-
2
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68849126887
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-
Gibbs (Ref.) referred to γ (which he denoted σ) as "tension" of a "surface of discontinuity" (interface). In current literature this quantity is usually called interface free energy.
-
Gibbs (Ref.) referred to γ (which he denoted σ) as "tension" of a "surface of discontinuity" (interface). In current literature this quantity is usually called interface free energy.
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3
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68849083477
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The equilibrium condition M21 =const with M21 defined by Eq. applies not only to solid-liquid but also to solid-solid equilibria. Solid-solid interfaces will be discussed in a separate publication.
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The equilibrium condition M21 =const with M21 defined by Eq. applies not only to solid-liquid but also to solid-solid equilibria. Solid-solid interfaces will be discussed in a separate publication.
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23
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68849115503
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In Ref., as well as in our previous paper (Ref.), the quantity was denoted [Z/XY]. We find that equations involving this quantity look more clear with the notation [Z] XY, which we will adopt from now on.
-
In Ref., as well as in our previous paper (Ref.), the quantity was denoted [Z/XY]. We find that equations involving this quantity look more clear with the notation [Z] XY, which we will adopt from now on.
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-
-
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24
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33747642981
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0965-0393,. 10.1088/0965-0393/14/5/002
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P. L. Williams, Y. Mishin, and J. C. Hamilton, Modell. Simul. Mater. Sci. Eng. 0965-0393 14, 817 (2006). 10.1088/0965-0393/14/5/002
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26
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0003689862
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0001766772
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68849090476
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Despite these variations, the solid layer thickness always remained at least 60 Å and the thickness of each liquid layers at least 45 Å.
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Despite these variations, the solid layer thickness always remained at least 60 Å and the thickness of each liquid layers at least 45 Å.
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31
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68849092761
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For curved interfaces, even γ is not unique as was discussed by Gibbs (Ref.) for fluid systems. The identification of γ with an excess of relative to the surface of tension has certain advantages but is just one of many possible placements of the dividing surface, each giving a different value of γ.
-
For curved interfaces, even γ is not unique as was discussed by Gibbs (Ref.) for fluid systems. The identification of γ with an excess of relative to the surface of tension has certain advantages but is just one of many possible placements of the dividing surface, each giving a different value of γ.
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32
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68849128485
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Gibbs (Ref.) referred to interface stress as "true tension," as opposed to the interface free energy which we called "tension."
-
Gibbs (Ref.) referred to interface stress as "true tension," as opposed to the interface free energy which we called "tension."
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