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.
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.
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, ; 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
where
is the Cauchy stress;
is the elasticity matrix;
is the total strain;
is the eigenstrain; and
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:
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, (degree of freedom 9).
Electric potential in the electrolyte, (degree of freedom 32).
Temperature, (degree of freedom 11).
Ion concentration in the electrolyte, (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.
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 (see Parameter Table Type Reference and Property Table Type Reference). 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.