (A5) ◽  
pp. n/a-n/a ◽  
Author(s):  
K. Jelínek ◽  
Z. Němeček ◽  
J. Šafránková

2011 ◽  
Vol 180 ◽  
pp. 288-296 ◽  
Author(s):  
Andrzej Grządziela

Ship shock tests have been conducted for shock qualification of hull integrity and proper operation systems and subsystems. The ship shock trial identifies design and construction and it also validates shock hardening criteria. The main problem is that ship shock trials are costly. Numerical modeling and simulation, using FEM, may provide information to look into the details of fluid model, dynamic characteristics of ship hull and its internal component. The ship shock modeling and simulation has been performed and the predicted results were compared with ship shock test data made into sea trials. The preliminary studies of shock analysis approach is presented and the important parameters are discussed.


Atomic Energy ◽  
2011 ◽  
Vol 109 (3) ◽  
pp. 213-220
Author(s):  
E. Uspuras ◽  
A. Kaliatka ◽  
V. Kopustinskas ◽  
M. Vaisnoras

2009 ◽  
Vol 9 (2) ◽  
pp. 501-506 ◽  
Author(s):  
G. Chouliaras

Abstract. This investigation has applied a recent methodology to identify seismic quiescence and seismic acceleration, prior to the occurrence of the 13 December 2008, Ms=5.7 earthquake in Central Greece. Anomalous seismic quiescence is observed around the epicentral area almost twelve years prior to the main shock and it lasted for a period of about four and a half years. After this period an acceleration in seismic activity began and lasted until the main shock. Modeling this seismic sequence with the time-to-failure equation and with a fixed value of the exponent "m" equal to 0.32, shows a successful estimation of the occurrence time of the main event within a few days. The physical meaning of this particular choice of the "m" value is discussed.


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