The Wedge Product .... Tu, Section 3.7

In summary: Your Name]In summary, the section on the wedge product in Loring W.Tu's book "An Introduction to Manifolds" (Second Edition) discusses the concept of permutations and the role of the sign function in alternating multilinear maps. The sign function helps us keep track of changes in sign when swapping inputs in wedge products of differential forms. An example is provided to demonstrate how the sign function works in practice.
  • #1
Math Amateur
Gold Member
MHB
3,990
48
I am reading Loring W.Tu's book: "An Introduction to Manifolds" (Second Edition) ...

I need help in order to fully understand Tu's section on the wedge product (Section 3.7 ... ) ... ...

The start of Section 3.7 reads as follows:
?temp_hash=95e2e678b5cea7a98901538248d96796.png


In the above text from Tu we read the following:

" ... ... for every permutation ##\sigma \in S_{ k + l }##, there are ##k!## permutations ##\tau## in ##S_k## that permute the first ##k## arguments ##v_{ \sigma (1) }, \cdot \cdot \cdot , v_{ \sigma (k) }## and leave the arguments of ##g## alone; for all ##\tau## in ##S_k##, the resulting permutations ##\sigma \tau## in ##S_{ k + l }## contribute the same term to the sum, ... ... "Since I did not completely understand the above quoted statement I developed an example with ##f \in A_2 (V)## and ##g \in A_3 (V)## ... ... so we have##f \wedge g ( v_1 \cdot \cdot \cdot v_5) ##

## = \frac{1}{2!} \frac{1}{3!} \sum_{ \sigma \in S_5 } f ( v_{ \sigma (1) }, v_{ \sigma (2) } ) g( v_{ \sigma (3) }, v_{ \sigma (4) }, v_{ \sigma (5) } )##Now ... translating Tu's quoted statement above into the terms of the example we have ... ...

" ... for every permutation ##\sigma \in S_{ 2 + 3 }## there are ##2! = 2## permutations ##\tau## in ##S_2## that permute the first ##2## arguments ##v_{ \sigma (1) }, v_{ \sigma (2) }## and leave the arguments of ##g## alone ... ... "

Now, following the above quoted text ... consider a specific permutation ##\sigma## ... say## \sigma_1 = \begin{bmatrix} 1 & 2 & 3 & 4 & 5 \\ 2 & 3 & 4 & 5 & 1 \end{bmatrix}##Now there are ##2!= 2## permutations ##\tau## in ##S_2## that permute the first ##k = 2## arguments ##( v_{ \sigma (1) }, v_{ \sigma (2) } ) = ( v_2, v_3 )## ...

[Note ... one of the ##k!## permutations is essentially ##\sigma_1## itself ... ]

These permutations may be represented by (is this correct?)

... in ##S_2## ...

##\tau_1 = \begin{bmatrix} 2 & 3 \\ 2 & 3 \end{bmatrix}##

##\tau_2 = \begin{bmatrix} 2 & 3 \\ 3 & 2 \end{bmatrix}##and in ##S_{ 2 + 3 }## ...## \tau_1 = \begin{bmatrix} 2 & 3 & 4 & 5 & 1 \\ 2 & 3 & 4 & 5 & 1 \end{bmatrix}##

## \tau_2 = \begin{bmatrix} 2 & 3 & 4 & 5 & 1 \\ 3 & 2 & 4 & 5 & 1 \end{bmatrix}##Now the resulting permutations ##\sigma \tau## are supposed to contribute the same term to the sum ...... ... ##\sigma_1 \tau_1 = \begin{bmatrix} 1 & 2 & 3 & 4 & 5 \\ 2 & 3 & 4 & 5 & 1 \end{bmatrix} \begin{bmatrix} 2 & 3 & 4 & 5 & 1 \\ 2 & 3 & 4 & 5 & 1 \end{bmatrix}##

## = \begin{bmatrix} 1 & 2 & 3 & 4 & 5 \\ 2 & 3 & 4 & 5 & 1 \end{bmatrix}##and## \sigma_1 \tau_2 = \begin{bmatrix} 1 & 2 & 3 & 4 & 5 \\ 2 & 3 & 4 & 5 & 1 \end{bmatrix} \begin{bmatrix} 2 & 3 & 4 & 5 & 1 \\ 3 & 2 & 4 & 5 & 1 \end{bmatrix}#### = \begin{bmatrix} 1 & 2 & 3 & 4 & 5 \\ 2 & 4 & 3 & 5 & 1 \end{bmatrix} ##
Now the two permutations are not identical ... but ... maybe the difference is accounted for in the ##( \text{ sgn } ) ## function somehow ... but how ... ?
Can someone please clarify the above ...

... ... could someone also confirm that the above analysis is basically correct ... ?

Peter
 

Attachments

  • Tu - Start of Section 3.7 ... Wedge Product ... ... .png
    Tu - Start of Section 3.7 ... Wedge Product ... ... .png
    56.8 KB · Views: 441
  • ?temp_hash=95e2e678b5cea7a98901538248d96796.png
    ?temp_hash=95e2e678b5cea7a98901538248d96796.png
    56.8 KB · Views: 619
Physics news on Phys.org
  • #2
Math Amateur said:
" ... ... for every permutation ##\sigma \in S_{ k + l }##, there are ##k!## permutations ##\tau## in ##S_k## that permute the first ##k## arguments ##v_{ \sigma (1) }, \cdot \cdot \cdot , v_{ \sigma (k) }## and leave the arguments of ##g## alone; for all ##\tau## in ##S_k##, the resulting permutations ##\sigma \tau## in ##S_{ k + l }## contribute the same term to the sum, ... ... "
I think there is a bit of abuse of notation from the author there. What he means that there is a perm ##\tau\in S_{k+l}## (not ##S_k##) that permutes the first ##k## elements and is the identity map on the last ##l## elements. So the two possible values for ##\tau## are ##\tau_1 =##(1 2 3 4 5) and##\tau_2=## (2 1 3 4 5).
If ##\sigma## is (5 1 3 4 2) then
##\sigma\tau_1=##(5 1 3 4 2)(1 2 3 4 5) = (5 1 3 4 2)
and
##\sigma\tau_2=##(5 1 3 4 2)(2 1 3 4 5) = (1 5 3 4 2)

In this case the two terms in the sum (3.5) from this ##\sigma## are:

##\textrm{sgn} (\sigma\tau_1) f(v_5, v_1) g(v_3,v_4,v_2)
= \textrm{sgn} (\sigma)\textrm{sgn}(\tau_1) f(v_5, v_1) g(v_3,v_4,v_2)##
and
##\textrm{sgn} (\sigma\tau_2) f(v_1, v_5) g(v_3,v_4,v_2)
= \textrm{sgn} (\sigma)\textrm{sgn}(\tau_2) f(v_1, v_5) g(v_3,v_4,v_2)##
and the signs of both the second 'sgn' piece and the ##f## piece change between the two, cancelling each other out and making the values the same.
 
  • Like
Likes Math Amateur
  • #3
Hello Peter,

Your example and analysis seem to be correct. The difference between the two permutations is accounted for by the sign function, also known as the signature or parity function. This function assigns a value of either +1 or -1 to each permutation, depending on whether it is an even or odd permutation. In your example, the first permutation, ##\sigma_1 \tau_1##, has a sign of +1 while the second permutation, ##\sigma_1 \tau_2##, has a sign of -1. This is because the second permutation involves an odd number of swaps, while the first permutation does not involve any swaps.

In general, when we are dealing with wedge products of differential forms, the sign function comes into play because we are dealing with alternating multilinear maps. This means that the order of the inputs matters and swapping inputs changes the sign of the output. The sign function helps us keep track of these changes in sign.

I hope this helps clarify the concept of the sign function in the context of wedge products. Let me know if you have any further questions.
 

What is the Wedge Product in Tu, Section 3.7?

The Wedge Product is a mathematical operation that combines two vectors to create a new vector that is perpendicular to both of the original vectors. It is also known as the exterior product or outer product.

How is the Wedge Product calculated?

The Wedge Product is calculated by taking the cross product of two vectors and multiplying it by the sine of the angle between the two vectors. This results in a new vector that is perpendicular to both of the original vectors.

What are the properties of the Wedge Product?

The Wedge Product has several properties, including bilinearity, anti-commutativity, and associativity. It also follows the distributive law and can be used to calculate the area of a parallelogram or the volume of a parallelepiped.

How is the Wedge Product used in mathematics?

The Wedge Product is used in many areas of mathematics, including linear algebra, differential geometry, and topology. It is also used in physics, particularly in the study of electromagnetism and quantum mechanics.

What are some real-world applications of the Wedge Product?

The Wedge Product has various applications in engineering, such as in computer graphics, robotics, and mechanics. It is also used in computer vision and image processing to calculate the orientation and motion of objects in 3D space.

Similar threads

Replies
2
Views
2K
  • Topology and Analysis
Replies
12
Views
377
Replies
2
Views
2K
Replies
6
Views
2K
  • Quantum Physics
2
Replies
43
Views
2K
Replies
22
Views
1K
Replies
6
Views
2K
  • Precalculus Mathematics Homework Help
Replies
21
Views
1K
  • Linear and Abstract Algebra
Replies
5
Views
959
Replies
16
Views
2K
Back
Top