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2
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1542572472
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reprinted in Werke, vol. 5, Gottingen, 1876, p. 29 (in Latin)
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Gauss K.F. Comment. Soc. Regiae. Scient. Gottingensis Rec. 7:1830;. reprinted in Werke, vol. 5, Gottingen, 1876, p. 29 (in Latin).
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(1830)
Comment. Soc. Regiae. Scient. Gottingensis Rec.
, vol.7
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Gauss, K.F.1
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9
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1542467893
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At this point it should be emphasized that a much more recent nonlocal derivation due to Boruvka et al. [35] (see also the main text) generalizes Gibb's results to include additional energy terms.
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At this point it should be emphasized that a much more recent nonlocal derivation due to Boruvka et al. [35] (see also the main text) generalizes Gibb's results to include additional energy terms.
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10
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14944365766
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A Textbook of Physics. Properties of Matter
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London: Griffin. pp. 139-140
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Poynting J.H., Thomson J.J. A Textbook of Physics. Properties of Matter. eighth ed. 1902;Griffin, London. pp. 139-140.
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(1902)
Eighth Ed.
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Poynting, J.H.1
Thomson, J.J.2
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11
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0004002507
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Physical Chemistry of Surfaces
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Wiley. p. 353
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Adamson A.W. Physical Chemistry of Surfaces. sixth ed. 1997;Wiley. p. 353.
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(1997)
Sixth Ed.
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Adamson, A.W.1
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12
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0042602721
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Mechanics of Deformable Bodies
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New York: Academic Press. p. 127
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Sommerfield A. Mechanics of Deformable Bodies. Lectures on Theoretical Physics. vol. 2:1964;Academic Press, New York. p. 127.
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(1964)
Lectures on Theoretical Physics
, vol.2
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Sommerfield, A.1
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17
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0010255117
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London: Butterworth
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Pethica B.A., Pethica T.J. Second International Congress on Surface Activity, vol. III, Electrical Phenomena, Solid-Liquid Interface. 1957;131-135 Butterworth, London.
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(1957)
Second International Congress on Surface Activity, Vol. III, Electrical Phenomena, Solid-Liquid Interface
, pp. 131-135
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Pethica, B.A.1
Pethica, T.J.2
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22
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1542467892
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This point of view is also shared by W.A. Zisman: see his comments at the end of the paper in Ref. [15].
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This point of view is also shared by W.A. Zisman: see his comments at the end of the paper in Ref. [15].
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25
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1542572469
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In addition, it is significant that these authors do not try to invalidate Gibbs' derivation.
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In addition, it is significant that these authors do not try to invalidate Gibbs' derivation.
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26
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84953598190
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Shimizu S., Kusunase T., Kimura H., Ooyama M., Imura M., Ishikura S., Sahira K., Kitamura H., Shiraishi H., Nakada Y., Wada M., Suzuki M., Narite T. NASDA-JSUP. 1:1991;49.
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(1991)
NASDA-JSUP
, vol.1
, pp. 49
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Shimizu, S.1
Kusunase, T.2
Kimura, H.3
Ooyama, M.4
Imura, M.5
Ishikura, S.6
Sahira, K.7
Kitamura, H.8
Shiraishi, H.9
Nakada, Y.10
Wada, M.11
Suzuki, M.12
Narite, T.13
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28
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41349094751
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A microscopic derivation based on statistical mechanics does exist. Of course, any microscopic approach relies on several particular assumptions, e.g., concerning the molecular interactions. Thus, any microscopic approach necessarily has a lesser degree of generality compared to a thermodynamical derivation
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A microscopic derivation based on statistical mechanics does exist De Coninck J., et al. Phys. Rev. E. 65:2002;036139. Of course, any microscopic approach relies on several particular assumptions, e.g., concerning the molecular interactions. Thus, any microscopic approach necessarily has a lesser degree of generality compared to a thermodynamical derivation.
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(2002)
Phys. Rev. e
, vol.65
, pp. 036139
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De Coninck, J.1
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31
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1542677440
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Although implicitly, this assumption is also made in Ref. [11].
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Although implicitly, this assumption is also made in Ref. [11].
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36
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1542467890
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Although in our derivation the energy balance is written in terms of the Gibbs free energy, the results are exactly the same if the Hemoltz free energy is used instead. It should be remarked here that the process is not carried out at constant pressure nor at constant volume (both δV and δP are, in general, different from zero in Eq. (6)).
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Although in our derivation the energy balance is written in terms of the Gibbs free energy, the results are exactly the same if the Hemoltz free energy is used instead. It should be remarked here that the process is not carried out at constant pressure nor at constant volume (both δV and δP are, in general, different from zero in Eq. (6)).
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