How Do You Solve Particle Motion Equations in an Electromagnetic Field?

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SUMMARY

The discussion focuses on solving particle motion equations in an electromagnetic field, specifically using the Lorentz force equation F=qE + qvxB for low velocities (v< PREREQUISITES

  • Understanding of the Lorentz force equation in electromagnetism
  • Familiarity with differential equations and their applications
  • Knowledge of vector calculus, particularly in three-dimensional space
  • Basic concepts of particle dynamics in electromagnetic fields
NEXT STEPS
  • Learn how to derive second-order differential equations from coupled first-order equations
  • Study the method of solving differential equations using substitution techniques
  • Explore numerical methods for solving particle motion in electromagnetic fields
  • Investigate the implications of varying magnetic and electric fields on particle trajectories
USEFUL FOR

Physics students, researchers in electromagnetism, and engineers working on particle dynamics in electromagnetic environments will benefit from this discussion.

akinoshigure
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So I'm stuck on the second part of this problem and really don't know hwere to go from here... let me type it up and show where I got stuck at.

3. The motion of particle of chage q in an electromagnetic field is governed by the Lorentz force (for low velocities v<<c): F=qE + qvxB.
With both constant B=B k and E=Ey j + Ez K show that:
z(t)=z(sub-o)+v(sub-zo)t+qE(sub-z)t^2/2m
vx(t)=Asin(omega-t)+E(sub-y)/B
vx(t)=+Acos(omega-t)

I did F=qE+qVxB=m (dv/dt)

dvx/dt= q/m(vyBz)
dvy/dt= q/m(Ey-vxBo)
dvz/dt= q/m (Ez)

I think I'm suppose to now take a second derivative and find the second order differential equation but I'm not too sure how to approach that.
 
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akinoshigure said:
So I'm stuck on the second part of this problem and really don't know hwere to go from here... let me type it up and show where I got stuck at.

3. The motion of particle of chage q in an electromagnetic field is governed by the Lorentz force (for low velocities v<<c): F=qE + qvxB.
With both constant B=B k and E=Ey j + Ez K show that:
z(t)=z(sub-o)+v(sub-zo)t+qE(sub-z)t^2/2m
vx(t)=Asin(omega-t)+E(sub-y)/B
vx(t)=+Acos(omega-t)

I did F=qE+qVxB=m (dv/dt)

dvx/dt= q/m(vyBz)
dvy/dt= q/m(Ey-vxBo)
dvz/dt= q/m (Ez)
One slight error here: the strength of the magnetic field is just "B", not
"Bz" or "Bo".

I think I'm suppose to now take a second derivative and find the second order differential equation but I'm not too sure how to approach that.
What you are "supposed" to do is solve those equations. Since the last one (for dvz/dt) does not involve the other two components, you can solve it directly. The other two are "entwined". One method of solving a pair of equations is to differentiate the first (so that you have dvy/dt on the right side) and then replace dvy/dt from the second equation. That will give you one second order differential equation for vx/
 

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