Time Derivatives of Vector Integrals in Griffiths E&M

In summary: What Griffiths and M are trying to say is that there's a current (or flux)of charge flowing through the region.The current is zero at the boundary because there is no flux going out of the region.
  • #1
ehrenfest
2,020
1

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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  • #2
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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  • #3
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?
 
  • #4
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.
 
  • #5
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?
 
  • #6
r is an integration variable.
Nothing outside the integral can affect it.
Go back to your calculus book on differentiating an integral.
 
  • #7
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.
 
  • #8
[tex]d\tau[/tex] in this notation stands for [tex]d^3 r[/tex].
 
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1. What is the definition of a vector integral in Griffiths E&M?

A vector integral in Griffiths E&M refers to the mathematical operation of integrating a vector quantity over a defined volume or surface in three-dimensional space. This is often used to calculate electric or magnetic fields in electromagnetic problems.

2. How is the time derivative of a vector integral defined in Griffiths E&M?

The time derivative of a vector integral in Griffiths E&M is calculated by taking the derivative of the integrand with respect to time, and then integrating over the same volume or surface as the original vector integral. This allows for the calculation of time-varying electric and magnetic fields.

3. What is the significance of the time derivative of a vector integral in Griffiths E&M?

The time derivative of a vector integral in Griffiths E&M is important because it allows for the calculation of time-varying electric and magnetic fields, which are essential in understanding and predicting electromagnetic phenomena. This is especially useful in applications such as circuit analysis and electromagnetic wave propagation.

4. How is the time derivative of a vector integral related to Maxwell's equations?

The time derivative of a vector integral is closely related to Maxwell's equations, as it allows for the calculation of time-varying electric and magnetic fields, which are described by these equations. Specifically, the time derivative of a vector integral is related to the time-dependent terms in the equations, such as the displacement current term in Ampere's law.

5. Can the time derivative of a vector integral be used in non-stationary problems?

Yes, the time derivative of a vector integral can be used in non-stationary problems, as it allows for the calculation of time-varying electric and magnetic fields. This is especially useful in problems where the electric and magnetic fields are changing over time, such as in electromagnetic wave propagation or in circuits with time-varying currents.

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