Why Is This Basis Non-Coordinate?

Click For Summary

Homework Help Overview

The discussion revolves around the concept of a non-coordinate basis in the context of vector fields, specifically related to an exercise from Schutz's "Geometric Methods of Mathematical Physics." The original poster is attempting to demonstrate that a given basis is non-coordinate by showing that the commutator is non-zero.

Discussion Character

  • Exploratory, Conceptual clarification, Assumption checking

Approaches and Questions Raised

  • Participants discuss the definitions and implications of a non-coordinate basis, with some exploring the commutation of vector fields. The original poster attempts to apply a formula to derive parametric equations but expresses confusion over the results. Others question the clarity of variable definitions and the relationship between the parameters.

Discussion Status

The discussion is ongoing, with participants sharing their interpretations and confusion regarding the problem. Some provide insights into the geometric interpretation of the commutator, while others seek clarification on definitions and the original poster's approach. There is no explicit consensus, but various lines of reasoning are being explored.

Contextual Notes

Participants note the complexity of the problem and the potential for confusion arising from the definitions and relationships between the variables involved. The original poster's reference to specific equations and parameters suggests a need for careful consideration of the assumptions being made.

desic
Messages
4
Reaction score
0
I'm self-studying Schutz Geometric methods of mathematical physics, having problems with ex. 2.1. page 44.

r=cos(theta)x+sin(theta)y
theta=-sin(theta)x+cos(theta)y

show this is non-coordinate basis, i.e. show commutator non-zero.

I try to apply his formula 2.7, assuming

V1=cos(theta), V2=sin(theta)
W1=-sin(theta), W2=cos(theta)
x(r)=r cos(theta)
y(r)=r sin(theta)
x(theta)=cos(theta)
y(theta)=sin(theta)

These parametrics I got from integrating back from the components of r and theta

I believe the component of x should be (sin(theta))/r, however I get (sin(theta) - r sin(theta))/r.

would appreciate any help
 
Physics news on Phys.org
I'm sorry I can't help you but I'm intrigued by this notion of "non-coordinate basis". Does the author give a definition? (And if so can you post it here please o:))
 
I'm as confuzed as quasar, but I noticed you defined x and y in terms of r and theta... if they're two separate functions, you're going to confuse the heck out of yourself. If they're not, then you've confused the heck out of yourself. Either way, better labelling is better
 
Well according to Schutz, "any linearly indepedent set of vector fields can serve as a basis, and one can easily show that not all of them are derivable from coordinate systems". The basic test is whether the fields commute. So if:
l and m are independent parameters that generate integral curves over a space
components of vector V are dx/dl, applied to basis d/dx partial derivative for each coordinate x
likewise W=dx/dm
then if commutator of vectors [V,W]=VW-WV does not equal 0, then the parameters l and m form a non-coordinate basis.

Geometrically, if you travel from P along V curve (delta l = e) to point R, then along W curve (delta m = e) to point A, and travel from P along W curve (delta m = e) to Q, then along V curve (delta l = e) to B, then A is not necessarily the same point as B. The distance from A to be is e squared times the commutator [V,W].

As to the original problem, yes I remain confused. I'm only guessing that is how you derive the parametric equations, and in my calculations I try to keep the processing of parameters separate. It seems to get a near result, and a non-zero result, but not the right result.
 
2nd last para of my previous note should read (that's what happens when you type too fast):

Geometrically, if you travel from P along V curve (delta l = e) to point R, then along W curve (delta m = e) to point A, and travel from P along W curve (delta m = e) to Q, then along V curve (delta l = e) to B, then A is not necessarily the same point as B. The vector from A to B is e squared times the commutator [V,W] (which is a vector on basis of partial derivatives of x coordinates).
 
Dear DESIC, I´m having same problem with Ex 2.1 p. 44 of Schutz Geom. Methods of Math. Physics. Have you come any closer to resolving your querry? The answer given by Schutz is
[r,theta]= -theta/r. Isn´t the magnitude of r just unity? Bendon
 
first of all whether you have a coordinate basis or not depends on what coordinates you use on local patches of the manifold..
and by that i mean that in r,θ coordinates [tex]\frac{\partial}{\partial r}[/tex]
and [tex]\frac{\partial}{\partial \theta}[/tex]
are a coordinate basis indeed...
but if you re-express these basis vectors in x,y coordinate language the first becomes
[tex]\frac{\x}{\sqrt[x^2+y^2]}\frac{\partial}{\partial x} + \frac{\y}{\sqrt{x^2+y^2}}\frac{\partial}{\partial y}[/tex]
and etc for the second...
so in x,y basis they are non coordinate vectors and their commutator if you do the math is not zero
[tex]\frac{\x}{\sqrt{x^2+y^2}}[/tex]
 
:rolleyes:sry i messed up my latex
 

Similar threads

  • · Replies 4 ·
Replies
4
Views
2K
  • · Replies 0 ·
Replies
0
Views
2K
  • · Replies 1 ·
Replies
1
Views
2K
  • · Replies 9 ·
Replies
9
Views
4K
  • · Replies 1 ·
Replies
1
Views
2K
Replies
2
Views
3K
Replies
12
Views
2K
Replies
26
Views
6K
Replies
1
Views
2K
Replies
5
Views
3K