Battery knowledge · Thermal management and heat transfer

Thermal gradient

A change of temperature with position — within a cell from core to surface, or across a pack from coolant inlet to outlet. Packs are commonly designed to keep cells within about 5 °C of each other, because warmer cells age faster and, in parallel, carry more current, so a gradient grows into an imbalance.

Also called
temperature gradient, temperature spread, temperature uniformity

Example

Thermal management and heat transfer: an example situation

Equal total heat in different layouts can produce different gradients. Average temperature can miss a hot spot.

Read Thermal gradient alongside Biot number in this context. The ratio of the resistance to heat conduction inside a body to the resistance to convection at its surface. Below about 0.1 the body heats almost uniformly and a lumped thermal model is adequate; large, strongly cooled cells with poor through-plane conductivity exceed it and need a model that resolves the internal gradient.

Use in Lemonergy

Lemonergy Studio blocks

Edge-cooled plate worked example

A plate with four thermal contacts and a defined coolant path. Explore which body connects to each contact and how pressure drives coolant through the plate.

Blocks to use

  1. Edge-cooled plate

    Four metal temperature nodes form a fixed 2 × 2 conduction mesh with four thermal contact ports. Coolant follows one two-segment edge path. Metal and coolant have finite heat storage. Pressure difference drives reversible mass and enthalpy transport; hydraulic dissipation enters the coolant energy balance. Each liquid boundary requires an explicit pressure/temperature reservoir.

    Inputs & settings
    • Use the parameter values in the block reference.
    • Bundled example verified on the production release of 28 October 2026.
  2. Coolant inlet boundary

    Sets 200 kPa and 300 K at plate a; supplies coolant for the positive pressure difference.

  3. Coolant outlet boundary

    Sets 100 kPa at plate b; receives coolant. Its 300 K supply temperature is used if flow reverses.

  4. Warm bodies 1–4

    Four passive bodies initially at 320 K, connected through h to plate h1–h4. Stored heat falls as the bodies cool; no continuous heater is attached.

This overview identifies the components to use. Follow the example in Lemonergy for their connections and settings.

  1. Review the block inputs, units and model limits.
  2. Open the Studio example and run its bundled model.
  3. Compare the output channels with the numerical checks; change one input and run again.

Example. The bundled model connects four thermal masses initially at 320 K to a 310 K plate, with 300 K coolant reservoirs at 200 kPa and 100 kPa. With channel resistance 10^6 Pa s/kg, the total flow is 0.1 kg/s and hydraulic dissipation is 10 W. After 0.2 s all four loads cool below their initial temperature. The loads cool from stored sensible heat; no continuous heater is attached.

Observe. Inspect the outputs and numerical checks on the block reference page.

Fixed 2 × 2 metal mesh and the stated coolant path. Constant properties and single-phase incompressible coolant. No arbitrary liquid junction solver, configurable grid, resolved channel geometry or phase change.

Open Studio example →

Lemonergy Studio blocks

Parallel-channel plate worked example

A plate with four thermal contacts and a defined coolant path. Explore which body connects to each contact and how pressure drives coolant through the plate.

Blocks to use

  1. Parallel-channel plate

    Four metal temperature nodes form a fixed 2 × 2 conduction mesh with four thermal contact ports. Coolant follows two parallel two-segment paths. Metal and coolant have finite heat storage. Pressure difference drives reversible mass and enthalpy transport; hydraulic dissipation enters the coolant energy balance. Each liquid boundary requires an explicit pressure/temperature reservoir.

    Inputs & settings
    • Use the parameter values in the block reference.
    • Bundled example verified on the production release of 28 October 2026.
  2. Coolant inlet boundary

    Sets 200 kPa and 300 K at plate a; supplies coolant for the positive pressure difference.

  3. Coolant outlet boundary

    Sets 100 kPa at plate b; receives coolant. Its 300 K supply temperature is used if flow reverses.

  4. Warm bodies 1–4

    Four passive bodies initially at 320 K, connected through h to plate h1–h4. Stored heat falls as the bodies cool; no continuous heater is attached.

This overview identifies the components to use. Follow the example in Lemonergy for their connections and settings.

  1. Review the block inputs, units and model limits.
  2. Open the Studio example and run its bundled model.
  3. Compare the output channels with the numerical checks; change one input and run again.

Example. The bundled model connects four thermal masses initially at 320 K to a 310 K plate, with 300 K coolant reservoirs at 200 kPa and 100 kPa. With channel resistance 10^6 Pa s/kg, the total flow is 0.2 kg/s and hydraulic dissipation is 20 W. After 0.2 s all four loads cool below their initial temperature. The loads cool from stored sensible heat; no continuous heater is attached.

Observe. Inspect the outputs and numerical checks on the block reference page.

Fixed 2 × 2 metal mesh and the stated coolant path. Constant properties and single-phase incompressible coolant. No arbitrary liquid junction solver, configurable grid, resolved channel geometry or phase change.

Open Studio example →

Lemonergy Studio blocks

U-channel plate worked example

A plate with four thermal contacts and a defined coolant path. Explore which body connects to each contact and how pressure drives coolant through the plate.

Blocks to use

  1. U-channel plate

    Four metal temperature nodes form a fixed 2 × 2 conduction mesh with four thermal contact ports. Coolant follows one four-segment U path. Metal and coolant have finite heat storage. Pressure difference drives reversible mass and enthalpy transport; hydraulic dissipation enters the coolant energy balance. Each liquid boundary requires an explicit pressure/temperature reservoir.

    Inputs & settings
    • Use the parameter values in the block reference.
    • Bundled example verified on the production release of 28 October 2026.
  2. Coolant inlet boundary

    Sets 200 kPa and 300 K at plate a; supplies coolant for the positive pressure difference.

  3. Coolant outlet boundary

    Sets 100 kPa at plate b; receives coolant. Its 300 K supply temperature is used if flow reverses.

  4. Warm bodies 1–4

    Four passive bodies initially at 320 K, connected through h to plate h1–h4. Stored heat falls as the bodies cool; no continuous heater is attached.

This overview identifies the components to use. Follow the example in Lemonergy for their connections and settings.

  1. Review the block inputs, units and model limits.
  2. Open the Studio example and run its bundled model.
  3. Compare the output channels with the numerical checks; change one input and run again.

Example. The bundled model connects four thermal masses initially at 320 K to a 310 K plate, with 300 K coolant reservoirs at 200 kPa and 100 kPa. With channel resistance 10^6 Pa s/kg, the total flow is 0.1 kg/s and hydraulic dissipation is 10 W. After 0.2 s all four loads cool below their initial temperature. The loads cool from stored sensible heat; no continuous heater is attached.

Observe. Inspect the outputs and numerical checks on the block reference page.

Fixed 2 × 2 metal mesh and the stated coolant path. Constant properties and single-phase incompressible coolant. No arbitrary liquid junction solver, configurable grid, resolved channel geometry or phase change.

Open Studio example →

References & further reading

Further reading on this topic

These sources provide broader context; they are not presented as citations for every statement in this entry.

  1. A General Energy Balance for Battery Systems

    Dawn Bernardi, Ellen Pawlikowski, John Newman · Journal of The Electrochemical Society · 1985

    Topic background · Battery energy balance and irreversible and reversible heat contributions. Reduced thermal models require explicit assumptions and current-sign conventions.

  2. University Physics Volume 2, §1.6: Mechanisms of Heat Transfer

    OpenStax, Rice University

    Topic background · Conduction, convection, radiation and thermal resistance.