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exercises:2014_uzh_molsim:chp_cu111

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exercise:mm_uzh:chp_cu111 [2014/07/03 17:34] – talirzexercise:2014_uzh_molsim:chp_cu111 [2014/10/15 13:42] – oschuett
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 The problem with this approach is that the lack of any surfaces makes it very hard for the liquid phase to nucleate in a small cell and within a reasonable simulation time. In such a simulation, melting will typically be observed only at temperatures significantly above $T_m$. The problem with this approach is that the lack of any surfaces makes it very hard for the liquid phase to nucleate in a small cell and within a reasonable simulation time. In such a simulation, melting will typically be observed only at temperatures significantly above $T_m$.
  
-{{ :exercise:mm_uzh:folded.png?700 |Half-molten Cu slab.}}+{{ folded.png?700 |Half-molten Cu slab.}}
  
 Here, we will use the so-called //phase coexistence technique// developed by [[doi>10.1007/978-94-011-1729-6|Ercolessi et al.]]. Here, we will use the so-called //phase coexistence technique// developed by [[doi>10.1007/978-94-011-1729-6|Ercolessi et al.]].
exercises/2014_uzh_molsim/chp_cu111.txt · Last modified: 2020/08/21 10:15 by 127.0.0.1