Verify Integration and differentiation of a vector.

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Discussion Overview

The discussion revolves around the integration and differentiation of a vector, specifically examining the directions of the derivative and integral of a vector compared to the original vector. Participants explore theoretical aspects, mathematical reasoning, and implications in the context of vector magnetic potential related to current distributions.

Discussion Character

  • Technical explanation
  • Mathematical reasoning
  • Debate/contested

Main Points Raised

  • One participant presents the differentiation and integration of a vector, asserting that the direction of the derivative and integral is not the same as the original vector.
  • Another participant corrects a notation error in the differentiation expression but questions the expectation that a triple integral could be the inverse of a single derivative.
  • Some participants argue that the vector can have different directions at different points within the integration volume, making it nonsensical to discuss a single direction for the integral.
  • A participant raises a specific example of a vector A = (x, x, 0) to illustrate the difference between the direction of A and its derivative.
  • Concerns are expressed regarding the relationship between the vector magnetic potential A and the current density J, with examples provided to illustrate potential discrepancies in direction.
  • One participant suggests that if J is continuous, some J within the integration volume might align with A, but acknowledges uncertainty about this claim.
  • Another participant emphasizes that while special cases may exist where A and J align, generally, they do not share the same direction.

Areas of Agreement / Disagreement

Participants express multiple competing views regarding the relationship between the directions of the vector, its derivative, and its integral. The discussion remains unresolved, with no consensus reached on the implications of these relationships.

Contextual Notes

Participants note that the direction of the vector can vary within the integration volume, and there are limitations in determining a general directional relationship between A and J without specific conditions or symmetries.

yungman
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I want to verify simple integration and differentiation of a vector and verify that the direction of the derivative and integral of a vector is not the same direction of the original vector. Let:

[tex]\vec A = \hat x A_x + \hat y A_y + \hat z A_z[/tex]

1) Differentiation:

[tex]\frac {d \vec A}{dx} = \hat x \frac {d A_x}{dx} \;+\; \hat y \frac {d A_y}{dx} \;+\; \hat z \frac {d A_z}{dx}[/tex]


2) Integration:

[tex]\int\int\int \vec A \;dxdydz \;\;= \;\; \hat x \int\int\int A_x \;dxdydz \;\;+\;\; \hat y \int\int\int A_y \;dxdydz \;\;+\;\; \hat z \int\int\int A_z \;dxdydz[/tex]

eg. If

[tex]\vec A = \hat x x \;+\; \hat y y \;+\; \hat z z \;\Rightarrow\; \int\int\int \vec A \;dxdydz \;\;=\;\; \hat x (\frac 1 2 x^2yz +C_1)\;\;+\;\; \hat y (\frac 1 2 xy^2z +C_2)\;\;+\;\; \hat z (\frac 1 2 xyz^2 +C_3)[/tex]

For simplification, I did not perform a true volume integral that have limits on x, y and z.

Therefore the direction of the derivative and integral of a vector is not the same direction as the original vector.
 
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hi yungman! :smile:
yungman said:
[tex]\frac {d \vec A}{dx} = \hat x \frac {d A_x}{dx} \;+\; \hat y \frac {d A_y}{dy} \;+\; \hat z \frac {d A_z}{dz}[/tex]

no, [tex]\frac {d \vec A}{dx} = \hat x \frac {d A_x}{dx} \;+\; \hat y \frac {d A_y}{dx} \;+\; \hat z \frac {d A_z}{dx}[/tex]

but anyway i don't understand why you expect a triple integral to be the inverse of a single derivative :confused:
 
tiny-tim said:
hi yungman! :smile:


no, [tex]\frac {d \vec A}{dx} = \hat x \frac {d A_x}{dx} \;+\; \hat y \frac {d A_y}{dx} \;+\; \hat z \frac {d A_z}{dx}[/tex]

but anyway i don't understand why you expect a triple integral to be the inverse of a single derivative :confused:

Hi Tiny-Tim, thanks, I was just typing too fast. I corrected that already.

I am not expecting triple integral to be the inverse of a single derivative, I just want to verify the direction of the derivative and integral of a vector is not the same as the direction of the original vector A.
 
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For the triple integral, in general, the vector can have different directions at different points within the integration volume. So it doesn't make sense to talk about the direction of the vector. The integral will give a weighted average of the directions the vector has within the integration volume.

As for the derivative (as defined in Post #1), consider A = (x, x, 0). What is the direction of A? What is the direction of the derivative?
 
Redbelly98 said:
For the triple integral, in general, the vector can have different directions at different points within the integration volume. So it doesn't make sense to talk about the direction of the vector. The integral will give a weighted average of the directions the vector has within the integration volume.

As for the derivative (as defined in Post #1), consider A = (x, x, 0). What is the direction of A? What is the direction of the derivative?

Thanks for the reply, I am referring to the vector A has different direction than the volume ingtegral of vector A at ANY point.

The reason I ask was mainly because of the discussion of finding vector magnetic potential for a distribution of current. I want to understand why vector A is not necessary the same direction as vector J in this equation:

1) [tex]\vec A \;=\; \frac {\mu_0}{4\pi}\int_{v'} \frac {\vec J}{|\vec r - \vec r_0|} dv'[/tex]




2)If A = (x, x, 0).

[tex]\frac{\partial \vec A}{\partial x} = (1,0,0)[/tex]

So the direction of A is not necessary same as the direction of it's derivative.
 
yungman said:
Thanks for the reply, I am referring to the vector A has different direction than the volume ingtegral of vector A at ANY point.

The reason I ask was mainly because of the discussion of finding vector magnetic potential for a distribution of current. I want to understand why vector A is not necessary the same direction as vector J in this equation:

1) [tex]\vec A \;=\; \frac {\mu_0}{4\pi}\int_{v'} \frac {\vec J}{|\vec r - \vec r_0|} dv'[/tex]

Hmmm, my suspicion is that if J is continuous, then some J within the integration volume would have the same direction as A. But I could be wrong. (EDIT: I believe I am wrong.)

If J need not be continuous, then I can come up with a fairly simple counterexample:

You're obviously talking about the magnetic vector potential. Consider a square loop of current in the xy plane, oriented so that J always points in the (±1,0,0) or (0,±1,0) direction:

[PLAIN]http://www.lei.ucl.ac.be/~matagne/ELECMAGN/SEM05/S05F64.GIF[/INDENT][/INDENT]

However, in the vicinity of the corners of the square, A will point at roughly 45 degrees to the J's, or the (±1,±1,0) directions.

2)If A = (x, x, 0).

[tex]\frac{\partial \vec A}{\partial x} = (1,0,0)[/tex]

So the direction of A is not necessary same as the direction of it's derivative.

Correct.
 
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Redbelly98 said:
Hmmm, my suspicion is that if J is continuous, then some J within the integration volume would have the same direction as A. But I could be wrong. (EDIT: I believe I am wrong.)

If J need not be continuous, then I can come up with a fairly simple counterexample:

You're obviously talking about the magnetic vector potential. Consider a square loop of current in the xy plane, oriented so that J always points in the (±1,0,0) or (0,±1,0) direction:

[PLAIN]http://www.lei.ucl.ac.be/~matagne/ELECMAGN/SEM05/S05F64.GIF[/INDENT][/INDENT]

However, in the vicinity of the corners of the square, A will point at roughly 45 degrees to the J's, or the (±1,±1,0) directions.


Correct.​


Thanks for your time.

From what we have so far, I think the integral of a vector is not "usually" in the same direction of the original vector. When you talk about some special cases, yes, they cound be in the same direction, but the main point is that they are "usually" not in the same direction and one cannot count on any directional relation.

All these are just to proof that there is no easy way to find the direction of the vector magnetic potential just by the given B. One can only derive A from B only in some cases that have particular symetry where you can apply something like the Gauss law or Amperes' law like int E and B resp.​
 
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