A derivative identity (Zangwill)

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SUMMARY

The discussion centers on proving the identity ##\nabla \cdot [\vec{A}(r) \times \vec{r}] = 0## without using vector identities. The solution utilizes the Levi-Civita symbol and the properties of the dot and cross products, demonstrating that both terms derived from the divergence vanish. The final conclusion confirms that the identity holds true regardless of the specific form of ##\vec{A}(r)##, provided that the curl of ##\vec{A}## is zero.

PREREQUISITES
  • Understanding of vector calculus, specifically divergence and curl.
  • Familiarity with Levi-Civita symbols and their properties.
  • Knowledge of Kronecker delta and its application in tensor calculus.
  • Ability to manipulate mathematical expressions involving dot and cross products.
NEXT STEPS
  • Study the properties of the Levi-Civita symbol in depth.
  • Learn about the implications of the curl of a vector field being zero.
  • Explore advanced vector calculus identities, particularly those involving divergence and curl.
  • Review the application of Kronecker delta in vector calculus problems.
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Students and professionals in mathematics, physics, and engineering who are working with vector calculus and need to understand advanced identities and their proofs.

jack476
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Homework Statement


Without using vector identities, show that ##\nabla \cdot [\vec{A}(r) \times \vec{r}] = 0##.

Homework Equations


The definitions and elementary properties of the dot and cross products in terms of Levi-Civita symbols. The "standard" calculus III identities for the divergence and curl are not allowed.

The Attempt at a Solution


$$
\begin{align*}
\nabla \cdot(\vec{A}\times \vec{r}) &= \epsilon_{ijk}\partial_i(A_jr_k)\\
&= \epsilon_{ijk}r_k\partial_iA_j + \epsilon_{ijk}A_j\partial_ir_k\\
&= \epsilon_{ijk}r_k\partial_iA_j + \epsilon_{ijk}A_j\delta_{ik}
\end{align*}$$

The ##\epsilon_{ijk}A_j\delta_{ik}## term disappears because ##\delta_{ik}\epsilon_{ijk}=0## and the ##\epsilon_{ijk}r_k\partial_iA_j## term disappears because ##\epsilon_{ijk}r_k\partial_iA_j = \epsilon_{ijk}\delta_{ik}r_i\partial_iA_j = 0## for the same reason. Therefore ##\nabla \cdot [\vec{A}(r) \times \vec{r}] = 0##.

Is the use of the Kronecker delta in the final step valid?
 
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jack476 said:

Homework Statement


Without using vector identities, show that ##\nabla \cdot [\vec{A}(r) \times \vec{r}] = 0##.

Homework Equations


The definitions and elementary properties of the dot and cross products in terms of Levi-Civita symbols. The "standard" calculus III identities for the divergence and curl are not allowed.

The Attempt at a Solution


$$
\begin{align*}
\nabla \cdot(\vec{A}\times \vec{r}) &= \epsilon_{ijk}\partial_i(A_jr_k)\\
&= \epsilon_{ijk}r_k\partial_iA_j + \epsilon_{ijk}A_j\partial_ir_k\\
&= \epsilon_{ijk}r_k\partial_iA_j + \epsilon_{ijk}A_j\delta_{ik}
\end{align*}$$

The ##\epsilon_{ijk}A_j\delta_{ik}## term disappears because ##\delta_{ik}\epsilon_{ijk}=0## and the ##\epsilon_{ijk}r_k\partial_iA_j## term disappears because ##\epsilon_{ijk}r_k\partial_iA_j = \epsilon_{ijk}\delta_{ik}r_i\partial_iA_j = 0## for the same reason. Therefore ##\nabla \cdot [\vec{A}(r) \times \vec{r}] = 0##.

Is the use of the Kronecker delta in the final step valid?

Are you sure it does not depend on the form of ##\vec{A}(r)?## If that is the case, can you prove it?
 
Lets cheat a bit and use the vector calculus identity ##\nabla \cdot (A\times B)=(\nabla \times A)\cdot B - A\cdot(\nabla\times B)## then it seems we can prove it but we need that ##\nabla\times A=\vec{0}##. Is this fact about the curl of A given as additional assumption which you omitted to write here?
 
You know there's a solution manual in the internet, right?
 

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