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What is thermodynamics and what is it for? I. Equilibrium and non-equilibrium in discrete systems
Peter Ván HAS, RIPNP, Department of Theoretical Physics
– Introduction– Stability and thermodynamics– Gases– Discussion
Centre of Nonlinear Studies, Tallinn, Estonia, 29/5/2006.
Thermodynamics:
Statics Dynamics
Point-mass Continuum
Mechanics:
Equilibrium Non-equilibrium
Phenomenological Statistical
Discrete (homogeneous)
Continuum
Equilibrium - non-equilibrium?– Mechanics – thermodynamics
• Differential equations?– Equilibrium - time independent– Quasistatic processes – time? (Zeno)– Irreversible processes – something more (internal variables)
II. law?– Heat can flow from a hotter body to the colder.
(Clausius)– There is no perpetuum mobile of the second kind.
(Planck)– In a closed system, in case of spontaneous processes the entropy
increases.– dS = drS + diS és diS0– ….
Discrete systems – equilibrium thermodynamics
Equilibrium thermodynamics
– S entropy
– de = q+w = Tds – pdv Gibbs relation
– There is a tendency to equilibrium
– Thermodynamic stability
What is?
Basic ingredients:
L: E is a Ljapunov function of the equilibrium, if:i) L has a strict maximum at ,
ii) , the derivative of L along the differential equation has a strict minimum at .
Theorem: If there is a Ljapunov function of , then is
asymptotically stable (stable and attractive).
EEfxfx :),()((*) t
Equilibrium of (*): 0xf )( 0
0x
)()()( xfxx DLL
0x 0x
))(())(()())(())(( ttDLttDLtL
dt
dxfxxxx
0x
0x
What is?
Instead of proof:
),()(
),()(
2122
2111
xxftx
xxftx
),,( 21 xxx
0)()()()( 0 xxfxx LDLL
x2
x1
0,, 2121
ffx
L
x
L
What is?
Dynamics without differential equation?
pdvqwqde
fv
vpqe
)( 0TTq
?
.,1
T
p
v
s
Te
s
‘dynamic law?’
A) entropy
B)
T, p T0, p0
as a potential.
q
What is?
Stability structure:
.
.,
0
0
constvvv
consteee
T
T
),(),(),( 000 vesvesvesT
,11
),(0TT
vee
sT
.),(0
0
T
p
T
pve
v
sT fv
vpqe
Ljapunov function
i) )0,0(,),( 00
v
s
e
sveDs TT
T
sDsD T22
0)(11
)(11
),(,),(
00
00
0
0
T
fppq
TTf
T
p
T
ppfq
TT
fpfqv
s
e
sfpfqDss TT
TTii)
convex – thermodynamic stability
Direction of heat: 00 qTT
)(
),()(
0
00
ppv
pppTTe
sD2
0)(11
00
0
T
fppq
TT
convex
E.g. ppf
TTq
0
0
v
RTp
cTe
0,0
.0,0 cR
Dynamic Law
Dynamic material functions(heat exchange, …)
Static material functions (ideal gas)
fv
vpqe
Thermodynamic theory in general
)a(fa Dynamic Law:
1 Statics (properties of equilibrium): existence of entropy
2 Dynamics (properties of interactions): increasing entropy
0)()()()( afaDSaaDSaS
Stability structure Dynamic structure
What for?
Quasistatic processes of a Van der Waals gas:
1 2 3 4 5 6v
0.25
0.5
0.75
1
1.25
1.5
1.75
2
p
2
3
13
8
3
vv
Tp
veT
5.0
9.0
1
0
0
p
T
1 2 3 4 5 6v
0.25
0.5
0.75
1
1.25
1.5
1.75
2
p
fv
vpqe
Pitchfork bifurcation of a Van der Waals gas (bifurcation diagram)
v0
T0
p0
Second order equation – internal variables
fv
vpqe
ˆ
ˆˆ
.0)0,,(~),,,(~),(),,(
vep
uvepvepuvep
Non-equilibrium state functions:
T, p T0, p0
State space: q
What is?
),,( vuve
uuvep ),,(~e.g.
Stability structure:
Ljapunov function
0~11
0
T
upq
TTsT
Viscous-damping: 0~ up
)ˆ(ˆ
ˆˆ
0ppfv
vpqe
0
2
000 2),(),(),,(
T
uvesvesuvesTNE
What is?
Entropy of the body:
T
up
T
qs
~ dS = drS + diS és diS0
vpTsvpvpqe )~ˆ(
Irreversible processes of a Van der Waals gas:
1 2 3 4 5 6v
0.25
0.5
0.75
1
1.25
1.5
1.75
2
p
2
3
13
8
3
vv
Tp
veT
0
5.0
9.0
1
0
0
p
T
1 2 3 4 5 6v
0.25
0.5
0.75
1
1.25
1.5
1.75
2
p
1 2 3 4 5 6v
0.25
0.5
0.75
1
1.25
1.5
1.75
2
p
1
5.0
9.0
1
0
0
p
T
Movie-like:
1 2 3 4 5 6v
0.25
0.5
0.75
1
1.25
1.5
1.75
2
p
1 2 3 4 5 6v
0.25
0.5
0.75
1
1.25
1.5
1.75
2
p
1 2 3 4 5 6v
0.25
0.5
0.75
1
1.25
1.5
1.75
2
p
1 2 3 4 5 6v
0.25
0.5
0.75
1
1.25
1.5
1.75
2
p
1 2 3 4 5 6v
0.25
0.5
0.75
1
1.25
1.5
1.75
2
p
1 2 3 4 5 6v
0.25
0.5
0.75
1
1.25
1.5
1.75
2
p
1 2 3 4 5 6v
0.25
0.5
0.75
1
1.25
1.5
1.75
2
p
1 2 3 4 5 6v
0.25
0.5
0.75
1
1.25
1.5
1.75
2
p
1 2 3 4 5 6v
0.25
0.5
0.75
1
1.25
1.5
1.75
2
p
1 2 3 4 5 6v
0.25
0.5
0.75
1
1.25
1.5
1.75
2
p
1 2 3 4 5 6v
0.25
0.5
0.75
1
1.25
1.5
1.75
2
p
1 2 3 4 5 6v
0.25
0.5
0.75
1
1.25
1.5
1.75
2
p
1 2 3 4 5 6v
0.25
0.5
0.75
1
1.25
1.5
1.75
2
p
Conclusions
– A thermodynamic structure is a stability structure• Time dependent discrete systems!• Equilibrium – quasistatic – irreversible
– Completing the structure: theory construction• Static: consistency, thermic caloric• Dynamics: Onsager reciprocity, constitutive functions, • Constructive!
– Stability of the theory: stability of the calculations.• Robust numerical codes: numerical viscosity
– Discrete – continuum: the same principles.
What is for what?
Thanks:
To the Hungarian thermodynamic tradition:
Julius Farkas, Imre Fényes, István Gyarmati,...Joe Verhás, Tamás MatolcsiThermodynamic Division
of the Hungarian Physical Society,