By A.S. Kompaneyets

A process Theoretical Physics, quantity 2. Statistical legislation: Statistical Physics, Hydrodynamics and gasoline Dynamics, Electrodynamics of continuing Media, actual Kinetics. writer: A. S. Kompaneyets. MIR Publishers, Moscow.

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T. Boublik, Mol. Phys. 27, 1415 (1974) 28. A. E. Martire, J. Chem. Phys. 52, 1970 (1909) 29. A. Cotter, Phys. Rev. A 10, 625 (1974) 30. G. Lasher, J. Chem. Phys. 53, 4141 (1970) 31. M. Holovko, V. Shmotolokha, T. Patsahan, J. Mol. Liq. 189, 30 (2014) 32. M. Holovko, V. Shmotolokha, T. Patsahan, (in preparation) 33. R. F. Holovko, Statistical theory of Classical Equilibrium Systems (Naukova Dumka, Kyiv, 1980) 34. P. R. McDonald, Theory of Simple Liquids (Academic Press, London, 2006) 35. G. E. Gubbins, Theory of Molecular Fluids (Clarendon Press, Oxford, 1984) 36.

The probability to ﬁnd scaled spherocylinder in an empty HS matrix is equal to p0 ðas ; ks Þ ¼ 1 À g0 ! 63) one can ﬁnd the derivatives needed for the description of thermodynamic properties of a conﬁned fluid: p00a ¼ À3 D1 3 L1 g0 ; p00a ¼ À g0 ; D0 2 D0 D2 p000kk ¼ À6g0 12 ; D0 p000ak ¼ À3g0 L1 D1 ; D0 D0 ð1:64Þ where g0 is the packing fraction of HS matrix particles. The probe particle porosity in this case is equal to [32] Fig. 2 Coexistence lines of isotropic-nematic phases of a hard spherocylinder fluid in a hard sphere matrix for L1 =D1 ¼ 20 and D0 ¼ L1 presented as a dependence of the spherocylinder fluid density c ¼ 14 pq1 L21 D1 on the matrix packing fraction g0 .

P. R. McDonald, Theory of Simple Liquids (Academic Press, London, 2006) 35. G. E. Gubbins, Theory of Molecular Fluids (Clarendon Press, Oxford, 1984) 36. D. Frenkel, B. Smith, Understanding Molecular Simulations (Academic, San Diego, 1995) 37. J. E. W. Wingate, Macromolecules 17, 1718 (1984) 38. L. Onsager, Ann. N. Y. Acad. Sci. 51, 627 (1949) 39. M. C. Wacker, Phys. Rev. A 18, 2669 (1978) 40. R. Tuinier, T. H. Wensink, Eur. Phys. J. E 23, 355 (2007) 41. F. J. Raveche, Phys. Rev. A 17, 2067 (1978) 42.

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