Understanding Griffith's Velocity Argument for Charge Integration

AI Thread Summary
Griffith's velocity argument in section 10.3.1 asserts that only one point along a particle's trajectory can affect a field point due to the constraint of light speed. If two points were involved, the particle's velocity component towards the field point would exceed the speed of light, which is not possible. The discussion highlights the relationship between distance and time in determining the particle's average speed, emphasizing that motion directly towards or away from the point maximizes distance change. A difference in distances, as discussed, can imply a required speed greater than light if not aligned with the original direction. The conversation concludes with a clarification on basic kinematics principles in the context of relativistic electrodynamics.
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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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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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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##?
 
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?
 
Which distance does ##\mathscr{r}_1-\mathscr{r}_2## represent?
 
schniefen said:
Which distance does ##\mathscr{r}_1-\mathscr{r}_2## represent?
A difference of two distances is not itself a distance.
 
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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##(3-1)/1=2## km/s. In this case then, ##\mathscr{r}_1-\mathscr{r}_2## does represent a distance, or?
 
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!
 
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Thanks for the replies. Clarified it.
 
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