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Published byJames Singleton Modified over 9 years ago
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Weakly nonlocal non-equilibrium thermodynamics Peter Ván Budapest University of Technology and Economics, Department of Chemical Physics Non-equilibrium thermodynamics Beyond local equilibrium and local state Exploitations of the Second Law - Liu procedure Examples Guyer-Krumhansl equation Ginzburg-Landau equation One component fluid mechanics - quantum (?) fluids Conclusions
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Local equilibrium (~ there is no microstructure)
Classical Irreversible Thermodynamics Local equilibrium (~ there is no microstructure) Beyond local equilibrium (nonlocality): in time (memory effects) in space (structure effects) dynamic variables ? Method: local state and beyond …
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Nonlocalities: Restrictions from the Second Law.
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Non-equilibrium thermodynamics
basic balances (and more) basic state: constitutive state: constitutive functions: weakly nonlocal Second law: (universality) Constitutive theory Method: Liu procedure Speciality: constructive
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Weakly nonlocal extended thermodynamics
state space constitutive functions local state: Liu procedure (Farkas’s lemma): solution?
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extended (Gyarmati) entropy
entropy current (Nyíri) (B – current multiplier) balance? local?
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Weakly nonlocal internal variables
Ginzburg-Landau (variational): Second Law Variational (!)
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? Ginzburg-Landau (thermodynamic, relocalized) local state
state space constitutive functions local state Liu procedure (Farkas’s lemma) ?
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current multiplier isotropy
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Ginzburg-Landau (thermodynamic, non relocalizable)
state space constitutive functions Liu procedure (Farkas’s lemma)
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One component weakly nonlocal fluids
and quantum mechanics
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Schrödinger equation:
Madelung transformation: de Broglie-Bohm form: Hydrodynamic form:
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One component weakly nonlocal fluid
basic state constitutive state constitutive functions Liu procedure (Farkas’s lemma):
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Schrödinger-Madelung fluid
reversible pressure (Fisher entropy) Schrödinger-Madelung fluid
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Schrödinger equation:
Madelung transformation: de Broglie-Bohm form: Hydrodynamic form:
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One component weakly nonlocal fluid
basic state constitutive state constitutive functions Liu procedure (Farkas’s lemma):
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Schrödinger-Madelung fluid
reversible pressure (Fisher entropy) Schrödinger-Madelung fluid
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Potential form: Bernoulli equation Schrödinger equation Euler-Lagrange form Variational origin
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Why nonequilibrium thermodynamics?
science of temperature Thermodynamics science of macroscopic energy changes general framework of any Thermodynamics (?) macroscopic (?) continuum (?) theories General framework: fundamental balances objectivity - frame indifference Second Law reversibility – special limit
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Conclusions Not everything is a balance
Second order nonlocality is interesting Constitutive entropy current Force-current systems: constructivity Variational principles Second Law
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