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Energy and Thermodynamic Relations

Conservation of total energy is a law of mechanical systems, and it serves as the first law of fhermod5mamics. From the conservation of energy of a closed, isolated system, we can identify cerfain energy quantities that are state functions their values do not depend on the path the system followed to reach its current state. [Pg.37]

Problem Find an expression for the isothermal compressibility of a gas that obeys Equation 2.30, a Berthelot gas. [Pg.38]

Solution The isothermal compressibility, p in Equation 2.36, requires finding the derivative of V with respect to P at constant temperature. We start with the equation of state for the Berthelot gas. Equation 2.30. [Pg.38]

Substituting this into Equation 2.36 yields p for a Berthelot gas. [Pg.38]

This answer may be sufficient however, we could go back to the original equation of state and use it to express p in terms of only two variables, not three. From taking the inverse of the second form of the equation of state, 1/V is expressed in terms of P and T. [Pg.39]


See other pages where Energy and Thermodynamic Relations is mentioned: [Pg.394]    [Pg.37]   


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