1947
DOI: 10.2136/sssaj1947.036159950011000c0019x
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Thermodynamic Potential and Soil Moisture

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“…In most cases, only the infinitesimal changes in these quantities are of practical interest, rather than their absolute values. As such, expressions can be derived by differentiating the above three thermodynamic functions and combining the First and Second Laws of thermodynamics (e.g., Edlefsen & Anderson, 1943; Gardner & Chatelain, 1947; Schroeder, 2000). These are normaldHbadbreak=TnormaldSgoodbreak+VnormaldPgoodbreak−normaldWm\begin{equation}{\rm{d}}H = T{\rm{d}}S + V{\rm{d}}P - {\rm{d}}{W_{\rm{m}}}\end{equation} normaldFbadbreak=SnormaldTgoodbreak−PnormaldVgoodbreak−normaldWm\begin{equation}{\rm{d}}F = - S{\rm{d}}T - P{\rm{d}}V - {\rm{d}}{W_{\rm{m}}}\end{equation} normaldGbadbreak=SnormaldTgoodbreak+VnormaldPgoodbreak−normaldWm\begin{equation}{\rm{d}}G = - S{\rm{d}}T + V{\rm{d}}P - {\rm{d}}{W_{\rm{m}}}\end{equation}…”
Section: Thermodynamic Treatment Of Soil Water Potentialmentioning
confidence: 99%
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“…In most cases, only the infinitesimal changes in these quantities are of practical interest, rather than their absolute values. As such, expressions can be derived by differentiating the above three thermodynamic functions and combining the First and Second Laws of thermodynamics (e.g., Edlefsen & Anderson, 1943; Gardner & Chatelain, 1947; Schroeder, 2000). These are normaldHbadbreak=TnormaldSgoodbreak+VnormaldPgoodbreak−normaldWm\begin{equation}{\rm{d}}H = T{\rm{d}}S + V{\rm{d}}P - {\rm{d}}{W_{\rm{m}}}\end{equation} normaldFbadbreak=SnormaldTgoodbreak−PnormaldVgoodbreak−normaldWm\begin{equation}{\rm{d}}F = - S{\rm{d}}T - P{\rm{d}}V - {\rm{d}}{W_{\rm{m}}}\end{equation} normaldGbadbreak=SnormaldTgoodbreak+VnormaldPgoodbreak−normaldWm\begin{equation}{\rm{d}}G = - S{\rm{d}}T + V{\rm{d}}P - {\rm{d}}{W_{\rm{m}}}\end{equation}…”
Section: Thermodynamic Treatment Of Soil Water Potentialmentioning
confidence: 99%
“…The preceding thermodynamic principles reveal a unique advantage of the Gibbs function in studying soil water potential over other thermodynamic potentials (e.g., Edlefsen & Anderson, 1943; Slatyer & Taylor, 1960), because temperature and external pressure (usually atmosphere) in Equation are generally easy to determine or control for soil systems (e.g., Gardner & Chatelain, 1947). A decade after the first formal definition of soil water potential by the ISSS in 1963 (Aslyng et al., 1963), this concept was updated again by the second Terminology Committee of Commission I with further detail, and more thoroughly from the perspective of thermodynamics:
The total potential, ψ t , of the constituent water in soil at temperature T 0 , is the amount of useful work per unit mass of pure water, in J/kg, that must be done by means of externally applied forces to transfer reversibly and isothermally an infinitesimal amount of water from the state S 0 to the soil liquid phase at the point under consideration.
…”
Section: Thermodynamic Treatment Of Soil Water Potentialmentioning
confidence: 99%
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