Gradient ∇4: Generalizing for Spacetime and Proving its Four-Vector Properties

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Homework Help Overview

The discussion revolves around the generalization of the gradient operator for spacetime, specifically the expression for ∇4 as a four-vector. The original poster presents a mathematical statement and seeks to demonstrate that ∇4 is indeed a four-vector.

Discussion Character

  • Conceptual clarification, Assumption checking, Mixed

Approaches and Questions Raised

  • Participants explore the definition of a four-vector and question whether the gradient operator can be classified as such. Some express confusion over the terminology and the implications of the original poster's statement.

Discussion Status

There is an ongoing examination of the definitions and properties of four-vectors versus vector operators. Some participants suggest that the original poster needs to clarify their understanding of what constitutes a four-vector in the context of relativity. Multiple interpretations of the term "4-vector" are being explored.

Contextual Notes

Participants note potential misunderstandings regarding the terminology used in the original poster's question, particularly in relation to the transformation properties of the gradient operator in Minkowski space-time.

Unicorn.
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Hi,

Homework Statement


The gradient ∇3 can be generalized for spacetime as:
4 =(∇3 ,d/dct)=(d/dx,d/dy,d/dz,d/dct)
Show that ∇4 is a four-vector.

Homework Equations





The Attempt at a Solution


I just have to write that :
d/dx'=γ(d/dx-βd/dct)
d/dy'=d/dy
d/dz'=d/dz
d/dct'=γ(d/dct-βd/dx)
And
4 =(d/dx,d/dy,d/dz,d/dct)=(∇3 ,d/dct) ..?

Thanks
 
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I don't understand the question. Of course it's a 4-vector. (a, b, c, d) is a 4-vector. Is there some wording missing?
 
Hi,
No, this is the complete wording.
 
What? The 4-gradient ##\nabla_{a}## is a derivative operator. It isn't a 4-vector of any kind. I don't think you are phrasing it correctly.
 
WannabeNewton said:
What? The 4-gradient ##\nabla_{a}## is a derivative operator. It isn't a 4-vector of any kind. I don't think you are phrasing it correctly.
A vector operator is still a vector. You can add them, and multiply them by scalar values.
 
haruspex said:
A vector operator is still a vector. You can add them, and multiply them by scalar values.
An operator acting on a vector isn't an element of the vector space that the vector belongs to. ##\nabla_{a}## is certainly not a 4-vector just because it is linear (it isn't a linear functional - it's just linear). How are you claiming that ##\nabla_{a}\in \mathbb{R}^{4}## (I used ##\mathbb{R}^{4}## because the OP is working in minkowski space-time). That doesn't make any sense.

In fact what is true is that ##\frac{\partial }{\partial x}|_{p},\frac{\partial }{\partial y}|_{p},\frac{\partial }{\partial z}|_{p},\frac{\partial }{\partial t}|_{p}## are 4-vectors in ##\mathbb{R}^{4}##.
 
Last edited:
haruspex said:
A vector operator is still a vector. You can add them, and multiply them by scalar values.

The OP is asking about 4-vectors. So saying that ∇ is a 4-vector is the same as saying that ∇ is an element of ##\mathbb{R}^4##. This is obviously nonsense.

Of course, we can add ∇ and multiply it by scalars. But that means that it is a vector in a vector space. But since the OP asks about 4-vectors, he's specifically asking about the vector space ##\mathbb{R}^4##. At least, that's how I interpret the question.
 
The OP is supposed to show that ##\nabla## transforms like a four-vector. In other words, he or she needs to show that it makes sense to say that ##\partial'_\mu = \Lambda_\mu{}^\nu \partial_\nu##.
 
Last edited:
Actually, strictly speaking, shouldn't it transform like a 1-form?
 
  • #10
Chestermiller said:
Actually, strictly speaking, shouldn't it transform like a 1-form?
The coordinate vector fields ##\partial_{\mu}## do indeed transform like one-forms (hence why they are usually written with a lower index) but they are still 4-vectors as they form a basis for the tangent space when evaluated at each point. Also it doesn't make any sense to say ##\nabla## transforms like a 4-vector because it is not a vector in minkowski space-time, it is map on the ring of smooth functions on minkowski space-time. This bad notation is the kind you would see in Srednicki's QFT text.
 
  • #11
micromass said:
The OP is asking about 4-vectors. So saying that ∇ is a 4-vector is the same as saying that ∇ is an element of ##\mathbb{R}^4##. This is obviously nonsense.

Of course, we can add ∇ and multiply it by scalars. But that means that it is a vector in a vector space. But since the OP asks about 4-vectors, he's specifically asking about the vector space ##\mathbb{R}^4##. At least, that's how I interpret the question.
I gather from various posts that, within relativity theory at least, "4-vector" has a more specific meaning than I was aware of. It's not clear to me whether this is a matter of definition or just common usage.
 
  • #12
haruspex said:
I gather from various posts that, within relativity theory at least, "4-vector" has a more specific meaning than I was aware of. It's not clear to me whether this is a matter of definition or just common usage.

Ah, maybe you're right. I don't know any relativity. I just looked up 4-vector in wikipedia.

To avoid confusion, perhaps we should let the OP tell us how he defined "4-vector" in his course.
 

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