Proof of identity involving del

Click For Summary

Homework Help Overview

The discussion revolves around proving the vector identity ∇.(u×v) = v.(∇×u) - u.(∇×v), where ∇ is a vector differential operator and u, v are vectors. Participants are exploring the implications of vector calculus rules and the properties of the differential operator.

Discussion Character

  • Exploratory, Conceptual clarification, Mathematical reasoning, Assumption checking

Approaches and Questions Raised

  • Some participants attempt to apply the scalar product rule to the identity, questioning whether the left-hand side can be simplified to either v.(∇×u) or -u.(∇×v). Others express confusion about the nature of the operator ∇ and its implications for the identity. There are discussions about breaking the expression into components and the results of such attempts, with some participants noting discrepancies in their findings.

Discussion Status

The discussion is active, with participants sharing their thoughts on various approaches, including the use of Cartesian tensors and component breakdowns. Some participants have provided insights into potential errors in reasoning, while others are seeking hints or alternative methods to prove the identity without using tensors. There is acknowledgment of a factor of two appearing in some calculations, prompting further exploration of how to address this issue.

Contextual Notes

Participants note that certain methods, such as using tensors, are not part of the curriculum, which may limit the approaches available for proving the identity. There is also mention of confusion regarding notation and the proper application of the product rule in the context of vector calculus.

Aziza
Messages
189
Reaction score
1
Prove that ∇.(u×v) = v.(∇×u) - u.(∇×v), where "." means dot product and u,v are vectors.

So by scalar product rule, A.(B×C) = C.(A×B)
So applying same logic to above identity, shouldn't the left hand side just be equal to v.(∇×u)?
Or just to -u.(∇×v), since A.(B×C) = -B.(A×C) ?
 
Physics news on Phys.org
Aziza said:
Prove that ∇.(u×v) = v.(∇×u) - u.(∇×v), where "." means dot product and u,v are vectors.

So by scalar product rule, A.(B×C) = C.(A×B)
So applying same logic to above identity, shouldn't the left hand side just be equal to v.(∇×u)?
Or just to -u.(∇×v), since A.(B×C) = -B.(A×C) ?

[itex]\displaystyle \vec{\nabla}[/itex] is not just any vector. It's a vector differential operator .

So it's no more true that [itex]\displaystyle \vec{\nabla}\cdot(\vec{u}\times\vec{v})=\vec{v} \cdot(\vec{\nabla}\times\vec{u})[/itex] than it is that [itex]\displaystyle \vec{\nabla}\cdot\vec{u}=\vec{u}\cdot\vec{\nabla}[/itex] or that [itex]\displaystyle \vec{\nabla}\times\vec{u}=-\vec{u}\times\vec{\nabla}\ .[/itex]
 
SammyS said:
[itex]\displaystyle \vec{\nabla}[/itex] is not just any vector. It's a vector differential operator .

So it's no more true that [itex]\displaystyle \vec{\nabla}\cdot(\vec{u}\times\vec{v})=\vec{v} \cdot(\vec{\nabla}\times\vec{u})[/itex] than it is that [itex]\displaystyle \vec{\nabla}\cdot\vec{u}=\vec{u}\cdot\vec{\nabla}[/itex] or that [itex]\displaystyle \vec{\nabla}\times\vec{u}=-\vec{u}\times\vec{\nabla}\ .[/itex]

Oh ok...but then when I broke everything into components it comes out to just be zero..?
 
Aziza said:
Oh ok...but then when I broke everything into components it comes out to just be zero..?
It is not zero.
 
The only proof I can think of is the one using cartesian tensors.

[tex]\partial_{i}\left(\epsilon_{ijk}u_{j}v_{k}\right) =...[/tex]
 
dextercioby said:
The only proof I can think of is the one using cartesian tensors.

[tex]\partial_{i}\left(\epsilon_{ijk}u_{j}v_{k}\right) =...[/tex]


Thats definitely not how we're supposed to prove that lol, we did not learn that yet
 
SammyS said:
It is not zero.

I have attached my proof that it is...what am I doing wrong?edit: oops nvm nvm
 

Attachments

  • proof.jpeg
    proof.jpeg
    29.7 KB · Views: 648
ok starting with the right hand side I arrived to left side but with additional factor of 2...
 

Attachments

  • proof2.jpeg
    proof2.jpeg
    30.8 KB · Views: 870
Could someone please give hint as to how to prove this (not using tensors)? Breaking into components does not work for some reason
 
  • #10
if no one knows the answer, perhaps someone knows a book with proofs of these things? I can't find anything whatsoever. I found one proof of this involving tensors, but again, this is not how we're supposed to prove this. I've also attached another picture showing that the right hand side is actually equal to twice the left hand side...perhaps the last picture was not clear enough..I started with the right side and arrived at twice the left..is there perhaps some way to cancel this factor of 2?
 

Attachments

  • proof3.jpeg
    proof3.jpeg
    30.6 KB · Views: 688
  • #11
How do you figure that
[itex]\displaystyle \left\langle \frac{\partial}{\partial x},\,\frac{\partial}{\partial y},\,\frac{\partial}{\partial z}\right\rangle\cdot\left\langle u_yv_z-u_zv_y,\,u_zv_x-u_xv_z,\,u_xv_y-u_yv_x \right\rangle[/itex]​
is zero?

Expand that out. Don't forget to use the product rule.

Added in Edit:

Remember that [itex]u_x[/itex] is the x component of vector u, and not [itex]\displaystyle \frac{\partial u}{\partial x}\,,\[/itex] etc.
 
Last edited:
  • #12
SammyS said:
How do you figure that
[itex]\displaystyle \left\langle \frac{\partial}{\partial x},\,\frac{\partial}{\partial y},\,\frac{\partial}{\partial z}\right\rangle\cdot\left\langle u_yv_z-u_zv_y,\,u_zv_x-u_xv_z,\,u_xv_y-u_yv_x \right\rangle[/itex]​
is zero?

Expand that out. Don't forget to use the product rule.

Added in Edit:

Remember that [itex]u_x[/itex] is the x component of vector u, and not [itex]\displaystyle \frac{\partial u}{\partial x}\,,\[/itex] etc.

yea I know in my previous edit I said nvm about it being zero. I did in fact mix up my own notation. But if you read my posts after that, I show picture of how I got twice the identity I was supposed to get...there is factor of two for some reason and I don't know how to get rid of it. I am pretty sure I am doing everything right tho...
 
  • #13
Aziza said:
yea I know in my previous edit I said nvm about it being zero. I did in fact mix up my own notation. But if you read my posts after that, I show picture of how I got twice the identity I was supposed to get...there is factor of two for some reason and I don't know how to get rid of it. I am pretty sure I am doing everything right tho...
You can't move things from the left of the partial derivative operator to the right of it.

So the 4th line of the following (the third line which starts with an '=' sign)

attachment.php?attachmentid=52591&d=1351955400.jpg


should start out as
[itex]\displaystyle =<br /> v_x \frac{\partial}{\partial y}u_z-v_x \frac{\partial}{\partial z}u_y<br /> +v_y \frac{\partial}{\partial z}u_x-v_y \frac{\partial}{\partial x}u_z \ \ <br /> \dots[/itex]​

Then use the product rule in reverse to collect terms.
 

Similar threads

  • · Replies 7 ·
Replies
7
Views
1K
Replies
4
Views
2K
  • · Replies 1 ·
Replies
1
Views
3K
  • · Replies 1 ·
Replies
1
Views
1K
  • · Replies 4 ·
Replies
4
Views
3K
Replies
4
Views
3K
  • · Replies 1 ·
Replies
1
Views
1K
  • · Replies 1 ·
Replies
1
Views
4K
  • · Replies 8 ·
Replies
8
Views
3K
  • · Replies 8 ·
Replies
8
Views
3K