Particle in a mag field with linear drag

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Homework Help Overview

The problem involves a particle with mass and charge moving in a uniform magnetic field while experiencing linear drag. The original poster outlines a multi-part question requiring the application of the Lorentz force law and complex variable techniques to analyze the motion of the particle.

Discussion Character

  • Exploratory, Conceptual clarification, Mathematical reasoning

Approaches and Questions Raised

  • The original poster attempts to apply the Lorentz force law to derive equations of motion in the presence of drag. They express uncertainty about whether to incorporate time dependence in their equations or reserve that for a later part of the problem.

Discussion Status

Some participants are seeking assistance, while one participant claims to have resolved their confusion independently. The discussion reflects a mix of attempts to clarify concepts and share insights without reaching a definitive consensus.

Contextual Notes

The original poster expresses frustration with the structure of the problem, indicating that the linking of questions may complicate their understanding. There is also a mention of a specific technique discussed in class that is relevant to the solution.

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Homework Statement



A particle of mass m and electric charge q>0 is subject to a uniform, constant mag field of [tex]\vec{B} = B \hat{k}[/tex]. At t=0 its velocity vector is [tex]\hat{v}[/tex]naught which lies in the x-y plane. The particle is also subject to a linear drag force fd=-b[tex]\vec{v}[/tex]

a)Draw a free body diagram showing all the forces action on the particle. Use this to find expressions for F=ma in the x and y directions respectively, assuming that the force of gravity is negligible.

b) Use the equations from part a) and the complex variable technique discussed in class (see also taylor, section 2.5) to solve for the complex velocity n(t)= vx+ivy as a function of time, in terms of the initial condition [tex]\vec{v}[/tex]naught

c) use your solution to part b) to find an expression for the particle's speed as a function of time.

hate that my prof links the questions...


Homework Equations



[tex]\omega = \frac{qB}{m}[/tex]

ay = -[tex]\omega v_{x}[/tex]

ax = [tex]\omega v_{y}[/tex]

-bv = [tex]\beta Dv[/tex]


The Attempt at a Solution



Lorentz force law where E=0 qvxb = qB{i j k}{vx vy 0}{0 0 k}

=qB(vyi - vxj)


F = ma = qB(vyi - vxj) - b(vyi - vxj)

after some shuffling around dividing by mass subbing in ay and ax

[1-(b/m[tex]\omega[/tex])]*[ ay + ax ] = a

multiply by mass

F= ma = [m - (b/[tex]\omega[/tex])]* [ ay + ax ]

I'm not sure if i was supposed to make this a function of t or if that is with part b
 
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anyone have an idea?
 
ehild your a smart guy. want to help a guy out?
 
I figured it out, needed to clear my head and it was easy
 

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