0:00:03 | hello my name easily the enough and then going to include use the article local |
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0:00:07 | numerical study of than obvious talk transform coefficient for a two-dimensional ground or a gas |
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0:00:13 | and the mic out those are some the professors and then you can read your |
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0:00:17 | professor classes and when your professor with anything are so i'm professor tossed in question |
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0:00:23 | in this article we present an american the study of a two-dimensional ground or assisting |
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0:00:27 | comparing the well-known even dreaming molecular dynamics simulation with a two different approaches for than |
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0:00:34 | obvious to transform coefficient for the kind of the next inhalation |
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0:00:38 | these two approaches are thinking treatment theory which is considered for the more they really |
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0:00:43 | then scores elastic greens and improve not filled of t let's go fairly which includes |
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0:00:48 | the effect of the elasticity and the transfer coefficient |
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0:00:52 | previous studies of the natural instability fourteen elastic are these compare it molecular dynamics simulation |
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0:00:57 | with aging can treatment hundred and i'm assimilation finding a good description of the particular |
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0:01:04 | flow |
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0:01:04 | or where aim is to check if one can get the weather agreement using improve |
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0:01:09 | it times per coefficient |
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0:01:11 | this instability appear when a free teaching kidding vertical direction considering and external force like |
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0:01:18 | gravity |
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0:01:20 | and in this media we can see the then significant for the three them with |
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0:01:24 | different simulation |
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0:01:26 | and the jenkins treatment had an i means energy the other hand the dynamics |
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0:01:30 | when the front of a instability "'cause" already formant this happens after about fifty periods |
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0:01:36 | of shaking |
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0:01:37 | we observe that super money per to dynamics where the period it's twice the palatal |
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0:01:42 | forcing |
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0:01:44 | we study in different quantities to analyze the mechanism to find a study supersonic general |
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0:01:49 | flow |
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0:01:50 | we are representing a vertical cut of before informing the goods as a function of |
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0:01:54 | the hyping diameters at the position where the maximum had a hike of the batteries |
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0:02:00 | achieve |
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0:02:01 | from left to right and from top to bottom we have presented |
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0:02:05 | marking fraction internal energy templates or vertical component of heat clocks only coefficient and kinetic |
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0:02:12 | energy |
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0:02:14 | all of them are to scholar we gravity and particles the amateurs |
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0:02:20 | let us draw the attention at the back and to the packing fraction and attempted |
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0:02:24 | to feel |
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0:02:25 | i t zero the piston is going down of the cleveland position |
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0:02:29 | from that point the g d l prediction is then so then j r |
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0:02:33 | in time between ten and twenty diameters |
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0:02:36 | then we have found the dissolution of the peak on the bali appears |
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0:02:40 | after that we have another in but with the plate forming again a peak |
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0:02:45 | it maximum density and the is a smaller than in high the dynamics |
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0:02:51 | the most striking difference between t v l and a are solution is the temperature |
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0:02:56 | where at large phase difference is about one order of magnitude |
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0:03:00 | this is related with fixed at that the peers in the heat well actually it |
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0:03:04 | with the gradient of the dancing |
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0:03:07 | all these fields that explain it in the iron and discuss it along the paper |
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0:03:12 | the perspective is to understand the role of the so that the piercing the temperature |
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0:03:17 | a question |
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0:03:18 | and in other setups a set a shift rule |
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0:03:23 | enjoyed everything |
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