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Dimensionless Numbers

Physical and chemical dimensionless quantities - Reynolds number, Euler, Nusselt, and Prandtl number - and many more.

The table shows the definitions of a lot of dimensionless quantities used in chemistry, fluid flow and physics engineering. Below the table, the symbols used in the formulas are explained and given with SI units.

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Dimensionless Numbers Used in Chemistry, Fluid Flow and Physics Engineering
Name Symbol Formula Areas of application
Alfvén number Al Al = ν (ρ μ)½/ B Study of magnetic fields
Cowling number Co Co = B2/ (μ ρ ν2) Study of magnetic fields
Euler number Eu Eu = Δp / (ρ ν2) Characterization of energy losses in fluid flows
Fourier number Fo Fo = a t / l2 The ratio of diffusive or conductive heat transport rate to the heat storage rate
Fourier number for mass transfer Fo* Fo* = D t / l2 The ratio of diffusive mass transport rate to the mass storage rate
Froude number Fr Fr = ν / (l g)½ Determine the resistance of a partially submerged object moving through water
Grashof number Gr Gr = l3 g α ΔT ρ2/ η2 Study situations involving natural heat convection
Grashof number for mass transfer Gr* Gr* = l3 g (∂p/∂x)T,p (Δx p / η) Predictions of mass flow patterns
Hartmann number Ha Ha = B l (κ / η)1/2 Describes the ratio of electromagnetic force to the viscous force
Knudsen number Kn Kn = λ / l Determine whether statistical mechanics or the continuum mechanics formulation of fluid dynamics should be used to model a situation
Lewis number Le Le = a / D Characterize fluid flows where there is simultaneous heat and mass transfer
Mach number Ma Ma = ν / c Determine the approximation with which a flow can be treated as an incompressible flow
Nusselt number Nu Nu = h l / k The ratio of convective to conductive heat transfer across (normal to) a boundary surface, predicts flow patterns.
Nusselt number for mass transfer Nu* Nu* = kd l / D Predicts mass flow patterns
Peclet number Pe Pe = ν l / a For transport phenomena in a continuum, the ratio of advective to diffusive heat transport rates, to decide the simplicity/complexity of computational models
Peclet number for mass transfer Pe* Pe* = ν l / D The ratio of advective to diffusive mass transport rates
Prandtl number Pr Pr = η / (ρ a) Determine the thermal conductivity of gases at high temperatures
Rayleigh number Ra Ra = l3 g α ΔT ρ / (η a) Predict if heat transfer appear as conduction or convection
Reynolds number Re Re = p ν l / η Predictions of fluid flow patterns
Magnetic Reynolds number Rem Rem = ν μ κ l Estimates of the relative effects of advection or induction of a magnetic field
Schmidt number Sc Sc = η / (ρ D) Characterization of fluid flows in which there are simultaneous momentum and mass diffusion convection processes
Stanton number St St = h / (ρ ν cp) Characterization of heat transfer in forced convection flows, the ratio of heat transferred into a fluid to the thermal capacity of fluid
Stanton number for mass transfer St* St* = kd / ν To characterize mass transfer in forced convection flows
Strouhal number Sr Sr = l f / ν Describing oscillating flow mechanisms
Weber number We We = ρ ν2 l / γ Analysing fluid flows where there is an interface between two different fluids

where

ν = speed  (m/s)
η = viscosity  (kg/(m s))
ρ = density, mass density, (kg/m3)
m = mass (kg)
V = volume (m3)
l = length (m)
a = thermal diffusivity  (m2/s)
t = time (s)
μ = permeability (kg m/(s2A2))
B = magnetic flux density (kg/(s2A))
Δp = pressure difference  (kg/(m s2))
g = acceleration of free fall (m/s2)
α = cubic expansion coefficient (1/K)
ΔT = temperature difference
κ = electric conductivity (s3 A2/(kg m3))
λ = mean free path (m)
D = diffusion coefficient (m2/s)
c = speed of sound (m/s)
h = coefficient of heat transfer (kg/(s3 K))
k = thermal conductivity (kg m/(s3 K))
cp = specific heat apacity at constant pressure  (kg m2/(s2K))
f = frequency (1/s)
γ = surface tension (kg/s2)
x = mole fraction (1)
kd = mass transfer coefficient  (m/s)

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