Enthalpy

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Enthalpy (\(H\)) [1][2] is defined as:

\[\left.H\right.=U+pV\]

where \(U\) is the internal energy, \(p\) is the pressure, \(V\) is the volume. \(pV\) is a conjugate pair. The differential of this function is

\[\left.dH\right.=dU+pdV+Vdp\]

From the Second law of thermodynamics one obtains

\[\left.dH\right.=TdS -pdV +pdV+Vdp\]

thus we arrive at

\[\left.dH\right.=TdS +Vdp\]

For \(H(S,p)\) we have the following total differential

\[dH=\left(\frac{\partial H}{\partial S}\right)_p dS + \left(\frac{\partial H}{\partial p}\right)_S dp\]

[edit] References

  1. J. P. Dalton "Researches on the Joule-Kelvin effect, especially at low temperatures. I. Calculations for hydrogen", KNAW Proceedings 11 pp. 863-873 (1909)
  2. Irmgard K. Howard "H Is for Enthalpy, Thanks to Heike Kamerlingh Onnes and Alfred W. Porter", Journal of Chemical Education 79 pp. 697-698 (2002)
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