Thermodynamic Equilibrium of Plasmas
Plasmas can exhibit a large variety of properties. There are plasmas with high and low ionization degrees, as well as those with high and low pressures and hot and cold temperatures. Different equations and modeling approaches are necessary for each kind of plasma. This blog post gives an overview of the different plasma types and shows when to use which of the interfaces available in the Plasma Module.
Thermodynamic Equilibrium (TE)
If a plasma is located in a closed system, each process is in equilibrium with its reverse process (detailed balance) and the plasma is in thermodynamic equilibrium. Such a plasma can be characterized with a few parameters: The (typically very high) temperature, pressure, and number densities of each single species. The radiation corresponds to black-body radiation and can be described with Planck’s law. The population of the excited states obeys a Boltzmann distribution, while the velocity distribution is Maxwellian. The Saha equation gives the ionization degree.
Local Thermodynamic Equilibrium (LTE)
In a real plasma, deviations from equilibrium occur. For example, radiation escapes out of the plasma, disturbing the detailed balance. If the equilibrium still holds in a local sense, the plasma is in local thermodynamic equilibrium (LTE). The plasma can still be described (locally) by the above mentioned relations, with the exception of Planck’s law. Local thermodynamic equilibrium can only exist if the radiation processes can be neglected and the plasma is collision-determined. Therefore, a sufficiently high electron density is required.
Partial Local Thermodynamic Equilibrium (PLTE)
Electrons are more susceptible to the electric field than the heavy particles, due to their significantly lower mass. Electrons therefore gain more energy than the heavy particles per unit time. If the pressure is low or the electron density is small, the heavy particle temperature remains lower than the electron temperature. The plasma can no longer be described by a single temperature.
The energy difference between the ground state and the first excited state is normally large, whereas the energy difference between the excited states is small, especially in noble gases. If the electron density is sufficiently high, the excited states can be in equilibrium among each other (excluding the ground state). The velocity distribution within the different kind of species can still be Maxwellian (in spite of different temperatures). In such a case, the plasma is in partial local thermodynamic equilibrium (PLTE).
In non-equilibrium plasma, the heavy particle temperature is much lower than the electron temperature. The background gas in which the electrons and ions reside is more or less close to room temperature. There are considerable deviations from equilibrium. None of the aforementioned relations are still valid. In this case, a more elaborate approach is necessary.
Which Interface Do I Need for My Plasma Simulation?
The Plasma Module brings with it several different interfaces. Here is a screenshot of the expanded Plasma node, to give you an overview:
The Equilibrium Discharges interfaces are suitable for modeling thermal plasmas. These plasmas can be considered as a conductive fluid mixture and may therefore be modeled using the magnetohydrodynamics (MHD) equations. MHD combines the Navier-Stokes, heat, and Maxwell’s equations to describe the motion of the conducting fluid in an electromagnetic field. The chemical composition of the plasma is neglected.
The following figure shows the Model Builder of an inductively coupled plasma torch. You can find this model in the Model Library. The Magnetic Fields interface is used to solve Ampère’s law. The Heat Transfer interface solves an energy balance equation and the Laminar Flow interface the Navier-Stokes equation. In addition, there is a Multiphysics node for the coupling terms.
The Equilibrium Discharges interfaces assume that the plasma is fully ionized and that the plasma is under local thermodynamic equilibrium (LTE) conditions.
The Equilibrium DC Discharge interface is used to study equilibrium discharges that are sustained by a static or slow-varying electric field where induction currents and fluid flow effects are negligible.
The Combined Inductive/DC Discharge interface is used to study equilibrium discharges that are sustained by induction currents and/or static or slow-varying electric field, such as in arc welding simulations, for instance.
The Equilibrium Inductively Coupled Plasma interface is used to study equilibrium discharges that are sustained by induction currents, for example in inductively coupled plasma torches.
The other interfaces are suitable for modeling non-thermal or non-equilibrium plasmas. Here, a fluid model with drift diffusion approximation is used. A mass conservation equation for each species, an energy balance equation for the electrons, and Poisson equation for the electric field are solved. Here, the plasma chemistry is an essential part of the model.
The following screenshot shows the Model Builder of an inductively coupled non-equilibrium argon plasma. You can find this model in the Model Library, too. The plasma chemistry can be seen. The Plasma Model node contains the equations for the fluid model with drift diffusion approximation. Ampère’s law is needed for the electromagnetic field of the coil.
The Inductively Coupled Plasma interface is used to study discharges that are sustained by induction currents.
The Microwave Plasma interface is suitable for studying discharges that are sustained by electromagnetic waves (wave-heated discharges).
The Capacitively Coupled Plasma interface is used to study discharges that are sustained by a time-varying electrostatic field.
The DC Discharge interface is used to study discharges that are sustained by a static electric field.
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