What is the Position Vector of an Electron Moving in a Helix?

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Homework Help Overview

The problem involves an electron moving in a helical path, described by a position vector that incorporates relativistic effects. Participants are tasked with finding the position vector in a different reference frame, determining the central frequency of emitted radiation, and calculating the angular distribution of that radiation.

Discussion Character

  • Exploratory, Conceptual clarification, Problem interpretation

Approaches and Questions Raised

  • Participants discuss using Lorentz transformations to find the position vector in a moving reference frame, noting that the electron's motion simplifies to circular in that frame. Questions arise regarding the meaning of "central frequency" and how to calculate it, as well as the significance of time variables in the equations.

Discussion Status

Some participants have offered guidance on approaching the calculation of the central frequency by suggesting transformations between reference frames. There is ongoing clarification about terminology and the implications of specific terms used in the context of the problem.

Contextual Notes

Participants are navigating potential ambiguities in terminology, such as "central frequency" versus "peak frequency," and are referencing specific sections of a textbook for clarification. The problem context includes relativistic effects and the need for transformations between different frames of reference.

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Homework Statement



An electron moves in a helix : [tex]\vec{r}(t)=v_{z}t \hat{z}+a e^{i\omega_{0}t}(\hat{x}-i\hat{y})[/tex], where [tex]a[/tex] is the radius of the helix and [tex]v_{z}[/tex] the relativistic z-component of the velocity.
1) Find the position vector of the electron in a system of reference that is moving with velocity [tex]v_{z}\hat{z}[/tex]
2) Find the central frequency of radiation that the electron emits in the [tex]\hat{z}[/tex] direction in the laboratory reference frame.
3)Calculate the angular distribution of the power of radiation, [tex]\frac{dP(t')}{d\Omega}[/tex]


Homework Equations



Jackson 3rd edition, chapter 14 (par. 14.4)


The Attempt at a Solution



1) is easy, just a lorentz transformation to find [tex]\vec{r}'(t')[/tex]. It turns out that in the moving frame [tex]\vec{r}'(t')[/tex] has no z-component. So in that frame it actually moves in a circle rather than a helix.


For 2)I have no idea.

3)I can maybe calculate [tex]\frac{dP(t')}{d\Omega}[/tex] from equation 14.38 but I am not sure


Any ideas? Especially for 2)...
 
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For 2), what about calculating in the frame from 1), and then transforming to the lab frame?

For 3), why is the t primed?
 
turin,

2) yes but what does "central frequency" means and how do I calculate it?

3) If you check Jackson (3rd edition page 668), t' refers to the moving particle's own time.
 
I thought that central frequency would just mean peak frequency. However, after reading Chapter 14, I didn't see the term "central frequency" used once. Maybe I missed it. Or maybe "critical frequency". I don't know. If I had to solve this problem, I would assume peak frequency.
 
You are right, it's just peak frequency
 

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