Dual basis and differential forms

Click For Summary
SUMMARY

The discussion focuses on the relationship between dual bases and differential forms, specifically referencing the book "Linear Algebra" by Friedberg, Spence, and Insel (FSI) and "Differential Forms" by do Carmo. It establishes that the dual basis {f_1, f_2, ..., f_n} defined by FSI is indeed unique, as any linear functionals satisfying φ_i(x_j) = δ_ij must be equal to f_i(x). Furthermore, the discussion clarifies that the differential forms dx_i in R³ correspond to the linear functionals f_i, maintaining consistency across both linear algebra and differential geometry contexts.

PREREQUISITES
  • Understanding of dual spaces and dual bases in linear algebra
  • Familiarity with the Kronecker delta function (δ_ij)
  • Basic knowledge of differential forms and their applications
  • Concept of manifolds and tangent spaces in differential geometry
NEXT STEPS
  • Study the properties of dual spaces and bases in linear algebra
  • Explore the implications of the Kronecker delta function in functional analysis
  • Learn about differential forms and their role in manifold theory
  • Investigate the relationship between linear functionals and differential forms in various contexts
USEFUL FOR

Mathematicians, students of linear algebra and differential geometry, and anyone interested in the theoretical foundations of dual spaces and differential forms.

Buri
Messages
271
Reaction score
0
I was reading about dual spaces and dual bases in the book Linear Algebra by Friedberg, Spence and Insel (FSI) and they give an example of a linear functional, f_i (x) = a_i where [x]_β = [a_1 a_2 ... a_n] denotes the matrix representation of x in terms of the basis β = {x_1, x_2, ..., x_n} of V. Now they go on to prove that {f_1, f_2, ..., f_n} is in fact the dual basis of β for V* by actually never using the fact that f_i (x) = a_i, but rather that f_i (x_j) = δ_ij, where δ_ij denotes the Kronecker delta function. I also happened to have read other references by Halmos and Lang and they did not go about actually finding the linear functionals, but rather use the fact that a linear functional that satisfies φ_i (x_j) = δ_ij exists. Now I suppose my question is, doesn't it so happen that the dual basis of β ALWAYS equals {f_1, f_2, ..., f_n} as defined by FSI? Because since φ and f agree on the basis elements in turns out that φ_i = f_i for all x.

Now here is where differential forms come in. I was reading do Carmo's book on Differential forms and he says that the basis of R³ is {dx_i; i = 1,2,3} where x_i represents the i-th coordinate function. So I guess its true that dx_i = f_i(x) from above then right? I, to be honest, find this a bit unexpected as x_i is precisely f_i when we're using the canonical basis, yet differentiating doesn't mess it up. So I actually went on to check it on some values that dx_i really does equal f_i(x). And so it seems to also verify what I was asking in the first paragraph.

Is this all right? I'd appreciate someone clarifying some of this stuff to me.

Thanks!

EDIT: I guess another way of putting my question is, is the dual basis unique, in the sense that the linear functionals that form the basis are always identically equal to f_i(x) as given by FSI?
 
Last edited:
Physics news on Phys.org
Another way of putting your question is:

If you have two lists f and g of linear functionals satisfying:
fi(xj) = δ_ij
gi(xj) = δ_ij​

Can you prove that, for each i,
fi = gi
?
 
I guess I could since they agree on basis elements they should be equal - that's a result from linear algebra. I guess that answers my question, but the differential form example sort of throws me off...
 
I suppose the purpose of 'rewriting' the f_i (x) as dx_i is probably just more convenient as it is "differential" forms.
 
...purpose of 'rewriting' the f_i (x) as dx_i is probably just more convenient as it is "differential" forms.
The purpose is that do Carmo's is interested in differential forms defined on a manifold (or in an open set of it), not just on a single point. Therefore, given a manifold M and p \in M and R3 is its tangent space at p, then the dual basis to the canonical one is indeed dx_i(p) and is exactly the same as the dual basis as defined in linear algebra.

This notation is useful when, for example, you have a function f defined on an open set U of M and you need df, which is then written (usually supressing p):

df(p) = \sum_{i = 1}^{n}a_{i}\left(p\right)dx_{i}\left(p\right)

Where the a_i's are (usually) smooth functions on U.
 
JSuarez said:
The purpose is that do Carmo's is interested in differential forms defined on a manifold (or in an open set of it), not just on a single point. Therefore, given a manifold M and p \in M and R3 is its tangent space at p, then the dual basis to the canonical one is indeed dx_i(p) and is exactly the same as the dual basis as defined in linear algebra.

This notation is useful when, for example, you have a function f defined on an open set U of M and you need df, which is then written (usually supressing p):

df(p) = \sum_{i = 1}^{n}a_{i}\left(p\right)dx_{i}\left(p\right)

Where the a_i's are (usually) smooth functions on U.

Ahh that makes sense to me now. Thanks a lot JSuarez! Also thanks to Hurkyl for helping me out too! :smile:
 

Similar threads

  • · Replies 0 ·
Replies
0
Views
2K
  • · Replies 1 ·
Replies
1
Views
3K
  • · Replies 3 ·
Replies
3
Views
2K
  • · Replies 5 ·
Replies
5
Views
2K
  • · Replies 3 ·
Replies
3
Views
4K
  • · Replies 6 ·
Replies
6
Views
4K
  • · Replies 12 ·
Replies
12
Views
3K
  • · Replies 1 ·
Replies
1
Views
2K
  • · Replies 2 ·
Replies
2
Views
951
  • · Replies 5 ·
Replies
5
Views
4K