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Quantities of work in thermodynamic equations

Journal of Chemical Education, 1969
Examines distinctions to be made between work done by forces exerted by external bodies and acting on a system with work done by forces exerted by the system on external bodies.
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Lorentz transformations of the thermodynamic quantities

Annals of Physics, 2019
zbMATH Open Web Interface contents unavailable due to conflicting licenses.
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Lorentz transformation of thermodynamic quantities

Proceedings of the Physical Society, 1966
It is shown that, to be consistent with the formalism of statistical mechanics, the absolute temperature T of, and the reversible heat δQ for, a thermodynamical system moving with a uniform velocity v with respect to a given frame of reference K should be related to the values T0 and δQ0 appropriate to the rest frame K0 by the old Planck-Einstein ...
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A COMPREHENSIVE PRESENTATION OF THE THERMODYNAMICS OF ADSORPTION EXCESS QUANTITIES

Pure and Applied Chemistry, 1976
Abstract A common general framework of thermodynamic relations between interfacial excess quantities in multicomponent systems is derived, based essentially on the fundamental Gibbsian treatment of adsorption phenomena. Both adjoining bulk phases are regarded as equivalent constituents of the system concerned—not only in the case of fluid interfaces,
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Lorentz transformations of thermodynamic quantities

Il Nuovo Cimento, 1965
The transformation formulae for basic thermodynamic quantities are derived within phenomenological thermodynamics by use of three assumptions or from relativistic mechanics and statistical thermodynamics. It is found that the transformation for thermodynamic pressure is different than that for mechanical pressure, the two pressures being the same only ...
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Balances of thermodynamic quantities in electrochemical systems

Electrochimica Acta, 1990
Abstract The balance for an arbitrary extensive quantity is dealt with in an open electrochemical system. ‘In particular, the balances of mass, energy, and entropy will be discussed. The similarities and differences in the flow and source terms of the balance equations are illustrated, thus revealing some essential general features of non-equilibrium
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Thermodynamic Quantities for Finite Overlap

1999
This chapter deals with the thermodynamic properties of the solution. As quantity of central importance we identify the thermodynamic scaling function P, defined in terms of the osmotic pressures as $$\frac{{\hat{\prod }}}{{{{k}_{B}}T}} = {{C}_{p}}\left[ {1 + \tilde{\mathcal{P}} (\tilde{s} ,\tilde{z} ,{\mkern 1mu} [p])} \right]$$ (17.1)
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THERMODYNAMIC QUANTITIES

1980
L.D. LANDAU, E.M. LIFSHITZ
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