Jump to content
 







Main menu
   


Navigation  



Main page
Contents
Current events
Random article
About Wikipedia
Contact us
Donate
 




Contribute  



Help
Learn to edit
Community portal
Recent changes
Upload file
 








Search  

































Create account

Log in
 









Create account
 Log in
 




Pages for logged out editors learn more  



Contributions
Talk
 

















Contravariant







Add links
 









Article
Talk
 

















Read
Edit
View history
 








Tools
   


Actions  



Read
Edit
View history
 




General  



What links here
Related changes
Upload file
Special pages
Permanent link
Page information
Cite this page
Get shortened URL
Download QR code
 




Print/export  



Download as PDF
Printable version
 




Print/export  



















Appearance
   

 






From Wikipedia, the free encyclopedia
 


This is an old revision of this page, as edited by Mirwin (talk | contribs)at23:03, 22 October 2002 (stub). The present address (URL) is a permanent link to this revision, which may differ significantly from the current revision.
(diff)  Previous revision | Latest revision (diff) | Newer revision  (diff)

Contravariant is a mathematical term with a precise definition in tensor analysis. It specifies precisely the method used to derive the components by projecting the magnitude of the tensor quantity onto the coordinate system being used. Another method is used to derive covariant tensor components. When performing tensor transformations it is critical that the method used to map to the coordinate systems in use be tracked so that operations may be applied correctly for accurate meaningful results.

In 2 dimensions, for an oblique rectilinear coordinate system, contravariant coordinates of a directed line segment (in two dimensions this is termed a vector) are established by placing the origin of the coordinate axis at the tail of the vector. Parallel lines are placed through the head of the vector. The intersection of the line parallel to the x1 axis with the x2 axis provides the x2 coordinate. Similarly, the intersection of the line parallel to the x2 axis with the x1 axis provides the x1 coordinate.

insert jpeg,gif,or svg? sketch here

Thus, by definition; the oblique, rectilinear, contravariant coordinates of the point P above are summarized as: xi = (x1,x2)

Notice the superscript, this is a standard nomenclature convention for contravariant tensor components and should not be confused with the subscript which is used to designate covariant tensor components.

Using the definition above, the contravariant components of a position vector vi, where i=2, can be defined as the differences between coordinates on the same coordinate axis. Stated in another way, the vector components are the projection onto an axis from the direction parallel to the other axis.

so, since we have placed our origin at the tail of the vector,

v2=( (x1 - 0), (x2 - 0 ) )

v2=(x1, x2)

This result is generalized into n-dimensions. Contravariant is a fundamental concept or property within tensor theory and applies to tensors of all ranks over all manifolds. Since whether tensor components are contravariant or covariant, how they are mixed, and the order of operations all impact the results it is imperative to track for correct application of methods.


Retrieved from "https://en.wikipedia.org/w/index.php?title=Contravariant&oldid=377858"





This page was last edited on 22 October 2002, at 23:03 (UTC).

This version of the page has been revised. Besides normal editing, the reason for revision may have been that this version contains factual inaccuracies, vandalism, or material not compatible with the Creative Commons Attribution-ShareAlike License.



Privacy policy

About Wikipedia

Disclaimers

Contact Wikipedia

Code of Conduct

Developers

Statistics

Cookie statement

Mobile view



Wikimedia Foundation
Powered by MediaWiki