Understanding Griffith's Velocity Argument for Charge Integration

In summary, Griffith argues that there can only ever be one point along the trajectory of the particle that “communicates” with the field point, and this would imply a speed of ##c##.
  • #1
schniefen
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Homework Statement
This regards section 10.3.1 in Griffith’s Introduction to electrodynamics, specifically the proof for why an extra factor is added when integrating the charge density when it depends on the retarded time.
Relevant Equations
Average speed: ##\frac{x_f-x_i}{t_f-t_i}##
In Griffith’s section 10.3.1, when proving why there is an extra factor in integrating over the charge density when it depends on the retarded time, he makes the argument that there can only ever be one point along the trajectory of the particle that “communicates” with the field point. Because if there were two such points, the component of the particles velocity towards ##\mathbf r## would be greater than the speed of light ##c##.

I don’t follow the geometric argument for this. How can one determine the velocity of the particle in a given direction?

The argument is that ##\mathscr{r}_1-\mathscr{r}_2 =c(t_2-t_1)## (where ##\mathscr{r}## is the magnitude of a scripted r). ##\mathbf{w}(t_r)## is the position of the particle at the retarded time. The times ##t_2,t_1## is the time it takes the light to travel the distances to ##\mathbf r##. How is this related to the average speed of the particle?

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  • #2
That seems like a fairly elementary argument. The way to maximise the change in distance from a point over a time ##t_2 - t_1## is to move directly towards or directly away from the point. That would, in this case, imply a speed of ##c##. If motion is not in that direction, then the speed would have to be ##> c##.
 
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  • #3
PeroK said:
That would, in this case, imply a speed of ##c##. If motion is not in that direction, then the speed would have to be ##> c##.
Makes sense. Why would it imply a speed of ##c##?
 
  • #4
schniefen said:
Makes sense. Why would it imply a speed of ##c##?
If you really have to, you could look at components of displacement and do some calculations, but it's elementary kinematics, surely?
 
  • #5
Which distance does ##\mathscr{r}_1-\mathscr{r}_2## represent?
 
  • #6
schniefen said:
Which distance does ##\mathscr{r}_1-\mathscr{r}_2## represent?
A difference of two distances is not itself a distance.
 
  • #7
Let me ask you this. If you are ## 1 km ## away from me, and one second later you need to be ##3km## away from me. What is the mininum speed you need?
 
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  • #8
##(3-1)/1=2## km/s. In this case then, ##\mathscr{r}_1-\mathscr{r}_2## does represent a distance, or?
 
  • #9
schniefen said:
##(3-1)/1=2## km/s. In this case then, ##\mathscr{r}_1-\mathscr{r}_2## does represent a distance, or?
Only if motion is in the same direction as the original displacement. If it's not, then you need a speed in excess of ##2 km/s##.

You really don't see this and can't do basic kinematics?

You're studying relativistic electrodynamics!
 
  • #10
Thanks for the replies. Clarified it.
 

1. What is Griffith's Velocity Argument for Charge Integration?

Griffith's Velocity Argument for Charge Integration is a mathematical method used in the field of electromagnetism to calculate the total charge within a given volume by integrating the velocity of the charge distribution over that volume.

2. Why is Griffith's Velocity Argument important in understanding charge integration?

Griffith's Velocity Argument is important because it provides a more accurate and comprehensive method for calculating the total charge within a given volume compared to other methods. It takes into account the velocity of the charge distribution, which is a crucial factor in many electromagnetism problems.

3. How does Griffith's Velocity Argument differ from other methods of charge integration?

Griffith's Velocity Argument differs from other methods of charge integration in that it considers the velocity of the charge distribution, while other methods may only take into account the charge density or the electric field. This makes it a more accurate and comprehensive method for calculating total charge within a given volume.

4. What are the limitations of Griffith's Velocity Argument?

One limitation of Griffith's Velocity Argument is that it assumes a steady-state situation, meaning that the charge distribution and velocity remain constant over time. It also assumes a continuous charge distribution, which may not always be the case in real-world scenarios.

5. How is Griffith's Velocity Argument used in practical applications?

Griffith's Velocity Argument is commonly used in practical applications such as calculating the total charge within a capacitor, determining the charge distribution on a conducting wire, and analyzing the electric field in a charged particle accelerator. It is also used in theoretical studies and simulations in the field of electromagnetism.

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