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Material Type: Notes; Professor: Richard; Class: PHYSICAL CHEMISTRY I; Subject: Chemistry; University: The Richard Stockton College of New Jersey; Term: Fall 2008;
Typology: Study notes
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Chemistry Program, School of Natural Sciences and Mathematics PO Box 195, Pomoma, NJ
October 6, 2008
Lecture 15: Chemical potential of an ideal gas
μ(T, P ) = μ◦(T ) + RT ln
where μ◦(T ) is the chemical potential of the pure gas in the reference state (usually P = 1 bar)
∂G ∂T
P,n
∂μ ∂T
P,n (where the bar above the quantity means per mole, or the molar entropy).
PA = XAPT OT AL
μmixturei (T, P ) = μpurei (T, P ) + RT ln XA
item The mixing of ideal gases is completely driven by entropy. There is no interaction between gas atoms/molecules in an ideal gas, therefore ∆Hmix = 0. Going from the unmixed to mixed state results in an increase in entropy (∆Smix > 0) meaning that ∆Gmix < 0 (∆G = ∆H − T ∆S).
∆Gmix = RT
Xi ln Xi
∆Gmix = RT (XA ln XA + XB ln XB )
Exercises: 4.40, 6.