Double Curl Identity: Vector or Scalar?

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Homework Help Overview

The discussion revolves around the double curl identity in vector calculus, specifically the identity rot(rot(E)) = grad(div(E)) - div(grad(E)). Participants are exploring the nature of the terms involved, questioning whether grad(div(E)) should be a vector and div(grad(E)) a scalar, and how these can be combined in the identity.

Discussion Character

  • Conceptual clarification, Assumption checking

Approaches and Questions Raised

  • Some participants express confusion regarding the dimensionality of the terms in the identity, questioning how a vector and a scalar can be added or subtracted. Others suggest that the identity can be interpreted differently, considering the vector Laplacian and its application to vector fields.

Discussion Status

Participants are actively engaging with the concepts, with some providing clarifications about the definitions of the Laplacian and its application to vectors and scalars. There is an ongoing exploration of interpretations, particularly regarding the terminology of the vector Laplacian and its use in different contexts.

Contextual Notes

Some participants note their limited background in the mathematical aspects of the topic, indicating a desire for deeper understanding without having encountered certain mathematical concepts in their studies.

ShamelessGit
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This isn't a homework problem, but it won't let me post on the other page.

A well known vector identity is that rot(rot(E)) = grad(div(E)) - div(grad(E)).
I've actually used this before without encountering any problems, so I don't know if I'm just having a brain fart or something, but shouldn't grad(div(E)) be equal to a vector and div(grad(E)) be equal to a scalar? How can you add or subtract them? It doesn't make any sense.
 
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ShamelessGit said:
This isn't a homework problem, but it won't let me post on the other page.

A well known vector identity is that rot(rot(E)) = grad(div(E)) - div(grad(E)).
I've actually used this before without encountering any problems, so I don't know if I'm just having a brain fart or something, but shouldn't grad(div(E)) be equal to a vector and div(grad(E)) be equal to a scalar? How can you add or subtract them? It doesn't make any sense.

Hi ShamelessGit! :smile:

In that identity E is a vector and grad(E) is a component wise gradient yielding a matrix.
The divergence is taken of the gradient of each of the components of E.
 
ShamelessGit said:
This isn't a homework problem, but it won't let me post on the other page.

A well known vector identity is that rot(rot(E)) = grad(div(E)) - div(grad(E)).
I've actually used this before without encountering any problems, so I don't know if I'm just having a brain fart or something, but shouldn't grad(div(E)) be equal to a vector and div(grad(E)) be equal to a scalar? How can you add or subtract them? It doesn't make any sense.

Isn't it ∇ × ∇ × E = ∇ (∇ · E) - ∇ ^2 E, where ∇ ^2 is the vector Laplacian (as in, ∇ ^2 E instead of ∇ · (∇ E) or the scalar Laplacian)? That way they are both vectors. At least that's what I've been told.
 
Last edited:
DeIdeal said:
Isn't it ∇ × ∇ × E = ∇ (∇ · E) - ∇ ^2 E, where ∇ ^2 is the vector Laplacian (as in, ∇ ^2 E instead of ∇ · (∇ E) or the scalar Laplacian)? That way they are both vectors. At least that's what I've been told.

The Laplacian is defined as the divergence of the gradient.
It's just a shorthand notation.
 
I like Serena said:
The Laplacian is defined as the divergence of the gradient.
It's just a shorthand notation.

(I'm sure you're correct, don't get me wrong. I just want to understand this myself. I don't actually know that much about the maths behind this, I've only had to use nablas in physics and haven't even encountered partial derivatives in actual mathematics classes yet.)

Yeah, I know that using ∇ is just a shorter notation, but isn't ∇ ^2 A for a vector field A defined as the vector Laplacian

\nabla^2 \overline{A} = \frac{\partial^2 A_{x}}{\partial^2 x}\hat{i} + \frac{\partial^2 A_{y}}{\partial^2 y}\hat{j} + \frac{\partial^2 A_{z}}{\partial^2 z}\hat{k}

and ∇ ^2 A for a scalar field A separately defined as the scalar Laplacian

\nabla^2 {A} = \nabla \cdot (\nabla A) = \frac{\partial^2 A_{x}}{\partial^2 x} + \frac{\partial^2 A_{y}}{\partial^2 y} + \frac{\partial^2 A_{z}}{\partial^2 z}

Or have I just understood something wrong?
 
Last edited:
Yes, I'm afraid you've misunderstood.

\Delta \mathbf{A} = \nabla^2 \mathbf{A} = (\frac{\partial^2 A_{x}}{\partial^2 x} + \frac{\partial^2 A_{x}}{\partial^2 y} + \frac{\partial^2 A_{x}}{\partial^2 z})\hat{i} + (\frac{\partial^2 A_{y}}{\partial^2 x} + \frac{\partial^2 A_{y}}{\partial^2 y} + \frac{\partial^2 A_{y}}{\partial^2 z})\hat{j} + (\frac{\partial^2 A_{z}}{\partial^2 x} + \frac{\partial^2 A_{z}}{\partial^2 y} + \frac{\partial^2 A_{z}}{\partial^2 z})\hat{k}

The vector laplacian is the same as the scalar laplacian, but it is applied component-wise on the vector.
 
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I like Serena said:
Yes, I'm afraid you've misunderstood.

\nabla^2 \overline{A} = (\frac{\partial^2 A_{x}}{\partial^2 x} + \frac{\partial^2 A_{x}}{\partial^2 y} + \frac{\partial^2 A_{x}}{\partial^2 z})\hat{i} + (\frac{\partial^2 A_{y}}{\partial^2 x} + \frac{\partial^2 A_{y}}{\partial^2 y} + \frac{\partial^2 A_{y}}{\partial^2 z})\hat{j} + (\frac{\partial^2 A_{z}}{\partial^2 x} + \frac{\partial^2 A_{z}}{\partial^2 y} + \frac{\partial^2 A_{z}}{\partial^2 z})\hat{k}

The vector laplacian is the same as the scalar laplacian, but it is applied component wise on the vector.

Ok, thanks a lot for the clarification! :smile:

IIRC my lecturer actually used the word 'vector Laplacian' (not in English, but still), when deriving the wave equation for electromagnetic waves. I might just remember wrong, though, or it might've been a careless mistake by him. Now I know better, so thanks!
 
I like Serena said:
The word 'vector Laplacian' is not wrong.
It just means that the Laplacian is applied component-wise to a vector.

Yeah, that's what I figured from your previous post.

I like Serena said:
Did your lecturer use the vector Laplacian as you defined it in your previous post?

I thought he did, in the very same "curl of the curl"-sense, when taking the curl of Maxwell's third and fourth equations. But I tried to search our lecture notes for the word and couldn't find it, so now I'm starting to think I just remember wrong or something. Nevertheless, sorry for the trouble I caused (apologies to OP as well!) & thanks for explaining this to me.
 

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