Vector Calculus: Prove ∇ × (a×r/r^n) = (2-n)a/r^n + n(a.r)r/r^(n+2)

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Homework Help Overview

The discussion revolves around proving a vector calculus identity involving the curl of a vector field defined as the cross product of a constant vector and a position vector, divided by a power of the magnitude of the position vector. The participants are exploring the implications of treating certain variables as constants and the correct application of vector calculus identities.

Discussion Character

  • Exploratory, Mathematical reasoning, Assumption checking

Approaches and Questions Raised

  • Participants discuss the implications of treating the position vector's magnitude as a constant and question the validity of applying certain vector identities. Some express confusion over the assumptions made regarding the variables involved.

Discussion Status

There is an ongoing exploration of different approaches to the problem, with some participants sharing their attempts and corrections. While some have proposed methods to simplify the expression, there is no explicit consensus on a single approach or solution yet.

Contextual Notes

Participants note that the variable r is not a constant, which is a critical point in their reasoning. There are references to corrections made in previous posts, indicating a dynamic discussion with evolving understanding.

MrWarlock616
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Homework Statement



Prove that ##∇ × (\frac{\vec{a} × \vec{r}}{r^n})= \frac{2-n}{r^n}\vec{a}+\frac{n(\vec{a}.\vec{r}) \vec{r}}{r^{n+2}}##

Nothing is mentioned about ##\vec{a}## so I'm assuming it is a constant vector. Also ##\vec{r} = <x, y, z> ## and ##|r|=r##

Homework Equations





The Attempt at a Solution



What I don't get is why am I not allowed to do the following:

##L.H.S = \frac{1}{r^n} (∇ × (\vec{a} × \vec{r}) ) ##

## = \frac{1}{r^n} ((∇.\vec{r})\vec{a} - (∇.\vec{a})\vec{r} )## ---(using vector triple product formula)

And since ##∇.\vec{a} = 0## since ##\vec{a}## is a constant and also ##∇.\vec{r}=3##

##L.H.S = \frac{3\vec{a}}{r^n} ##

But then a black hole gets generated somewhere in the universe because the identity cannot be proved from here.
 
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I get it... r is not a constant. damn me
 
MrWarlock616 said:
I get it... r is not a constant. damn me

If you don't mind, can you please post the solution you have found? Thanks!
 
Easy way:

Using that for scalar valued point function ∅ and a vector valued point function ##\vec{f}##,

##∇× (∅\vec{f}) = ∇∅ × \vec{f} + ∅ (∇ × \vec{f})##

L.H.S. ## = ∇(\frac{1}{r^n}) × \vec{f} + ∅ (∇ × \vec{f}) ##

## = (-nr^{-n-2}\vec{r} ) × (\vec{a} × \vec{r}) + \frac{1}{r^n} (∇ × (\vec{a} × \vec{r}) )##

## = -nr^{-n-2} (\vec{r} × (\vec{a} × \vec{r})) + r^{-n} (2\vec{a}) ##

## = -nr^{-n-2} [(\vec{r} . \vec{r})\vec{a}-(\vec{r}.\vec{a})\vec{r}] + r^{-n} (2\vec{a}) ##

## = -nr^{-n-2} r^2\vec{a} + nr^{-n-2}(\vec{r} . \vec{a})\vec{r} + 2r^{-n}\vec{a} ##

phew..simplifying further will yield the RHS.

Note that I've used the following:

## ∇r^n=nr^{n-2} \vec{r}##

##∇ × (\vec{a} × \vec{r}) = 2\vec{a} ##

Hard way:

You can do it by finding the actual cross product on the LHS like I did, keeping in mind that r is not a constant scalar xD

Also, later on you have to make an adjustment by adding and subtracting ## \frac{n}{r^{n+2}} a_{1,2,3} x^2 ## in each component of the cross product.
 
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From my book

I've made many corrections to my last post
 

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MrWarlock616 said:
From my book

I've made many corrections to my last post

Thanks a lot MrWarlock! :)

The alternative method is much better.
 

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