Motion in B Field: Deduce Conditions & Find Angle for x>b

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Homework Help Overview

The discussion revolves around a particle of mass m and charge +q moving in a uniform magnetic field B directed in the y-direction. The participants are tasked with deducing the conditions under which the particle can reach the region beyond x = b and determining the angle at which it will enter that region.

Discussion Character

  • Exploratory, Assumption checking, Mathematical reasoning

Approaches and Questions Raised

  • Some participants express confusion about why the particle would not reach the region x > b, questioning the role of the x-component of velocity and the effects of the magnetic field. Others suggest writing out the equations of motion in detail to clarify the situation.
  • There are attempts to derive conditions for the particle's motion, with various expressions for velocity and angle being proposed. Participants also explore different methods, including using the Larmor radius and solving differential equations.
  • Several participants question the correctness of their derived conditions and angles, seeking validation and clarification on their reasoning.

Discussion Status

The discussion is active, with multiple interpretations and approaches being explored. Participants are sharing their reasoning and calculations, while also questioning each other's conclusions. Some guidance has been offered regarding the use of the Larmor radius and the relationship between velocity and the particle's trajectory.

Contextual Notes

Participants are working under the constraints of a homework assignment, which may limit the information available and the assumptions they can make. There is an ongoing exploration of the implications of the magnetic field on the particle's motion and the conditions required for it to reach the specified region.

bon
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Homework Statement



In a particular experiment, a particle of mass m and charge +q moves with speed v along the x-axis towards increasing x. Between x = 0 and x = b there is a region of uniform magnetic flied B in the y-direction. Deduce the conditions under which the particle will reach the region x>b. In the even that it does reach this region, find an expression for the angle to the x-axis at which it will enter it.


Homework Equations





The Attempt at a Solution



I\'m struggling to understand why the particle wouldn't reach the region x>b! Surely it has an x-component of velocity v which is unchanged because the B field produces a perp force (i.e. in the z-direction) so the x-position would grow as x=vt..?
What am i missing? THanks!
 
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bon said:

Homework Statement



In a particular experiment, a particle of mass m and charge +q moves with speed v along the x-axis towards increasing x. Between x = 0 and x = b there is a region of uniform magnetic flied B in the y-direction. Deduce the conditions under which the particle will reach the region x>b. In the even that it does reach this region, find an expression for the angle to the x-axis at which it will enter it.


Homework Equations





The Attempt at a Solution



I\'m struggling to understand why the particle wouldn't reach the region x>b! Surely it has an x-component of velocity v which is unchanged because the B field produces a perp force (i.e. in the z-direction) so the x-position would grow as x=vt..?
What am i missing? THanks!
When the particle's velocity points along the x-axis the force points in the +z direction. But, what about when the velocity no longer points along the x-axis? You need to
write out the equations of motion in detail.

RGV
 
Aha. ok i see.

I work it out to be v > (qB/m)^2 b

is this right?

Thanks!
 
bon said:
Aha. ok i see.

I work it out to be v > (qB/m)^2 b

is this right?

Thanks!

Can you show your work for how you arrived at that answer?
 
ell from the eom you get

x\'\' = -qB/m z\'

and z\'\' = qB/m x\'

and then solving for x you get x\' = v- (qB/m)^2 x

and so we need x\'(b) to be greater than 0, hence the condition..

I\'m now trying to work out the angle though and am having problems..
 
For the angle i get tan theta = (qBb/m) / [v - b(qB/m)^2 ]

This seems too complicated! Have i gone wrong?
 
When I (or, rather, Maple) solve the DEs m*dvx/dt = -qB*vz and m*dvz/dt = qB*vx with vx(0)=v and vz(0)=0 I get a solution very different from yours. I then get a crossing condition different from yours, and a tangent of the crossing angle more complicated than yours.

Hint: try a solution of the form sin(w*t) and/or cos(w*t) for an appropriate w.

RGV
 
bon said:
ell from the eom you get

x\'\' = -qB/m z\'

and z\'\' = qB/m x\'

and then solving for x you get x\' = v- (qB/m)^2 x

and so we need x\'(b) to be greater than 0, hence the condition..

I\'m now trying to work out the angle though and am having problems..

bon said:
For the angle i get tan theta = (qBb/m) / [v - b(qB/m)^2 ]

This seems too complicated! Have i gone wrong?

Another way to approach the problem is to realize that the charged particle will trace a circular path due to the perpendicular magnetic field, and calculate the Lamor radius of that motion...

http://en.wikipedia.org/wiki/Larmor_radius

.
 
berkeman said:
Another way to approach the problem is to realize that the charged particle will trace a circular path due to the perpendicular magnetic field, and calculate the Lamor radius of that motion...

http://en.wikipedia.org/wiki/Larmor_radius

.

Ok thanks I've now seen where I went wrong.

I get x = v/w sin wt where w = qB/m

So the condition is v > qbB/m

is this right by any chance?

Thanks!
 
  • #10
I get the angle to be given by:

tan theta = cot[ arcsin(wb/v) ]
 
  • #11
bon said:
Ok thanks I've now seen where I went wrong.

I get x = v/w sin wt where w = qB/m

So the condition is v > qbB/m

is this right by any chance?

Thanks!

Drawing the circular orbit shows that r = b for the Lamor radius to keep the particle from going past b. But does the Lamor radius go up or down with velocity?
 
  • #12
But if x = v/w sin wt then x max = v/w

so it reaches it x max > b i.e. v > bw surely?

Also is my angle right?

thanks.
 
  • #13
bon said:
But if x = v/w sin wt then x max = v/w

so it reaches it x max > b i.e. v > bw surely?

Also is my angle right?

thanks.

Sorry, I'm not tracking your sin(wt) path -- I was just using the equation for the Lamor radius from the page I linked for you.
 
  • #14
hmm surely the same applies?

the radius gets bigger with v, so my equation is right?

Is the angle right also?
 
  • #15
bon said:
hmm surely the same applies?

the radius gets bigger with v, so my equation is right?

Is the angle right also?

Yes, the radius gets bigger with v. But in your answer above, you wrote "v > qbB/m" for containment...

I didn't check the angle -- if you could post a sketch, that would make it easier to check.

And please don't call me Shirley.
 
  • #16
No - I said v > ... for the particle to reach x>b, which is what the question asks! :S

And I didn\'t call you Shirley.
 
  • #17
bon said:
No - I said v > ... for the particle to reach x>b, which is what the question asks! :S

And I didn\'t call you Shirley.

Oh nuts, I misread the original question! So your solution is correct. Sorry I haven't checked the angle, but it's probably right since you understand what the orbit looks like.
 
  • #18
bon said:
I get the angle to be given by:

tan theta = cot[ arcsin(wb/v) ]

I've had time to look at the entry angle for cases when the orbit radius r > b. I get a simpler answer than you did, and different. For one thing, the mass m is not in your equation, but it affects the radius of the orbit. And w is not one of the fundamental things you are given in the problem, so your answer should probably be expressed in terms of m, B, q and v.

I used a sketch of the orbit and the x-y axes, and used the triangle that is formed by the radius of the orbit and the dimension b inside the orbit circle...
 

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