Time Derivatives of Vector Integrals in Griffiths E&M

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Homework Help Overview

This discussion revolves around a problem from Griffiths' Electricity and Magnetism concerning the time derivatives of vector integrals. The original poster expresses confusion regarding the application of the product rule to an integral involving a position vector and a charge density function.

Discussion Character

  • Conceptual clarification, Assumption checking

Approaches and Questions Raised

  • Participants explore the meaning of the time derivative of a position vector within the context of the integral. There are attempts to clarify the distinction between the trajectory of a charge distribution and the static nature of the position vector used in the integral.

Discussion Status

Some participants have offered insights into the nature of the position vector and its role as a static variable in the integral. There is ongoing exploration of the implications of treating the position vector as a function of spatial coordinates rather than time.

Contextual Notes

There appears to be some confusion regarding the definitions and roles of the variables involved, particularly between the integration variable and the position vector. Participants are addressing assumptions about the relationship between time and spatial variables in the context of the problem.

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Homework Statement


This question refers to Griffiths E and M book.

To finish the problem, I just need to show that

[tex]\frac{d}{dt}\int_V \vec{r} \rho d\tau = \int_V \vec{r} \frac{\partial \rho}{\partial t} d\tau[/tex]

When you apply the product rule to the integral, why do you get

[tex]\frac{\partial \vec{r}}{\partial t} = 0[/tex]

?

Actually I am really not really sure what that derivative even means here. My instinct would say you just get [itex]\dot{\vec{r}}[/itex], but what does that mean? I am so confused! So, r is a position vector and position vectors can be functions of time and Griffiths says there is current in the region... But what is it the position vector of?? Ahhh, this is insane--can someone just explain the whole situation regarding that integral and the time derivative of it?

Homework Equations


The Attempt at a Solution

 
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To do this problem,simply evaluate [tex]\int\ div( x \vec J ) dV[/tex] using the product rule.Also this integral is also equal to a closed surface integral using divergence theorem. Using the volume as all space,you get the boundary at infinity where this surface integral vanishes.Rearranging the other side of the integral, you will get the result for x direction.Compute for all x,y, and z directions.This gives you the result.
 
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neelakash said:
To do this problem,simply evaluate [tex]\int\ div( x \vec J ) dV[/tex] using the product rule.Also this integral is also equal to a closed surface integral using divergence theorem. Using the volume as all space,you get the boundary at infinity where this surface integral vanishes.Rearranging the other side of the integral, you will get the result for x direction.Compute for all x,y, and z directions.This gives you the result.

I did all of that before I opened the thread. Can someone answer my questions?
 
You are confusing between the trajectory concept and co-ordinate concept.In this problem r is a function of x,y,z and not t.You are not worried about the trajectory of the charge distribution.
 
neelakash said:
You are confusing between the trajectory concept and co-ordinate concept.In this problem r is a function of x,y,z and not t.You are not worried about the trajectory of the charge distribution.

Hmmm...that makes some sense. Can someone say more about that please?
 
r is an integration variable.
Nothing outside the integral can affect it.
Go back to your calculus book on differentiating an integral.
 
clem said:
r is an integration variable.
Nothing outside the integral can affect it.
Go back to your calculus book on differentiating an integral.

No, it's not. The integration variable is tau. It looks similar to r in this font.


To the OP: [itex]\vec r[/itex] is just a static position; the location at which you are measuring the field. It doesn't change with time.
 
[tex]d\tau[/tex] in this notation stands for [tex]d^3 r[/tex].
 
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