What is the current I in a wire that repels an electron at a certain distance?

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Homework Help Overview

The discussion revolves around determining the current in a straight wire that repels an electron approaching it at a specific angle and distance. The problem involves concepts from electromagnetism and mechanics, particularly the forces acting on charged particles in magnetic fields.

Discussion Character

  • Exploratory, Conceptual clarification, Mathematical reasoning, Problem interpretation

Approaches and Questions Raised

  • Participants explore various methods to relate kinetic energy and work done on the electron as it moves in the presence of the wire's magnetic field. There are attempts to express the velocity components and magnetic field interactions mathematically. Some participants question the validity of decomposing kinetic energy into components, while others suggest using Newton's laws and the Lorentz force to analyze the problem.

Discussion Status

The discussion is active, with multiple approaches being explored. Some participants have proposed specific equations and methods, while others have raised concerns about the assumptions made in these approaches. There is no explicit consensus, but various lines of reasoning are being examined.

Contextual Notes

Participants note the complexity of the problem and the challenges in integrating the equations due to the changing variables involved, such as the velocity of the electron and the magnetic field strength. There are references to the need for careful consideration of the forces acting on the electron and the implications of averaging values in non-linear scenarios.

happy thoughts
there is a sraight wire carrying current i. an electron is approaching the wire, in the same plane as the wire, at a 45 degree angle with velocity v0 when it is a distance r0 from the wire. the electron makes it to a distance of rf from the wire before it is repelled away. what is i?

I was thinking that I know that K.E.=Me(v0*sin(45))/2 initially in the y direction (this would be the y-component of K) if y is taken as the coordinate perpendicular to the wire and x the one parallel to the wire. K.E.=0 once the electron is at a distance of rf. I also know that Work=integral Fdr in the y direction.

so here is an equation that should work:

K.E.=Me*v0*sin(45)/2=[inte][e*vx*mu0*i/(2*pi*r)]dr from r=r0 to r=rf

e=charge of electron
mu0=permeability of free space
vx=x-component of velocity
i=current I'm trying to solve for
r=dist. from wire

the problem is that i can't figure out a way to express vx as a function of r so that i can integrate this.

somebody help!

thanks, rick.
 
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that makes great sense- the force is perpendicular to the direction of motion. I am thinking though: the particle does move in the y direction and there is a force component in the y direction- so it seems that there is some work done when considering the y component only even though there is obviously no net work done. could it be that one might imagine some work done in the y direction when doing calculations. this would imply that the work done in the x direction is exactly negative of the work in the y direction. does that make sense at all?
 
just in case anyone is interested, here is a nasty solution that works:

1) find an average B between r0 and rf

(1/ro-rf)*mu0*i*ln(rf/r0)/(2*pi)

2) find an average vx

vx(1+1/sqrt(2))/2

3) use the work idea above, namely

[inte]Fdr where F=q*vx*B

if anyone knows the better and easier approach to this problem please let me know.
 
Why not use Newton'w Law?
(I'm too lazy to fill in all the constants, so it's just a rough sketch)

Lorentz force is: F = v x B
Newton says: v x B = a

Since vz = Bx = By = 0, this boils down to:

I. vy Bz = ax
II. -vx Bz = ay.

Now, let's write Bz = -c/y, where c is a measure of the field's strength that we want to find. Then,

I. cy'/y = x''
This integrates to
c ln(y) = x'
Now, as Ambitwistor pointed out, in the final state, x' = v0. Thus
c ln(rf/r0) = v0 - vx0, or
c = (v0-vx0) / ln(rf/r0).

As I said, just a sketch.
 
Originally posted by happy thoughts
I was thinking that I know that K.E.=Me(v0*sin(45))/2 initially in the y direction (this would be the y-component of K) if y is taken as the coordinate perpendicular to the wire and x the one parallel to the wire. K.E.=0 once the electron is at a distance of rf.

This approach won't work. KE is not a vector with x and y components. KE is a scalar. As arcnets said, just use F=ma. F definitely can be decomposed into x and y components.

just in case anyone is interested, here is a nasty solution that works: 1) find an average B between r0 and rf (1/ro-rf)*mu0*i*ln(rf/r0)/(2*pi) 2) find an average vx vx(1+1/sqrt(2))/2

This is a naive approach to say the least. One cannot hope to solve a non-linear problem of this nature by taking averages.

Use arcnets approach. Or if you want to be fancier, derive the vector potential and use the fact that the x-component of the canonical momentum is conserved.
 
This is a naive approach to say the least.

thanks for the "friendly encouragement" Bruno... 8=* !

As it turns out, after doing the correct approach, the averaged approach turns out to be exactly what it was for the correct approach, but only in the case of an initial 45 degree angle (lucky me):

if you draw a line through the particle parallel to the wire and let the angle between that line and the velocity vector be [the],

Fy=q*v*B*sin([the])

vy=v*sin([the])

*********************************************************

F=m*a

(q*v*[mu]0*i*cos([the])/(2[pi]*y)=m*d/dt(vy)

solve for i here and you get an equivilent expression in the case of [the]initial=[pi]/4
 
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