Dimensionless quantity

[2][3] Typically expressed as ratios that align with another system, these quantities do not necessitate explicitly defined units.

[4] Radians serve as dimensionless units for angular measurements, derived from the universal ratio of 2π times the radius of a circle being equal to its circumference.

[5] Dimensionless quantities play a crucial role serving as parameters in differential equations in various technical disciplines.

In the 19th century, French mathematician Joseph Fourier and Scottish physicist James Clerk Maxwell led significant developments in the modern concepts of dimension and unit.

Later work by British physicists Osborne Reynolds and Lord Rayleigh contributed to the understanding of dimensionless numbers in physics.

Building on Rayleigh's method of dimensional analysis, Edgar Buckingham proved the π theorem (independently of French mathematician Joseph Bertrand's previous work) to formalize the nature of these quantities.

[10] Numerous dimensionless numbers, mostly ratios, were coined in the early 1900s, particularly in the areas of fluid mechanics and heat transfer.

Measuring logarithm of ratios as levels in the (derived) unit decibel (dB) finds widespread use nowadays.

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.