Treatise on analytical dynamics of particles and rigid by E. T. Whittaker

By E. T. Whittaker

There might be few books on mathematical mechanics as well-known as this, a piece that kinds a finished account of all of the classical result of analytical dynamics.

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S. L. Price & A. J. Stone, Molec. , submitted for publication. S. L. Price & A. J. Stone, 1982, Molec. , Ji7, 1457. P. Ricci, D. ll. R. INTRODUCTION Transport phenomena are the irreversible decay processes that occur spontaneously when a system, per tubed to a non equilibrium state by some external or internal disturbance, advances through a series of non equilibrium states until equilibrium is reached. ) are constant at all times and have the same magnitude at all position in the system. Therefore at equilibrium there are no gradients of the state parameters in the system and there is no net flux of matter or momentum or energy through the system.

J. C. Teixeira-Dias, 1970, Molec. , 19, 521. -C. Ng, W. J. Meath & A. R. Allnatt, 1979, Molec. , 37, 237. [46] s. L. Price & A. J. Stone, 1980, Molec. , 40, 805. [47] J. C. Raich & N. S. Gillis, 1977, J. chem. , 66, 846. [48] D. J. Evans & R. O. Watts, 1976, Molec. , 32, 93. [49] s. L. Price & A. J. Stone, 1983, Chem. Phys. Letters, 98, 419; Molec. , submitted for publication. [50] B. J. Berne & P. Pechukas, 1972, J. chem. , 56, 4213. [51 J R. T. Pack, 1978, Chem. Phys. Letters, 55, 197. [52J S.

In this case there is no difference among the various frames of reference and we call the mutual diffusion coefficient as the "self-diffusion coefficient, D ". e. tracer). In this case the mutual diffusion coeffi- DIFFUSION IN LIQUIDS 43 cient is practically equal to the diffusion coefficient of the tracer in respect to the solvent (see eq. 26); the tracer diffusion coefficient, [-i, in a binary mixture is practically the self diffusion coefficient of the tracer itself in the binary mix ture (to be correct to measure the self diffusion coefficient ofspecies 1 in a tw¥ component system we should have a three component system 1 + 1 + 2).

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