Electron in magnetic field and center of circumference

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SUMMARY

The discussion focuses on determining the center of the circular path of an electron moving in a uniform magnetic field B along the z-axis. The Lorentz force equation, $$L_F= qv×B$$, is utilized to derive the radius of the circular motion, given by $$R=\frac{mv}{qB}$$. Participants explore using velocity components to find the center coordinates (x_c, y_c) through relationships involving the velocities and the radius. The conclusion emphasizes that the center lies at a 90° angle to the direction of motion, specifically to the left of the electron's trajectory when viewed from above.

PREREQUISITES
  • Understanding of Lorentz force and its equation $$L_F= qv×B$$
  • Knowledge of circular motion dynamics and radius calculation $$R=\frac{mv}{qB}$$
  • Familiarity with vector mathematics, particularly orthogonal vectors
  • Basic proficiency in Euclidean distance calculations in 2D space
NEXT STEPS
  • Study the derivation and implications of the Lorentz force in electromagnetic fields
  • Learn about circular motion in magnetic fields and its applications in physics
  • Explore vector orthogonality and its applications in determining motion paths
  • Investigate the use of Euclidean distance in physics problems involving trajectories
USEFUL FOR

Physics students, educators, and professionals interested in electromagnetism, particularly those studying the motion of charged particles in magnetic fields.

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Homework Statement



We have an electron in 3D space in which there is also a magnetic uniform field B=Bz.
At t=0, we have z=0 and $v_z=0$.
We have to find the center of the circumference traveled by the electron using only x, y, v_x and v_y (coordinates and velocity of the electron at the general istant t) .

Homework Equations


$$L_F= qv×B$$ : this is the equation of Lorentz force.

The Attempt at a Solution


The first thing that I have done was finding the radius: $R=\frac{mv}{qB}$
Then, I have thought that I could obtain the center considering:

$$R_x= \frac{m \dot x}{qB} \rightarrow x-x_c=\frac{m \dot x}{qB} $$

$$R_y= \frac{m \dot y}{qB} \rightarrow y-y_c=\frac{m \dot y}{qB} $$

.. but probably this way is wrong.

And so I have thought to use Lorentz equation

$$F_{L,x}=q v_y B$$ $$ F_{L,y}=-q v_x B$$ $$F_{L,z}=0$$
but I don't know how I can obtain the center using this equation... what can I do?

Thank you so much!
 
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If the electron moves in some direction at t=0, where is the center of the circle? In the direction of motion, behind it, left*, right*, something in between?
*as seen from "above" (positive z), for example

How can you find a point in that direction with a distance of R?
 
mfb said:
If the electron moves in some direction at t=0, where is the center of the circle? In the direction of motion, behind it, left*, right*, something in between?
*as seen from "above" (positive z), for example

How can you find a point in that direction with a distance of R?

on the left? (negative charge move in anticlockwise..)

I have thought to use the euclidean distance between points, but I obtain only one relation and I don't obtain the coordinates of the center using the velocities.. can you help me? thanks a lot!
 
Hmm, let's view that from below, along the magnetic field. Ok, to the left, so at a 90°-angle to the direction of motion. Do you know how you can find an orthogonal line in 2 dimensions? The velocity components will help. And the euclidian distance will be used, too.
 
mfb said:
Hmm, let's view that from below, along the magnetic field. Ok, to the left, so at a 90°-angle to the direction of motion. Do you know how you can find an orthogonal line in 2 dimensions? The velocity components will help. And the euclidian distance will be used, too.

I'm not sure to have correctly understood your answer.

If I consider the line that have the direction of motion, I obtain
$$y-y_T=y'(x-x_T)$$

and the radius belongs to the line

$$y-y_T=-1/y'(x-x_T)$$

(y' is v_y, isn't it?)

and the euclidean distance between the position of the electron at generical istant t (x_T,y_T) and the center of the circumference (x_c,y_c) is

$$sqrt ((x_T-x_c)^2+(y_t-y_c)^2))=R$$

now I don't know what I have to do...
 
What is yT?

For simplicity, let's use x=y=0. You can add them afterwards.

If the velocity vector is (x',y'), can you find an orthogonal vector?
 
mfb said:
What is yT?

For simplicity, let's use x=y=0. You can add them afterwards.

If the velocity vector is (x',y'), can you find an orthogonal vector?

If the vector a=(a1,a2) si orthogonal to (x',y') then
a1*x'+a2*y'=0..
 
You can use this to generate some orthogonal vector. In 2 dimensions, there is a very nice way to chose a1 and a2.
 

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