Dimensionless groups reference

A durable lookup for the scaling groups that appear across fluid mechanics, heat transfer, and aerothermal experiments, with definitions, typical use, and pointers to the full derivations in the fluid mechanics curriculum.

Reference Similarity Fluid mechanics Heat transfer
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Start with your question

Why visitors arrive: You need a quick lookup for Reynolds, Mach, Nusselt, or similarity checklists.

Your question: Which dimensionless groups apply to my flow or heat-transfer problem?

You may also be asking

  • Where is the full dimensional analysis lesson?
  • How do I get fluid properties?
  • How are groups used in experiments?

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When to reach for a Pi group

Each group is a ratio of two effects. Fluid mechanics: Reynolds, Re, inertia over viscous forces; Mach, Ma, flow speed over sound speed; Froude, Fr, inertia over gravity; Weber, We, inertia over surface tension; Stokes, Stk, viscous effects over gravitational effects; Euler, Eu, pressure forces over inertia. Heat transfer: Nusselt, Nu, convective transport over conductive transport; Prandtl, Pr, momentum diffusivity over thermal diffusivity; Péclet, Pe, advection of energy over diffusion of energy; Biot, Bi, external convection over internal conduction; Stanton, St, heat transfer over enthalpy flux..FLUID MECHANICSReReynoldsinertiaviscous forcesMaMachflow speedsound speedFrFroudeinertiagravityWeWeberinertiasurface tensionStkStokesviscous effectsgravitational effectsEuEulerpressure forcesinertiaHEAT TRANSFERNuNusseltconvective transportconductive transportPrPrandtlmomentum diffusivitythermal diffusivityPePécletadvection of energydiffusion of energyBiBiotexternal convectioninternal conductionStStantonheat transferenthalpy flux
FLUID MECHANICSReReynoldsinertiaviscous forcesMaMachflow speedsound speedFrFroudeinertiagravityWeWeberinertiasurface tensionStkStokesviscous effectsgravitational effectsEuEulerpressure forcesinertiaHEAT TRANSFERNuNusseltconvective transportconductive transportPrPrandtlmomentum diffusivitythermal diffusivityPePécletadvection of energydiffusion of energyBiBiotexternal convectioninternal conductionStStantonheat transferenthalpy flux
FLUID MECHANICSReReynoldsinertiaviscous forcesMaMachflow speedsound speedFrFroudeinertiagravityWeWeberinertiasurface tensionStkStokesviscous effectsgravitational effectsEuEulerpressure forcesinertiaHEAT TRANSFERNuNusseltconvective transportconductive transportPrPrandtlmomentum diffusivitythermal diffusivityPePécletadvection of energydiffusion of energyBiBiotexternal convectioninternal conductionStStantonheat transferenthalpy flux
Each group compresses two competing effects into one ratio; the tables below give the definitions and where each is used.

Dimensionless numbers compress competing physical effects into ratios. They are how wind-tunnel tests claim relevance to engine conditions, how probe calibrations are transferred between facilities, and how low-order heat-exchanger models stay traceable.

Fluid mechanics

Group Definition Physical meaning Typical use
Reynolds Re \(\mathrm{Re} = \dfrac{\rho U L}{\mu}\) Inertia ÷ viscous forces Laminar/turbulent transition; dynamic similarity in pipe and external flows; probe calibration transfer
Mach Ma \(\mathrm{Ma} = \dfrac{U}{a}\) Flow speed ÷ sound speed Compressibility; choking; high-speed tunnel matching
Froude Fr \(\mathrm{Fr} = \dfrac{U}{\sqrt{g L}}\) Inertia ÷ gravity Free-surface flows; wave phenomena
Weber We \(\mathrm{We} = \dfrac{\rho U^2 L}{\sigma}\) Inertia ÷ surface tension Jet breakup; capillary-dominated flows
Stokes Stk \(\mathrm{Stk} = \dfrac{\mu U}{\rho g D^2} = \dfrac{\mathrm{Fr}^2}{\mathrm{Re}}\) (form varies) Viscous ÷ gravitational effects on particles Particle settling; related to Fr/Re ratios, see curriculum problem set
Euler Eu \(\mathrm{Eu} = \dfrac{\Delta p}{\rho U^2}\) Pressure forces ÷ inertia Cavitation; pressure-loss coefficients in internal flows

Heat transfer

How the groups connect. The Stokes number is the Froude number squared over the Reynolds number, a form that varies, used for particle settling. The Péclet number is the Reynolds number times the Prandtl number, used for thermal entrance lengths. The Nusselt and Biot numbers share the same form, h L over a conductivity: the fluid's for Nusselt, convective over conductive transport at a wall, and the solid's for Biot, external convection over internal conduction in a solid.GROUPS BUILT FROM OTHER GROUPSSAME FORM, DIFFERENT CONDUCTIVITYFrFroudeinertia ÷ gravityReReynoldsinertia ÷ viscous forcesPrPrandtlmomentum ÷ thermal diffusivityStk = Fr2 / Reform varies; particle settlingPe = Re · Prthermal entrance lengthsNuNusselth L / kfluidconvective ÷ conductivetransport at a wallBiBioth L / ksolidexternal convection ÷ internalconduction in a solidthe same h L, over the fluid's k or the solid's
GROUPS BUILT FROM OTHER GROUPSFrFroudeinertia ÷ gravityReReynoldsinertia ÷viscous forcesPrPrandtlmomentum ÷ thermaldiffusivityStk = Fr2 / Reform varies;particle settlingPe = Re · Prthermal entrance lengthsSAME FORM, DIFFERENT CONDUCTIVITYNuNusselth L / kfluidconvective ÷ conductivetransport at a wallBiBioth L / ksolidexternal convection ÷ internalconduction in a solidthe same h L, over the fluid's k or the solid's
GROUPS BUILT FROM OTHER GROUPSFrFroudeReReynoldsPrPrandtlStk = Fr2 / Reform varies;particle settlingPe = Re · Prthermal entrancelengthsSAME FORM, DIFFERENT CONDUCTIVITYNuh L / kfluidconvective ÷ conductive transport at a wallBih L / ksolidexternal convection ÷ internal conduction
Two groups on this page are built from others, and two that look alike differ only in whose conductivity sits underneath.
Group Definition Physical meaning Typical use
Nusselt Nu \(\mathrm{Nu} = \dfrac{h L}{k_{\mathrm{fluid}}}\) Convective ÷ conductive transport at a wall Convective HTC correlations; heat-exchanger segment sizing
Prandtl Pr \(\mathrm{Pr} = \dfrac{c_p \mu}{k} = \dfrac{\nu}{\alpha}\) Momentum diffusivity ÷ thermal diffusivity Coupling velocity and thermal boundary layers; property evaluation from air properties
Péclet Pe \(\mathrm{Pe} = \mathrm{Re}\,\mathrm{Pr}\) Advection ÷ diffusion of energy Thermal entrance lengths; conjugate problems
Biot Bi \(\mathrm{Bi} = \dfrac{h L}{k_{\mathrm{solid}}}\) External convection ÷ internal conduction in a solid Lumped-capacitance validity; transient thermography interpretation, see HPT thermography note
Stanton St \(\mathrm{St} = \dfrac{h}{\rho U c_p}\) Heat transfer ÷ enthalpy flux Boundary-layer heat transfer; Reynolds analogy contexts

Similarity checklist for experiments

Before claiming a model test represents a prototype, state which Pi groups are matched and which are relaxed, and document the consequence in the uncertainty budget.

Test type Usually matched Often relaxed Read next
Incompressible internal flow Re, geometry (scale) Absolute pressure if density weakly varying Viscous flow module
High-speed external aerodynamics Re, Ma, γ (gas) Wall temperature if adiabatic assumption holds CFD-experiment validation
Convective heat transfer Re, Pr, boundary-layer state Bi in the solid if lumped model justified Thermal & additive design
Pneumatic probe calibration Re at calibration point, Mach regime Facility-specific polynomial bias, see probe uncertainty note Instrumentation theme

About this work

Lucas Rey, aerothermal systems engineer and academic tutor.

  • University of Oxford: DPhil Researcher, Thermofluids Institute.
  • University of Cambridge: Alumnus.
  • Rolls-Royce: Sponsored researcher (High-pressure turbine programme).

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