# Dimensionless quantity

In dimensional analysis, a **dimensionless quantity** or **quantity of dimension one** is a quantity without an associated physical dimension. It is thus a "pure" number, and as such always has a dimension of 1.^{[1]} Dimensionless quantities are widely used in mathematics, physics, engineering, economics, and in everyday life (such as in counting). Numerous well-known quantities, such as π, [[Euler's number|Template:Mvar]], and [[Golden ratio|Template:Mvar]], are dimensionless. By contrast, non-dimensionless quantities are measured in units of length, area, time, etc.

Dimensionless quantities are often defined as products or ratios of quantities that are not dimensionless, but whose dimensions cancel out when multiplied or divided, respectively. This is the case, for instance, with the engineering strain, a measure of deformation. It is defined as change in length, divided by initial length, but since these quantities both have dimensions *L* (length), the result is a dimensionless quantity.

## Contents

## Properties

{{ safesubst:#invoke:Unsubst||$N=Unreferenced section |date=__DATE__ |$B= {{ safesubst:#invoke:Unsubst||$N=Unreferenced |date=__DATE__ |$B= {{#invoke:Message box|ambox}} }} }}

- Even though a dimensionless quantity has no physical dimension associated with it, it can still have dimensionless units. To show the quantity being measured (for example mass fraction or mole fraction), it is sometimes helpful to use the same units in both the numerator and denominator (kg/kg or mol/mol). The quantity may also be given as a ratio of two different units that have the same dimension (for instance, light years over meters). This may be the case when calculating slopes in graphs, or when making unit conversions. Such notation does not indicate the presence of physical dimensions, and is purely a notational convention. Other common dimensionless units are % (= 0.01), ‰ (= 0.001), ppm (= 10
^{−6}), ppb (= 10^{−9}), ppt (= 10^{−12}), angle units (degrees, radians, grad), dalton and mole. Units of number such as the dozen and the gross are also dimensionless.

- The ratio of two quantities with the same dimensions is dimensionless, and has the same value regardless of the units used to calculate them. For instance, if body
**A**exerts a force of magnitude*F*on body**B**, and**B**exerts a force of magnitude*f*on**A**, then the ratio*F*/*f*is always equal to 1, regardless of the actual units used to measure*F*and*f*. This is a fundamental property of dimensionless proportions and follows from the assumption that the laws of physics are independent of the system of units used in their expression. In this case, if the ratio*F*/*f*was not always equal to 1, but changed if one switched from SI to CGS, that would mean that Newton's Third Law's truth or falsity would depend on the system of units used, which would contradict this fundamental hypothesis. This assumption that the laws of physics are not contingent upon a specific unit system is the basis for the Buckingham π theorem. A statement of this theorem is that any physical law can be expressed as an identity involving only dimensionless combinations (ratios or products) of the variables linked by the law (e. g., pressure and volume are linked by Boyle's Law – they are inversely proportional). If the dimensionless combinations' values changed with the systems of units, then the equation would not be an identity, and Buckingham's theorem would not hold.

## Buckingham π theorem

Another consequence of the Buckingham π theorem of dimensional analysis is that the functional dependence between a certain number (say, *n*) of variables can be reduced by the number (say, *k*) of independent dimensions occurring in those variables to give a set of *p* = *n* − *k* independent, dimensionless quantities. For the purposes of the experimenter, different systems that share the same description by dimensionless quantity are equivalent.

### Example

The power consumption of a stirrer with a given shape 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:

- Length:
*L*(m) - Time:
*T*(s) - Mass:
*M*(kg)

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

- Reynolds number (a dimensionless number describing the fluid flow regime)
- Power number (describing the stirrer and also involves the density of the fluid)

## Standards efforts

The International Committee for Weights and Measures contemplated defining the unit of 1 as the 'uno', but the idea was dropped.^{[2]}^{[3]}^{[4]}

## Examples

- Proportional occurrences,
*e.g.*Sarah says, "Out of every 10 apples I gather, 1 is rotten." The rotten-to-gathered ratio is (1 apple) / (10 apples) = 0.1 = 10%, which is a dimensionless quantity. - Radian measure of angles – An angle is measured as the ratio of the length of a circle's arc subtended by an angle whose vertex is the centre of the circle to some other length. The ratio—i.e., length divided by length—is dimensionless. When using radians as the unit, the length that is compared is the length of the radius of the circle. When using degree as the units, the arc's length is compared to 1/360 of the circumference of the circle.
- In the case of the dimensionless quantity π, being the ratio of a circle's circumference to its diameter, the number would be constant regardless of what unit is used to measure a circle's circumference and diameter (e.g., centimetres, miles, light-years, etc.), as long as the same unit is used for both.
- Reynolds number is commonly used in fluid mechanics to characterize flow, incorporating both properties of the fluid and the flow. It is interpreted as the ratio of inertial forces to viscous forces and can indicate flow regime as well as correlate to frictional heating in application to flow in pipes
- Cost of transport is the efficiency in moving from one place to another

## Dimensionless physical constants

Certain fundamental physical constants, such as the speed of light in a vacuum, the universal gravitational constant, Planck's constant and Boltzmann's constant can be normalized to 1 if appropriate units for time, length, mass, charge, and temperature are chosen. The resulting system of units is known as the natural units. However, not all physical constants can be normalized in this fashion. For example, the values of the following constants are independent of the system of units and must be determined experimentally:

- α ≈ 1/137.036, the fine structure constant which is the coupling constant for the electromagnetic interaction;
- β (or μ) ≈ 1836, the proton-to-electron mass ratio. This ratio is the rest mass of the proton divided by that of the electron. An analogous ratio can be defined for any elementary particle;
- α
_{s}, the coupling constant for the strong force; - α
_{G}≈ 1.75×10^{−45}, the gravitational coupling constant.

## List of dimensionless quantities

All numbers are dimensionless quantities. Certain dimensionless quantities of some importance are given below:

## See also

- Similitude (model)
- Orders of magnitude (numbers)
- Dimensional analysis
- Dimensionless physical constant
- Normalization (statistics) and standardized moment, the analogous concepts in statistics
- Buckingham π theorem

## References

- ↑ Template:Cite web
- ↑ Template:Cite web
- ↑ Template:Cite web
- ↑ {{#invoke:Citation/CS1|citation |CitationClass=journal }}
- ↑
^{5.0}^{5.1}^{5.2}Template:Cite web - ↑ Bagnold number
- ↑ {{#invoke:Citation/CS1|citation |CitationClass=journal }}
- ↑ {{#invoke:Citation/CS1|citation |CitationClass=journal }}
- ↑ Template:Cite doi
- ↑ Bond number
- ↑ http://www.onepetro.org/mslib/servlet/onepetropreview?id=00020506
- ↑ Courant–Friedrich–Levy number
- ↑ {{#invoke:citation/CS1|citation |CitationClass=book }}
- ↑ Fanning friction factor
- ↑ Feigenbaum constants
- ↑ Fresnel number
- ↑ Gain Ratio - Sheldon Brown
- ↑ {{#invoke:citation/CS1|citation |CitationClass=book }}
- ↑ Template:Cite doi
- ↑ Lockhart–Martinelli parameter
- ↑ Manning coefficient PDF (109 KB)
- ↑ Template:Cite doi
- ↑ {{#invoke:citation/CS1|citation |CitationClass=book }}
- ↑ Richardson number
- ↑ Schmidt number
- ↑ Sommerfeld number
- ↑ Strouhal number, Engineering Toolbox
- ↑ Template:Cite doi
- ↑ Template:Cite doi
- ↑ Template:Cite doi
- ↑ Weissenberg number
- ↑ Womersley number

## External links

- John Baez, "How Many Fundamental Constants Are There?"
- Huba, J. D., 2007,
*NRL Plasma Formulary: Dimensionless Numbers of Fluid Mechanics.*Naval Research Laboratory. p. 23, 24, 25 - Sheppard, Mike, 2007, "Systematic Search for Expressions of Dimensionless Constants using the NIST database of Physical Constants."