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Dimensionless number

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In dimensional analysis, a dimensionless number (or more precisely, a number with the dimensions of 1) is a pure number without any physical units. Such a number is typically defined as a product or ratio of quantities which do have units, in such a way that all units cancel.

For example: "one out of every 10 apples I gather is rotten." -- the rotten-to-gathered ratio is (1 apple) / (10 apples) = 0.1, which is a dimensionless quantity. Another more typical example in physics and engineering is the measure of plane angles with the unit of "radian". An angle measured this way is the length of arc lying on a circle (with center being the vertex of the angle) swept out by the angle to the length of the radius of the circle. The units of the ratio is length divided by length which is dimensionless.

Dimensionless numbers are widely used in the fields of mathematics, physics, and engineering but also in everyday life. Whenever one measures anything, any physical quantity, they are measuring that physical quantity against a like dimensioned standard. Whenever one commonly measures a length with a ruler or tape measure, they are counting tick marks on the standard of length they are using, which is a dimensionless number. When they attach that dimensionless number (the number of tick marks) to the units that the standard represents, they conceptually are referring to a dimensionful quantity. But, ultimately, we always work with dimensionless numbers in measuring and manipulating even dimensionful quantities.

The CIPM Consultative Committee for Units toyed with the idea of defining the unit of 1 as the 'uno', but the idea was dropped. [link] [link] [link] [link]

Properties

Buckingham π-theorem

According to the Buckingham π-theorem of dimensional analysis, the functional dependence between a certain number (e.g., n) of variables can be reduced by the number (e.g., k) of independent dimensions occurring in those variables to give a set of p = nk independent, dimensionless numbers. For the purposes of the experimenter, different systems which share the same description by dimensionless numbers are equivalent.

Example

The power consumption of a stirrer with a particular geometry is a function of the density and the viscosity of the fluid to be stirred, the size of the stirrer given by its diameter, and the speed of the stirrer. Therefore, we have n = 5 variables representing our example.

Those n = 5 variables are built up from k = 3 dimensions which are:

According to the π-theorem, the n = 5 variables can be reduced by the k = 3 dimensions to form p = nk = 5 − 3 = 2 independent dimensionless numbers which are in case of the stirrer

List of dimensionless numbers

There are infinitely many dimensionless numbers. Some of those that are used most often have been given names, as in the following list of examples (alphabetical order):
| magnetohydrodynamics [link]
Name Field of application
Abbe number optics (dispersion in optical materials)
Albedo climatology, astronomy (reflectivity of surfaces or bodies)
Archimedes number motion of fluids due to density differences
Bagnold number flow of grain [link]
Biot number surface vs. volume conductivity of solids
Bodenstein number residence-time distribution
Bond number capillary action driven by buoyancy [link]
Brownell Katz number combination of capillary number and Bond number
Capillary number fluid flow influenced by surface tension
Coefficient of static friction
| friction of solid bodies at rest
Coefficient of kinetic friction
| friction of solid bodies in translational motion
Courant-Friedrich-Levy number  
| non-hydrostatic dynamics [link]
Damköhler numbers reaction time scales vs. transport phenomena
Darcy friction factor fluid flow
Deborah number rheology of viscoelastic fluids
Drag coefficient flow resistance
Eckert number convective heat transfer
Ekman number geophysics (frictional (viscous) forces)
Eötvös number determination of bubble/drop shape
Euler number
| hydrodynamics (pressure forces vs. inertia forces)
Fanning friction factor fluid flow in pipes [link]
Feigenbaum constants chaos theory (period doubling) [link]
Fourier number heat transfer
Fresnel number slit diffraction [link]
Froude number wave and surface behaviour
Gain electronics (signal output to signal input)
Galilei number gravity-driven viscous flow
Graetz number heat flow
Grashof number free convection
Hagen number forced convection
Knudsen number continuum approximation in fluids
Laplace number free convection within immiscible fluids
Lewis number ratio of mass diffusivity and thermal diffusivity
Lockhart-Martinelli parameter
| flow of wet gases [link]
Lift coefficient lift available from an airfoil at a given angle of attack
Mach number gas dynamics
Manning roughness coefficient
| open channel flow (flow driven by gravity)  [
PDF]
Nusselt number heat transfer with forced convection
Ohnesorge number atomization of liquids
Péclet number viscous vs. Brownian forces
Peel number adhesion of microstructures with substrate [link]
Pressure coefficient pressure experienced at a point on an airfoil
Poisson's ratio load in transverse and longitudinal direction
Power factor electronics (real power to apparent power)
Power number power consumption by agitators
Prandtl number forced and free convection
Rayleigh number buoyancy and viscous forces in free convection
Reynolds number flow behaviour
Richardson number effect of buoyancy on flow stability [link]
Rockwell scale mechanical hardness
Rossby number inertial forces in geophysics
Schmidt number fluid dynamics (mass transfer and diffusion) [link]
Sherwood number mass transfer with forced convection
Sommerfeld number boundary lubrication [link]
Stanton number heat transfer in forced convection
Stokes number particle dynamics
Strouhal number continuous and pulsating flow [link]
van 't Hoff factor quantitative analysis (Kf and Kb)
Weaver flame speed number laminar burning velocity relative to hydrogen gas [link]
Weber number multiphase flow with strongly curved surfaces
Weissenberg number viscoelastic flows [link]
Womersley number continuous and pulsating flows [link]

Dimensionless physical constants

Certain physical constants, such as the speed of light in a vacuum, are normalized to 1 if the units for time, length, mass, charge, and temperature are chosen appropriately. The resulting system of units is known as Planck units. However, a handful of dimensionless physical constants cannot be eliminated in any system of units; their values must be determined experimentally. The resulting fundamental physical constants include:

See also

External links

 


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