Electron's response to a oscillating Electric field.

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SUMMARY

The discussion centers on the motion of an electron subjected to an oscillating electric field described by E = E0sin(ωt). The derived position function x(t) = (a0/ω)t - (a/ω)sin(ωt) indicates that the electron exhibits both linear and oscillatory motion. The linear term arises from the initial response to the electric field, while the oscillatory term reflects the continuous influence of the electric field over time. This dual behavior challenges intuitive expectations about charge motion in electric fields.

PREREQUISITES
  • Understanding of classical mechanics, particularly Newton's laws of motion.
  • Familiarity with electric fields and their effects on charged particles.
  • Knowledge of sinusoidal functions and their properties.
  • Basic grasp of oscillatory motion and inertia.
NEXT STEPS
  • Study the derivation of the Lorentz force law and its implications for charged particle motion.
  • Learn about the mathematical modeling of oscillatory systems in classical mechanics.
  • Investigate the concept of damping in oscillatory motion and its effects on charged particles.
  • Explore the role of initial conditions in the motion of particles under external forces.
USEFUL FOR

Physics students, educators, and anyone interested in the dynamics of charged particles in electric fields will benefit from this discussion.

Himanshu
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Homework Statement



The problem is to find the motion of the electron of charge -e and mass m which is initially at rest and which is suddenly subjected to an electric field E= E0sin(\omegat).

The following mathematical expression is safe and sound but I am having trouble with the Physics involved.x=(a0/\omega)t-(a/\omega)sin(\omegat).

where a0=-eE0/m.

The result x(t) is varying linearly as well as oscillating in time. This means that the electron is responding to the electric field in a manner which jiggling as well as drifting away.

That's against our intuition. A charge should respond in accordance to the electric field. So what is happening here.

My speculation is that the drifting motion is due to the inertia of the electron and that the motion was due to the initial electric field.
 
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Himanshu said:
The problem is to find the motion of the electron of charge -e and mass m which is initially at rest and which is suddenly subjected to an electric field E= E0sin(\omegat).

x=(a0/\omega)t-(a/\omega)sin(\omegat).

where a0=-eE0/m.

The result x(t) is varying linearly as well as oscillating in time. This means that the electron is responding to the electric field in a manner which jiggling as well as drifting away.

That's against our intuition

Hi Himanshu! :smile:

(have an omega: ω :smile:)

Why isn't it just (a0/ω)cos(ωt) ? :confused:
 
I cannot understand. How does the above expression appears? Can you please elaborate.
 
Don't mean to revive an old thread, but the physics behind this situation is confusing me as well. The acceleration is purely sinusoidal, varying with time, but the position somehow has a linear term in there as well as a sine. What's the physical explanation for this?
 

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