How to calculate the Biot number Bi transient heat conduction

Calculate Biot number Bi = h*Lc/k_solid ratio external convection to internal conduction resistance. Bi<0.1 lumped capacitance method valid (uniform T solid). Bi>0.1 Heisler charts series. Jean-Baptiste Biot 1804 Sorbonne Paris heat conduction.

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How to calculate the Biot number (Bi): fundamental dimensionless number transient heat conduction measuring ratio of external convection to internal conduction resistance. Formula: Bi = h*Lc/k_solid where h convection coefficient (W/m²·K), Lc characteristic length (V/A volume per surface area), k_solid SOLID thermal conductivity (W/m·K). Critical: distinguish k_solid vs k_fluid (Nu uses fluid k).

Lumped capacitance criterion: Bi<0.1 uniform T in solid, lumped method valid. T(t) = T_inf + (T_0 - T_inf) * exp(-t/tau), tau = rho*cp*V/(h*A) time constant.

Bi>0.1: significant T gradients, Heisler charts (1947) or one-term approximation required. History: Jean-Baptiste Biot (France 1774-1862) Paris École Polytechnique 1797 Sorbonne professor + Collège de France 1804 paper Bibliothèque Britannique 27:310 'Mémoire sur la propagation de la chaleur' first mathematical heat propagation solids. Joseph Fourier 1822 'Théorie analytique de la chaleur' heat equation. M.P. Heisler 1947 ASME 69:227 charts.

Essential tool for: electronics cooling CPU GPU heat sinks; food industry sterilization pasteurization; metallurgy quenching tempering; automotive brake rotor cooling; aerospace reentry heat shields; buildings thermal mass; nuclear fuel rods UO2 cladding.

USA heat transfer research: MIT Cambridge MA 1861 mechanical engineering Bird Stewart Lightfoot Transport Phenomena 1960; Stanford Mechanical Palo Alto CA 1925; Caltech Pasadena CA 1891; UC Berkeley CA 1868; Princeton NJ 1746; Cornell NY 1865; Carnegie Mellon Pittsburgh PA 1900; Georgia Tech Atlanta GA 1885; Purdue West Lafayette IN 1869; Notre Dame Indiana 1842 Frank Incropera 'Fundamentals of Heat and Mass Transfer' 1981.

USA companies cooling electronics: Intel Santa Clara CA 1968 130000 employees CPU manufacturer; Nvidia Santa Clara CA 1993 30000 GPU AI; AMD Santa Clara CA 1969 26000 CPU GPU; Apple Cupertino CA 1976 165000 M-series chips; Cooler Master Taiwan heat sinks; Noctua Austria CPU coolers.

USA food industry sterilization: Tetra Pak USA Vernon Hills IL aseptic packaging UHT; Dean Foods Dallas TX dairy pasteurization; Conagra Brands Chicago IL 1919 frozen foods; Kraft Heinz Pittsburgh Chicago 2015 39000 employees; General Mills Minneapolis MN 1866 35000 employees; PepsiCo Purchase NY 1965 309000 employees; Coca-Cola Atlanta GA 1892 79000 employees.

USA metallurgy heat treatment: Nucor Charlotte NC 1955 31000 employees largest US steel; US Steel Pittsburgh PA 1901 23000 employees; Cleveland-Cliffs Cleveland OH 1847 21000; Steel Dynamics Fort Wayne IN 1993; Inductotherm Group Rancocas NJ 1953 induction heating equipment; Ipsen Cherry Valley IL 1948 heat treatment furnaces.

USA aerospace reentry: NASA Washington DC 1958 17000 employees space shuttle thermal protection tiles; SpaceX Hawthorne CA 2002 Dragon Starship reentry; Boeing Chicago IL 1916 100000 employees CST-100 Starliner; Lockheed Martin Bethesda MD 1995 116000 Orion capsule; NASA Ames Research Center Moffett Field CA arc-jet testing; NASA Johnson Space Center Houston TX 1961. USA software heat transfer: ANSYS Canonsburg PA 1970 transient FEA; COMSOL Stockholm 1986; Abaqus Dassault 1978; FlowTherm Mentor Graphics; HTRI Navasota TX 1962; OpenFOAM ESI Group.

Biot formula

Definition: Bi = h*Lc/k_solid. Dimensionless. h convection coefficient (W/m²·K), Lc characteristic length (V/A), k_solid SOLID thermal conductivity (W/m·K). Critical distinction: k_solid for conduction inside solid; k_fluid for Nusselt convection.

Physical meaning: Bi ratio external convection resistance (1/h) to internal conduction resistance (Lc/k_solid). Bi<>1: fast convection, slow conduction, important spatial gradients.

Lumped capacitance method: Bi<0.1 valid. T(t) = T_inf + (T_0 - T_inf)*exp(-t/tau) where tau = rho*cp*V/(h*A) = rho*cp*Lc/h time constant. 5*tau ~ 99% completion.

Heisler charts (1947): Bi>0.1 use dimensionless time tau* = alpha*t/Lc² (Fourier number Fo) and dimensionless temperature theta = (T(t)-T_inf)/(T_0-T_inf). Three classic shapes: plane slab, infinite cylinder, sphere. One-term approximation: theta_0 = C*exp(-zeta_1²*Fo) for Fo>0.2.

Characteristic length: plane slab thickness 2L: Lc = L (half thickness); infinite cylinder radius R: Lc = R/2; sphere radius R: Lc = R/3; irregular geometry Lc = V/A. Distinguish Lc transient (V/A) from L convection correlations (geometric).

History and context

Jean-Baptiste Biot (France 1774-1862) Paris born, École Polytechnique 1794 mathematics 1797 graduate first class, Sorbonne professor mathematics 1800-1809 + Collège de France 1800-1862 long career 62 years, Académie des Sciences 1803 elected. Biot polymath: astronomy (Biot crater Moon), geomagnetism (Biot-Savart law magnetism Felix Savart 1820), polarization light 1812 (Biot-Fresnel law optics), spectroscopy, heat conduction 1804 paper Bibliothèque Britannique 27:310 first mathematical treatment heat propagation solids preceded Fourier 1822. Joseph Fourier (France 1768-1830) Auxerre Paris École Polytechnique 1794 mathematics + Egypt expedition 1798 Napoleon scientific commission 1801-1802 prefect Isère Grenoble, 1822 magnum opus 'Théorie analytique de la chaleur' Paris classic heat equation Fourier law q = -k*grad(T) + Fourier series + Fourier transform. M.P. Heisler 1947 paper Transactions ASME 69:227 charts. Modern textbook references: Frank Incropera (USA 1939-) Notre Dame 'Fundamentals of Heat and Mass Transfer' 1981 textbook 7 editions Wiley classic; Adrian Bejan (Romania-USA 1948-) Duke entropy generation minimization 1996 constructal theory; Yunus Cengel (Turkey-USA 1953-) UNR Heat Transfer textbook; Theodore Bergman + John Lavine 7th-8th edition Incropera. USA heat transfer pioneers: Theodore von Kármán (Hungary-USA 1881-1963) Caltech aerodynamics;

Bird Stewart Lightfoot (USA 1924-2020 + collaborators) University Wisconsin Madison Transport Phenomena 1960 Wiley classic chemical engineering 1500 pages; Hermann Schlichting + Klaus Gersten Boundary Layer Theory 8th edition 2017. USA universities heat transfer: MIT Cambridge MA 1861; Stanford Palo Alto CA 1925; Caltech Pasadena CA 1891; UC Berkeley CA 1868; Princeton NJ 1746; Cornell NY 1865; Carnegie Mellon Pittsburgh PA 1900; Georgia Tech Atlanta GA 1885; Purdue West Lafayette IN 1869; Notre Dame Indiana 1842 Frank Incropera; Illinois Urbana-Champaign 1867; Texas A&M College Station 1876; Michigan Ann Arbor 1817; Northwestern Evanston IL 1851; Penn State University Park 1855; Virginia Tech Blacksburg 1872. USA national labs: Lawrence Berkeley LBNL CA 1931; Argonne ANL IL 1946; Oak Ridge ORNL TN 1943 reactor heat transfer; Sandia National Labs Albuquerque NM Livermore CA 1949 thermal physics combustion; Idaho National Lab INL ID 1949 nuclear reactor research. USA companies cooling electronics: Intel Santa Clara CA 1968 founded 130000 employees CPU manufacturer thermal management; Nvidia Santa Clara CA 1993 founded 30000 GPU AI; AMD Santa Clara CA 1969 26000 CPU GPU; Apple Cupertino CA 1976 165000 M-series chips thermal design; Cooler Master Taiwan heat sinks fans; Noctua Austria CPU coolers premium; Arctic Switzerland; Corsair Milpitas CA 1994. USA food industry sterilization: Tetra Pak USA Vernon Hills IL Lund Sweden parent aseptic packaging UHT;

Dean Foods Dallas TX dairy pasteurization; Conagra Brands Chicago IL 1919 frozen foods Birds Eye Healthy Choice Marie Callender's; Kraft Heinz Pittsburgh Chicago 2015 fusion 39000 employees; General Mills Minneapolis MN 1866 35000 employees Cheerios Pillsbury Häagen-Dazs; PepsiCo Purchase NY 1965 309000 employees Pepsi Frito-Lay Quaker; Coca-Cola Atlanta GA 1892 79000 employees soft drinks; Mars Inc McLean VA 1911 candy chocolate; Hershey Hershey PA 1894 chocolate. USA metallurgy heat treatment: Nucor Charlotte NC 1955 31000 employees largest US steel electric arc furnace; US Steel Pittsburgh PA 1901 founded JP Morgan Andrew Carnegie 23000 employees integrated; Cleveland-Cliffs Cleveland OH 1847 21000 employees acquired AK Steel 2020; Steel Dynamics Fort Wayne IN 1993 11000 employees mini-mills; Inductotherm Group Rancocas NJ 1953 induction heating equipment; Ipsen Cherry Valley IL 1948 heat treatment furnaces vacuum atmosphere; ASM International Materials Park OH 1913 metallurgy society. USA aerospace reentry thermal protection: NASA Washington DC 1958 17000 employees Space Shuttle thermal tiles 1981-2011 24000 silica HRSI HRSI tiles; SpaceX Hawthorne CA 2002 Dragon capsule PICA-X heat shield ablative + Starship stainless steel + tiles; Boeing Chicago IL 1916 CST-100 Starliner; Lockheed Martin Bethesda MD 1995 Orion capsule Avcoat heat shield; NASA Ames Research Center Moffett Field CA arc-jet testing high-enthalpy; NASA Johnson Space Center Houston TX 1961;

NASA Kennedy Space Center FL 1962; ATK Northrop Grumman Innovation Systems propulsion. USA software heat transfer: ANSYS Canonsburg PA 1970 founded John Swanson finite element + Fluent + Mechanical 5500 employees market leader; Abaqus Dassault Systèmes 1978; COMSOL Stockholm 1986 multiphysics; FlowTherm Mentor Graphics Wilsonville OR 1981 (acquired Siemens 2017); HTRI Heat Transfer Research Inc Navasota TX 1962 industry standard heat exchanger; OpenFOAM ESI Group open source CFD foundation; LS-DYNA Livermore CA crash thermal; Solidworks Simulation Dassault Waltham MA.

Biot values table

  • Bi = h*Lc/k_solid: definition
  • Bi < 0.01: very low, lumped highly accurate
  • Bi < 0.1: low, lumped capacitance valid <5%
  • Bi 0.1-1: moderate, Heisler charts
  • Bi 1-10: high, conduction-dominated
  • Bi > 100: extreme, T_surface = T_fluid
  • Lumped tau: rho*cp*V/(h*A)
  • Slab Lc: half thickness L
  • Cylinder Lc: R/2
  • Sphere Lc: R/3
  • Steel k: 50 W/m·K
  • Copper k: 400 W/m·K
  • Aluminum k: 240 W/m·K
  • Brick k: 0.7 W/m·K
  • Food k: 0.4-0.6 W/m·K
  • h air free: 5-25 W/m²K
  • h air forced: 25-250 W/m²K
  • h water free: 100-1000 W/m²K
  • h water forced: 500-15000 W/m²K
  • h boiling: 2500-50000 W/m²K
  • h condensation: 5000-100000 W/m²K
  • Biot 1804 paper: Bibliothèque Britannique 27:310
  • Fourier 1822: Théorie analytique chaleur
  • Heisler 1947: ASME 69:227 charts
  • Incropera 1981 textbook: Notre Dame 7 editions
  • USA Intel Santa Clara 1968: 130000 CPU
  • USA Nvidia Santa Clara 1993: 30000 GPU
  • USA Tetra Pak Vernon Hills: aseptic UHT
  • USA Conagra Chicago 1919: frozen foods
  • USA Kraft Heinz 2015: 39000 employees
  • USA Nucor Charlotte 1955: 31000 steel largest
  • USA Inductotherm NJ 1953: induction heating
  • USA Ipsen IL 1948: heat treatment furnaces
  • USA NASA 1958: 17000 thermal protection
  • USA SpaceX 2002: PICA-X heat shield
  • USA ANSYS 1970: FEA market leader

Numerical examples

Example 1 - Steel sphere cooling air. Steel sphere R=0.05 m air-cooled. h=25 W/m²K natural convection, k_steel=50 W/m·K. Lc = R/3 = 0.017 m. Bi = 25*0.017/50 = 0.0083 < 0.01 very low. Lumped highly accurate <2%. USA: heat treatment Inductotherm NJ 1953; Ipsen IL 1948 furnaces.

Example 2 - Brick oven water. Brick Lc=0.1 m water boiling forced convection h=500 W/m²K, k_brick=0.7 W/m·K. Bi = 500*0.1/0.7 = 71.4 high. Large gradients, T_surface ~ 100°C, interior cools slowly. Heisler charts required. USA: brick industry; ASTM C90 Standard Specification CMU concrete masonry units.

Example 3 - Copper component oil. Copper component Lc=0.01 m oil-cooled h=200 W/m²K, k_copper=400 W/m·K. Bi = 200*0.01/400 = 0.005 very low. Lumped <2%. USA: cooling electronics Intel Santa Clara CA 1968 130000 + Nvidia 1993 30000 GPU + AMD 1969 26000.

Example 4 - Food sterilization steam. Cylindrical can Lc=0.02 m saturated steam h=5000 W/m²K, k_food=0.5 W/m·K. Bi = 5000*0.02/0.5 = 200 extreme high. T_surface = 121°C immediately; interior cooks slowly Fourier series. USA: food industry Conagra Chicago 1919; Kraft Heinz 2015 39000; Tetra Pak Vernon Hills.

Example 5 - Aluminum plate water time constant. Aluminum plate Lc=0.005 m water cooled h=100, k=200, rho*cp=3.5e6 J/m³K. Bi = 100*0.005/200 = 0.0025 very low. tau = 3.5e6*0.005/100 = 175 s = 2.9 min. 5*tau = 14.6 min 99% completion. USA: heat sinks Intel CPU Apple M-series chips; Cooler Master Noctua Corsair.

Limitations

  1. Lumped Bi<0.1 only: applicable Bi<0.1 (error <5%); above requires Heisler charts or Fourier series.
  2. Simple geometry: Heisler charts only plane slab, infinite cylinder, sphere. Irregular shapes need FEA.
  3. Single-phase solid: homogeneous isotropic. Composites multi-phase separate treatment.
  4. Constant h: assumes h convection coefficient time/space constant. T variations require iterative.
  5. No phase change: melting solidification require Stefan number + latent heat.
  6. Anisotropy: anisotropic solids (wood, composites) require tensor k.
  7. Variable natural convection: complex geometries h varies with position.
  8. Radiation effects: T>500°C radiation contribution h_rad combined with h_conv.
  9. Steady state vs transient: Bi for transient only. Steady state uses thermal resistance R = L/(k*A).
  10. Internal heat generation: solid generating heat (Joule, nuclear) requires Q_gen + Bi separate.

Common errors

k_solid vs k_fluid: Bi uses solid k (steel=50, copper=400, aluminum=240, brick=0.7); Nu uses fluid k. Common error confuses.

Characteristic length: slab Lc = half thickness L; cylinder Lc = R/2; sphere Lc = R/3; irregular Lc = V/A. Error using full R instead of R/2 or R/3.

Lumped Bi<0.1: lumped criterion Bi<0.1 error <5%; above Heisler charts. Error applying lumped Bi=0.5 gives 30-50% errors.

Time constant tau: tau = rho*cp*Lc/h. Time to reach 63.2% final. 5*tau ~ 99%. Error confusing tau with total time.

T_inf vs T_initial: T(t) = T_inf + (T_0 - T_inf)*exp(-t/tau). T_inf ambient fluid (asymptotic); T_0 initial solid. Error inverts the two.

Practical applications

  1. Electronics cooling: CPU GPU heat sinks Bi<0.1 lumped. USA Intel Santa Clara 1968 130000; Nvidia Santa Clara 1993 30000; AMD 1969; Apple Cupertino 1976 M-series.
  2. Food industry sterilization: USA Conagra Chicago 1919; Kraft Heinz 2015 39000; General Mills 1866 35000; Tetra Pak Vernon Hills aseptic UHT.
  3. Metallurgy quenching: USA Nucor Charlotte 1955 31000 largest; US Steel Pittsburgh 1901; Cleveland-Cliffs 1847; Inductotherm NJ 1953 induction; Ipsen IL 1948 furnaces.
  4. Automotive brake: USA Ford Dearborn MI 1903; GM Detroit MI 1908; Tesla Austin TX 2003 EV brake disc cooling.
  5. Aerospace reentry heat shield: NASA Washington DC 1958 17000 Space Shuttle tiles; SpaceX Hawthorne CA 2002 PICA-X Starship; Boeing Chicago 1916 Starliner; Lockheed Martin Bethesda MD Orion.
  6. Buildings thermal mass: USA passive cooling; ASHRAE Atlanta GA 1894 building science; LEED certification.
  7. Body cooling hypothermia: Newton's law of cooling lumped capacitance human body; CDC Atlanta GA 1946 health.
  8. Glass tempering: tempered glass quenching Bi>0.1; USA Owens-Illinois Perrysburg OH 1903.
  9. Nuclear fuel rod: UO2 ceramic + cladding. USA Westinghouse Pittsburgh PA 1886; Idaho National Lab 1949; Sandia Albuquerque NM 1949.
  10. Dental implants: titanium heat treatment. USA Zimmer Biomet Warsaw IN 1927.

Updated July 2026

Frequently Asked Questions

What is the Biot number?

Dimensionless number transient heat conduction ratio external convection to internal conduction resistance. Formula: Bi = h*Lc/k_solid where h convection coefficient (W/m²K), Lc characteristic length (V/A), k_solid SOLID thermal conductivity. Critical: k_solid not k_fluid (Nu). Bi0.1 Heisler charts series. Jean-Baptiste Biot 1804 Sorbonne paper Bibliothèque Britannique heat conduction. USA: MIT Cambridge MA 1861; Stanford 1925; Caltech 1891; UC Berkeley 1868; Notre Dame 1842 Incropera textbook 1981 7 editions.

How to calculate Biot?

Bi = h*Lc/k_solid. Procedure: (1) determine h convection coefficient (Nusselt correlation or experimental); (2) Lc characteristic length (slab L, cylinder R/2, sphere R/3, irregular V/A); (3) k_solid solid thermal conductivity (steel=50, copper=400, aluminum=240, brick=0.7); (4) divide. Example: steel sphere R=0.05 m, h=25, k=50: Lc=R/3=0.017, Bi=0.0083 lumped accurate. USA: ANSYS Canonsburg PA 1970 FEA; COMSOL multiphysics; HTRI Navasota TX 1962 heat exchanger software.

Who defined the Biot number?

Jean-Baptiste Biot (France 1774-1862) Paris École Polytechnique 1797 Sorbonne professor + Collège de France 1804 paper Bibliothèque Britannique 27:310 'Mémoire sur la propagation de la chaleur' first mathematical treatment heat propagation in solids preceded Fourier 1822. Joseph Fourier (France 1768-1830) 1822 'Théorie analytique de la chaleur' heat equation. M.P. Heisler 1947 ASME charts. Biot polymath: Biot-Savart magnetism 1820 + Biot-Fresnel optics 1812 + Biot crater Moon. USA: Frank Incropera Notre Dame 1981 textbook; Adrian Bejan Duke; MIT 1861.

What is lumped capacitance method?

Simplified concentrated method Bi<0.1: solid temperature spatially uniform, varies only in time. Solution T(t) = T_inf + (T_0 - T_inf)*exp(-t/tau) where tau = rho*cp*V/(h*A) = rho*cp*Lc/h time constant. Time to reach 63.2% (1-1/e). 5*tau ~ 99%. Error <5% Bi<0.1, <2% Bi0.1 invalid: significant spatial gradients. USA: cooling electronics Intel Santa Clara CA 1968 130000 employees CPU; Nvidia Santa Clara 1993 30000 GPU; AMD 1969 26000.

Difference Bi and Nu?

Biot Bi = h*Lc/k_solid uses SOLID conductivity. Nusselt Nu = h*L/k_fluid uses FLUID conductivity. Bi measures internal solid conduction resistance vs external convection; Nu measures convection intensity vs fluid conduction. Bi transient heat transfer; Nu convective steady-state. Example water on steel h=500: Bi=500*0.05/50=0.5 (k_steel); Nu=500*0.05/0.6=42 (k_water). USA: MIT Cambridge MA 1861; Stanford Palo Alto CA 1925; Caltech Pasadena CA 1891; Incropera textbook Notre Dame 1981.

What are Biot applications?

Applications: electronics cooling CPU GPU heat sinks lumped USA Intel 1968 130000 + Nvidia 1993 + AMD; food sterilization Conagra Chicago 1919 + Kraft Heinz 2015 39000 + General Mills 1866 35000; metallurgy quenching Nucor Charlotte 1955 31000 + US Steel Pittsburgh 1901 + Inductotherm NJ 1953 + Ipsen IL 1948; aerospace reentry NASA Space Shuttle tiles + SpaceX PICA-X Starship + Boeing Starliner + Lockheed Orion; brake disc Ford GM Tesla; nuclear fuel Westinghouse Pittsburgh 1886.

When is lumped capacitance invalid?

Lumped capacitance valid only Bi < 0.1 error 0.1 invalid because significant temperature gradients inside solid. Alternative solutions: (1) Heisler charts (1947) dimensionless slab cylinder sphere; (2) One-term approximation theta_0 = C*exp(-zeta_1²*Fo) for Fo>0.2; (3) Full Fourier series; (4) FEA finite element ANSYS Abaqus complex geometries. Typical Bi>0.1: high-convection foods + low k; large bricks; brick kiln. USA: ANSYS Canonsburg PA 1970 FEA; COMSOL Stockholm 1986 multiphysics; Abaqus Dassault Systèmes 1978.

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