Proof of identity involving del

In summary: v_x \frac{\partial}{\partial y}u_z-v_x \frac{\partial}{\partial z}u_y+v_y \frac{\partial}{\partial z}u_x-v_y \frac{\partial}{\partial x}u_z \ \ \dots=u_z \left(v_x \frac{\partial}{\partial y}u_z-v_x \frac{\partial}{\partial z}u_y+v_y \frac{\partial}{\partial z}u_x-v_y \frac{\partial}{\partial x}u_z\right)
  • #1
Aziza
190
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) ?
 
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  • #2
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]
 
  • #3
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..?
 
  • #4
Aziza said:
Oh ok...but then when I broke everything into components it comes out to just be zero..?
It is not zero.
 
  • #5
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]
 
  • #6
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
 
  • #7
SammyS said:
It is not zero.

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

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  • #8
ok starting with the right hand side I arrived to left side but with additional factor of 2...
 

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  • #9
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?
 

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  • #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 =
v_x \frac{\partial}{\partial y}u_z-v_x \frac{\partial}{\partial z}u_y
+v_y \frac{\partial}{\partial z}u_x-v_y \frac{\partial}{\partial x}u_z \ \
\dots[/itex]​

Then use the product rule in reverse to collect terms.
 

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