A coordinate-free, or component-free, treatment of a scientific theory or mathematical topic develops its concepts on any form of manifold without reference to any particular coordinate system.
Coordinate-free treatments generally allow for simpler systems of equations and inherently constrain certain types of inconsistency, allowing greater mathematical elegance at the cost of some abstraction from the detailed formulae needed to evaluate these equations within a particular system of coordinates.
In addition to elegance, coordinate-free treatments are crucial in certain applications for proving that a given definition is well formulated. For example, for a vector space
V
v1,...,vn
V*
*, | |
v | |
1 |
...,
* | |
v | |
n |
\langle\sum\alphaivi,\sum\betai
* | |
v | |
i |
\rangle:=\sum\alphai\betai
V*
\langlev,\varphi\rangle=\varphi(v)
Nonetheless it may sometimes be too complicated to proceed from a coordinate-free treatment, or a coordinate-free treatment may guarantee uniqueness but not existence of the described object, or a coordinate-free treatment may simply not exist. As an example of the last situation, the mapping
vi\mapsto
* | |
v | |
i |
Coordinate-free treatments were the only available approach to geometry (and are now known as synthetic geometry) before the development of analytic geometry by Descartes. After several centuries of generally coordinate-based exposition, the modern tendency is generally to introduce students to coordinate-free treatments early on, and then to derive the coordinate-based treatments from the coordinate-free treatment, rather than vice versa.
Fields that are now often introduced with coordinate-free treatments include vector calculus, tensors, differential geometry, and computer graphics.[2]
In physics, the existence of coordinate-free treatments of physical theories is a corollary of the principle of general covariance.