- #1
nonequilibrium
- 1,439
- 2
(In the following discussion, when I use the word "always", I mean "as good as always" if you're willing to ignore exotic systems with negative temperature and such)
In the following discussion I will assume we're working in a heat bath with constant T and P:
So there are several ways to see the total Gibbs free energy of an object, defined G = U - TS + PV, is negative.
Two simple ways:
(*) Chemical potential is defined as [tex]\mu = -T \left( \frac{dS}{dN} \right)_{U,V}[/tex] and thus is always negative. We also can prove [tex]G = \mu N[/tex].
(*) We know [tex]T \Delta S \geq Q = Q + P \Delta V - P \Delta V \geq Q + P \Delta V + W = \Delta U + P \Delta V[/tex] so [tex]TS \geq U + PV[/tex] or [tex]G \leq 0[/tex].
So now the problem is, when we 'make something' its G function goes from zero to something negative (as was just shown in two ways). This implies it should happen spontaneously, since in constant T and P the second law becomes "G goes to a minimum".
So does this say things should randomly pop into existence? Obviously there is a thinking error?
In the following discussion I will assume we're working in a heat bath with constant T and P:
So there are several ways to see the total Gibbs free energy of an object, defined G = U - TS + PV, is negative.
Two simple ways:
(*) Chemical potential is defined as [tex]\mu = -T \left( \frac{dS}{dN} \right)_{U,V}[/tex] and thus is always negative. We also can prove [tex]G = \mu N[/tex].
(*) We know [tex]T \Delta S \geq Q = Q + P \Delta V - P \Delta V \geq Q + P \Delta V + W = \Delta U + P \Delta V[/tex] so [tex]TS \geq U + PV[/tex] or [tex]G \leq 0[/tex].
So now the problem is, when we 'make something' its G function goes from zero to something negative (as was just shown in two ways). This implies it should happen spontaneously, since in constant T and P the second law becomes "G goes to a minimum".
So does this say things should randomly pop into existence? Obviously there is a thinking error?