Fully Coupled Thermal-Electrochemical-Structural Analysis

Fully coupled thermal-electrochemical-structural analysis is intended for the analysis of battery electrochemistry applications that require solving simultaneously for displacements, temperature, electric potentials in the solid electrodes, electric potential in the electrolyte, concentration of ions in the electrolyte, and concentration in the solid particles used in the electrodes.

A fully coupled thermal-electrochemical-structural analysis is a monolithic solve of the coupled thermal-displacement (see Fully Coupled Thermal-Stress Analysis in Abaqus/Standard) and coupled thermal-electrochemical (see Coupled Thermal-Electrochemical Analysis) analyses.

A fully coupled thermal-electrochemical-structural analysis:

  • is used when the mechanical, thermal, electrical, and ion concentration fields affect each other strongly; and

  • requires the use of coupled thermal-electrochemical-structural elements.

This page discusses:

Typical Application

The primary example of a battery electrochemistry application is the charging and discharging of lithium-ion battery cells. During the charging cycle, the lithium ions are extracted (deintercalated) from the active particles of the positive electrode (cathode). This process results in a reduction of the volume of the active particles. The ions move through the electrolyte by migration and diffusion from the positive electrode to the negative electrode (anode). At the anode, the ions intercalate into the active particles. This process results in an increase of the volume of the active particles and induces significant variation in tortuosities on both electrodes, thus strongly influencing the overall electrochemical behavior. Heat is generated during the flow of current in the solid and liquid phases, flow of current in the solid-liquid interface, and flow of ions in the electrolyte. During discharging, the cycle is reversed.

Coupled Thermal-Electrochemical-Structural Analysis

Rechargeable lithium-ion batteries are widely used in a variety of applications, including portable electronic devices and electric vehicles. The performance of a battery highly depends on the effects of repeated charging and discharging cycles, which can cause the degradation of the battery capacity over time. The porous electrode theory (Newman et al., 2004) is commonly accepted as the leading method for modeling the charge-discharge behavior of lithium-ion cells. The method is based on a homogenized Newman-type approach that does not consider the details of the pore geometry. The porous electrode theory is based on a concurrent solution of a highly coupled multiphysics-multiscale formulation. For further details on the thermal-electrochemical analysis, see Coupled Thermal-Electrochemical Analysis.

In some applications, a detailed understanding of the effects of the thermal-electrochemical fields on the mechanical state (deformations) of the lithium-ion cell is important and can have a strong influence on the overall performance of the cell. Battery performance characteristics (such as energy storage capacity and discharge voltages) can degrade with deformations caused by particle swelling and thermal strains. Large deformations can cause failure of the separator, resulting in thermal runaways in batteries. In such applications, the coupling between temperature and displacement fields may be due to temperature-dependent material properties, internal heat generation, or thermal expansion. The volume changes in the active electrode particles resulting from the intercalation/deintercalation of lithium ions are modeled as particle concentration–dependent eigenstrains at the macroscale level. These volume changes affect the displacement field in the cell and porosity and tortuosity evolutions. In addition, they generate a convective transport term in the electrolyte that influences the movement of lithium ions through the electrolyte.

Governing Equations

The governing equations for the thermal-electrochemical process are based on the porous electrode theory and are described in detail in Governing Equations. The governing equations for particle swelling are also described in Particle Swelling. The volumetric strain that is computed based on particle swelling affects the macroscale quantities, such as the solid volume fraction, ε s ; porosities; tortuosities; and eigenstrain.

Eigenstrain (also referred to as inherent strain, assumed strain, or "stress-free" strain) is an engineering concept used to account for all sources of inelastic deformation that lead to residual stresses and distortions in manufactured components. For example, thermal strains are an example of eigenstrains. Abaqus solves for mechanical equilibrium of all internal and external forces in the system.

In linear elastic deformation, the stress induced by an eigenstrain can be represented as

σ = D e l : ( ε ε * ) = D e l : ε e l ,

where

σ
is the Cauchy stress;
D e l
is the elasticity matrix;
ε
is the total strain;
ε *
is the eigenstrain; and
ε e l
is the elastic strain.

Using constitutive equations (such as that shown above), eigenstrains can be used to compute the stresses coming from mechanical, thermal, and microstructural sources.

It is possible to include the effects of particle swelling in both the coupled thermal-electrochemical and the coupled thermal-electrochemical-structural analyses. In a purely coupled thermal-electrochemical analysis, particle swelling results in convection of the electrolyte, which leads to changes in the porosity and the tortuosity of the electrodes. In a coupled thermal-electrochemical-structural analysis, particle swelling also results in mechanical deformations that are modeled as eigenstrains and results in stresses in the medium. Such mechanical deformations can also have an impact on the performance of a battery cell.

Fully Coupled Solution Scheme

A fully coupled solution scheme is needed when the stress analysis is dependent on the other fields involved in an electrochemical analysis, such as temperature, electric potentials in the solid and electrolyte, and ion concentration. In Abaqus/Standard, the temperature is integrated in time using a backward-difference scheme. The nonlinear coupled system is solved using Newton's method. The coupled thermal-electrochemical-structural analysis in Abaqus uses an exact implementation of Newton’s method, leading to an unsymmetric Jacobian matrix in the form:

[ K u u K u φ s K u θ K u φ e K u C e K φ s u K φ s φ s K φ s θ K φ s φ e K φ s C e K θ u K θ φ s K θ θ K θ φ e K θ C e K φ e u K φ e φ s K φ e θ K φ e φ e K φ e C e K C e u K C e φ s K C e θ K C e φ e K C e C e ] { Δ u Δ φ s Δ θ Δ φ e Δ C e } = { R u R φ s R θ R φ e R C e } .

Steady-State Analysis

Steady-state analysis provides the steady-state solution by neglecting the transient terms in the continuum scale equations. It can be used to achieve a balanced initial state or to assess conditions in the cell after a long storage period.

In the thermal equation, the internal energy term in the governing heat transfer equation is omitted. Similarly, the transient term is omitted in the diffusion equations for the lithium ion concentration in the electrolyte. Electrical transient effects are not included in the equations because they are very rapid compared to the characteristic times of thermal and diffusion effects. A steady-state analysis has no effect on the microscale solution; the transient terms are always considered in the solution of the lithium concentration in the solid particle.

Transient Analysis

In a transient analysis, the transient effects in the heat transfer and diffusion equations are included in the solution. Electrical transient effects are always omitted because they are very rapid compared to the characteristic times of thermal and mass diffusion effects.

Initial Conditions

By default, the initial values of electric potential in the solid, temperature, electric potential in the electrolyte, and ion concentration of all nodes are set to zero. You can specify nonzero initial values for the primary solution variables (see Initial Conditions).

Boundary Conditions

You can prescribe the following boundary conditions:

  • Displacement degrees of freedom (degrees of freedom 1, 2, and 3).
  • Electric potential in the solid, φ s = φ s ( x , t ) (degree of freedom 9).
  • Electric potential in the electrolyte, φ e = φ e ( x , t ) (degree of freedom 32).
  • Temperature, θ = θ ( x , t ) (degree of freedom 11).
  • Ion concentration in the electrolyte, C e = C e ( x , t ) (degree of freedom 33) at the nodes.

You can specify boundary conditions as functions of time by referring to amplitude curves.

A boundary without any prescribed boundary conditions corresponds to an insulated (zero flux) surface.

The typical boundary condition consists of only grounding (setting to zero) the solid electric potential at the anode. Thermal boundary conditions vary.

Loads

You can apply mechanical, thermal, electrical, and electrochemical loads in a coupled thermal-electrochemical-structural analysis.

You can prescribe the following types of mechanical loads (as described in Concentrated Loads and Distributed Loads):

  • Concentrated nodal forces on displacement degrees of freedom.
  • Distributed forces.

You can prescribe the following types of thermal loads (as described in Thermal Loads):

  • Concentrated heat flux.
  • Body flux and distributed surface flux.
  • Convective film and radiation conditions.

You can prescribe the following types of electrical loads on the solid (as described in Electromagnetic Loads):

  • Concentrated current.
  • Distributed surface current densities and body current densities.

You can prescribe the following types of electrical loads on the electrolyte (as described in Electromagnetic Loads):

  • Concentrated current.
  • Distributed surface current densities and body current densities.

You can prescribe the following types of ion concentration loads (as described in Thermal Loads):

  • Concentrated flux.
  • Distributed body flux.

The typical loads include specification of a solid electric flux (current) at the cathode. Thermal boundary conditions vary but typically include convective film on the exterior surfaces. Customarily, no loads are applied on the concentrations and electrolyte potential.

Predefined Fields

Predefined temperature fields are not allowed in coupled thermal-electrochemical-structural analyses. Instead, you can use boundary conditions to prescribe degree of freedom 11. You can specify other predefined field variables in a fully coupled thermal-electrochemical-structural analysis. These values affect only field variable–dependent material properties, if any.

Material Options

The material definition in a fully coupled thermal-electrochemical-structural analysis must include thermal, electrical, electrochemical, and mechanical properties.

The electrochemistry framework requires that the material definition contain the complete specification of properties required for the porous electrode theory, as described in Material Options. In addition, the material name must begin with "ABQ_EChemPET_" to enable the coupled micro-macro solution at the different electrodes. Special-purpose parameter and property tables of type names starting with “ABQ_EChemPET_” are required in these material definitions. For more details about the material definitions for the thermal-electrochemical behavior, see Material Options.

You can define anisotropic swelling of the particle to be used in eigenstrain computations.

Elements

A fully coupled thermal-electrochemical-structural analysis requires the use of elements that have displacement (degrees of freedom 1, 2, 3), electric potential in the solid (degree of freedom 9), temperature (degree of freedom 11), electric potential in the electrolyte (degree of freedom 32), and ion concentration in the electrolyte (degree of freedom 33) as nodal variables. The coupled thermal-electrochemical-structural elements are available in Abaqus/Standard only in three dimensions (see Coupled Thermal-Electrochemical-Structural Elements).

Output

In addition to the output quantities available for the coupled thermal-electric and the coupled thermal-electrochemical procedures, you can request the Abaqus/Standard output variables for mechanical degrees of freedom.

References

  1. Newman J. and KEThomas-Alyea, Electrochemical Systems,” Wiley-Interscience, Third Edition, 2004.