2 Flashcards
Non- equilibrium thermodynamics
Deals with states and processes in systems that are not in thermodynamic equilibrium. In some cases these states and processes are stable for certain period of time in open systems: Steady state and Dissipative structures.
Equilibrium state
Values of all variables of the system are constant and equal in each point of the system and in the surroundings ⇒ no gradients, no structure, the system is homogeneous = HIGH ENTROPY
Non-equilibrium state
Values of all variables of the system are not constant and not equal in each point of the system and in the surroundings ⇒ gradients, structure, the system is inhomogeneous = LOW ENTROPY
Equilibrium process
Transition between two equilibrium states. The system is reversible; can return to the initial state spontaneously.
Non-equilibrium process
At least one state is a non-equilibrium state. The system is irreversible; cannot return to the initial state spontaneously.
Onsager’s relation
= A gradient is the driving force of a flow (flux) in non-equilibrium processes:
Steady (stationary) state
All state variables are constant in spite of ongoing processes
Jin = -Jex ⇒ constant values of all parameters of the system
Prigogine’s theorem
In a steady (stationary) state, the rate ot production of entropy (ΔS/Δt)in inside the system is always positive but has a minimal value. ⇒ The consumption of free energy is minimal.
Dissipative structure
- non-equilibrium steady state in open systems
- non-linear processes Li = f(Xi)
- super critical values of gradients in the system
- cooperative behaviour of fluxes
Example: Benard cells, fire, turbines, ect.