{
  "node": {
    "id": "term:thermal-conductivity",
    "type": "Term",
    "label": "Thermal conductivity",
    "properties": {
      "id": "thermal-conductivity",
      "name": "Thermal conductivity",
      "abbr": "k",
      "aka": [
        "λ",
        "through-plane conductivity",
        "in-plane conductivity"
      ],
      "section": "topic-thermal",
      "definition": "How readily a material conducts heat: the heat flux per unit temperature gradient. Cells are strongly anisotropic — around 25–45 W/(m·K) in-plane, along the metal foils, but below 1 W/(m·K) through-plane, across separators and coatings — so the side a cell is cooled from decides how hot its core runs.",
      "formula": "q″ = −k·dT/dx",
      "unit": "W/(m·K)",
      "related": [
        "thermal-resistance",
        "thermal-diffusivity",
        "thermal-characterisation",
        "thermal-interface-material",
        "biot-number",
        "thermal-model"
      ],
      "example": {
        "title": "Calculate a slab heat flow",
        "text": "An illustrative 2 mm layer with k = 1 W/(m·K), area 0.01 m² and a 10 K temperature difference transfers 50 W in steady one-dimensional conduction. Contact resistances and edge losses are omitted."
      },
      "url": "https://lemonergy.com/learn/glossary/thermal-conductivity/",
      "mentions": [
        "heat-flux",
        "thermal-gradient"
      ]
    }
  },
  "edges": [
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      "target": "topic:topic-thermal",
      "type": "belongsTo",
      "properties": {
        "sourceFile": "terms.json"
      }
    },
    {
      "id": "edge:4545",
      "source": "term:thermal-conductivity",
      "target": "term:thermal-resistance",
      "type": "relatedTo",
      "properties": {
        "sourceFile": "terms.json",
        "meaning": "Related context; not a causal claim"
      }
    },
    {
      "id": "edge:4546",
      "source": "term:thermal-conductivity",
      "target": "term:thermal-diffusivity",
      "type": "relatedTo",
      "properties": {
        "sourceFile": "terms.json",
        "meaning": "Related context; not a causal claim"
      }
    },
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      "id": "edge:4547",
      "source": "term:thermal-conductivity",
      "target": "term:thermal-characterisation",
      "type": "relatedTo",
      "properties": {
        "sourceFile": "terms.json",
        "meaning": "Related context; not a causal claim"
      }
    },
    {
      "id": "edge:4548",
      "source": "term:thermal-conductivity",
      "target": "term:thermal-interface-material",
      "type": "relatedTo",
      "properties": {
        "sourceFile": "terms.json",
        "meaning": "Related context; not a causal claim"
      }
    },
    {
      "id": "edge:4549",
      "source": "term:thermal-conductivity",
      "target": "term:biot-number",
      "type": "relatedTo",
      "properties": {
        "sourceFile": "terms.json",
        "meaning": "Related context; not a causal claim"
      }
    },
    {
      "id": "edge:4550",
      "source": "term:thermal-conductivity",
      "target": "term:thermal-model",
      "type": "relatedTo",
      "properties": {
        "sourceFile": "terms.json",
        "meaning": "Related context; not a causal claim"
      }
    },
    {
      "id": "edge:mentions/thermal-conductivity/heat-flux",
      "source": "term:thermal-conductivity",
      "target": "term:heat-flux",
      "type": "mentions",
      "properties": {
        "sourceFile": "terms.json",
        "method": "build_glossary.mention_index + mentions",
        "field": "definition",
        "meaning": "Text mention; not a causal claim"
      }
    },
    {
      "id": "edge:mentions/thermal-conductivity/thermal-gradient",
      "source": "term:thermal-conductivity",
      "target": "term:thermal-gradient",
      "type": "mentions",
      "properties": {
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        "method": "build_glossary.mention_index + mentions",
        "field": "definition",
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      }
    },
    {
      "id": "edge:4553",
      "source": "term:thermal-conductivity",
      "target": "visual:fourier",
      "type": "illustratedBy",
      "properties": {
        "sourceFile": "visual-pages.json"
      }
    },
    {
      "id": "edge:4554",
      "source": "term:thermal-conductivity",
      "target": "reference:openstax-heat",
      "type": "cites",
      "properties": {
        "sourceFile": "wiki-references.json",
        "scope": "direct technical reference"
      }
    }
  ],
  "neighbors": [
    {
      "id": "topic:topic-thermal",
      "type": "Topic",
      "label": "Thermal management and heat transfer",
      "properties": {
        "id": "topic-thermal",
        "name": "Thermal management and heat transfer",
        "lede": "How heat is made, moved and removed in cells and packs, and the hardware that keeps a battery at the right temperature.",
        "context": "Select spatial detail for the question.",
        "example": "Equal total heat in different layouts can produce different gradients. Average temperature can miss a hot spot.",
        "lesson_url": "https://lemonergy.com/learn/fundamentals/battery-aging/",
        "lesson_label": "Open temperature and aging"
      }
    },
    {
      "id": "term:thermal-resistance",
      "type": "Term",
      "label": "Thermal resistance",
      "properties": {
        "id": "thermal-resistance",
        "name": "Thermal resistance",
        "section": "topic-thermal",
        "definition": "The temperature difference needed to drive one watt of heat along a path, in kelvin per watt. A 1 mm layer of gap filler at 3 W/(m·K) over 100 cm² has about 0.03 K/W, so 30 W through it costs 1 K. Resistances in series add like electrical ones, which is how cell-to-coolant paths are budgeted.",
        "formula": "R_th = ΔT / Q = L / (k·A)",
        "unit": "K/W",
        "related": [
          "thermal-conductivity",
          "thermal-interface-material",
          "cooling-plate",
          "heat-flux",
          "thermal-model"
        ],
        "example": {
          "title": "Translate heat into a temperature difference",
          "text": "A 2 K/W thermal path carrying a steady 5 W heat flow has a 10 K temperature difference across it. The temperature at the cold boundary is needed to obtain an absolute hot-side temperature."
        },
        "url": "https://lemonergy.com/learn/glossary/thermal-resistance/",
        "mentions": [
          "watt"
        ]
      }
    },
    {
      "id": "term:thermal-diffusivity",
      "type": "Term",
      "label": "Thermal diffusivity",
      "properties": {
        "id": "thermal-diffusivity",
        "name": "Thermal diffusivity",
        "abbr": "α",
        "section": "topic-thermal",
        "definition": "How quickly temperature evens out inside a material: thermal conductivity divided by density times specific heat. Heat spreads a distance L in roughly L²/α, so crossing a 10 mm cell at about 0.2 mm²/s through-plane takes several minutes, while aluminium, near 100 mm²/s, equalises almost at once.",
        "formula": "α = k / (ρ·cₚ)",
        "unit": "m²/s",
        "related": [
          "thermal-conductivity",
          "specific-heat-capacity",
          "thermal-gradient",
          "biot-number",
          "thermal-model"
        ],
        "example": {
          "title": "Compare heat-spreading rates",
          "text": "For an illustrative material with k = 1 W/(m·K), density 2000 kg/m³ and cₚ = 1000 J/(kg·K), α = 5×10⁻⁷ m²/s. A higher α means a temperature disturbance spreads faster for the same geometry."
        },
        "url": "https://lemonergy.com/learn/glossary/thermal-diffusivity/",
        "mentions": []
      }
    },
    {
      "id": "term:thermal-characterisation",
      "type": "Term",
      "label": "Thermal characterisation",
      "properties": {
        "id": "thermal-characterisation",
        "name": "Thermal characterisation",
        "aka": [
          "heat capacity test",
          "entropy test"
        ],
        "section": "topic-testing",
        "definition": "Measuring the thermal properties a model needs: specific heat capacity in a calorimeter, thermal conductivity through and along the layers, the entropy coefficient from OCV against temperature, and heat generation under load. Without them a thermal model is a guess.",
        "related": [
          "heat-generation",
          "entropy-coefficient",
          "thermal-model",
          "accelerating-rate-calorimetry"
        ],
        "url": "https://lemonergy.com/learn/glossary/thermal-characterisation/",
        "mentions": [
          "open-circuit-voltage",
          "thermal-conductivity",
          "specific-heat-capacity"
        ]
      }
    },
    {
      "id": "term:thermal-interface-material",
      "type": "Term",
      "label": "Thermal interface material",
      "properties": {
        "id": "thermal-interface-material",
        "name": "Thermal interface material",
        "abbr": "TIM",
        "aka": [
          "gap filler"
        ],
        "section": "topic-thermal",
        "definition": "A soft, thermally conductive paste or pad that fills the gap between cells and the cooling plate so heat does not have to cross air. It is dispensed by the kilogram in a pack and is a surprising share of its cost.",
        "related": [
          "cooling-plate",
          "thermal-management"
        ],
        "url": "https://lemonergy.com/learn/glossary/thermal-interface-material/",
        "mentions": []
      }
    },
    {
      "id": "term:biot-number",
      "type": "Term",
      "label": "Biot number",
      "properties": {
        "id": "biot-number",
        "name": "Biot number",
        "abbr": "Bi",
        "section": "topic-thermal",
        "definition": "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.",
        "formula": "Bi = h·L / k",
        "related": [
          "heat-transfer-coefficient",
          "thermal-conductivity",
          "thermal-model",
          "thermal-gradient"
        ],
        "example": {
          "title": "Check a lumped-temperature assumption",
          "text": "For h = 10 W/(m²·K), characteristic length L = 0.005 m and k = 1 W/(m·K), Bi = 0.05. Small Bi supports a lumped-temperature approximation; the characteristic length must match the geometry."
        },
        "url": "https://lemonergy.com/learn/glossary/biot-number/",
        "mentions": [
          "heat-transfer-modes"
        ]
      }
    },
    {
      "id": "term:thermal-model",
      "type": "Term",
      "label": "Thermal model",
      "properties": {
        "id": "thermal-model",
        "name": "Thermal model",
        "aka": [
          "lumped thermal model"
        ],
        "section": "topic-thermal",
        "definition": "A model of cell temperature: at its simplest one thermal mass with heat generation inside and convection outside, at its most detailed a 3D simulation of the pack. Temperature feeds back into every rate, so electrical and thermal models are usually solved together.",
        "related": [
          "heat-generation",
          "thermal-management",
          "arrhenius",
          "newman-model",
          "thermal-characterisation"
        ],
        "url": "https://lemonergy.com/learn/glossary/thermal-model/",
        "mentions": [
          "thermal-mass",
          "heat-transfer-modes"
        ]
      }
    },
    {
      "id": "term:heat-flux",
      "type": "Term",
      "label": "Heat flux",
      "properties": {
        "id": "heat-flux",
        "name": "Heat flux",
        "abbr": "q″",
        "section": "topic-thermal",
        "definition": "The rate of heat flow through a surface per unit area. Dividing a cell’s heat by its cooled area gives the flux the cooling must carry: a 21700 cell shedding 5 W through its roughly 46 cm² side sees about 1 kW/m². Cooling only one face concentrates the flux and steepens the gradient inside.",
        "formula": "q″ = Q / A",
        "unit": "W/m²",
        "related": [
          "heat-transfer-coefficient",
          "thermal-conductivity",
          "thermal-resistance",
          "thermal-gradient",
          "cooling-plate"
        ],
        "example": {
          "title": "Compare equal heat across different areas",
          "text": "A 10 W heat flow spread uniformly across 0.02 m² has an average flux of 500 W/m². Concentrating the same heat into half the area doubles the average flux."
        },
        "url": "https://lemonergy.com/learn/glossary/heat-flux/",
        "mentions": [
          "cylindrical-cell"
        ]
      }
    },
    {
      "id": "term:thermal-gradient",
      "type": "Term",
      "label": "Thermal gradient",
      "properties": {
        "id": "thermal-gradient",
        "name": "Thermal gradient",
        "aka": [
          "temperature gradient",
          "temperature spread",
          "temperature uniformity"
        ],
        "section": "topic-thermal",
        "definition": "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.",
        "related": [
          "hot-spot",
          "cell-to-cell-variation",
          "cooling-plate",
          "thermal-management",
          "biot-number"
        ],
        "url": "https://lemonergy.com/learn/glossary/thermal-gradient/",
        "mentions": []
      }
    },
    {
      "id": "visual:fourier",
      "type": "Visual",
      "label": "Heat flows down a temperature gradient",
      "properties": {
        "title": "Heat flows down a temperature gradient",
        "summary": "Thermal conductivity scales heat flux for the same spatial temperature gradient.",
        "readout": "A +100 K/m gradient gives -200 W/m². Through 0.01 m², that is -2 W in the positive coordinate direction.",
        "formula": "q″ = −k dT/dx; heat rate = q″ × area",
        "note": "One-dimensional, constant isotropic conductivity. Layered cells generally need direction-specific values and boundary conditions.",
        "software": {
          "status": "reference",
          "label": "Reference concept",
          "body": "Fourier’s law is a reference conduction relationship. A lumped temperature model does not resolve internal temperature gradients or directional conductivity.",
          "href": "../chapter-1/"
        },
        "html": "<figure class=\"visual-figure\"><figcaption>Fourier conduction</figcaption><svg class=\"visual-chart\" viewBox=\"0 0 360 330\" role=\"img\" aria-labelledby=\"static-fourier-0-title static-fourier-0-desc\"><title id=\"static-fourier-0-title\">Fourier conduction</title><desc id=\"static-fourier-0-desc\">Temperature gradient (K/m) versus Heat flux (W/m²). Signed heat flux. Interpretation follows the graphs.</desc><path d=\"M74,238h268\" stroke=\"currentColor\" opacity=\".13\"/><text x=\"64\" y=\"242\" text-anchor=\"end\" font-size=\"13\" fill=\"currentColor\">-2,000</text><text x=\"74\" y=\"265\" text-anchor=\"middle\" font-size=\"13\" fill=\"currentColor\">-1,000</text><path d=\"M74,188.5h268\" stroke=\"currentColor\" opacity=\".13\"/><text x=\"64\" y=\"192.5\" text-anchor=\"end\" font-size=\"13\" fill=\"currentColor\">-1,000</text><text x=\"141\" y=\"265\" text-anchor=\"middle\" font-size=\"13\" fill=\"currentColor\">-500</text><path d=\"M74,139h268\" stroke=\"currentColor\" opacity=\".13\"/><text x=\"64\" y=\"143\" text-anchor=\"end\" font-size=\"13\" fill=\"currentColor\">0</text><text x=\"208\" y=\"265\" text-anchor=\"middle\" font-size=\"13\" fill=\"currentColor\">0</text><path d=\"M74,89.5h268\" stroke=\"currentColor\" opacity=\".13\"/><text x=\"64\" y=\"93.5\" text-anchor=\"end\" font-size=\"13\" fill=\"currentColor\">1,000</text><text x=\"275\" y=\"265\" text-anchor=\"middle\" font-size=\"13\" fill=\"currentColor\">500</text><path d=\"M74,40h268\" stroke=\"currentColor\" opacity=\".13\"/><text x=\"64\" y=\"44\" text-anchor=\"end\" font-size=\"13\" fill=\"currentColor\">2,000</text><text x=\"342\" y=\"265\" text-anchor=\"middle\" font-size=\"13\" fill=\"currentColor\">1,000</text><path d=\"M74,40v198h268\" fill=\"none\" stroke=\"currentColor\" opacity=\".3\"/><polyline fill=\"none\" stroke=\"#2459a8\" stroke-width=\"2.8\" points=\"74.00,40.00 76.68,41.98 79.36,43.96 82.04,45.94 84.72,47.92 87.40,49.90 90.08,51.88 92.76,53.86 95.44,55.84 98.12,57.82 100.80,59.80 103.48,61.78 106.16,63.76 108.84,65.74 111.52,67.72 114.20,69.70 116.88,71.68 119.56,73.66 122.24,75.64 124.92,77.62 127.60,79.60 130.28,81.58 132.96,83.56 135.64,85.54 138.32,87.52 141.00,89.50 143.68,91.48 146.36,93.46 149.04,95.44 151.72,97.42 154.40,99.40 157.08,101.38 159.76,103.36 162.44,105.34 165.12,107.32 167.80,109.30 170.48,111.28 173.16,113.26 175.84,115.24 178.52,117.22 181.20,119.20 183.88,121.18 186.56,123.16 189.24,125.14 191.92,127.12 194.60,129.10 197.28,131.08 199.96,133.06 202.64,135.04 205.32,137.02 208.00,139.00 210.68,140.98 213.36,142.96 216.04,144.94 218.72,146.92 221.40,148.90 224.08,150.88 226.76,152.86 229.44,154.84 232.12,156.82 234.80,158.80 237.48,160.78 240.16,162.76 242.84,164.74 245.52,166.72 248.20,168.70 250.88,170.68 253.56,172.66 256.24,174.64 258.92,176.62 261.60,178.60 264.28,180.58 266.96,182.56 269.64,184.54 272.32,186.52 275.00,188.50 277.68,190.48 280.36,192.46 283.04,194.44 285.72,196.42 288.40,198.40 291.08,200.38 293.76,202.36 296.44,204.34 299.12,206.32 301.80,208.30 304.48,210.28 307.16,212.26 309.84,214.24 312.52,216.22 315.20,218.20 317.88,220.18 320.56,222.16 323.24,224.14 325.92,226.12 328.60,228.10 331.28,230.08 333.96,232.06 336.64,234.04 339.32,236.02 342.00,238.00\"/><text transform=\"translate(208 303)\" text-anchor=\"middle\" font-size=\"14\" fill=\"currentColor\"><tspan x=\"0\" dy=\"0\">Temperature gradient (K/m)</tspan></text><text transform=\"translate(20 139) rotate(-90)\" text-anchor=\"middle\" font-size=\"14\" fill=\"currentColor\"><tspan x=\"0\" dy=\"0\">Heat flux (W/m²)</tspan></text></svg><div class=\"visual-legend\"><span><i style=\"background:#2459a8\"></i>Signed heat flux</span></div></figure>"
      }
    },
    {
      "id": "reference:openstax-heat",
      "type": "Reference",
      "label": "University Physics Volume 2, §1.6: Mechanisms of Heat Transfer",
      "properties": {
        "title": "University Physics Volume 2, §1.6: Mechanisms of Heat Transfer",
        "publisher": "OpenStax, Rice University",
        "url": "https://openstax.org/books/university-physics-volume-2/pages/1-6-mechanisms-of-heat-transfer",
        "type": "Textbook section",
        "scope": "Conduction, convection, radiation and thermal resistance.",
        "accessed": "2026-10-27"
      }
    }
  ]
}
