Automotive

Battery cells, chemistries and packs

What separates LFP from NMC and NCA, why cell format changes how a pack is cooled and repaired, how cells become modules and packs, and what thermal runaway actually is.

IntermediateAutomotive

Standards referencedUN 38.3ISO 6469-1IEC 62660-2SAE J2464

A traction battery is a few thousand small energy stores wired into one large one. Almost every difficulty in designing, cooling, managing and repairing a pack follows from that one sentence — because the pack can only ever be as good as its worst cell.

Three lithium ion cell formats laid out on a workshop bench side by side, a cylindrical cell standing on end, a flat rectangular prismatic cell in an aluminium can with two terminals on its top face, and a soft pouch cell with foil tabs at one edge, with a partly disassembled battery module behind them showing cells stacked against a cooling plate.
The three formats, and behind them the reason the choice matters — cells stacked against a cooling plate, where the distance from the middle of a cell to that plate sets what the pack can do.

The cell is where everything starts

A lithium-ion cell is a sandwich. Lithium ions move from one electrode to the other through an electrolyte during discharge, and back during charge. The electrons cannot take that route, so they go round the external circuit instead, which is the useful part.

Part What it does Typical material
Cathode Holds lithium when discharged; sets most of the cell’s character LFP, NMC, NCA
Anode Holds lithium when charged Graphite, sometimes with silicon
Electrolyte Carries ions between them Organic solvent with a lithium salt
Separator Keeps the electrodes apart while letting ions through Porous polymer film

Nearly everything people mean by “the chemistry” is the cathode. That is what the abbreviations refer to.

LFP, NMC and NCA

A diagram comparing three lithium ion cathode chemistries. Three columns compare LFP, NMC and NCA on nominal cell voltage, specific energy in watt hours per kilogram, cycle life, thermal runaway onset temperature and cost drivers. A bar chart shows specific energy rising from LFP through NMC to NCA while a second bar chart shows thermal runaway onset temperature falling in the same direction, making the trade explicit. A panel shows the nickel manganese cobalt ratio shifting from a third each towards eight parts nickel in ten, with an arrow showing energy density rising and thermal stability falling. A further panel describes solid state cells replacing the liquid electrolyte with a solid one and the lithium metal anode that this may permit.
Energy density and thermal stability run in opposite directions. Every chemistry choice is a position on that line rather than a solution to it.

LFP — lithium iron phosphate. No cobalt, no nickel. Lower energy density, so the pack is heavier and bulkier for a given range. In exchange it cycles several thousand times instead of one to two thousand, costs less, and begins to decompose around 270 °C rather than 210 °C. Its decomposition also releases much less oxygen, so a runaway is slower and less violent.

NMC — nickel manganese cobalt. The general-purpose choice. Higher energy density than LFP, and the ratio between the three metals is a design lever rather than a fixed recipe.

NCA — nickel cobalt aluminium. Highest energy density of the three, shortest cycle life, and the least thermal margin. Used where range per kilogram matters most.

Thermal runaway

Runaway is not simply overheating. It is a reaction that feeds itself.

Above an onset temperature the cell chemistry starts to break down, and that breakdown is exothermic. The heat raises the temperature further, which speeds up the breakdown, which releases more heat. Once the loop closes, removing whatever started it changes nothing — the cell is now its own heat source.

Three things can start it:

  • Mechanical — a crush or puncture creating an internal short.
  • Electrical — overcharge, or an external short.
  • Thermal — external heating, most often a neighbouring cell already in runaway.

Three formats, and why the shape matters

A diagram of battery pack construction. The upper half compares three cell formats, showing a cylindrical cell with heat travelling radially outward to a narrow line of contact with a cooling channel, a prismatic cell in a rigid aluminium can with a large flat face against a cold plate, and a pouch cell with foil tabs needing external compression. The lower half shows the hierarchy from cell to module to pack, with a module containing cells, a cooling plate, interconnects and sense wires, and a pack containing several modules, the service disconnect in the electrical middle, contactors, fuse and the battery management controller. A final panel contrasts module based construction with cell-to-pack construction, noting that deleting the module level recovers volume and mass but makes individual cell replacement far harder.
Heat has to get from the middle of a cell to a cooling surface. The format decides how far it has to travel and how wide the path is.

Cylindrical. A wound roll in a steel can. Cheap, mechanically self-supporting, extremely well understood. The difficulty is thermal — heat must travel radially outward to a curved surface that touches its cooling channel along a narrow line.

Prismatic. A rigid aluminium can with a large flat face. That face sits against a cold plate, giving a short, wide thermal path. The can also resists the swelling that cells undergo as they cycle.

Pouch. Electrodes in a foil bag with tabs at the edge. Lightest and most space-efficient, with good flat-face cooling, but it has no structure of its own. The module has to hold it in compression, and it must be given room to swell.

From cell to pack

The hierarchy is cell → module → pack.

A module holds cells in a frame with a cooling plate, the interconnects that join them, and the sense wires that let the management system see each cell group.

A pack holds several modules plus the contactors, the main fuse, the service disconnect, the management controller and the thermal circuit — inside a sealed enclosure that is usually also a structural member of the vehicle.

Packs are described in series and parallel counts. 96s2p means ninety-six cells in series, two such strings in parallel. Series adds voltage, parallel adds capacity:

Series Parallel
Voltage Adds Unchanged
Capacity Unchanged Adds
96s at 3.7 V About 355 V —
2p of 50 Ah cells — 100 Ah

Why the worst cell decides everything

A series string carries one current. Every cell in it sees the same amps.

So when the weakest cell reaches its upper voltage limit during charging, charging has to stop — even though every other cell still has room. On discharge the same cell hits its lower limit first and discharge has to stop, even though the rest have charge left.

The usable capacity of the pack is set by its worst cell, not its average. That single fact is the reason cell balancing exists, and it is taken up in battery management systems.

Cold is a charging problem, not just a range problem

Below about 5 °C the graphite anode cannot absorb lithium fast enough during a high charge current. The lithium deposits on the anode surface as metal instead — plating.

That metal does not come back. Capacity is permanently lost, and over repeated events the deposits grow structures that can eventually pierce the separator and cause an internal short.

Cell-to-pack, and what it costs

Module housings, fasteners and interconnects store no energy. Deleting the module level and bonding cells directly into the pack structure recovers a useful fraction of volume and mass.

The cost is repairability. Where a failed module could once be unbolted and replaced, a cell-to-pack assembly is closer to a single bonded unit. That shifts the economics of a pack fault from a module replacement to something much larger, and it is a live argument in the industry rather than a settled one.

Solid state

The liquid electrolyte is an organic solvent, and it is the main fuel in a runaway. Replacing it with a solid removes that fuel.

It may also permit a lithium metal anode in place of graphite, holding far more charge for its mass, because a solid electrolyte can resist the growth of the lithium structures that would otherwise short the cell.

The unsolved problems are mechanical and industrial rather than chemical — keeping solid surfaces in intimate contact as the cell swells and shrinks through every cycle, and manufacturing the thing by the million at a competitive price.

What to take away

  • The cathode is what people mean by the chemistry. LFP trades energy density for safety margin, cycle life and cost; NCA trades in the opposite direction; NMC sits between them.
  • Runaway feeds itself. Containment is about stopping one cell taking its neighbours, not about preventing the first failure.
  • Cell format decides the thermal path. Flat faces against a cold plate beat a line contact on a curved can.
  • Series adds voltage, parallel adds capacity, and the worst cell in a series string limits the whole pack.
  • Charging a cold pack hard plates lithium onto the anode permanently. That is why the vehicle warms the pack before accepting full current.
  • Cell-to-pack buys energy density and spends repairability.

Next, the electronics that watch every one of those cells — battery management systems.

Check your understanding

10 questions. Nothing is recorded — this is just for you.

1What is the main practical advantage of LFP over NMC?
2Why does the nickel content of an NMC cathode keep rising in newer designs?
3What is thermal runaway?
4Why does a prismatic or pouch cell cool differently from a cylindrical one?
5A pack is described as 96s2p. What does that mean?
6Why is the weakest cell in a series string the one that limits the whole pack?
7What does a cell vent do, and why is it there?
8Why does a pack need heating as well as cooling?
9What does cell-to-pack construction change?
10What problem is a solid-state cell trying to solve?

#vehicle systems#lithium ion#LFP#NMC#NCA#cell chemistry#thermal runaway#battery pack#energy density#solid state