Ridiculous Question (Derivatives)

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Homework Help Overview

The discussion revolves around the conditions under which temporal and spatial derivatives can be interchanged, particularly in the context of vector calculus and fields. Participants reference the divergence and its relationship to partial derivatives in the context of electromagnetic fields.

Discussion Character

  • Conceptual clarification, Mathematical reasoning, Assumption checking

Approaches and Questions Raised

  • Participants explore the definitions and properties of derivatives, questioning when it is valid to interchange them. Some express uncertainty about their understanding and seek clarification on the implications for electromagnetic fields.

Discussion Status

The discussion is active, with participants sharing insights about the interchangeability of derivatives and its relevance to vector fields. There is a mix of interpretations regarding the movement of electromagnetic fields, with some participants questioning the necessity of proving certain statements.

Contextual Notes

Participants are navigating through definitions and properties of derivatives, with some expressing a desire to refresh their understanding. There is mention of the independence of variables and the implications for the behavior of fields in space.

tshafer
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Homework Statement



Under what conditions may I change temporal and spatial derivatives? I cannot remember for the life of me.

EG:
\frac{\partial }{\partial t}\left( \nabla \cdot \mathbf{A} \right) = \nabla \cdot \left( \frac{\partial \mathbf{A}}{\partial t}\right)

Thanks.
 
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tshafer said:

Homework Statement



Under what conditions may I change temporal and spatial derivatives? I cannot remember for the life of me.

EG:
\frac{\partial }{\partial t}\left( \nabla \cdot \mathbf{A} \right) = \nabla \cdot \left( \frac{\partial \mathbf{A}}{\partial t}\right)

Thanks.

partial derivative? Any time you want, I think.
 
That's what I thought, too, but I was unsure. Trying to de-rust, here, heh.
 
Go back to the definition of the divergence, so that your equation contains terms like

\frac {\partial } {\partial t} \frac {\partial } {\partial x} \mathbf{A}_x \right) \ .

While x and t are independent variables,

\frac {\partial } {\partial t} \frac {\partial } {\partial x} = \frac {\partial } {\partial x} \frac {\partial } {\partial t} \ .
 
This works for gradient and curl too, by the way. It's basically a matter of


∂²A/∂x∂t = ∂²A/∂t∂x

and similarly for y and z.
 
Redbelly98 said:
This works for gradient and curl too, by the way. It's basically a matter of


∂²A/∂x∂t = ∂²A/∂t∂x

and similarly for y and z.

Could you use this to show that electric and magnetic fields don't move in space?
 
Phrak said:
Could you use this to show that electric and magnetic fields don't move in space?

Hmmm, not sure I understand your question ... E-M fields can and do move through space.
 
Redbelly98 said:
Hmmm, not sure I understand your question ... E-M fields can and do move through space.

The value of the fields change over time for any given coordinate, but the fields are not considered moving objects. The field is attached to a coordinate. A propagating electromagnetic wave is like a sound wave. The wave moves, the molecules stay (nominally) in place. I may be confused about the math, though.
 
Okay. Well, if you're going to say by definition that the fields don't move through space, not sure why you'd need a proof of that.

Or even if you're not saying this is by definition, I don't see how my earlier statement in post #5 could be used to prove it. That statement is a basic consequence of multivariable calculus.
 

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