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Stability of Matter
Stability of Matter

... In Section 3.2, we will pull out the e-dependence6 from VC . Note 2.2.1. Let us collect some properties of (2.9) and (2.10). (i) The direction of the Coulomb force is determined by the relative sign of q and Q. If their signs are the same, the force is repulsive. Otherwise, it is attractive. (ii) Th ...
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... causing a greater decrease of -potential. So, if an electrolyte, having bivalent negative ions will be applied for causing of coagulation in this sole, its coagulating ability will be much greater, than of an electrolyte, containing univalent negative ions. Now we can formulate Shultze-Hardy’s law: ...
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... We can see from the plots that the Poisson distribution is well defined for large values of N, in actuallity the Binomial distribution becomes the Poisson distribution for large value of N. Problem # 4 The Meaning of Never It has been said that “six monkeys, set to strum unintellegently on typewrite ...
The Kinetic Theory of Gases - Department of Applied Physics
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On a Report by the German Physical Society Concerning

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Thermodynamics Theory + Questions.0001

... Fig. A quasi q – static process one the pressure of the gass will displace the piston gradually. It is quasista atic. • On the other hand if we remove all a the weights at once th he piston will be kicked up p by the gas pressure. (This is un nrestrained expansion) but b we don’tt consider th hat th ...
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Thermodynamics of a pure substance at the triple point
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Thermodynamics and Statistical Mechanics

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Thermodynamic Properties of a single component fluid PV UH += TS
Thermodynamic Properties of a single component fluid PV UH += TS

... Since we have 8 different variables (T, P, V, U, H, S, G, & A) and three ways they can be entered into X, Y, and Z, we have a total of 83 = 512 different partial derivatives. The Bridgeman Tables can give us any of these partials, although some are not as useful as others. The Bridgeman Tables requi ...
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H-theorem



In classical statistical mechanics, the H-theorem, introduced by Ludwig Boltzmann in 1872, describes the tendency to increase in the quantity H (defined below) in a nearly-ideal gas of molecules. As this quantity H was meant to represent the entropy of thermodynamics, the H-theorem was an early demonstration of the power of statistical mechanics as it claimed to derive the second law of thermodynamics—a statement about fundamentally irreversible processes—from reversible microscopic mechanics.The H-theorem is a natural consequence of the kinetic equation derived by Boltzmann that has come to be known as Boltzmann's equation. The H-theorem has led to considerable discussion about its actual implications, with major themes being: What is entropy? In what sense does Boltzmann's quantity H correspond to the thermodynamic entropy? Are the assumptions (such as the Stosszahlansatz described below) behind Boltzmann's equation too strong? When are these assumptions violated?↑
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