The Battery Pack (bp) interface (

), found under the
Electrochemistry >
Battery Interfaces branch (

) offers a one-to-many approach for setting up multiple battery cell models, and for connecting them in a 3D geometry. The interface is typically used together with a heat transfer interface for modeling of thermal pack management and thermal runaway propagation problems.
The interface defines two types of domain nodes by default — Batteries and
Current Conductors, which are used to define the active battery cells and the electrical wiring (current collectors, feeders, and busbars, and so on) of the pack, respectively. The location of the interconnects between the batteries and the current conductors are defined by the
Negative Connectors and
Positive Connectors boundary nodes, which are always also present by default.
The battery cell models (Lumped cell model and
Two electrodes model) are defined similarly as for
The Lumped Battery Interface. All battery models defined by a Battery Pack interface share the same parameter settings. Modeling of packs with cells different individual parameter settings can be accomplished by either using the
Specify battery properties from materials checkbox available on the
Batteries node or by coupling multiple separate Battery Pack and/or Lumped Battery interfaces together.
The Label is the default physics interface name.
The Name is used primarily as a scope prefix for variables defined by the physics interface. Refer to such physics interface variables in expressions using the pattern
<name>.<variable_name>. In order to distinguish between variables belonging to different physics interfaces, the
name string must be unique. Only letters, numbers, and underscores (_) are permitted in the
Name field. The first character must be a letter.
The default Name (for the first physics interface in the model) is
bp.
In this section you can set the checkbox Exclude heat source variable from Jacobian. The checkbox is selected by default. Note that this checkbox is relevant only when coupling to heat transfer interfaces. Excluding the heat source from the Jacobian may decrease the computation time.