Magnetic field motion different scenario

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Homework Help Overview

The discussion revolves around a physics problem involving a proton moving through a magnetic field. The scenario includes the proton's initial and final velocities, the direction of the magnetic field, and the effects of the magnetic force on the proton's motion.

Discussion Character

  • Exploratory, Conceptual clarification, Assumption checking

Approaches and Questions Raised

  • Participants express uncertainty about the initial setup and direction of the magnetic field. There are discussions about the application of the right-hand rule and its variations depending on the charge of the particle. Some participants attempt to clarify the relationship between the velocity, magnetic field, and force vectors.

Discussion Status

Participants are actively engaging with the problem, questioning assumptions, and exploring different interpretations of the right-hand rule. Some guidance has been offered regarding the need for diagrams and geometry to visualize the problem better. However, there is no explicit consensus on the correct approach or interpretation yet.

Contextual Notes

Participants note that the components of velocity may change while the speed remains constant. There is also mention of specific questions that need to be addressed regarding the radius of curvature, the y-coordinate of the proton upon exiting the magnetic field, and the z-component of the magnetic field.

woaname
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Homework Statement


A proton (q = 1.6 X 10-19 C, m = 1.67 X 10-27 kg) moving with constant velocity enters a region containing a constant magnetic field that is directed along the z-axis at (x,y) = (0,0) as shown. The magnetic field extends for a distance D = 0.7 m in the x-direction. The proton leaves the field having a velocity vector (vx, vy) = (3.1 X 105 m/s, 1.4 X 105 m/s).


Homework Equations





The Attempt at a Solution


i don't know how to even start this
 
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Can you post a picture?
 
sandy.bridge said:
Can you post a picture?

i can't even tell what direction the magnetic field is in
 

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You can discern the direction of the magnetic field the position of the particle before and after entering the magnetic field Remember, the force on a negative charge acts opposite in direction to the force on a positive charge.
 
so, B will point out of the screen, and F in positive y direction (initially).
i've tried using pytagoras' theorem to get a value for Vnet, but that would be for the exit velocity, not the velocity on entrance...?
 
No, B will not be out of the screen. Look at the image.
 

Attachments

  • 28_13A_Orbit_in_B_field.jpg
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is there an alternate version to the right hand rule? i pointed my index finger towards velocity vector, and the force vector inwards using my middle finger, which gave me the magnetic field pointing outward. i understand that the positioning would be different each time, but is there any particular way to "start" the right hand rule interpretation?
 
sandy.bridge said:
No, B will not be out of the screen. Look at the image.

using this picture, the magnetic field is represented by the middle finger. but before, in other questions, the direction of the thumb indicated the magnetic field. why does the representation change?
 
I have seen a couple variations to the rule. If you are not comfortable with it yet, I would stick to the one in your textbook. You want to ensure all three vectors are mutually perpendicular, and pointing a way from a common point (like an origin).
 
  • #10
woaname said:
using this picture, the magnetic field is represented by the middle finger. but before, in other questions, the direction of the thumb indicated the magnetic field. why does the representation change?

It depends on the sign of the charge. This charge is positive, the other is negative. The right hand rule works for positive charges. If the charge is negative, you have to visualize the vector pointing in the opposite direction that the right hand rule tells you.
 
  • #11
sandy.bridge said:
It depends on the sign of the charge. This charge is positive, the other is negative. The right hand rule works for positive charges. If the charge is negative, you have to visualize the vector pointing in the opposite direction that the right hand rule tells you.

OH! FLASHBACK! i just remembered an unconsciously learned moment from class. our prof actually DID say that negative and positive charges will change the RHR directions. thanks sandy.bridge for reminding me. won't forget it for my test tomorrow :D
 
  • #12
but getting back to the question, how do i get around solving the questions? so the velocity is towards positive x direction, force is towards positive y, and magnetic field is pointing into screen (negative z direction).
if i use a consolidated equation v = (rQB)/m , i have two unknowns.
 
  • #13
Note: the components of the velocity may change, however, the magnitude of the velocity (speed) will remain constant!
 
  • #14
i realized that i didn't post the questions that needed answering, so here they are:
1)What is R, the radius of curvature of the motion of the proton while it is in the region containing the magnetic field?
2)What is h, the y co-ordinate of the proton as it leaves the region conating the magnetic field?
3) What is Bz, the z-component of the magnetic field? Note that Bz is a signed number.

need a little guidance on how to solve them
 
  • #15
For starters, you should draw a diagram including any angles you know, along with the vectors for the velocity. You will have to use some geometry.
 
  • #16
sandy.bridge said:
For starters, you should draw a diagram including any angles you know, along with the vectors for the velocity. You will have to use some geometry.

i found θ=24 using arctan(vy/vx), and the trace of the radius with the center of the circle in the top left of the square, as the picture shows.
 

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  • #17
Your drawing is off. The velocity vector that you solved theta for will be tangent to the curve of the circle. The line connecting the center of the circle and the point both velocity components extend from will be perpendicular to the resultant velocity vector.
 

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