4. Derive the maxwell equations for U, H, G and A Table 6.2.1: Maxwell Relations Function U H A G Differential dU = TdS-pdV dH TdS+Vdp dApdV SdT dG = Vdp - SdT Natural Variables S, V S, p V, T P, T Maxwell Relation Әр (7), - - (85), = av as V ƏT Әр op/s as as (F), - (55), (ar), - - (), Р T

4. Derive the maxwell equations for U, H, G and A Table 6.2.1: Maxwell Relations Function U H A G Differential dU = TdS-pdV dH TdS+Vdp dApdV SdT dG = Vdp - SdT Natural Variables S, V S, p V, T P, T Maxwell Relation Әр (7), - - (85), = av as V ƏT Әр op/s as as (F), - (55), (ar), - - (), Р T

College Physics

11th Edition

ISBN:9781305952300

Author:Raymond A. Serway, Chris Vuille

Publisher:Raymond A. Serway, Chris Vuille

Chapter1: Units, Trigonometry. And Vectors

Section: Chapter Questions

Problem 1CQ: Estimate the order of magnitude of the length, in meters, of each of the following; (a) a mouse, (b)...

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Concept explainers

Osmosis

In simple words, osmosis is the slow, gradual movement of a liquid through a membrane. But there are nuances to this process. For instance, there has to be an imbalance in the distribution of solute in the liquid on either side of the membrane, which has to be semipermeable. The liquid in the region with a lower solute concentration moves to the region with a higher concentration, thereby displacing the solution in the process. The objective is to equalize the concentration of molecules on both sides of the membrane; the displacement of liquid can be viewed as a byproduct of this equalization. Since there is no energy required to carry osmosis, it is considered a passive process.

Question

4. Derive the maxwell equations for U, H, G and A
Table 6.2.1: Maxwell Relations
Function
U
H
A
G
Differential
dU = TdS-pdV
dH = TdS + Vdp
dA=-pdV - SdT
dG = Vdp - SdT
Natural Variables
S, V
S, P
V, T
P, T
Maxwell Relation
(or)--(
др
as V
(37), = (35),
as
(OP), - (OV),
=
V
(3r), - - (35),
=
T

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