Vector differential identity proof (using triple product)

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Homework Help Overview

The problem involves proving a vector differential identity related to the operation of the vector field \( v \) and the differential operator \( \nabla \). The identity to be proven is \((v \cdot \nabla)v = \frac{1}{2}\nabla(v \cdot v) + (\nabla \times v) \times v\), which falls within the subject area of vector calculus and differential operators.

Discussion Character

  • Exploratory, Assumption checking, Mathematical reasoning

Approaches and Questions Raised

  • The original poster attempts to use the vector triple product to simplify the proof but questions the validity of this approach, particularly regarding the treatment of the differential operator \( \nabla \) and its application to the vector \( v \).
  • Some participants question the application of the triple product identity and emphasize the importance of tracking which vector \( v \) the operator \( \nabla \) is acting on.
  • Others suggest considering the implications of the gradient of \( v \cdot v \) and the potential need for tensor or index notation to clarify the relationships involved.

Discussion Status

The discussion is ongoing, with participants exploring different interpretations of the problem and the application of vector identities. There is a focus on clarifying the roles of the differential operator and the vectors involved, but no consensus has been reached on a definitive approach or solution.

Contextual Notes

Participants note the complexity introduced by the differential operator \( \nabla \) and its interaction with the vector fields, highlighting the need for careful consideration of how these operators act on the vectors involved. The discussion reflects a common challenge in vector calculus problems, particularly in maintaining clarity about the operations being performed.

Earthland
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Homework Statement



Need to prove that:

(v⋅∇)v=(1/2)∇(v⋅v)+(∇×v)×v

Homework Equations



Vector triple product

(a×b)×c=-(c⋅b)a+(c⋅a)b

The Attempt at a Solution



I know I could prove that simply by applying definitions directly to both sides. I haven't done that because that is tedious, and I strive for a more elegant proof and thought that triple product would give it to me.

Since we are dealing with operators the order of the vectors is important and applying triple product would give me

(v⋅∇)v=(v⋅v)∇+(∇×v)×v

But it seems to me that (v⋅v)∇≠ (1/2)∇(v⋅v). It can't be right, because (v⋅v)∇still needs to be applied to something, while the left hand of the equation is something definite. And I can't see where the 1/2 should come from.

Is it wrong to apply triple product to this problem? How else could I prove this identity? Any help?
 
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It is wrong to apply the triple product in the way you have done, you need to keep track of which v the differential operator is acting on, which should be the same before and after applying the identity.
 
I can't quite understand what you mean. I kept track of the order according to triple product definition, but what does it even mean to keep track on the v that ∇ is acting on? I can't just make it act on v where it isn't acting on v.
 
You cannot simply treat the nabla as if it was a vector. You can do this for the vector structure, but not for what function the differential operator is acting on. The differential operator is always going to act on the v that corresponds to the v that was standing to the right of the nabla in your original expression. Thus the term with both v to the left of the nabla has no meaning unless you realize that the differential operators in this nabla are actually acting on the components of one of the vs.
 
Earthland said:
I can't quite understand what you mean. I kept track of the order according to triple product definition, but what does it even mean to keep track on the v that ∇ is acting on? I can't just make it act on v where it isn't acting on v.

No, but you have made it not act on v where it should!
 
Last edited:
Orodruin said:
You cannot simply treat the nabla as if it was a vector. You can do this for the vector structure, but not for what function the differential operator is acting on. The differential operator is always going to act on the v that corresponds to the v that was standing to the right of the nabla in your original expression. Thus the term with both v to the left of the nabla has no meaning unless you realize that the differential operators in this nabla are actually acting on the components of one of the vs.

That's what I thought also, but I blindly followed the triple product structure provided by wikipedia. So should I just change it to

∇(v⋅v)

But still, 1/2 is missing
 
Yes, in there the nabla is acting on both vs. You have to relate this to the case where it is only acting on one of them.

This is why I clearly prefer tensor/index notation for deriving vector relations. You get rid of these ambiguities that appear from trying to apply vector relations to nabla operators.
 
Both v-s produce a scalar field and thus ∇ acting on it produces a vector field, which it must be because another vector is added to it. ∇ acting on only one v means acting on vector field which would produce a tensor field. So there is some kind of relation I should use?
 
You can either note that the gradient of v^2 is going to be symmetric in terms of which v the nabla acts, or you could simply apply index notation.
 

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