0:00:04 | hello and welcome to live video offset to quantification of this additional information |
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0:00:09 | you know not only for making |
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0:00:11 | this work concerns quantification of mechanical phenomenon than a scale we had only for my |
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0:00:16 | school |
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0:00:20 | first take a look at an example for distance dependencies between sp of no scaling |
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0:00:25 | mentions and the surface of the sphere is over |
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0:00:29 | and mechanical that the curves this weekend so as before |
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0:00:33 | the maximum deformation doubled and the disability versus according in the mechanical contact i think |
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0:00:39 | weekly a known |
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0:00:41 | these parameters are characteristic of the sample be real and thus the quantification provide important |
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0:00:47 | information |
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0:00:51 | in this slide i joint goals you of the six initial |
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0:00:55 | the people you can be modeled as a sphere of radius r |
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0:00:58 | but the example interaction f t s is in general unknown |
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0:01:04 | one exhibiting process that been identified |
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0:01:08 | as dominating the interaction you namely if there is this force this t |
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0:01:12 | the energy dissipated by discourse history |
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0:01:15 | is linear in the distribution of variance with this war obviously shown in figure eight |
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0:01:21 | a quadratically with the maximum deformation or cycle tell and |
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0:01:29 | another linguistically processed in the context is served as energies three six |
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0:01:34 | the energy dissipated you the service energies there is easily handled without the surface energy |
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0:01:40 | how much information don't that m |
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0:01:45 | the initial dissipated in the interaction can be computed from the not experimental parameters |
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0:01:50 | but with this allows you with the energy dissipated by discourse dct and surface energy |
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0:01:54 | his thesis |
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0:01:56 | the unknowns can be recovered |
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0:02:00 | we can define a parameter k j but depends on you know experimental parameters |
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0:02:05 | from this parameter the sampled information can be quantified |
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0:02:08 | probably and the j minus k a k was you don't enforce that only three |
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0:02:14 | data points are quite looks like the deformation |
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0:02:20 | one information and the value of k j are known the difference in surface energy |
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0:02:25 | the data and the specific location you can then be readily computed |
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0:02:32 | an example of a typical a little versus complete separation is that the curve is |
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0:02:37 | shown in this slide |
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0:02:38 | what you exactly comparable to branches computer |
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0:02:44 | with the l a and the phase three |
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0:02:47 | which is not shown here the energy dissipated can be computed |
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0:02:52 | whether this corpus christi of surface energy stress is or isn't as the main disbelief |
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0:02:56 | mechanisms in the recorded version coming qualitatively established with the use of standard techniques |
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0:03:06 | finally the deformation basis coefficient to variations in service energy that are coming quantify we |
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0:03:14 | expect that that'll work will have implications of a purely on the interface between of |
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0:03:17 | the only a multiscale phenomena |
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