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The Functional Form of the Internal Energy
The Functional Form of the Internal Energy

... Therefore, is functionally dependent on the state variables T, P and V. However, since an equation of state will constrain the state variables, is formally a function of T and V, (T,V), or a function of T and P, (T,P). (T is not eliminated because we are considering thermodynamics afterall.) For rea ...
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... It is convenient to divide the universe into two parts: the system and the surroundings. The system contains all the matter involved in the change we are looking at. The system is defined so that it exchanges only heat with the surroundings, not matter. The surroundings are the rest of the universe. ...
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... ΔS = qrxn/T where qrxn is “reversible heat” Reversible processes may be reversed by very small changes, as in the expansion of this gas. Reversible processes are never very far from equilibrium. Entropy Increases with Temperature Entropy always increases with temperature …entropy increases dramatica ...
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... given in (4.5) and (4.38) of Ref. 4 and referred to as the “Boltzmann” energy) and the von Neumann expression (Sv N given in (4.36) of Ref. 4). In particular, the authors of Ref. 4 argue that “—neither the von Neumann entropy nor the Boltzmann entropy vanishes when the bath temperature is zero,” lea ...
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Notes 11 - CEProfs

... object B is 1 kg and it is initially at rest, what would be B’s final velocity from absorbing the potential from a 100 m drop of A? Assume that object B travels horizontally. ...
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Thermodynamics

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